scripts/CharmJet.ipynb

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   "id": "cc0d9320-c971-4574-99b9-b101c2e3e62d",
   "metadata": {
    "tags": []
   },
   "outputs": [],
   "source": [
    "import coffea\n",
    "import coffea.processor as processor\n",
    "import hist\n",
    "\n",
    "import awkward as ak\n",
    "import numpy as np\n",
    "import matplotlib.pyplot as plt"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 2,
   "id": "32f20eb2-3a48-4361-954c-047bbbef0421",
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    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_83.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_159.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_143.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_140.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_134.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_132.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_141.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_155.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_149.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_138.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_145.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_162.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_151.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_133.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_164.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_161.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_136.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_152.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_163.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_158.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_146.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_150.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_147.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_135.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_137.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_139.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_144.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_157.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_223.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_128.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_99.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_165.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_153.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_130.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_58.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_63.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_54.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_67.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_60.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_64.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_61.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_56.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_50.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_68.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_65.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_55.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_59.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_53.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_48.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_69.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_71.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_49.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_74.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_78.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_76.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_81.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_87.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_89.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_79.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_75.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_73.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_178.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_208.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_90.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_92.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_100.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_93.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_174.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_101.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_173.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_94.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_176.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_177.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_211.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_185.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_181.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_180.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_182.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_80.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_95.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_102.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_105.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_107.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_103.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_183.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_104.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_110.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_109.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_114.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_116.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_108.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_187.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_106.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_111.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_188.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_122.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_113.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_118.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_184.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_117.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_119.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_121.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_190.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_186.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_192.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_191.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_189.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_196.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_193.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_195.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_131.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_120.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_127.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_197.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_194.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_198.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_199.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_222.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_202.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_167.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_166.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_201.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_203.