def get_a0(
tseries: OpenPMDTimeSeries,
t: Optional[float] = None,
it: Optional[int] = None,
coord="x",
m="all",
slicing_dir="y",
theta=0.0,
lambda0=0.8e-6,
) -> Tuple[float, float, float, float]:
"""
Compute z₀, a₀, w₀, cτ.
:param tseries: whole simulation time series
:param t: time (in seconds) at which to obtain the data
:param it: time step at which to obtain the data
:param coord: which component of the field to extract
:param m: 'all' for extracting the sum of all the modes
:param slicing_dir: the direction along which to slice the data eg., 'x', 'y' or 'z'
:param theta: the angle of the plane of observation, with respect to the 'x' axis
:param lambda0: laser wavelength (meters)
:return: z₀, a₀, w₀, cτ
"""
# get E_x field in V/m
electric_field_x, info_electric_field_x = tseries.get_field(
field="E",
coord=coord,
t=t,
iteration=it,
m=m,
theta=theta,
slicing_dir=slicing_dir,
)
# normalized vector potential
e0 = electric_field_amplitude_norm(lambda0=lambda0)
a0 = electric_field_x / e0
# get pulse envelope
envelope = np.abs(hilbert(a0, axis=1))
envelope_z = envelope[envelope.shape[0] // 2, :]
a0_max = np.amax(envelope_z)
# index of peak
z_idx = np.argmax(envelope_z)
# pulse peak position
z0 = info_electric_field_x.z[z_idx]
# FWHM perpendicular size of beam, proportional to w0
fwhm_a0_w0 = (np.sum(np.greater_equal(envelope[:, z_idx], a0_max / 2)) *
info_electric_field_x.dr)
# FWHM longitudinal size of the beam, proportional to ctau
fwhm_a0_ctau = (np.sum(np.greater_equal(envelope_z, a0_max / 2)) *
info_electric_field_x.dz)
return z0, a0_max, fwhm_a0_w0, fwhm_a0_ctau
def field_snapshot(
tseries: OpenPMDTimeSeries,
it: int,
field_name: str,
normalization_factor=1,
coord: Optional[str] = None,
m="all",
theta=0.0,
chop: Optional[List[float]] = None,
path="./",
**kwargs,
) -> None:
"""
Plot the ``field_name`` field from ``tseries`` at step ``iter``.
:param path: path to output file
:param tseries: whole simulation time series
:param it: time step in the simulation
:param field_name: which field to extract, eg. 'rho', 'E', 'B' or 'J'
:param normalization_factor: normalization factor for the extracted field
:param coord: which component of the field to extract, eg. 'r', 't' or 'z'
:param m: 'all' for extracting the sum of all the azimuthal modes
:param theta: the angle of the plane of observation, with respect to the 'x' axis
:param chop: adjusting extent of simulation box plot
:param kwargs: extra plotting arguments, eg. labels, data limits etc.
