def make_it_easier(*args):
furman_pivi_surface_LHC = {
'use_modified_sigmaE': False,
'use_ECLOUD_theta0_dependence': False,
'use_ECLOUD_energy': False,
'conserve_energy': False,
'exclude_rediffused': True,
'choice': 'poisson',
'M_cut': M_cut,
'p_n': np.array(args[0:10]),
# 'eps_n': np.array(args[10:]),
'eps_n': 1.634185 / (np.array(args[0:10]) - 1),
# Parameters for backscattered electrons
'p1EInf': 0.02,
'p1Ehat': 0.496,
'eEHat': 0.,
'w': 60.86,
'p': 1.,
'e1': 0.26,
'e2': 2.,
'sigmaE': 2.,
# Parameters for rediffused electrons
'p1RInf': 0.2,
'eR': 0.041,
'r': 0.104,
'q': 0.5,
'r1': 0.26,
'r2': 2.,
# Parameters for true secondaries
'deltaTSHat': 1.8848,
'eHat0': 332.,
's': 1.35,
't1': 0.5, # t1 and t2 based on taylor expansion
't2': 1., # of PyECLOUD formula for E_max(theta)
't3': 0.7,
't4': 1.
}
sey_mod_FP = fp.SEY_model_furman_pivi(
furman_pivi_surface_LHC,
E_th=None,
sigmafit=None,
mufit=None,
switch_no_increase_energy=0,
thresh_low_energy=None,
secondary_angle_distribution='cosine_3D')
chamb = ellip_cham_geom_object(1., 1., flag_verbose_file=False)
impact_management_object = impact_management(chamb=chamb,
sey_mod=sey_mod_FP,
Dx_hist=.1,
scrub_en_th=25.,
Nbin_En_hist=100,
En_hist_max=3000,
flag_seg=False,
cos_angle_width=0.05,
flag_cos_angle_hist=True)
return sey_mod_FP, impact_management_object, furman_pivi_surface_LHC
N_steps = 1000000
B = 0
N_sub_steps = 1
B_map_file = 'analytic_qaudrupole_unit_grad'
fact_Bmap = 12. * 0.6
dynamicsB = dynB.pusher_Boris(Dt,
0.,
B,
0.,
B_map_file,
fact_Bmap,
None,
N_sub_steps=N_sub_steps)
chamb = ellip_cham_geom_object(.02, .02)
N_mp_max = 1000
nel_mp_ref_0 = -1
fact_split = -1
fact_clean = -1
N_mp_regen_low = -1
N_mp_regen = -1
N_mp_after_regen = -1
Dx_hist = -1
Nx_regen = -1
Ny_regen = -1
Nvx_regen = -1
Nvy_regen = -1
Nvz_regen = -1
regen_hist_cut = -1
import geom_impact_ellip as ell from scipy import rand import numpy as np sigma = .5 R_cham = 10*sigma Dh = sigma/20. from scipy.constants import e, epsilon_0 qe = e eps0 = epsilon_0 chamber = ell.ellip_cham_geom_object(x_aper = R_cham, y_aper = R_cham) #~ picFD = PIC_FD.FiniteDifferences_Staircase_SquareGrid(chamb = chamber, Dh = Dh) #~ picFDSW = PIC_FDSW.FiniteDifferences_ShortleyWeller_SquareGrid(chamb = chamber, Dh = Dh) picFFT = PIC_FFT.FFT_OpenBoundary_SquareGrid(x_aper = chamber.x_aper, y_aper = chamber.y_aper, Dh = Dh) YY,XX = np.meshgrid(picFFT.yg, picFFT.xg) sigmax = sigma sigmay = sigma x_beam_pos = 0. y_beam_pos = 0. rho_mat=1./(2.*np.pi*sigmax*sigmay)*np.exp(-(XX-x_beam_pos)**2/(2.*sigmax**2)-(YY-y_beam_pos)**2/(2.*sigmay**2)) #pic scatter #~ picFD.solve(rho = rho_mat)
import sys, os
BIN = os.path.expanduser('../')
sys.path.append(BIN)
from backwards_compatibility_1_03 import *
import numpy as np
from geom_impact_ellip import ellip_cham_geom_object
x_aper = .04
y_aper = .02
Dh = .5e-3
sigmax = 1e-3
sigmay = .5e-3
chamber = ellip_cham_geom_object(x_aper, y_aper)
import FiniteDifferences_ShortleyWeller_SquareGrid as PIC_FDSW
pic = PIC_FDSW.FiniteDifferences_ShortleyWeller_SquareGrid(chamb=chamber,
Dh=Dh)
filename_out = 'norepository_FDSW_Dh%.1fmm.mat' % (Dh * 1e3)
#import FiniteDifferences_ShortleyWeller_SquareGrid_extrapolation as PIC_FDSW
#pic = PIC_FDSW.FiniteDifferences_ShortleyWeller_SquareGrid(chamb = chamber, Dh = Dh)
#filename_out = 'norepository_FDSWextrap_Dh%.1fmm.mat'%(Dh*1e3)
#import Bassetti_Erskine as BE
#pic = BE.Interpolated_Bassetti_Erskine(x_aper=chamber.x_aper, y_aper=chamber.y_aper, Dh=Dh,
#sigmax=sigmax, sigmay=sigmay, n_imag_ellip=20)
#filename_out = 'norepository_BE_Dh%.1fmm.mat'%(Dh*1e3)
N_test = 1000
import sys, os
BIN=os.path.expanduser('../')
sys.path.append(BIN)
from backwards_compatibility_1_03 import *
import numpy as np
from geom_impact_ellip import ellip_cham_geom_object
x_aper = .04
y_aper = .02
Dh = .5e-3
sigmax=1e-3
sigmay=.5e-3
chamber = ellip_cham_geom_object(x_aper, y_aper)
import FiniteDifferences_ShortleyWeller_SquareGrid as PIC_FDSW
pic = PIC_FDSW.FiniteDifferences_ShortleyWeller_SquareGrid(chamb = chamber, Dh = Dh)
filename_out = 'norepository_FDSW_Dh%.1fmm.mat'%(Dh*1e3)
#import FiniteDifferences_ShortleyWeller_SquareGrid_extrapolation as PIC_FDSW
#pic = PIC_FDSW.FiniteDifferences_ShortleyWeller_SquareGrid(chamb = chamber, Dh = Dh)
#filename_out = 'norepository_FDSWextrap_Dh%.1fmm.mat'%(Dh*1e3)
#import Bassetti_Erskine as BE
#pic = BE.Interpolated_Bassetti_Erskine(x_aper=chamber.x_aper, y_aper=chamber.y_aper, Dh=Dh,
#sigmax=sigmax, sigmay=sigmay, n_imag_ellip=20)
#filename_out = 'norepository_BE_Dh%.1fmm.mat'%(Dh*1e3)
#
# vx_mpB=array([335546.817425])
# vy_mpB=array([-170848.411391])
# vz_mpB=array([223792.460031])
#===============================================================================
dynamicsB=dynB.pusher_Boris(Dt, 0., B, 0., \
B_map_file, fact_Bmap, None,N_sub_steps=N_sub_steps)
dynamicsGen= dyngen.pusher_strong_B_generalized(Dt, 0., B, \
B_map_file, fact_Bmap, 1e-6)
chamb=ellip_cham_geom_object(.02, .02)
N_mp_max = 1000
nel_mp_ref_0 = -1
fact_split = -1
fact_clean = -1
N_mp_regen_low = -1
N_mp_regen =-1
N_mp_after_regen = -1
Dx_hist=-1
Nx_regen=-1
Ny_regen=-1
Nvx_regen=-1
Nvy_regen =-1
Nvz_regen=-1
regen_hist_cut=-1
import mystyle as ms
from scipy.constants import m_e, e as q_e
parser = argparse.ArgumentParser()
parser.add_argument('-o', help='Path where to save the figure')
parser.add_argument('--noshow', help='Do not make a plot', action='store_true')
args = parser.parse_args()
ms.mystyle(12)
plt.close('all')
Dt = 5e-13
N_steps = 1
chamb = ellip_cham_geom_object(3., 3.)
N_mp_max = 1e4
nel_mp_ref_0 = -1
fact_split = -1
fact_clean = -1
N_mp_regen_low = -1
N_mp_regen = -1
N_mp_after_regen = -1
Dx_hist = 1.
Nx_regen = -1
Ny_regen = -1
Nvx_regen = -1
Nvy_regen = -1
Nvz_regen = -1
regen_hist_cut = -1
def read_input_files_and_init_components(pyecl_input_folder='./', **kwargs):
b_par, x_aper, y_aper, B,\
gas_ion_flag, P_nTorr, sigma_ion_MBarn, Temp_K, unif_frac, E_init_ion,\
Emax, del_max, R0, E_th, sigmafit, mufit,\
Dt, t_end, lam_th, t_ion, N_mp_max,\
N_mp_regen, N_mp_after_regen, fact_split, fact_clean, nel_mp_ref_0,\
Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen,regen_hist_cut,\
N_mp_regen_low,\
Dt_sc, Dh_sc, t_sc_ON,Dx_hist,r_center, scrub_en_th,\
progress_path, logfile_path, flag_movie, flag_sc_movie,\
Dt_En_hist, Nbin_En_hist,En_hist_max, \
photoem_flag, inv_CDF_refl_photoem_file, k_pe_st, refl_frac, alimit, e_pe_sigma,\
e_pe_max,x0_refl, y0_refl, out_radius, \
switch_model, switch_no_increase_energy, thresh_low_energy, save_mp_state_time_file, \
init_unif_flag, Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif,\
chamb_type, filename_chm, flag_detailed_MP_info, flag_hist_impact_seg,\
track_method, B0x, B0y, B0z, B_map_file, Bz_map_file, N_sub_steps, fact_Bmap, B_zero_thrhld,\
N_mp_soft_regen, N_mp_after_soft_regen,\
flag_verbose_file, flag_verbose_stdout,\
flag_presence_sec_beams, sec_b_par_list, phem_resc_fac, dec_fac_secbeam_prof, el_density_probes, save_simulation_state_time_file,\
x_min_hist_det, x_max_hist_det, y_min_hist_det, y_max_hist_det, Dx_hist_det, dec_fact_out, stopfile, sparse_solver, B_multip, \
PyPICmode, filename_init_MP_state,\
init_unif_edens_flag, init_unif_edens, E_init_unif_edens,\
x_max_init_unif_edens, x_min_init_unif_edens, y_max_init_unif_edens, y_min_init_unif_edens, flag_assume_convex, E0, s_param,\
filen_main_outp,\
f_telescope, target_grid, N_nodes_discard, N_min_Dh_main = \
read_parameter_files(pyecl_input_folder)
for attr in kwargs.keys():
print 'Ecloud init. From kwargs: %s = %s'%(attr, repr(kwargs[attr]))
tmpattr = kwargs[attr]
exec('%s=tmpattr'%attr)
##########################################
pyeclsaver=pysav.pyecloud_saver(logfile_path)
if switch_model=='ECLOUD_nunif':
flag_non_unif_sey = 1
else:
flag_non_unif_sey = 0
if chamb_type=='ellip':
chamb=ellip_cham_geom_object(x_aper, y_aper, flag_verbose_file=flag_verbose_file)
elif chamb_type=='polyg' or chamb_type=='polyg_cython':
import geom_impact_poly_fast_impact as gipfi
chamb=gipfi.polyg_cham_geom_object(filename_chm, flag_non_unif_sey,
flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout, flag_assume_convex=flag_assume_convex)
elif chamb_type=='polyg_numpy':
raise ValueError("chamb_type='polyg_numpy' not supported anymore")
#~ chamb=gip.polyg_cham_geom_object(filename_chm, flag_non_unif_sey,
#~ flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout)
elif chamb_type=='rect':
import geom_impact_rect_fast_impact as girfi
chamb = girfi.rect_cham_geom_object(x_aper, y_aper, flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout)
else:
raise ValueError('Chamber type not recognized (choose: ellip/rect/polyg)')
MP_e=MPs.MP_system(N_mp_max, nel_mp_ref_0, fact_split, fact_clean,
N_mp_regen_low, N_mp_regen, N_mp_after_regen,
Dx_hist, Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen, regen_hist_cut, chamb,
N_mp_soft_regen=N_mp_soft_regen, N_mp_after_soft_regen=N_mp_after_soft_regen)
beamtim=beatim.beam_and_timing(b_par.flag_bunched_beam, b_par.fact_beam, b_par.coast_dens, b_par.beam_field_file,lam_th,
