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openPMD Beam Input via Source
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.. _examples-solenoid-restart: | ||
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Solenoid channel (Restart) | ||
========================== | ||
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This is the same example as the :ref:`proton beam undergoing 90 deg X-Y rotation in an ideal solenoid channel <examples-solenoid>`, but it restarts the resulting beam and rotates it another 3 channel periods to the initial X-Y conditions. | ||
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The solenoid magnetic field corresponds to B = 2 T. | ||
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The second moments of the transverse particle distribution after the solenoid channel are rotated by 90 (start) + 270 = 360 degrees: the final transverse moments should coincide with the | ||
initial transverse moments to within the level expected due to noise due to statistical sampling. | ||
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In this test, the initial and final values of :math:`\sigma_x`, :math:`\sigma_y`, :math:`\sigma_t`, :math:`\epsilon_x`, :math:`\epsilon_y`, and :math:`\epsilon_t` must agree with nominal values. | ||
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Run | ||
--- | ||
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This example can be run **either** as: | ||
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* **Python** script: ``python3 run_solenoid.py`` or | ||
* ImpactX **executable** using an input file: ``impactx input_solenoid.in`` | ||
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For `MPI-parallel <https://www.mpi-forum.org>`__ runs, prefix these lines with ``mpiexec -n 4 ...`` or ``srun -n 4 ...``, depending on the system. | ||
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.. tab-set:: | ||
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.. tab-item:: Python: Script | ||
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.. literalinclude:: run_solenoid.py | ||
:language: python3 | ||
:caption: You can copy this file from ``examples/solenoid_restart/run_solenoid.py``. | ||
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.. tab-item:: Executable: Input File | ||
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.. literalinclude:: input_solenoid.in | ||
:language: ini | ||
:caption: You can copy this file from ``examples/solenoid_restart/input_solenoid.in``. | ||
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Analyze | ||
------- | ||
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We run the following script to analyze correctness: | ||
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.. dropdown:: Script ``analysis_solenoid.py`` | ||
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.. literalinclude:: analysis_solenoid.py | ||
:language: python3 | ||
:caption: You can copy this file from ``examples/solenoid_restart/analysis_solenoid.py``. |
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#!/usr/bin/env python3 | ||
# | ||
# Copyright 2022-2023 ImpactX contributors | ||
# Authors: Axel Huebl, Chad Mitchell | ||
# License: BSD-3-Clause-LBNL | ||
# | ||
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import numpy as np | ||
import openpmd_api as io | ||
from scipy.stats import moment | ||
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def get_moments(beam): | ||
"""Calculate standard deviations of beam position & momenta | ||
and emittance values | ||
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Returns | ||
------- | ||
sigx, sigy, sigt, emittance_x, emittance_y, emittance_t | ||
""" | ||
sigx = moment(beam["position_x"], moment=2) ** 0.5 # variance -> std dev. | ||
sigpx = moment(beam["momentum_x"], moment=2) ** 0.5 | ||
sigy = moment(beam["position_y"], moment=2) ** 0.5 | ||
sigpy = moment(beam["momentum_y"], moment=2) ** 0.5 | ||
sigt = moment(beam["position_t"], moment=2) ** 0.5 | ||
sigpt = moment(beam["momentum_t"], moment=2) ** 0.5 | ||
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epstrms = beam.cov(ddof=0) | ||
emittance_x = (sigx**2 * sigpx**2 - epstrms["position_x"]["momentum_x"] ** 2) ** 0.5 | ||
emittance_y = (sigy**2 * sigpy**2 - epstrms["position_y"]["momentum_y"] ** 2) ** 0.5 | ||
emittance_t = (sigt**2 * sigpt**2 - epstrms["position_t"]["momentum_t"] ** 2) ** 0.5 | ||
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return (sigx, sigy, sigt, emittance_x, emittance_y, emittance_t) | ||
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# initial/final beam | ||
series = io.Series("diags/openPMD/monitor.h5", io.Access.read_only) | ||
first_step = list(series.iterations)[0] | ||
last_step = list(series.iterations)[-1] | ||
initial = series.iterations[first_step].particles["beam"].to_df() | ||
final = series.iterations[last_step].particles["beam"].to_df() | ||
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# compare number of particles | ||
num_particles = 10000 | ||
assert num_particles == len(initial) | ||
assert num_particles == len(final) | ||
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print("Initial Beam:") | ||
sigx, sigy, sigt, emittance_x, emittance_y, emittance_t = get_moments(initial) | ||
print(f" sigx={sigx:e} sigy={sigy:e} sigt={sigt:e}") | ||
print( | ||
f" emittance_x={emittance_x:e} emittance_y={emittance_y:e} emittance_t={emittance_t:e}" | ||
) | ||
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atol = 0.0 # ignored | ||
rtol = 1.3 * num_particles**-0.5 # from random sampling of a smooth distribution | ||
print(f" rtol={rtol} (ignored: atol~={atol})") | ||
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assert np.allclose( | ||