:return: saves field plot image to disk
"""
if chop is None: # how much to cut out from simulation domain
chop = [40, -20, 15, -15] # CHANGEME
field, info = tseries.get_field(field=field_name,
coord=coord,
iteration=it,
m=m,
theta=theta)
field *= normalization_factor
plot = sliceplots.Plot2D(
arr2d=field,
h_axis=info.z * 1e6,
v_axis=info.r * 1e6,
xlabel=r"${} \;(\mu m)$".format(info.axes[1]),
ylabel=r"${} \;(\mu m)$".format(info.axes[0]),
extent=(
info.zmin * 1e6 + chop[0],
info.zmax * 1e6 + chop[1],
info.rmin * 1e6 + chop[2],
info.rmax * 1e6 + chop[3],
),
cbar=True,
text=f"iteration {it}",
**kwargs,
)
filename = os.path.join(path, f"{field_name}{it:06d}.png")
plot.canvas.print_figure(filename)
def check_identical_fields( folder1, folder2 ):
ts1 = OpenPMDTimeSeries( folder1 )
ts2 = OpenPMDTimeSeries( folder2 )
# Check the vector fields
for field, coord in [("J", "z"), ("E","r"), ("E","z"), ("B","t")]:
print("Checking %s%s" %(field, coord))
field1, info = ts1.get_field(field, coord, iteration=0)
field2, info = ts2.get_field(field, coord, iteration=0)
# For 0 fields, do not use allclose
if abs(field1).max() == 0:
assert abs(field2).max() == 0
else:
assert np.allclose(
field1/abs(field1).max(), field2/abs(field2).max() )
# Check the rho field
print("Checking rho")
field1, info = ts1.get_field("rho", iteration=0)
field2, info = ts2.get_field("rho", iteration=0)
assert np.allclose( field1/abs(field1).max(), field2/abs(field2).max() )
class Backend:
''' Use openPMD-viewer as the backend reader to read openPMD files
'''
def __init__(self, filename):
''' Constructor: store the dataset object
'''
self.dataset = OpenPMDTimeSeries(filename)
def fields_list(self):
''' Return the list of fields defined on the grid
'''
return self.dataset.avail_fields
def species_list(self):
''' Return the list of species in the dataset
'''
return self.dataset.avail_species
def n_levels(self):
''' Return the number of MR levels in the dataset
'''
return 1
def get_field_checksum(self, lev, field, test_name):
''' Calculate the checksum for a given field at a given level in the dataset
'''
Q = self.dataset.get_field(field=field,
iteration=self.dataset.iterations[-1])[0]
return np.sum(np.abs(Q))
def get_species_attributes(self, species):
''' Return the list of attributes for a given species in the dataset
'''
return self.dataset.avail_record_components[species]
def get_species_checksum(self, species, attribute):
''' Calculate the checksum for a given attribute of a given species in the dataset
'''
Q = self.dataset.get_particle(var_list=[attribute],
species=species,
iteration=self.dataset.iterations[-1])
# JSON complains with numpy integers, so if the quantity is a np.int64, convert to int
checksum = np.sum(np.abs(Q))
if type(checksum) in [np.int64, np.uint64]:
return int(checksum)
return checksum
def check_theory_gaussian():
"""
Check that the transverse E and B field are close to the high-gamma
theory for a gaussian bunch
"""
ts = OpenPMDTimeSeries( os.path.join(temporary_dir, 'diags_serial/hdf5/') )
Ex, info = ts.get_field( 'E', 'x', iteration=0 )
By, info = ts.get_field( 'B', 'y', iteration=0 )
r, z = np.meshgrid( info.r, info.z, indexing='ij' )
# High-gamma theory for Gaussian bunch
Eth = -Q/(2*np.pi)**1.5/sig_z/epsilon_0/r * \
(1 - np.exp(-0.5*r**2/sig_r**2)) * \
np.exp( -0.5*(z-zf)**2/sig_z**2)
Bth = Eth/c
# Check that the fields agree
assert np.allclose( Ex, Eth, atol=0.1*Eth.max() )
assert np.allclose( By, Bth, atol=0.1*Bth.max() )
default='diags/hdf5',
help='Path to the directory containing output files')
args = parser.parse_args()
ts = OpenPMDTimeSeries(args.output_dir)
if args.norm_units:
kp = 1.
ne = 1.
q_e = 1.