b_spac=b_par.b_spac, sigmaz=b_par.sigmaz,t_offs=b_par.t_offs, filling_pattern_file=b_par.filling_pattern_file, Dt=Dt, t_end=t_end,
beam_long_prof_file=b_par.beam_long_prof_file, Dh_beam_field=b_par.Dh_beam_field, f_telescope_beam = b_par.f_telescope_beam,
target_grid_beam = b_par.target_grid_beam, N_nodes_discard_beam = b_par.N_nodes_discard_beam, N_min_Dh_main_beam = b_par.N_min_Dh_main_beam,
chamb=chamb, sigmax=b_par.sigmax, sigmay=b_par.sigmay,
x_beam_pos = b_par.x_beam_pos, y_beam_pos = b_par.y_beam_pos, save_beam_field_file_as=b_par.save_beam_field_file_as,
Nx=b_par.Nx, Ny=b_par.Ny, nimag=b_par.nimag, progress_mapgen_file = (progress_path+'_mapgen'))
if sparse_solver=='klu':
print '''sparse_solver: 'klu' no longer supported --> going to PyKLU'''
sparse_solver='PyKLU'
spacech_ele = scc.space_charge(chamb, Dh_sc, Dt_sc=Dt_sc, sparse_solver=sparse_solver, PyPICmode=PyPICmode,
f_telescope = f_telescope, target_grid = target_grid, N_nodes_discard = N_nodes_discard, N_min_Dh_main = N_min_Dh_main)
sec_beams_list=[]
if flag_presence_sec_beams:
N_sec_beams = len(sec_b_par_list)
for ii in xrange(N_sec_beams):
print 'Initialize secondary beam %d/%d'%(ii+1, N_sec_beams)
sb_par = sec_b_par_list[ii]
sec_beams_list.append(beatim.beam_and_timing(sb_par.flag_bunched_beam, sb_par.fact_beam, sb_par.coast_dens, sb_par.beam_field_file,lam_th,
b_spac=sb_par.b_spac, sigmaz=sb_par.sigmaz,t_offs=sb_par.t_offs, filling_pattern_file=sb_par.filling_pattern_file, Dt=Dt, t_end=t_end,
beam_long_prof_file=sb_par.beam_long_prof_file, Dh_beam_field=sb_par.Dh_beam_field, f_telescope_beam = sb_par.f_telescope_beam,
target_grid_beam = sb_par.target_grid_beam, N_nodes_discard_beam = sb_par.N_nodes_discard_beam, N_min_Dh_main_beam = sb_par.N_min_Dh_main_beam,
chamb=chamb, sigmax=sb_par.sigmax, sigmay=sb_par.sigmay,
x_beam_pos = sb_par.x_beam_pos, y_beam_pos = sb_par.y_beam_pos, save_beam_field_file_as=sb_par.save_beam_field_file_as,
flag_secodary_beam = True, t_primary_beam = beamtim.t,
Nx=sb_par.Nx, Ny=sb_par.Ny, nimag=sb_par.nimag, progress_mapgen_file = (progress_path+('_mapgen_sec_%d'%ii))))
kwargs = {}
if E0 is not None:
kwargs.update({'E0':E0})
#If E0 is not provided use default value for each object
if s_param is not None:
if switch_model==0 or switch_model=='ECLOUD':
kwargs.update({'s':s_param})
else:
raise ValueError('s parameter can be changed only in the ECLOUD sec. emission model!')
if switch_model==0 or switch_model=='ECLOUD':
sey_mod=SEY_model_ECLOUD(Emax,del_max,R0,**kwargs)
elif switch_model==1 or switch_model=='ACC_LOW':
sey_mod=SEY_model_acc_low_ene(Emax,del_max,R0,**kwargs)
elif switch_model=='ECLOUD_nunif':
sey_mod=SEY_model_ECLOUD_non_unif(chamb, Emax,del_max,R0,**kwargs)
elif switch_model=='cos_low_ene':
sey_mod=SEY_model_cos_le(Emax,del_max,R0,**kwargs)
elif switch_model=='flat_low_ene':
sey_mod=SEY_model_flat_le(Emax,del_max,R0)
flag_seg = (flag_hist_impact_seg==1)
impact_man=imc.impact_management(switch_no_increase_energy, chamb, sey_mod, E_th, sigmafit, mufit,
Dx_hist, scrub_en_th, Nbin_En_hist, En_hist_max, thresh_low_energy=thresh_low_energy, flag_seg=flag_seg)
resgasion_sec_beam_list=[]
if gas_ion_flag==1:
resgasion=gic.residual_gas_ionization(unif_frac, P_nTorr, sigma_ion_MBarn,Temp_K,chamb,E_init_ion)
else:
