forked from BLAST-ImpactX/impactx
-
Notifications
You must be signed in to change notification settings - Fork 0
Commit
This commit does not belong to any branch on this repository, and may belong to a fork outside of the repository.
- Loading branch information
Showing
4 changed files
with
297 additions
and
0 deletions.
There are no files selected for viewing
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,49 @@ | ||
.. _examples-alignment: | ||
|
||
Quadrupole with Alignment Errors | ||
================================ | ||
|
||
A 2 GeV proton beam propagates through a single quadrupole with 3 mm horizontal misalignment and 30 degree rotation error. | ||
|
||
The first and second moments of the particle distribution before and after the quadrupole should coincide with | ||
analytical predictions, to within the level expected due to noise due to statistical sampling. | ||
|
||
In this test, the initial and final values of :math:`\mu_x`, :math:`\mu_y`, :math:`\sigma_x`, :math:`\sigma_y`, | ||
:math:`\sigma_t`, :math:`\epsilon_x`, :math:`\epsilon_y`, and :math:`\epsilon_t` must agree with nominal values. | ||
|
||
|
||
Run | ||
--- | ||
|
||
This example can be run **either** as: | ||
|
||
* **Python** script: ``python3 run_alignment.py`` or | ||
* ImpactX **executable** using an input file: ``impactx input_alignment.in`` | ||
|
||
For `MPI-parallel <https://www.mpi-forum.org>`__ runs, prefix these lines with ``mpiexec -n 4 ...`` or ``srun -n 4 ...``, depending on the system. | ||
|
||
.. tab-set:: | ||
|
||
.. tab-item:: Python: Script | ||
|
||
.. literalinclude:: run_alignment.py | ||
:language: python3 | ||
:caption: You can copy this file from ``examples/alignment/run_alignment.py``. | ||
|
||
.. tab-item:: Executable: Input File | ||
|
||
.. literalinclude:: input_alignment.in | ||
:language: ini | ||
:caption: You can copy this file from ``examples/alignment/input_alignment.in``. | ||
|
||
|
||
Analyze | ||
------- | ||
|
||
We run the following script to analyze correctness: | ||
|
||
.. dropdown:: Script ``analysis_alignment.py`` | ||
|
||
.. literalinclude:: analysis_alignment.py | ||
:language: python3 | ||
:caption: You can copy this file from ``examples/alignment/analysis_alignment.py``. |
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,137 @@ | ||
#!/usr/bin/env python3 | ||
# | ||
# Copyright 2022-2023 ImpactX contributors | ||
# Authors: Axel Huebl, Chad Mitchell | ||
# License: BSD-3-Clause-LBNL | ||
# | ||
|
||
|
||
import numpy as np | ||
import openpmd_api as io | ||
from scipy.stats import moment, tmean | ||
|
||
|
||
def get_moments(beam): | ||
"""Calculate standard deviations of beam position & momenta | ||
and emittance values | ||
Returns | ||
------- | ||
meanx, meany, sigx, sigy, sigt, emittance_x, emittance_y, emittance_t | ||
""" | ||
meanx = tmean(beam["position_x"]) | ||
meany = tmean(beam["position_y"]) | ||
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 | ||
|
||
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 | ||
|
||
return (meanx, meany, sigx, sigy, sigt, emittance_x, emittance_y, emittance_t) | ||
|
||
|
||
# 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() | ||
|
||
# compare number of particles | ||
num_particles = 100000 | ||
assert num_particles == len(initial) | ||
assert num_particles == len(final) | ||
|
||
print("Initial Beam:") | ||
meanx, meany, sigx, sigy, sigt, emittance_x, emittance_y, emittance_t = get_moments( | ||
initial | ||
) | ||
print(f" meanx={meanx:e} meany={meany:e}") | ||
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}" | ||
) | ||
|
||
atol = 3.0 * num_particles ** (-0.5) * sigx | ||
print(f" atol~={atol}") | ||
|
||
assert np.allclose( | ||
[meanx, meany], | ||
[ | ||
0.0, | ||
0.0, | ||
], | ||
atol=atol, | ||
) | ||
|
||
atol = 0.0 # ignored | ||
rtol = 1.8 * num_particles**-0.5 # from random sampling of a smooth distribution | ||
print(f" rtol={rtol} (ignored: atol~={atol})") | ||
|
||
assert np.allclose( | ||
[sigx, sigy, sigt, emittance_x, emittance_y, emittance_t], | ||
[ | ||
1.160982600086e-3, | ||
1.160982600086e-3, | ||
1.0e-3, | ||
6.73940299e-7, | ||
6.73940299e-7, | ||
2.0e-6, | ||
], | ||
rtol=rtol, | ||
atol=atol, | ||
) | ||
|
||
|
||
print("") | ||
print("Final Beam:") | ||
meanx, meany, sigx, sigy, sigt, emittance_x, emittance_y, emittance_t = get_moments( | ||
final | ||
) | ||
print(f" meanx={meanx:e} meany={meany:e}") | ||
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}" | ||
) | ||
|
||
|
||
atol = 3.0 * num_particles ** (-0.5) * sigx | ||
print(f" atol~={atol}") | ||
|
||
assert np.allclose( | ||
[meanx, meany], | ||
[ | ||
1.79719761842e-4, | ||
3.24815908981e-4, | ||
], | ||
atol=atol, | ||
) | ||
|
||
atol = 0.0 # ignored | ||
rtol = 3.0 * num_particles**-0.5 # from random sampling of a smooth distribution | ||
print(f" rtol={rtol} (ignored: atol~={atol})") | ||
|
||
assert np.allclose( | ||
[sigx, sigy, sigt, emittance_x, emittance_y, emittance_t], | ||
[ | ||
1.2372883901369e-3, | ||
1.3772750218080e-3, | ||
1.027364e-03, | ||
7.39388142e-7, | ||
7.39388142e-7, | ||
2.0e-6, | ||
], | ||
rtol=rtol, | ||
atol=atol, | ||
) |
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,47 @@ | ||
############################################################################### | ||
# Particle Beam(s) | ||
############################################################################### | ||
beam.npart = 100000 | ||
beam.units = static | ||
beam.kin_energy = 2.0e3 | ||
beam.charge = 1.0e-9 | ||
beam.particle = proton | ||
beam.distribution = waterbag | ||
beam.sigmaX = 1.16098260008648811e-3 | ||
beam.sigmaY = 1.16098260008648811e-3 | ||
beam.sigmaT = 1.0e-3 | ||
beam.sigmaPx = 0.580491300043e-3 | ||
beam.sigmaPy = 0.580491300043e-3 | ||
beam.sigmaPt = 2.0e-3 | ||
beam.muxpx = 0.0 | ||
beam.muypy = 0.0 | ||
beam.mutpt = 0.0 | ||
|
||
|
||
############################################################################### | ||
# Beamline: lattice elements and segments | ||
############################################################################### | ||
lattice.elements = monitor quad_err monitor | ||
lattice.nslice = 1 | ||
|
||
monitor.type = beam_monitor | ||
monitor.backend = h5 | ||
|
||
quad_err.type = quad | ||
quad_err.ds = 1.0 | ||
quad_err.k = 0.25 | ||
quad_err.dx = 0.003 | ||
quad_err.rotation = 30.0 | ||
|
||
|
||
############################################################################### | ||
# Algorithms | ||
############################################################################### | ||
algo.particle_shape = 2 | ||
algo.space_charge = false | ||
|
||
|
||
############################################################################### | ||
# Diagnostics | ||
############################################################################### | ||
diag.slice_step_diagnostics = true |
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,64 @@ | ||
#!/usr/bin/env python3 | ||
# | ||
# Copyright 2022-2023 ImpactX contributors | ||
# Authors: Axel Huebl, Chad Mitchell | ||
# License: BSD-3-Clause-LBNL | ||
# | ||
# -*- coding: utf-8 -*- | ||
|
||
import amrex.space3d as amr | ||
from impactx import ImpactX, RefPart, distribution, elements | ||
|
||
sim = ImpactX() | ||
|
||
# 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 | ||
|
||
# domain decomposition & space charge mesh | ||
sim.init_grids() | ||
|
||
# load a 2 GeV electron beam with an initial | ||
# unnormalized rms emittance of 2 nm | ||
kin_energy_MeV = 2.0e3 # reference energy | ||
bunch_charge_C = 1.0e-9 # used with space charge | ||
npart = 100000 # number of macro particles | ||
|
||
# reference particle | ||
ref = sim.particle_container().ref_particle() | ||
ref.set_charge_qe(1.0).set_mass_MeV(0.510998950).set_kin_energy_MeV(kin_energy_MeV) | ||
|
||
# particle bunch | ||
distr = distribution.Waterbag( | ||
sigmaX=1.16098260008648811e-3, | ||
sigmaY=1.16098260008648811e-3, | ||
sigmaT=1.0e-3, | ||
sigmaPx=0.580491300043e-3, | ||
sigmaPy=0.580491300043e-3, | ||
sigmaPt=2.0e-3, | ||
muxpx=0.0, | ||
muypy=0.0, | ||
mutpt=0.0, | ||
) | ||
sim.add_particles(bunch_charge_C, distr, npart) | ||
|
||
# add beam diagnostics | ||
monitor = elements.BeamMonitor("monitor", backend="h5") | ||
|
||
# design the accelerator lattice) | ||
ns = 1 # number of slices per ds in the element | ||
lattice = [ | ||
monitor, | ||
elements.Quad(ds=1.0, k=0.25, dx=0.003, dy=0.0, rotation=30.0, nslice=ns), | ||
monitor, | ||
] | ||
sim.lattice.extend(lattice) | ||
|
||
# run simulation | ||
sim.evolve() | ||
|
||
# clean shutdown | ||
del sim | ||
amr.finalize() |