else:
kp = 1./10.e-6
ne = scc.c**2 / scc.e**2 * scc.m_e * scc.epsilon_0 * kp**2
q_e = scc.e
rho_along_z, rho_meta = ts.get_field(field='rho', iteration=ts.iterations[-1],
slice_across=['x','y'], slice_relative_position=[0,0])
zeta_array = rho_meta.z
dzeta = rho_meta.dz
nz = len(rho_meta.z)
# generating the array with the beam density
nb_array = np.zeros(nz)
beam_starting_position = 1 / kp
distance_to_start_pos = rho_meta.zmax - beam_starting_position
index_beam_head = int(distance_to_start_pos / dzeta)
beam_length = 2 / kp
beam_length_i = int(beam_length / dzeta)
if (args.gaussian_beam):
sigma_z = 1.41 / kp
peak_density = 0.01*ne
nb_array = peak_density*np.sqrt(2*np.pi)*norm.pdf(np.linspace(-nz/2,nz/2,nz)*dzeta/sigma_z)
import matplotlib
import sys
import numpy as np
import math
import argparse
from openpmd_viewer import OpenPMDTimeSeries
parser = argparse.ArgumentParser(
description='Script to analyze the equality of two simulations')
parser.add_argument('--first',
dest='first',
required=True)
parser.add_argument('--second',
dest='second',
required=True)
args = parser.parse_args()
# Replace the string below, to point to your data
tss = OpenPMDTimeSeries(args.first)
tsp = OpenPMDTimeSeries(args.second)
iteration = 0
for field in ['Bx', 'By', 'Ez', 'ExmBy', 'EypBx']:
Fs, ms = tss.get_field(iteration=iteration, field=field)
Fp, mp = tsp.get_field(iteration=iteration, field=field)
error = np.sum((Fp-Fs)**2) / np.sum(Fs**2)
print(field, 'error = np.sum((Fp-Fs)**2) / np.sum(Fs**2) = ' +str(error))
assert(error<0.006)
# full IO and from a simulation with only slice IO
import matplotlib.pyplot as plt
import scipy.constants as scc
import matplotlib
import sys
import numpy as np
import math
import argparse
from openpmd_viewer import OpenPMDTimeSeries
do_plot = False
field = 'Ez'
ts1 = OpenPMDTimeSeries('full_io')
F_full = ts1.get_field(field=field, iteration=ts1.iterations[-1])[0]
F_full = np.swapaxes(F_full, 0, 2)
F_full_xz = (F_full[:, F_full.shape[1] // 2, :].squeeze() +
F_full[:, F_full.shape[1] // 2 - 1, :].squeeze()) / 2.
F_full_yz = (F_full[F_full.shape[0] // 2, :, :].squeeze() +
F_full[F_full.shape[0] // 2 - 1, :, :].squeeze()) / 2.
ts2 = OpenPMDTimeSeries('slice_io_xz')
F_slice_xz = ts2.get_field(field=field,
iteration=ts2.iterations[-1])[0].transpose()
ts3 = OpenPMDTimeSeries('slice_io_yz')
F_slice_yz = ts3.get_field(field=field,
iteration=ts3.iterations[-1])[0].transpose()
if do_plot:
def run_cpu_gpu_deposition(show=False, particle_shape='cubic'):
# Skip this test if cuda is not installed
if not cuda_installed:
return
# Perform deposition for a few timesteps, with both the CPU and GPU
for hardware in ['cpu', 'gpu']:
if hardware == 'cpu':
use_cuda = False
elif hardware == 'gpu':
use_cuda = True
# Initialize the simulation object
sim = Simulation(Nz,
zmax,
Nr,
rmax,
Nm,
dt,
zmin=zmin,
use_cuda=use_cuda,
particle_shape=particle_shape)
sim.ptcl = []
# Add an electron bunch (set the random seed first)
np.random.seed(0)