resgasion=None
if photoem_flag==1:
phemiss=gpc.photoemission(inv_CDF_refl_photoem_file, k_pe_st, refl_frac, e_pe_sigma, e_pe_max,alimit, \
x0_refl, y0_refl, out_radius, chamb, phem_resc_fac)
else:
phemiss=None
pyeclsaver.start_observing(MP_e, beamtim, impact_man,
r_center, Dt_En_hist, logfile_path, progress_path, flag_detailed_MP_info=flag_detailed_MP_info,
flag_movie=flag_movie, flag_sc_movie=flag_sc_movie, save_mp_state_time_file=save_mp_state_time_file,
flag_presence_sec_beams=flag_presence_sec_beams, sec_beams_list=sec_beams_list, dec_fac_secbeam_prof=dec_fac_secbeam_prof,
el_density_probes=el_density_probes, save_simulation_state_time_file = save_simulation_state_time_file,
x_min_hist_det=x_min_hist_det, x_max_hist_det=x_max_hist_det, y_min_hist_det=y_min_hist_det, y_max_hist_det=y_max_hist_det,
Dx_hist_det=Dx_hist_det, dec_fact_out=dec_fact_out, stopfile=stopfile, filen_main_outp=filen_main_outp)
if track_method == 'Boris':
dynamics=dynB.pusher_Boris(Dt, B0x, B0y, B0z, \
B_map_file, fact_Bmap, Bz_map_file,N_sub_steps=N_sub_steps)
elif track_method == 'StrongBdip':
dynamics=dyndip.pusher_dipole_magnet(Dt,B)
elif track_method == 'StrongBgen':
dynamics=dyngen.pusher_strong_B_generalized(Dt, B0x, B0y, \
B_map_file, fact_Bmap, B_zero_thrhld)
elif track_method == 'BorisMultipole':
import dynamics_Boris_multipole as dynmul
dynamics=dynmul.pusher_Boris_multipole(Dt=Dt, N_sub_steps=N_sub_steps, B_multip = B_multip)
else:
raise ValueError("""track_method should be 'Boris' or 'StrongBdip' or 'StrongBgen' or 'BorisMultipole'""")
if init_unif_flag==1:
print "Adding inital %.2e electrons to the initial distribution"%Nel_init_unif
MP_e.add_uniform_MP_distrib(Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif)
if init_unif_edens_flag==1:
print "Adding inital %.2e electrons/m^3 to the initial distribution"%init_unif_edens
MP_e.add_uniform_ele_density(n_ele=init_unif_edens, E_init=E_init_unif_edens,
x_max=x_max_init_unif_edens, x_min=x_min_init_unif_edens,
y_max=y_max_init_unif_edens, y_min=y_min_init_unif_edens)
if filename_init_MP_state!=-1 and filename_init_MP_state is not None:
print "Adding inital electrons from: %s"%filename_init_MP_state
MP_e.add_from_file(filename_init_MP_state)
return beamtim,MP_e, dynamics,impact_man, pyeclsaver, \
gas_ion_flag, resgasion, t_ion, \
spacech_ele,t_sc_ON, photoem_flag, phemiss,\
flag_presence_sec_beams, sec_beams_list
def read_input_files_and_init_components(pyecl_input_folder='./', **kwargs):
b_par, x_aper, y_aper, B,\
gas_ion_flag, P_nTorr, sigma_ion_MBarn, Temp_K, unif_frac, E_init_ion,\
Emax, del_max, R0, E_th, sigmafit, mufit,\
Dt, t_end, lam_th, t_ion, N_mp_max,\
N_mp_regen, N_mp_after_regen, fact_split, fact_clean, nel_mp_ref_0,\
Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen,regen_hist_cut,\
N_mp_regen_low,\
Dt_sc, Dh_sc, t_sc_ON,Dx_hist,r_center, scrub_en_th,\
progress_path, logfile_path, flag_movie, flag_sc_movie,\
Dt_En_hist, Nbin_En_hist,En_hist_max, \
photoem_flag, inv_CDF_refl_photoem_file, k_pe_st, refl_frac, alimit, e_pe_sigma,\
e_pe_max,x0_refl, y0_refl, out_radius, \
switch_model, switch_no_increase_energy, thresh_low_energy, save_mp_state_time_file, \
init_unif_flag, Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif,\
chamb_type, filename_chm, flag_detailed_MP_info, flag_hist_impact_seg,\