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_200.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_312.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_168.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_207.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_226.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_220.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_217.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_285.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_209.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_221.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_215.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_229.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_205.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_224.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_210.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_213.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_218.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_214.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_231.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_219.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_225.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_338.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_230.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_227.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_232.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_237.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_206.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_234.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_235.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_236.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_212.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_233.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_228.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_216.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_339.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_171.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_238.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_169.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_172.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_170.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_239.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_337.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_344.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_265.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_262.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_336.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_346.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_263.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_274.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_304.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_275.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_271.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_276.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_273.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_272.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_277.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_281.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_279.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_292.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_297.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_315.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_298.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_290.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_341.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_299.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_307.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_300.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_204.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_302.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_301.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_343.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_310.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_291.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_311.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_309.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_313.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_308.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_316.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_320.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_317.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_322.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_323.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_326.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_330.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_324.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_328.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_321.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_327.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_342.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_325.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_331.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_329.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_332.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_334.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_335.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_333.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_348.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_349.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_241.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_340.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_240.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_4.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_250.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_242.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_347.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_248.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_350.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_247.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_345.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_243.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_244.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_249.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_246.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_351.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_251.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_252.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_255.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_253.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_254.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_257.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_259.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_258.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_356.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_352.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_256.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_260.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_264.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_266.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_267.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_269.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_270.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_5.