Add PICMI Scripts for LWFA Tests

Examples/Physics_applications/laser_acceleration/PICMI_inputs_1d.py

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+from pywarpx import picmi
+
+# Physical constants
+c = picmi.constants.c
+q_e = picmi.constants.q_e
+
+# Number of time steps
+max_steps = 100
+
+# Number of cells
+nz = 256
+
+# Physical domain
+zmin = -56e-06
+zmax =  12e-06
+
+# Domain decomposition
+max_grid_size = 64
+blocking_factor = 32
+
+# Create grid
+grid = picmi.Cartesian1DGrid(
+    number_of_cells = [nz],
+    lower_bound = [zmin],
+    upper_bound = [zmax],
+    lower_boundary_conditions = ['dirichlet'],
+    upper_boundary_conditions = ['dirichlet'],
+    lower_boundary_conditions_particles = ['absorbing'],
+    upper_boundary_conditions_particles = ['absorbing'],
+    moving_window_velocity = [0., 0., c],
+    warpx_max_grid_size = max_grid_size,
+    warpx_blocking_factor = blocking_factor)
+
+# Particles: plasma electrons
+plasma_density = 2e23
+plasma_xmin = None
+plasma_ymin = None
+plasma_zmin = 10e-06
+plasma_xmax = None
+plasma_ymax = None
+plasma_zmax = None
+uniform_distribution = picmi.UniformDistribution(
+    density = plasma_density,
+    lower_bound = [plasma_xmin, plasma_ymin, plasma_zmin],
+    upper_bound = [plasma_xmax, plasma_ymax, plasma_zmax],
+    fill_in = True)
+electrons = picmi.Species(
+    particle_type = 'electron',
+    name = 'electrons',
+    initial_distribution = uniform_distribution)
+
+# Laser
+e_max = 16e12
+position_z = 9e-06
+profile_t_peak = 30.e-15
+profile_focal_distance = 100e-06
+laser = picmi.GaussianLaser(
+    wavelength = 0.8e-06,
+    waist = 5e-06,
+    duration = 15e-15,
+    focal_position = [0, 0, profile_focal_distance + position_z],
+    centroid_position = [0, 0, position_z - c*profile_t_peak],
+    propagation_direction = [0, 0, 1],
+    polarization_direction = [0, 1, 0],
+    E0 = e_max,
+    fill_in = False)
+laser_antenna = picmi.LaserAntenna(
+    position = [0., 0., position_z],
+    normal_vector = [0, 0, 1])
+
+# Electromagnetic solver
+solver = picmi.ElectromagneticSolver(
+    grid = grid,
+    method = 'Yee',
+    cfl = 0.9,
+    divE_cleaning = 0)
+
+# Diagnostics
+diag_field_list = ['B', 'E', 'J', 'rho']
+field_diag = picmi.FieldDiagnostic(
+    name = 'diag1',
+    grid = grid,
+    period = 100,
+    data_list = diag_field_list,
+    write_dir = '.',
+    warpx_file_prefix = 'Python_LaserAcceleration_1d_plt')
+
+# Set up simulation
+sim = picmi.Simulation(
+    solver = solver,
+    max_steps = max_steps,
+    verbose = 1,
+    particle_shape = 'cubic',
+    warpx_use_filter = 1,
+    warpx_serialize_ics = 1,
+    warpx_do_dynamic_scheduling = 0)
+
+# Add plasma electrons
+sim.add_species(
+    electrons,
+    layout = picmi.GriddedLayout(grid = grid, n_macroparticle_per_cell = [10]))
+
+# Add laser
+sim.add_laser(
+    laser,
+    injection_method = laser_antenna)
+
+# Add diagnostics
+sim.add_diagnostic(field_diag)
+
+# Write input file that can be used to run with the compiled version
+sim.write_input_file(file_name = 'inputs_1d_picmi')
+
+# Initialize inputs and WarpX instance
+sim.initialize_inputs()
+sim.initialize_warpx()
+
+# Advance simulation until last time step
+sim.step(max_steps)