track_method, B0x, B0y, B0z, B_map_file, Bz_map_file, N_sub_steps, fact_Bmap, B_zero_thrhld,\
N_mp_soft_regen, N_mp_after_soft_regen,\
flag_verbose_file, flag_verbose_stdout,\
flag_presence_sec_beams, sec_b_par_list, phem_resc_fac, dec_fac_secbeam_prof, el_density_probes, save_simulation_state_time_file,\
x_min_hist_det, x_max_hist_det, y_min_hist_det, y_max_hist_det, Dx_hist_det, dec_fact_out, stopfile, sparse_solver, B_multip, \
PyPICmode, filename_init_MP_state,\
init_unif_edens_flag, init_unif_edens, E_init_unif_edens,\
x_max_init_unif_edens, x_min_init_unif_edens, y_max_init_unif_edens, y_min_init_unif_edens, flag_assume_convex, E0,\
filen_main_outp = \
read_parameter_files(pyecl_input_folder)
for attr in kwargs.keys():
print 'Ecloud init. From kwargs: %s = %s'%(attr, repr(kwargs[attr]))
tmpattr = kwargs[attr]
exec('%s=tmpattr'%attr)
##########################################
pyeclsaver=pysav.pyecloud_saver(logfile_path)
if switch_model=='ECLOUD_nunif':
flag_non_unif_sey = 1
else:
flag_non_unif_sey = 0
if chamb_type=='ellip':
chamb=ellip_cham_geom_object(x_aper, y_aper, flag_verbose_file=flag_verbose_file)
elif chamb_type=='polyg' or chamb_type=='polyg_cython':
import geom_impact_poly_fast_impact as gipfi
chamb=gipfi.polyg_cham_geom_object(filename_chm, flag_non_unif_sey,
flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout, flag_assume_convex=flag_assume_convex)
elif chamb_type=='polyg_numpy':
raise ValueError("chamb_type='polyg_numpy' not supported anymore")
#~ chamb=gip.polyg_cham_geom_object(filename_chm, flag_non_unif_sey,
#~ flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout)
elif chamb_type=='rect':
import geom_impact_rect_fast_impact as girfi
chamb = girfi.rect_cham_geom_object(x_aper, y_aper, flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout)
else:
raise ValueError('Chamber type not recognized (choose: ellip/rect/polyg)')
MP_e=MPs.MP_system(N_mp_max, nel_mp_ref_0, fact_split, fact_clean,
N_mp_regen_low, N_mp_regen, N_mp_after_regen,
Dx_hist, Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen, regen_hist_cut, chamb,
N_mp_soft_regen=N_mp_soft_regen, N_mp_after_soft_regen=N_mp_after_soft_regen)
beamtim=beatim.beam_and_timing(b_par.flag_bunched_beam, b_par.fact_beam, b_par.coast_dens, b_par.beam_field_file,lam_th,
b_spac=b_par.b_spac, sigmaz=b_par.sigmaz,t_offs=b_par.t_offs, filling_pattern_file=b_par.filling_pattern_file, Dt=Dt, t_end=t_end,
beam_long_prof_file=b_par.beam_long_prof_file, Dh_beam_field=b_par.Dh_beam_field, chamb=chamb, sigmax=b_par.sigmax, sigmay=b_par.sigmay,
x_beam_pos = b_par.x_beam_pos, y_beam_pos = b_par.y_beam_pos, save_beam_field_file_as=b_par.save_beam_field_file_as,
Nx=b_par.Nx, Ny=b_par.Ny, nimag=b_par.nimag, progress_mapgen_file = (progress_path+'_mapgen'))
if sparse_solver=='klu':
print '''sparse_solver: 'klu' no longer supported --> going to PyKLU'''
sparse_solver='PyKLU'
spacech_ele = scc.space_charge(chamb, Dh_sc, Dt_sc=Dt_sc, sparse_solver=sparse_solver, PyPICmode=PyPICmode)
sec_beams_list=[]
if flag_presence_sec_beams:
N_sec_beams = len(sec_b_par_list)
for ii in xrange(N_sec_beams):
print 'Initialize secondary beam %d/%d'%(ii+1, N_sec_beams)
sb_par = sec_b_par_list[ii]
sec_beams_list.append(beatim.beam_and_timing(sb_par.flag_bunched_beam, sb_par.fact_beam, sb_par.coast_dens, sb_par.beam_field_file,lam_th,