add_elec_bunch_gaussian(sim, sig_r, sig_z, n_emit, gamma0, sig_gamma,
Q, N)
# Add a field diagnostic
sim.diags = [
FieldDiagnostic(diag_period,
sim.fld,
fieldtypes=['rho', 'J'],
comm=sim.comm,
write_dir=os.path.join('tests', hardware))
]
### Run the simulation
sim.step(N_step)
# Check that the results are identical
ts_cpu = OpenPMDTimeSeries('tests/cpu/hdf5')
ts_gpu = OpenPMDTimeSeries('tests/gpu/hdf5')
for iteration in ts_cpu.iterations:
for field, coord in [('rho', ''), ('J', 'x'), ('J', 'z')]:
# Jy is not tested because it is zero
print('Testing %s at iteration %d' % (field + coord, iteration))
F_cpu, info = ts_cpu.get_field(field, coord, iteration=iteration)
F_gpu, info = ts_gpu.get_field(field, coord, iteration=iteration)
tolerance = 1.e-13 * (abs(F_cpu).max() + abs(F_gpu).max())
if not show:
assert np.allclose(F_cpu, F_gpu, atol=tolerance)
else:
if not np.allclose(F_cpu, F_gpu, atol=tolerance):
plot_difference(field, coord, iteration, F_cpu, F_gpu,
info)
# Remove the files used
shutil.rmtree('tests/cpu')
shutil.rmtree('tests/gpu')
rho0 = -scc.e * dens
c = scc.c
mu_0 = scc.mu_0
eps_0 = scc.epsilon_0
# Radius of the can beam
R = 10.e-6
x_beam_mid = 2
y_beam_mid = -1
x_domain_len = 8
y_domain_len = 8
# Load HiPACE++ data for By in SI units
Bx_sim, Bx_meta = ts.get_field(
field='Bx',
iteration=0,
slice_across=['x', 'z'],
slice_relative_position=[2 * x_beam_mid / x_domain_len, 0])
By_sim, By_meta = ts.get_field(
field='By',
iteration=0,
slice_across=['y', 'z'],
slice_relative_position=[2 * y_beam_mid / y_domain_len, 0])
jz_sim = ts.get_field(
field='jz',
iteration=0,
slice_across=['y', 'z'],
slice_relative_position=[2 * y_beam_mid / y_domain_len, 0])[0]
rho_sim = ts.get_field(
field='rho',
iteration=0,
eps_0 = 1.
R = 1.
else:
# Density of the can beam
dens = 2.8239587008591567e23 # at this density, 1/kp = 10um, allowing for an easy comparison with normalized units
# Define array for transverse coordinate and theory for By and Bx
jz0 = - scc.e * scc.c * dens
rho0 = - scc.e * dens
c = scc.c
mu_0 = scc.mu_0
eps_0 = scc.epsilon_0
# Radius of the can beam
R = 10.e-6
# Load HiPACE++ data for By in SI units
Bx_sim, Bx_meta = ts.get_field(field='Bx', iteration=0, slice_across=['x','z'], slice_relative_position=[0,0])
By_sim, By_meta = ts.get_field(field='By', iteration=0, slice_across=['y','z'], slice_relative_position=[0,0])
jz_sim = ts.get_field(field='jz', iteration=0, slice_across=['y','z'], slice_relative_position=[0,0])[0]
rho_sim = ts.get_field(field='rho', iteration=0, slice_across=['y','z'], slice_relative_position=[0,0])[0]
Ex_sim = ts.get_field(field='ExmBy', iteration=0, slice_across=['y','z'], slice_relative_position=[0,0])[0] + c*By_sim
Ey_sim = ts.get_field(field='EypBx', iteration=0, slice_across=['x','z'], slice_relative_position=[0,0])[0] - c*Bx_sim
y = Bx_meta.y
x = By_meta.x
By_th = mu_0 * jz0 * x / 2.
By_th[abs(x)>=R] = mu_0 * jz0 * R**2/(2*x[abs(x)>R])
Ex_th = rho0 / eps_0 * x / 2.
Ex_th[abs(x)>=R] = rho0 / eps_0 * R**2/(2*x[abs(x)>R])
Bx_th = -mu_0 * jz0 * y / 2.