[sigx, sigy, sigt, emittance_x, emittance_y, emittance_t], | ||
[ | ||
2.205510139392e-3, | ||
1.559531175539e-3, | ||
6.404930308742e-3, | ||
2.0e-6, | ||
1.0e-6, | ||
1.0e-6, | ||
], | ||
rtol=rtol, | ||
atol=atol, | ||
) | ||
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print("") | ||
print("Final Beam:") | ||
sigx, sigy, sigt, emittance_x, emittance_y, emittance_t = get_moments(final) | ||
print(f" sigx={sigx:e} sigy={sigy:e} sigt={sigt:e}") | ||
print( | ||
f" emittance_x={emittance_x:e} emittance_y={emittance_y:e} emittance_t={emittance_t:e}" | ||
) | ||
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atol = 0.0 # ignored | ||
rtol = 2.3 * num_particles**-0.5 # from random sampling of a smooth distribution | ||
print(f" rtol={rtol} (ignored: atol~={atol})") | ||
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assert np.allclose( | ||
[sigx, sigy, emittance_x, emittance_y, emittance_t], | ||
[ | ||
1.559531175539e-3, | ||
2.205510139392e-3, | ||
1.0e-6, | ||
2.0e-6, | ||
1.0e-6, | ||
], | ||
rtol=rtol, | ||
atol=atol, | ||
) |
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############################################################################### | ||
# Reference Particle | ||
############################################################################### | ||
beam.kin_energy = 250.0 | ||
beam.particle = proton | ||
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# ignored | ||
beam.charge = 1.0e-9 | ||
beam.units = static | ||
beam.distribution = empty | ||
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############################################################################### | ||
# Beamline: lattice elements and segments | ||
############################################################################### | ||
lattice.elements = source monitor sols monitor | ||
lattice.nslice = 1 | ||
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source.type = source | ||
source.distribution = openPMD | ||
source.openpmd_path = "../solenoid/diags/openPMD/monitor.h5" | ||
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monitor.type = beam_monitor | ||
monitor.backend = h5 | ||
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sol1.type = solenoid | ||
sol1.ds = 3.820395 | ||
sol1.ks = 0.8223219329893234 | ||
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sols.type = line | ||
sols.elements = sol1 | ||
sols.repeat = 3 | ||
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############################################################################### | ||
# Algorithms | ||
############################################################################### | ||
algo.particle_shape = 2 | ||
algo.space_charge = false | ||
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############################################################################### | ||
# Diagnostics | ||
############################################################################### | ||
diag.slice_step_diagnostics = true |
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Original file line number | Diff line number | Diff line change |
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#!/usr/bin/env python3 | ||
# | ||
# Copyright 2022-2023 ImpactX contributors | ||
# Authors: Marco Garten, Axel Huebl, Chad Mitchell | ||
# License: BSD-3-Clause-LBNL | ||
# | ||
# -*- coding: utf-8 -*- | ||
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from impactx import ImpactX, elements, push | ||
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sim = ImpactX() | ||
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# set numerical parameters and IO control | ||
sim.particle_shape = 2 # B-spline order | ||
sim.space_charge = False | ||
# sim.diagnostics = False # benchmarking | ||
sim.slice_step_diagnostics = True | ||
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# domain decomposition & space charge mesh | ||
sim.init_grids() | ||
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# load a 250 MeV proton beam with an initial | ||
# horizontal rms emittance of 1 um and an | ||
# initial vertical rms emittance of 2 um | ||
kin_energy_MeV = 250.0 # reference energy | ||
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# reference particle | ||
pc = sim.particle_container() | ||
ref = pc.ref_particle() | ||
ref.set_charge_qe(1.0).set_mass_MeV(938.27208816).set_kin_energy_MeV(kin_energy_MeV) | ||
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# load particle bunch from file | ||
push(pc, elements.Source("openPMD", "../solenoid.py/diags/openPMD/monitor.h5")) | ||
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# add beam diagnostics | ||
monitor = elements.BeamMonitor("monitor", backend="h5") | ||
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# design the accelerator lattice | ||
sol1 = elements.Sol(name="sol1", ds=3.820395, ks=0.8223219329893234) | ||
sim.lattice.append(monitor) | ||
sim.lattice.extend([sol1] * 3) | ||
sim.lattice.append(monitor) | ||
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# run simulation | ||
sim.track_particles() | ||
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# clean shutdown | ||
sim.finalize() |
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Original file line number | Diff line number | Diff line change |
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PRIVATE | ||
Aperture.cpp | ||
Programmable.cpp | ||
Source.cpp | ||
) | ||
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add_subdirectory(diagnostics) |
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I skipped the
sigt
comparison here because I did not know the final value after a total of 4 solenoids and there seems to be some dispersion.There was a problem hiding this comment.
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From Slack: