Expanding Beam in Free Space
A coasting bunch expanding freely in free space under its own space charge.
We use a cold (zero emittance) 250 MeV electron bunch whose initial distribution is a uniformly-populated 3D ball of radius R0 = 1 mm when viewed in the bunch rest frame.
In the laboratory frame, the bunch is a uniformly-populated ellipsoid, which expands to twice its original size. This is tested using the second moments of the distribution.
In this test, the initial and final values of \(\sigma_x\), \(\sigma_y\), \(\sigma_t\), \(\epsilon_x\), \(\epsilon_y\), and \(\epsilon_t\) must agree with nominal values.
This test uses mesh-refinement to solve the space charge force. The coarse grid wraps the beam maximum extent by 300%, emulating “open boundary” conditions. The refined grid in level 1 spans 110% of the beam maximum extent. The grid spacing is adaptively adjusted as the beam evolves.
Run
This example can be run either as:
Python script:
python3 run_expanding.py
orImpactX executable using an input file:
impactx input_expanding.in
For MPI-parallel runs, prefix these lines with mpiexec -n 4 ...
or srun -n 4 ...
, depending on the system.
Analyze
We run the following script to analyze correctness:
Script analysis_expanding.py
#!/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
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
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 (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 = 10000
assert num_particles == len(initial)
assert num_particles == len(final)
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}"
)
atol = 0.0 # ignored
rtol = 1.5 * 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],
[
4.4721359550e-004,
4.4721359550e-004,
9.1224186858e-007,
0.0e-006,
0.0e-006,
0.0e-006,
],
rtol=rtol,
atol=atol,
)
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}"
)
atol = 0.0 # ignored
rtol = 1.6 * num_particles**-0.5 # from random sampling of a smooth distribution
print(f" rtol={rtol} (ignored: atol~={atol})")
assert np.allclose(
[sigx, sigy, sigt],
[
8.9442719100e-004,
8.9442719100e-004,
1.8244837370e-006,
],
rtol=rtol,
atol=atol,
)
atol = 1.0e-8
rtol = 0.0 # ignored
assert np.allclose(
[emittance_x, emittance_y, emittance_t],
[
0.0,
0.0,
0.0,
],
rtol=rtol,
atol=atol,
)