Examples/Physics_applications/laser_acceleration/PICMI_inputs_2d.py

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+from pywarpx import picmi
+
+# Physical constants
+c = picmi.constants.c
+q_e = picmi.constants.q_e
+
+# Number of time steps
+max_steps = 200
+
+# Number of cells
+nx = 64
+nz = 512
+
+# Physical domain
+xmin = -30e-06
+xmax =  30e-06
+zmin = -56e-06
+zmax =  12e-06
+xmin_refined = -5e-06
+xmax_refined =  5e-06
+zmin_refined = -35e-06
+zmax_refined = -25e-06
+
+# Domain decomposition
+max_grid_size = 64
+blocking_factor = 32
+
+# Create grid
+grid = picmi.Cartesian2DGrid(
+    number_of_cells = [nx, nz],
+    lower_bound = [xmin, zmin],
+    upper_bound = [xmax, zmax],
+    lower_boundary_conditions = ['open', 'open'],
+    upper_boundary_conditions = ['open', 'open'],
+    lower_boundary_conditions_particles = ['absorbing', 'absorbing'],
+    upper_boundary_conditions_particles = ['absorbing', 'absorbing'],
+    moving_window_velocity = [0., c],
+    warpx_max_grid_size = max_grid_size,
+    warpx_blocking_factor = blocking_factor,
+    refined_regions = [[1, [xmin_refined, zmin_refined], [xmax_refined, zmax_refined]]])
+
+# Particles: plasma electrons
+plasma_density = 2e23
+plasma_xmin = -20e-06
+plasma_ymin = None
+plasma_zmin = 10e-06
+plasma_xmax = 20e-06
+plasma_ymax = None
+plasma_zmax = None
+uniform_distribution = picmi.UniformDistribution(
+    density = plasma_density,
+    lower_bound = [plasma_xmin, plasma_ymin, plasma_zmin],
+    upper_bound = [plasma_xmax, plasma_ymax, plasma_zmax],
+    fill_in = True)
+electrons = picmi.Species(
+    particle_type = 'electron',
+    name = 'electrons',
+    initial_distribution = uniform_distribution)
+
+# Particles: beam electrons
+q_tot = 1e-12
+x_m = 0.
+y_m = 0.
+z_m = -28e-06
+x_rms = 0.5e-06
+y_rms = 0.5e-06
+z_rms = 0.5e-06
+ux_m = 0.
+uy_m = 0.
+uz_m = 500.
+ux_th = 2.
+uy_th = 2.
+uz_th = 50.
+gaussian_bunch_distribution = picmi.GaussianBunchDistribution(
+    n_physical_particles = q_tot / q_e,
+    rms_bunch_size = [x_rms, y_rms, z_rms],
+    rms_velocity = [c*ux_th, c*uy_th, c*uz_th],
+    centroid_position = [x_m, y_m, z_m],
+    centroid_velocity = [c*ux_m, c*uy_m, c*uz_m])
+beam = picmi.Species(
+    particle_type = 'electron',
+    name = 'beam',
+    initial_distribution = gaussian_bunch_distribution)
+
+# Laser
+e_max = 16e12
+position_z = 9e-06
+profile_t_peak = 30.e-15
+profile_focal_distance = 100e-06
+laser = picmi.GaussianLaser(
+    wavelength = 0.8e-06,
+    waist = 5e-06,
+    duration = 15e-15,
+    focal_position = [0, 0, profile_focal_distance + position_z],
+    centroid_position = [0, 0, position_z - c*profile_t_peak],
+    propagation_direction = [0, 0, 1],
+    polarization_direction = [0, 1, 0],
+    E0 = e_max,
+    fill_in = False)
+laser_antenna = picmi.LaserAntenna(
+    position = [0., 0., position_z],
+    normal_vector = [0, 0, 1])
+
+# Electromagnetic solver
+solver = picmi.ElectromagneticSolver(
+    grid = grid,
+    method = 'Yee',
+    cfl = 1.,
+    divE_cleaning = 0)
+
+# Diagnostics
+diag_field_list = ['B', 'E', 'J', 'rho']
+field_diag = picmi.FieldDiagnostic(
+    name = 'diag1',
+    grid = grid,
+    period = 200,
+    data_list = diag_field_list,
+    write_dir = '.',
+    warpx_file_prefix = 'Python_LaserAccelerationMR_plt')
+
+# Set up simulation
+sim = picmi.Simulation(
+    solver = solver,
+    max_steps = max_steps,
+    verbose = 1,
+    particle_shape = 'cubic',
+    warpx_use_filter = 1,
+    warpx_serialize_ics = 1)
+
+# Add plasma electrons
+sim.add_species(
+    electrons,
+    layout = picmi.GriddedLayout(grid = grid, n_macroparticle_per_cell = [1, 1, 1]))
+
+# Add beam electrons
+sim.add_species(
+    beam,
+    layout = picmi.PseudoRandomLayout(grid = grid, n_macroparticles = 100))
+
+# Add laser
+sim.add_laser(
+    laser,
+    injection_method = laser_antenna)
+
+# Add diagnostics
+sim.add_diagnostic(field_diag)
+
+# Write input file that can be used to run with the compiled version
+sim.write_input_file(file_name = 'inputs_2d_picmi')
+
+# Initialize inputs and WarpX instance
+sim.initialize_inputs()
+sim.initialize_warpx()
+
+# Advance simulation until last time step
+sim.step(max_steps)