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-51.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_355.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_358.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_245.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_261.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_278.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-50.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_280.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_283.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_282.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_286.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_288.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_284.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_353.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_295.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_289.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_293.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_287.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_294.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_296.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_359.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-44.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_360.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_361.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_364.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_363.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_362.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-45.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-48.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-47.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-49.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-14.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_365.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_366.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-1.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_369.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-46.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_305.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-7.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-42.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_368.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_367.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_372.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-43.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_371.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_370.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_303.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_306.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_375.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_376.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-34.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_373.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_377.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_378.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_318.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-40.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-41.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-11.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-5.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_383.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-4.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_314.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-35.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_379.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-38.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-9.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-36.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-37.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_381.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-39.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_384.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_319.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-6.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-10.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_380.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-12.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-2.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-13.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-8.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-16.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_387.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-17.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_386.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-32.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_42.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_392.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-24.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_389.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_390.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-25.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-18.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-28.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-26.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_388.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-27.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_394.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-30.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-3.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_393.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_354.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-19.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-20.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-15.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_395.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-53.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_399.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-21.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-33.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-55.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_402.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_397.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_396.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_398.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_411.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_409.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_404.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_400.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_405.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_414.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_407.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_401.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_410.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_406.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_412.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_413.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-54.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_416.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_419.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-23.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_415.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-52.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_421.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_432.