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.. _examples-linac-segment: | ||
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PIP-II Linac Segment | ||
======================= | ||
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This example illustrates a small segment of the PIP-II linac, which includes the last RF cavity in the MEBT section (a quarter-wave resonator cavity for longitudinal bunching) and the first | ||
RF cavity in the succeeding cryomodule (a superconducting half-wave resonator for acceleration). | ||
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For simplicity, aperture restrictions have been removed, and there are no active kickers. RF cavity and solenoid field maps are represented using the Fourier coefficients of the longitudinal fields on-axis. | ||
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The nominal beam current is 4.845 mA (29.83 pC at 162.5 MHz), which assumes ~3% beam loss relative to the 5 mA current entering the MEBT. | ||
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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_linac_segment.py`` or | ||
* ImpactX **executable** using an input file: ``impactx input_linac_segment.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_linac_segment.py | ||
:language: python3 | ||
:caption: You can copy this file from ``examples/linac_segment/run_linac_segment.py``. | ||
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.. tab-item:: Executable: Input File | ||
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.. literalinclude:: input_linac_segment.in | ||
:language: ini | ||
:caption: You can copy this file from ``examples/linac_segment/input_linac_segment.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_linac_segment.py`` | ||
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.. literalinclude:: analysis_linac_segment.py | ||
:language: python3 | ||
:caption: You can copy this file from ``examples/linac_segment/analysis_linac_segment.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 | ||
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) | ||
last_step = list(series.iterations)[-1] | ||
initial = series.iterations[1].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 = 2.2e12 * 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], | ||
[ | ||
7.5451170454175073e-005, | ||
7.5441588239210947e-005, | ||
9.9775878164077539e-004, | ||
1.9959540393751392e-009, | ||
2.0175015289132990e-009, | ||
2.0013820193294972e-006, | ||
], | ||
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 = 2.2e12 * 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], | ||
[ | ||
7.4790118496224206e-005, | ||
7.5357525169680140e-005, | ||
9.9775879288128088e-004, | ||
1.9959539836392703e-009, | ||
2.0175014668882125e-009, | ||
2.0013820380883801e-006, | ||
], | ||
rtol=rtol, | ||
atol=atol, | ||
) |
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