Bx_th[abs(y)>=R] = -mu_0 * jz0 * R**2/(2*y[abs(y)>R])
args = parser.parse_args()
ts_norm = OpenPMDTimeSeries(args.norm_data)
ts_si = OpenPMDTimeSeries(args.si_data)
ts_si_fixed_weight = OpenPMDTimeSeries(args.si_fixed_weight_data)
elec_density = 2.8239587008591567e23 # [1/m^3]
# calculation of the plasma frequency
omega_p = np.sqrt(elec_density * (scc.e**2) / (scc.epsilon_0 * scc.m_e))
E_0 = omega_p * scc.m_e * scc.c / scc.e
kp = omega_p / scc.c # 1./10.e-6
# Load HiPACE++ data for Ez in both normalized and SI units
Ez_along_z_norm, meta_norm = ts_norm.get_field(field='Ez',
iteration=1,
slice_across=['x', 'y'],
slice_relative_position=[0, 0])
Ez_along_z_si, meta_si = ts_si.get_field(field='Ez',
iteration=1,
slice_across=['x', 'y'],
slice_relative_position=[0, 0])
Ez_along_z_si_fixed_w, meta = ts_si_fixed_weight.get_field(
field='Ez',
iteration=1,
slice_across=['x', 'y'],
slice_relative_position=[0, 0])
zeta_norm = meta_norm.z
zeta_si = meta_si.z
if args.do_plot:
fig, ax = plt.subplots()
#
# This file is part of HiPACE++.
#
# Authors: MaxThevenet, Severin Diederichs
# License: BSD-3-Clause-LBNL
# This script calculates the sum of jz.
# The beam current and the grid current should cancel each other.
import argparse
import numpy as np
from openpmd_viewer import OpenPMDTimeSeries
parser = argparse.ArgumentParser(description='Script to analyze the correctness of the beam in vacuum')
parser.add_argument('--output-dir',
dest='output_dir',
default='diags/hdf5',
help='Path to the directory containing output files')
args = parser.parse_args()
ts = OpenPMDTimeSeries(args.output_dir)
# Load Hipace data for jz
jz_sim, jz_info = ts.get_field(field='jz', iteration=1)
# Assert that the grid current and the beam current cancel each other
error_jz = np.sum( (jz_sim)**2)
print("sum of jz**2: " + str(error_jz) + " (tolerance = 3e-3)")
assert(error_jz < 3e-3)
import scipy.constants as scc
import matplotlib
import sys
import numpy as np
import math
import argparse
from openpmd_viewer import OpenPMDTimeSeries
fields = ['Ez', 'ExmBy', 'EypBx']
ts1 = OpenPMDTimeSeries('fine_io')
ts2 = OpenPMDTimeSeries('coarse_io')
for field in fields:
F_full = ts1.get_field(field=field, iteration=ts1.iterations[-1])[0]
F_full_coarse = (F_full[2::5,1::4,1::3] + F_full[2::5,2::4,1::3])/2
F_coarse = ts2.get_field(field=field, iteration=ts2.iterations[-1])[0]
print("F_full.shape =", F_full.shape)
print("F_full_coarse.shape =", F_full_coarse.shape)
print("F_coarse.shape =", F_coarse.shape)
error = np.max(np.abs(F_coarse-F_full_coarse)) / np.max(np.abs(F_full_coarse))
print("error =", error)
assert(error < 3.e-14)
del ts1
del ts2
default='diags/hdf5',
help='Path to the directory containing output files')
args = parser.parse_args()
ts_ref = OpenPMDTimeSeries('./REF_diags/hdf5/')
ts = OpenPMDTimeSeries(args.output_dir)
if do_plot:
field = 'Bx'
step = 20
ms = .1
plt.figure()
F, meta = ts_ref.get_field(field=field, iteration=ts_ref.iterations[-1])
xp, yp, zp, uzp, wp = ts_ref.get_particle(
species='beam',
iteration=ts_ref.iterations[-1],
var_list=['x', 'y', 'z', 'uz', 'w'])
plt.subplot(221)
plt.title('ref xz')
extent = [meta.zmin, meta.zmax, meta.xmin, meta.xmax]
plt.imshow(F[:, F.shape[1] // 2, :],
extent=extent,
aspect='auto',
origin='lower',
interpolation='nearest')
plt.plot(zp[::step], xp[::step], '.', ms=ms)