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_423.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_435.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-31.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_420.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_436.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_444.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_445.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_452.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_450.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_408.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_1-29.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_461.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_470.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_472.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_385.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_469.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_471.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_473.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_475.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_480.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_479.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_476.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_481.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_477.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_391.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_482.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_483.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_486.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_474.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_487.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_488.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_492.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_490.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_491.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_489.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_493.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_403.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_495.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_497.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_496.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_417.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_418.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_422.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_433.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_430.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_425.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_427.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_426.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_431.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_424.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_429.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_439.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_501.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_500.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_437.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_428.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_438.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_441.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_442.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_498.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_443.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_434.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_440.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_446.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_447.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_448.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_502.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_509.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_506.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_504.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_508.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_456.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_513.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_505.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_451.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_507.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_515.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_514.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_503.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_517.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_453.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_516.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_510.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_511.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-21.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_512.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_454.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_460.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_455.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-20.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_462.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_457.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_499.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_466.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_518.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_458.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_520.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_459.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_464.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_463.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_468.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_465.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_521.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_522.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_467.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_519.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_525.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_523.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_524.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-13.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-12.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_527.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_530.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-22.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-17.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_529.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_526.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_531.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-14.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-9.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-10.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-11.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_478.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-25.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-2.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-1.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-16.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-23.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-30.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-4.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-26.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-24.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-27.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_485.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_484.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_532.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-28.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-15.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-6.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_534.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_535.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_553.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_550.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_547.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_528.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_546.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-18.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_549.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_545.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_542.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_552.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_537.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_543.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_544.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_382.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-19.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-7.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_540.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-3.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-5.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_562.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_555.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-8.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_2-29.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_494.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_556.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_538.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_536.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_541.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_558.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_560.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_559.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_565.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_533.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_539.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_548.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_551.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_564.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_268.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_561.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_563.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_554.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-1.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-31.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-25.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-5.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-19.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-6.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-13.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-7.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-10.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-8.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-11.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-9.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-14.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-17.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-26.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-28.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-15.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-27.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-2.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-20.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-30.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-23.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-3.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-18.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-16.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-12.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-4.root',\n",
    "                     #'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-21.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-24.root']}"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 157,
   "id": "f2640ec9-b497-45b8-8b24-a17fe4ed55e3",
   "metadata": {},
   "outputs": [],
   "source": [
    "fileset = {'ttbar': ['root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_17.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_9.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_10.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_7.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_15.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_19.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_11.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_14.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_12.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_16.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_20.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_24.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_32.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_27.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_35.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_125.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_6.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_8.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_18.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_30.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_31.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_25.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_28.root',\n",
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    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-14.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-17.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-26.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-28.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-15.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-27.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-2.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-20.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-30.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-23.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-3.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-18.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-16.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-12.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-4.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-21.root',\n",
    "                     'root://xcache//store/group/phys_top/byates/PFNano/TTToSemiLeptonic_TuneCP5_13TeV-powheg-pythia8/RunIISummer20UL16MiniAODv2-106X_mcRun2_asymptotic_v17-v1_PFtestNano/230420_165513/0000/nano_mc2017_ULv2_3-24.root']}"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 4,
   "id": "41015a28-6af4-4443-b7f5-88b6cf85e99c",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      "/opt/conda/lib/python3.8/site-packages/distributed/client.py:1288: VersionMismatchWarning: Mismatched versions found\n",
      "\n",
      "+---------+----------------+----------------+----------------+\n",
      "| Package | client         | scheduler      | workers        |\n",
      "+---------+----------------+----------------+----------------+\n",
      "| python  | 3.8.16.final.0 | 3.8.16.final.0 | 3.8.15.final.0 |\n",
      "+---------+----------------+----------------+----------------+\n",
      "  warnings.warn(version_module.VersionMismatchWarning(msg[0][\"warning\"]))\n"
     ]
    }
   ],
   "source": [
    "from dask.distributed import Client\n",
    "\n",
    "client = Client(\"tls://localhost:8786\")"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 5,
   "id": "76cddc5d-848a-4c01-ac0a-6257b8dc37c8",
   "metadata": {
    "tags": []
   },
   "outputs": [],
   "source": [
    "def is_ttbar(jets, bjets, leptons):\n",
    "        jets_pt = ak.fill_none(ak.pad_none(jets.pt, 1), 0)\n",
    "        leps_pt  = ak.fill_none(ak.pad_none(leptons.pt, 1), 0)\n",
    "        \n",
    "        jets_eta = ak.fill_none(ak.pad_none(jets.eta, 1), 0)\n",
    "        leps_eta  = ak.fill_none(ak.pad_none(leptons.eta, 1), 0)\n",
    "        \n",
    "        nJets = ak.num(jets)\n",
    "        nBJets = ak.num(bjets)\n",
    "        nLep = ak.num(leptons)\n",
    "        jpt30 = jets_pt[:,0] > 30\n",
    "        lpt25 = (leps_pt[:,0] > 25)\n",
    "        jeta24 = abs(jets_eta) < 2.4\n",
    "        leta24 = abs(leps_eta) < 2.4\n",
    "        #is_ttbar = (ak.num(jets)>4)&(ak.num(bjets_tight)>1)&((ak.num(ele)>1)|(ak.num(mu)>1))# & (pad_jets[:,0].pt>30)# & ((pad_ele[:,0].pt>25) | (pad_mu[:,0].pt>25))#&(ht>180)\n",
    "        return (nJets >= 1) & (nBJets >=1) & (nLep >= 1) & jpt30 & lpt25# & jeta24 & leta24"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 6,
   "id": "e2b87400-3112-451b-8ad6-f61bf17b2f26",
   "metadata": {
    "tags": []
   },
   "outputs": [],
   "source": [
    "class Processor(processor.ProcessorABC):\n",
    "    def __init__(self):\n",
    "        self.mass_bins = np.linspace(1.7, 2.0, 30)\n",
    "        self.xb_bins = np.linspace(0, 1, 11)\n",
    "\n",
    "        dataset_axis = hist.axis.StrCategory(name=\"dataset\", label=\"\", categories=[], growth=True)\n",
    "        # Split data into 50 bins, ranging from 0 to 100.\n",
    "        jpt_axis = hist.axis.Regular(name=\"j0pt\", label=\"Leading jet $p_{\\mathrm{T}}$ [GeV]\", bins=50, start=0, stop=300)\n",
    "        bpt_axis = hist.axis.Regular(name=\"b0pt\", label=\"Leading b jet $p_{\\mathrm{T}}$ [GeV]\", bins=50, start=0, stop=300)\n",
    "        lpt_axis = hist.axis.Regular(name=\"l0pt\", label=\"Leading lepotn $p_{\\mathrm{T}}$ [GeV]\", bins=50, start=0, stop=100)\n",
    "        D0pt_axis= hist.axis.Regular(name=\"D0pt\", label=\"Leading D0 $p_{\\mathrm{T}}$ [GeV]\", bins=50, start=0, stop=100)\n",
    "        D0pipt_axis= hist.axis.Regular(name=\"D0pipt\", label=\"Leading D0 pi $p_{\\mathrm{T}}$ [GeV]\", bins=50, start=0, stop=100)\n",
    "        D0kpt_axis= hist.axis.Regular(name=\"D0kpt\", label=\"Leading D0 k $p_{\\mathrm{T}}$ [GeV]\", bins=50, start=0, stop=100)\n",
    "        xb_axis  = hist.axis.Regular(name=\"xb\",   label=\"$x_{\\mathrm{b}}$\", bins=10, start=0, stop=1)\n",
    "        xb_ch_axis  = hist.axis.Regular(name=\"xb_ch\",   label=\"$x_{\\mathrm{b}} \\Sigma p_{\\mathrm{T}}^{\\mathrm{charged}}$\", bins=10, start=0, stop=1)\n",
    "        HT_axis  = hist.axis.Regular(name=\"HT\",   label=\"$H_{\\mathrm{T}}$\", bins=50, start=0, stop=1000)\n",
    "        pdgid_axis= hist.axis.Regular(name=\"pdgid\",   label=\"D0 id's\", bins=10, start=0, stop=250)\n",
    "        d0_axis  = hist.axis.Regular(name='d0',   label=\"$d_0$\", bins=10, start=0, stop=100)\n",
    "        njets_axis = hist.axis.Regular(name='njets', label='$N_{\\mathrm{jets}}$', bins=10, start=0, stop=10)\n",
    "        nbjets_axis = hist.axis.Regular(name='nbjets', label='$N_{\\mathrm{b-jets}}$', bins=10, start=0, stop=10)\n",
    "        nleps_axis = hist.axis.Regular(name='nleps', label='$N_{\\mathrm{leps}}$', bins=10, start=0, stop=10)\n",
    "        mass_axis = hist.axis.Regular(name='d0_mass', label='D0 mass [GeV]', bins=30, start=self.mass_bins[0], stop=self.mass_bins[-1])\n",
    "        mass_tag_axis = hist.axis.Regular(name='d0_mu_mass', label='D0 mu-tag mass [GeV]', bins=30, start=self.mass_bins[0], stop=self.mass_bins[-1])\n",
    "        mass_axes = [hist.axis.Regular(name=f'd0_{int(xb_bin*10)}', label='D0 mass [GeV] (' + str(round(self.xb_bins[ibin], 2)) + ' < $x_{\\mathrm{b}}$ < ' + str(round(self.xb_bins[ibin+1], 2)) + ')', bins=30, start=1.7, stop=2.0) for ibin,xb_bin in enumerate(self.xb_bins[:-1])]\n",
    "        self.output = processor.dict_accumulator({\n",
    "            'j0pt': hist.Hist(dataset_axis, jpt_axis),\n",
    "            'b0pt': hist.Hist(dataset_axis, bpt_axis),\n",
    "            'l0pt': hist.Hist(dataset_axis, lpt_axis),\n",
    "            'D0pt': hist.Hist(dataset_axis, D0pt_axis),\n",
    "            'D0pipt': hist.Hist(dataset_axis, D0pipt_axis),\n",
    "            'D0kpt': hist.Hist(dataset_axis, D0kpt_axis),\n",
    "            'xb'  : hist.Hist(dataset_axis, xb_axis),\n",
    "            'xb_ch'  : hist.Hist(dataset_axis, xb_ch_axis),\n",
    "            'HT'  : hist.Hist(dataset_axis, HT_axis),\n",
    "            'pdgid'  : hist.Hist(dataset_axis, pdgid_axis),\n",
    "            'd0'  : hist.Hist(dataset_axis, d0_axis),\n",
    "            'njets' : hist.Hist(dataset_axis, njets_axis),\n",
    "            'nbjets' : hist.Hist(dataset_axis, nbjets_axis),\n",
    "            'nleps' : hist.Hist(dataset_axis, nleps_axis),\n",
    "            'd0_mass': hist.Hist(dataset_axis, mass_axis),\n",
    "            'd0_mu_mass': hist.Hist(dataset_axis, mass_tag_axis),\n",
    "            # FIXME make these dynamically\n",
    "            'd0_0' : hist.Hist(dataset_axis, mass_axes[0]),\n",
    "            'd0_1' : hist.Hist(dataset_axis, mass_axes[1]),\n",
    "            'd0_2' : hist.Hist(dataset_axis, mass_axes[2]),\n",
    "            'd0_3' : hist.Hist(dataset_axis, mass_axes[3]),\n",
    "            'd0_4' : hist.Hist(dataset_axis, mass_axes[4]),\n",
    "            'd0_5' : hist.Hist(dataset_axis, mass_axes[5]),\n",
    "            'd0_6' : hist.Hist(dataset_axis, mass_axes[6]),\n",
    "            'd0_7' : hist.Hist(dataset_axis, mass_axes[7]),\n",
    "            'd0_8' : hist.Hist(dataset_axis, mass_axes[8]),\n",
    "            'd0_9' : hist.Hist(dataset_axis, mass_axes[9]),\n",
    "            #'d0_10' : hist.Hist(dataset_axis, mass_axes[10]),\n",
    "        })\n",
    "    \n",
    "    def process(self, events):\n",
    "        dataset = events.metadata[\"dataset\"]\n",
    "        #events = events[events.is_ttbar]\n",
    "        jets = events.Jet\n",
    "        ele  = events.Electron\n",
    "        mu   = events.Muon\n",
    "        leptons = ak.with_name(ak.concatenate([ele, mu], axis=1), 'PtEtaPhiMCandidate')\n",
    "        leptons = leptons[ak.argsort(leptons.pt, axis=1)][::-1]\n",
    "        \n",
    "        '''\n",
    "        jets_pt = ak.fill_none(ak.pad_none(jets.pt, 1), 0)\n",
    "        ele_pt  = ak.fill_none(ak.pad_none(ele.pt, 1), 0)\n",
    "        mu_pt   = ak.fill_none(ak.pad_none(mu.pt, 1), 0)\n",
    "        \n",
    "        jets_eta = ak.fill_none(ak.pad_none(jets.eta, 1), 0)\n",
    "        ele_eta  = ak.fill_none(ak.pad_none(ele.eta, 1), 0)\n",
    "        mu_eta   = ak.fill_none(ak.pad_none(mu.eta, 1), 0)\n",
    "        '''\n",
    "        \n",
    "        loose = 0.1355\n",
    "        medium = 0.4506\n",
    "        tight = 0.7738\n",
    "        is_bjets_tight = jets['btagDeepFlavB'] > tight\n",
    "        bjets_tight = ak.pad_none(jets[is_bjets_tight], 1)\n",
    "        events['is_ttbar'] = is_ttbar(jets, bjets_tight, leptons)\n",
    "        ht = ak.sum(jets.pt, axis=-1)\n",
    "        j0pt = ak.fill_none(ak.pad_none(jets.pt, 1), 0)[:,0]\n",
    "        l0pt = ak.fill_none(ak.pad_none(ak.pad_none(leptons.pt, 1), -1)[:,0], -1)\n",
    "        b0pt = ak.fill_none(bjets_tight.pt[:,0], -1)\n",
    "        \n",
    "        # Charm meson candidates from b-jets\n",
    "        charm_cand = events.BToCharm\n",
    "        chi2_mask = (charm_cand.chi2 < 5) & (charm_cand.svprob>0.02)\n",
    "        b_mask = jets[charm_cand.jetIdx].btagDeepFlavB > tight\n",
    "        d0 = charm_cand[chi2_mask & b_mask & (charm_cand.jetIdx>-1)]\n",
    "        d0mass = ak.fill_none(ak.flatten(d0.fit_mass[events.is_ttbar]), -1)\n",
    "        xb = ak.fill_none(ak.flatten((d0.fit_pt / jets[d0.jetIdx].pt)[events.is_ttbar]), -1)\n",
    "\n",
    "        binned_masses = [d0mass[(xb > low) & (xb < high)] for low,high in zip(self.xb_bins[:-1], self.xb_bins[1:])]\n",
    "        self.output['j0pt'].fill(dataset=dataset, j0pt=j0pt[events.is_ttbar])\n",
    "        self.output['b0pt'].fill(dataset=dataset, b0pt=b0pt[events.is_ttbar])\n",
    "        self.output['l0pt'].fill(dataset=dataset, l0pt=l0pt[events.is_ttbar])\n",
    "        self.output['njets'].fill(dataset=dataset, njets=ak.num(jets[events.is_ttbar]))\n",
    "        self.output['nbjets'].fill(dataset=dataset, nbjets=ak.num(bjets_tight[events.is_ttbar]))\n",
    "        self.output['nleps'].fill(dataset=dataset, nleps=ak.num(leptons[events.is_ttbar]))\n",
    "        self.output['HT'].fill(dataset=dataset, HT=ht)\n",
    "        #self.output['D0pt'].fill(dataset=dataset, D0pt=d0pt)\n",
    "        self.output['xb'].fill(dataset=dataset, xb=xb)\n",
    "        #self.output['xb_ch'].fill(dataset=dataset, xb_ch=xb_ch[events.is_ttbar])\n",
    "        #self.output['d0'].fill(dataset=dataset, d0=d0_imp)\n",
    "        self.output['d0_mass'].fill(dataset=dataset, d0_mass=d0mass)\n",
    "        # mu_tag is at jet level, cartesian associates each PF in a jet with the jet-level flag\n",
    "        #d0_tag, is_tag = ak.unzip(ak.cartesian([d0_mass, mu_tag]))\n",
    "        #self.output['d0_mu_mass'].fill(dataset=dataset, d0_mu_mass=ak.fill_none(ak.flatten(d0_tag[is_tag]), 0))\n",
    "        for ibin in range(len(self.xb_bins)-1):\n",
    "            self.output[f'd0_{ibin}'].fill(**{'dataset': dataset, f'd0_{ibin}': binned_masses[ibin]})\n",
    "        '''\n",
    "        # FIXME make these dynamically\n",
    "        self.output['d0_0'].fill(dataset=dataset, d0_0=binned_masses[0])\n",
    "        self.output['d0_1'].fill(dataset=dataset, d0_1=binned_masses[1])\n",
    "        self.output['d0_2'].fill(dataset=dataset, d0_2=binned_masses[2])\n",
    "        self.output['d0_3'].fill(dataset=dataset, d0_3=binned_masses[3])\n",
    "        self.output['d0_4'].fill(dataset=dataset, d0_4=binned_masses[4])\n",
    "        self.output['d0_5'].fill(dataset=dataset, d0_5=binned_masses[5])\n",
    "        self.output['d0_6'].fill(dataset=dataset, d0_6=binned_masses[6])\n",
    "        self.output['d0_7'].fill(dataset=dataset, d0_7=binned_masses[7])\n",
    "        self.output['d0_8'].fill(dataset=dataset, d0_8=binned_masses[8])\n",
    "        #self.output['d0_9'].fill(dataset=dataset, d0_9=binned_masses[9])\n",
    "        '''\n",
    "        #self.output['D0pipt'].fill(dataset=dataset, D0pipt=d0pi_lead_pt)\n",
    "        #self.output['D0kpt'].fill(dataset=dataset, D0kpt=d0pi_lead_pt)\n",
    "        return self.output\n",
    "\n",
    "    def postprocess(self, accumulator):\n",
    "        return accumulator"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "d6c64196-bad1-4d6f-9396-836e2cf6233d",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "[#########                               ] | 24% Completed |  8min 40.0ss"
     ]
    }
   ],
   "source": [
    "output = processor.run_uproot_job(fileset=fileset, \n",
    "                       treename=\"Events\",\n",
    "                       processor_instance=Processor(),\n",
    "                       executor=processor.dask_executor,\n",
    "                       executor_args={'client': client, 'schema': processor.NanoAODSchema},\n",
    "                       chunksize=50000)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 21,
   "id": "5e2dfc74-f065-4fd7-bd54-681fa863cb20",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7f605ee21fd0>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 21,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['d0_mass'].plot1d()\n",
    "#output['d0_mu_mass'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 10,
   "id": "af445b73-5bd3-48c7-acd4-93ee4d8cb3ec",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "<matplotlib.legend.Legend at 0x7fbc77ab88e0>"
      ]
     },
     "execution_count": 10,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['njets'].plot1d(label='njets')\n",
    "output['nbjets'].plot1d(label='nbjets')\n",
    "output['nleps'].plot1d(label='nleps')\n",
    "plt.legend()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 11,
   "id": "7d5a7064-66c6-42cf-8959-53526999af4a",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "<matplotlib.legend.Legend at 0x7fb872e81a30>"
      ]
     },
     "execution_count": 11,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['l0pt'].plot1d(label='l0 pt')\n",
    "output['j0pt'].plot1d(label='j0 pt')\n",
    "plt.legend()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 12,
   "id": "b2e466af-faba-45f2-891c-fa02bb8af5d4",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872c9e430>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 12,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['HT'].plot1d(label='HT')"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 13,
   "id": "4593df1d-07c3-4916-9a11-fd5cfe8d087a",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872b7ab50>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 13,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "#output['j0pt'].plot1d()\n",
    "output['b0pt'].plot1d()\n",
    "output['D0pt'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 14,
   "id": "48f3b24d-ba04-4f45-9a25-b0efc10b5a75",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872b0ab20>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 14,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['xb'].plot1d()\n",
    "output['xb_ch'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 15,
   "id": "cf8759fd-8136-4b72-b234-db94fb54e5f0",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872a6f880>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 15,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['HT'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 16,
   "id": "23b546ba-3148-4cc9-a6b4-e55a8cbff425",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872a18280>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 16,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['pdgid'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 17,
   "id": "bba3eb5a-c329-4820-b25c-46776fbb91b0",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872959610>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 17,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['d0'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 18,
   "id": "b0d91840-0cf7-489e-97ee-ef28b1009ff1",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "dict_keys(['j0pt', 'b0pt', 'l0pt', 'D0pt', 'D0pipt', 'D0kpt', 'xb', 'xb_ch', 'HT', 'pdgid', 'd0', 'njets', 'nbjets', 'nleps', 'd0_mass', 'd0_mu_mass', 'd0_0', 'd0_1', 'd0_2', 'd0_3', 'd0_4', 'd0_5', 'd0_6', 'd0_7', 'd0_8', 'd0_9'])"
      ]
     },
     "execution_count": 18,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "output.keys()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 19,
   "id": "9752e4a3-6631-4280-9091-efeab3373ac0",
   "metadata": {
    "tags": []
   },
   "outputs": [],
   "source": [
    "import matplotlib.pyplot as plt"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 42,
   "id": "4ff866b1-b734-4573-a0f0-cb34a39388c4",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "array([0. , 0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1. ])"
      ]
     },
     "execution_count": 42,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "xb_bins = np.linspace(0, 1, 11)\n",
    "#output['d0_1'].plot1d(label='d0_1')\n",
    "#output['d0_2'].plot1d(label='d0_2')\n",
    "#output['d0_3'].plot1d(label='d0_3')\n",
    "#output['d0_4'].plot1d(label='d0_4')\n",
    "#output['d0_5'].plot1d(label='d0_5')\n",
    "#output['d0_6'].plot1d(label='d0_6')\n",
    "#output['d0_7'].plot1d(label='d0_7')\n",
    "#output['d0_8'].plot1d(label='d0_8')\n",
    "for ibin in range(len(xb_bins)-1):\n",
    "    key = f'd0_{ibin}'\n",
    "    if 'd0_' in key and len(output[key].view()) != 0 and 'd0_' in key and 'mass' not in key:\n",
    "    #if 'd0_' in key and 'd0_9' not in key:\n",
    "        output[key].plot1d(label=f'{xb_bins[ibin]:.2f}' + ' < $x_{b}$ < ' + f'{xb_bins[ibin+1]:.2f}')\n",
    "plt.legend()\n",
    "xb_bins"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 21,
   "id": "9c1876df-bc9e-422c-8089-487d7f3ad394",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "[StairsArtists(stairs=<matplotlib.patches.StepPatch object at 0x7fb872882a60>, errorbar=None, legend_artist=None)]"
      ]
     },
     "execution_count": 21,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "output['d0_mu_mass'].plot1d()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 22,
   "id": "05f879ec-cf5d-480b-be12-e9f8be2f2753",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/html": [
       "<html>\n",
       "<div style=\"display:flex; align-items:center;\">\n",
       "<div style=\"width:290px;\">\n",
       "<svg xmlns=\"http://www.w3.org/2000/svg\" viewBox=\"-10 -105 270 120\">\n",
       "<line x1=\"-5\" y1=\"0\" x2=\"255\" y2=\"0\" style=\"fill:none;stroke-width:2;stroke:currentColor\"/>\n",
       "<text text-anchor=\"middle\" x=\"0\" y=\"15\" style=\"fill:currentColor;\">\n",
       "0\n",
       "</text>\n",
       "<text text-anchor=\"middle\" x=\"250\" y=\"15\" style=\"fill:currentColor;\">\n",
       "1\n",
       "</text>\n",
       "<text text-anchor=\"middle\" x=\"125.0\" y=\"15\" style=\"fill:currentColor;\">\n",
       "$x_{\\mathrm{b}}$\n",
       "</text>\n",
       "<polyline points=\"  0,0   0,-100  25,-100  25,-23  50,-23  50,-8.21  75,-8.21  75,-2.7 100,-2.7 100,-1.66 125,-1.66 125,-1.05 150,-1.05 150,-0.42 175,-0.42 175,-0.291 200,-0.291 200,-0.21 225,-0.21 225,-0.0646 250,-0.0646 250,0\" style=\"fill:none; stroke:currentColor;\"/>\n",
       "</svg>\n",
       "</div>\n",
       "<div style=\"flex=grow:1;\">\n",
       "Regular(10, 0, 1, name='xb', label='$x_{\\\\mathrm{b}}$')<br/>\n",
       "<hr style=\"margin-top:.2em; margin-bottom:.2em;\"/>\n",
       "Double() Σ=8527.0 <em>(1638758.0 with flow)</em>\n",
       "\n",
       "</div>\n",
       "</div>\n",
       "</html>"
      ],
      "text/plain": [
       "Hist(Regular(10, 0, 1, name='xb', label='$x_{\\\\mathrm{b}}$'), storage=Double()) # Sum: 8527.0 (1638758.0 with flow)"
      ]
     },
     "execution_count": 22,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "output['xb'][{'dataset': sum}][0:len(output['xb'].axes['xb'].edges)]"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 146,
   "id": "b99c63b5-7067-4283-861f-929a551474a5",
   "metadata": {
    "tags": []
   },
   "outputs": [],
   "source": [
    "def d0_mass_fit(mass, mean, sigma, nsig, mean_kk, sigma_kk, nkk, mean_pp, sigma_pp, npp, l, nbkg):\n",
    "    return \\\n",
    "    nsig * np.exp(-1/2 * (np.square(mass - mean) / np.square(sigma))) + \\\n",
    "    nkk  * np.exp(-1/2 * (np.square(mass - mean_kk) / np.square(sigma_kk))) + \\\n",
    "    npp  * np.exp(-1/2 * (np.square(mass - mean_pp) / np.square(sigma_pp))) + \\\n",
    "    nbkg * np.exp(l * mass)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 149,
   "id": "2512d74c-9680-4ca4-a9af-240f4e50ee42",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "N D0 104 +/- 1023136, N bkg 0 +/- 0\n",
      "N D0 38 +/- 25, N bkg 0 +/- 0\n",
      "N D0 95 +/- 17, N bkg 0 +/- 0\n",
      "N D0 53 +/- 45, N bkg 0 +/- 0\n",
      "N D0 24 +/- 6, N bkg 0 +/- 0\n",
      "N D0 18 +/- 3, N bkg 0 +/- 0\n",
      "N D0 11 +/- 2, N bkg 0 +/- 0\n",
      "N D0 7 +/- 1575446, N bkg 0 +/- 0\n",
      "N D0 1 +/- 0, N bkg 0 +/- 0\n",
      "N D0 0 +/- 0, N bkg 0 +/- 0\n"
     ]
    },
    {
     "data": {
      "text/plain": [
       "<matplotlib.legend.Legend at 0x7f6054f89d00>"
      ]
     },
     "execution_count": 149,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "from scipy.optimize import curve_fit\n",
    "\n",
    "mass_bins = np.linspace(1.7, 2.0, 31)\n",
    "d0_mean0, d0_sigma0, nd0, kk_mean0, kk_sigma0, nkk, pp_mean0, pp_sigma0, npp, l0, ne0 = 1.87, .01, 1, 1.78, 0.02, 100, 1.9, 0.02, 10, -2.27, 30\n",
    "xb_mass = []\n",
    "for ibin in range(len(xb_bins)-1):\n",
    "    h = output[f'd0_{ibin}'].values()[0]\n",
    "    plt.step(mass_bins[:-1], h, label=f'D0 {ibin}')\n",
    "    g = [d0_mass_fit(x, d0_mean0, d0_sigma0, nd0, kk_mean0, kk_sigma0, nkk, pp_mean0, pp_sigma0, npp, l0, ne0) for x in mass_bins]\n",
    "    popt, pcov = curve_fit(d0_mass_fit, mass_bins[:-1], h, p0=[d0_mean0, d0_sigma0, nd0, kk_mean0, kk_sigma0, nkk, pp_mean0, pp_sigma0, npp, l0, ne0], bounds=([1.85, 0, 0, 1.77, 0, 0, 1.88, 0, 0, -10, 0], [1.88, .02, 1000, 1.79, .02, 100, 1.91, .02, 10, 10, 10000]))\n",
    "    plt.plot(mass_bins, d0_mass_fit(mass_bins, *popt), label=f'Fit {i}')\n",
    "    #print(*popt)\n",
    "    #print({name: round(val,2) for name,val in zip(('D0 mean', 'D0 width', 'N D0', 'lambda', 'N bkg'), popt)})\n",
    "    print(f'N D0 {round(popt[2])} +/- {round(np.sqrt(pcov[2][2]))}, N bkg {round(popt[4])} +/- {round(np.sqrt(pcov[4][4]))}')\n",
    "    xb_mass.append(popt[2])\n",
    "plt.legend()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 134,
   "id": "d00fa010-bfd0-49b9-80a5-37ab94e0752c",
   "metadata": {
    "tags": []
   },
   "outputs": [
    {
     "data": {
      "text/plain": [
       "<matplotlib.legend.Legend at 0x7f6052da88e0>"
      ]
     },
     "execution_count": 134,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "xb_center = [np.average([low, high]) for low,high in zip(xb_bins[:-1], xb_bins[1:])]\n",
    "plt.step(x=xb_bins[:-1], y=xb_mass, label='$x_{\\mathrm{b}}$ signal')\n",
    "plt.legend()"
   ]
  }
 ],
 "metadata": {
  "kernelspec": {
   "display_name": "Python 3 (ipykernel)",
   "language": "python",
   "name": "python3"
  },
  "language_info": {
   "codemirror_mode": {
    "name": "ipython",
    "version": 3
   },
   "file_extension": ".py",
   "mimetype": "text/x-python",
   "name": "python",
   "nbconvert_exporter": "python",
   "pygments_lexer": "ipython3",
   "version": "3.8.16"
  },
  "toc-autonumbering": false,
  "toc-showcode": false,
  "toc-showmarkdowntxt": false,
  "toc-showtags": false
 },
 "nbformat": 4,
 "nbformat_minor": 5
}