b_spac=sb_par.b_spac, sigmaz=sb_par.sigmaz,t_offs=sb_par.t_offs, filling_pattern_file=sb_par.filling_pattern_file, Dt=Dt, t_end=t_end,
beam_long_prof_file=sb_par.beam_long_prof_file, Dh_beam_field=sb_par.Dh_beam_field, chamb=chamb, sigmax=sb_par.sigmax, sigmay=sb_par.sigmay,
x_beam_pos = sb_par.x_beam_pos, y_beam_pos = sb_par.y_beam_pos, save_beam_field_file_as=sb_par.save_beam_field_file_as,
flag_secodary_beam = True, t_primary_beam = beamtim.t,
Nx=sb_par.Nx, Ny=sb_par.Ny, nimag=sb_par.nimag, progress_mapgen_file = (progress_path+('_mapgen_sec_%d'%ii))))
if E0 is not None:
kwargs = {'E0':E0}
else: #If E0 is not provided use default value for each object
kwargs = {}
if switch_model==0 or switch_model=='ECLOUD':
sey_mod=SEY_model_ECLOUD(Emax,del_max,R0,**kwargs)
elif switch_model==1 or switch_model=='ACC_LOW':
sey_mod=SEY_model_acc_low_ene(Emax,del_max,R0,**kwargs)
elif switch_model=='ECLOUD_nunif':
sey_mod=SEY_model_ECLOUD_non_unif(chamb, Emax,del_max,R0,**kwargs)
elif switch_model=='cos_low_ene':
sey_mod=SEY_model_cos_le(Emax,del_max,R0,**kwargs)
elif switch_model=='flat_low_ene':
sey_mod=SEY_model_flat_le(Emax,del_max,R0)
flag_seg = (flag_hist_impact_seg==1)
impact_man=imc.impact_management(switch_no_increase_energy, chamb, sey_mod, E_th, sigmafit, mufit,
Dx_hist, scrub_en_th, Nbin_En_hist, En_hist_max, thresh_low_energy=thresh_low_energy, flag_seg=flag_seg)
resgasion_sec_beam_list=[]
if gas_ion_flag==1:
resgasion=gic.residual_gas_ionization(unif_frac, P_nTorr, sigma_ion_MBarn,Temp_K,chamb,E_init_ion)
else:
resgasion=None
if photoem_flag==1:
phemiss=gpc.photoemission(inv_CDF_refl_photoem_file, k_pe_st, refl_frac, e_pe_sigma, e_pe_max,alimit, \
x0_refl, y0_refl, out_radius, chamb, phem_resc_fac)
else:
phemiss=None
pyeclsaver.start_observing(MP_e, beamtim, impact_man,
r_center, Dt_En_hist, logfile_path, progress_path, flag_detailed_MP_info=flag_detailed_MP_info,
flag_movie=flag_movie, flag_sc_movie=flag_sc_movie, save_mp_state_time_file=save_mp_state_time_file,
flag_presence_sec_beams=flag_presence_sec_beams, sec_beams_list=sec_beams_list, dec_fac_secbeam_prof=dec_fac_secbeam_prof,
el_density_probes=el_density_probes, save_simulation_state_time_file = save_simulation_state_time_file,
x_min_hist_det=x_min_hist_det, x_max_hist_det=x_max_hist_det, y_min_hist_det=y_min_hist_det, y_max_hist_det=y_max_hist_det,
Dx_hist_det=Dx_hist_det, dec_fact_out=dec_fact_out, stopfile=stopfile, filen_main_outp=filen_main_outp)
if track_method == 'Boris':
dynamics=dynB.pusher_Boris(Dt, B0x, B0y, B0z, \
B_map_file, fact_Bmap, Bz_map_file,N_sub_steps=N_sub_steps)
elif track_method == 'StrongBdip':
dynamics=dyndip.pusher_dipole_magnet(Dt,B)
elif track_method == 'StrongBgen':
dynamics=dyngen.pusher_strong_B_generalized(Dt, B0x, B0y, \
B_map_file, fact_Bmap, B_zero_thrhld)
elif track_method == 'BorisMultipole':
import dynamics_Boris_multipole as dynmul
dynamics=dynmul.pusher_Boris_multipole(Dt=Dt, N_sub_steps=N_sub_steps, B_multip = B_multip)
else:
raise ValueError("""track_method should be 'Boris' or 'StrongBdip' or 'StrongBgen' or 'BorisMultipole'""")
if init_unif_flag==1:
print "Adding inital %.2e electrons to the initial distribution"%Nel_init_unif
MP_e.add_uniform_MP_distrib(Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif)
if init_unif_edens_flag==1:
print "Adding inital %.2e electrons/m^3 to the initial distribution"%init_unif_edens
MP_e.add_uniform_ele_density(n_ele=init_unif_edens, E_init=E_init_unif_edens,
x_max=x_max_init_unif_edens, x_min=x_min_init_unif_edens,
y_max=y_max_init_unif_edens, y_min=y_min_init_unif_edens)
if filename_init_MP_state!=-1 and filename_init_MP_state is not None:
print "Adding inital electrons from: %s"%filename_init_MP_state
MP_e.add_from_file(filename_init_MP_state)
return beamtim,MP_e, dynamics,impact_man, pyeclsaver, \
gas_ion_flag, resgasion, t_ion, \
spacech_ele,t_sc_ON, photoem_flag, phemiss,\
flag_presence_sec_beams, sec_beams_list
def __init__(self, L_ecloud, slicer, Dt_ref, pyecl_input_folder='./'):
print 'PyECLOUD for PyHEADTAIL'
print 'Initializing ecloud from folder: '+pyecl_input_folder
self.slicer = slicer
self.Dt_ref = Dt_ref
self.L_ecloud = L_ecloud
b_par, x_aper, y_aper, B,\
gas_ion_flag, P_nTorr, sigma_ion_MBarn, Temp_K, unif_frac, E_init_ion,\
Emax, del_max, R0, E_th, sigmafit, mufit,\
Dt, t_end, lam_th, t_ion, N_mp_max,\
N_mp_regen, N_mp_after_regen, fact_split, fact_clean, nel_mp_ref_0,\
Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen,regen_hist_cut,\
N_mp_regen_low,\
Dt_sc, Dh_sc, t_sc_ON,Dx_hist,r_center, scrub_en_th,\
progress_path, logfile_path, flag_movie, flag_sc_movie,\
Dt_En_hist, Nbin_En_hist,En_hist_max, \
photoem_flag, inv_CDF_refl_photoem_file, k_pe_st, refl_frac, alimit, e_pe_sigma,\
e_pe_max,x0_refl, y0_refl, out_radius, \
switch_model, switch_no_increase_energy, thresh_low_energy, save_mp_state_time_file, \
init_unif_flag, Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif,\
chamb_type, filename_chm, flag_detailed_MP_info, flag_hist_impact_seg,\
track_method, B0x, B0y, B0z, B_map_file, Bz_map_file, N_sub_steps, fact_Bmap, B_zero_thrhld,\
N_mp_soft_regen, N_mp_after_soft_regen,\
flag_verbose_file, flag_verbose_stdout,\
flag_presence_sec_beams, sec_b_par_list, phem_resc_fac, dec_fac_secbeam_prof, el_density_probes, save_simulation_state_time_file,\
x_min_hist_det, x_max_hist_det, y_min_hist_det, y_max_hist_det, Dx_hist_det, dec_fact_out, stopfile= \
read_parameter_files_pyhdtl(pyecl_input_folder)
#pyeclsaver=pysav.pyecloud_saver(logfile_path)
if switch_model=='ECLOUD_nunif':
flag_non_unif_sey = 1
else:
flag_non_unif_sey = 0
if chamb_type=='ellip':
chamb=ellip_cham_geom_object(x_aper, y_aper, flag_verbose_file=flag_verbose_file)
elif chamb_type=='polyg':
chamb=polyg_cham_geom_object(filename_chm, flag_non_unif_sey,
flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout)
else:
raise ValueError('Chamber type not recognized (choose: ellip/polyg)')
MP_e=MPs.MP_system(N_mp_max, nel_mp_ref_0, fact_split, fact_clean,
N_mp_regen_low, N_mp_regen, N_mp_after_regen,
Dx_hist, Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen, regen_hist_cut, chamb,
N_mp_soft_regen=N_mp_soft_regen, N_mp_after_soft_regen=N_mp_after_soft_regen)
spacech_ele = scc.space_charge(chamb, Dh_sc, Dt_sc=Dt_sc)
#~ sec_beams_list=[]
#~ if flag_presence_sec_beams:
#~ N_sec_beams = len(sec_b_par_list)
#~ for ii in xrange(N_sec_beams):
#~ print 'Initialize secondary beam %d/%d'%(ii+1, N_sec_beams)
#~ sb_par = sec_b_par_list[ii]
#~ sec_beams_list.append(beatim.beam_and_timing(sb_par.flag_bunched_beam, sb_par.fact_beam, sb_par.coast_dens, sb_par.beam_field_file,lam_th,
#~ b_spac=sb_par.b_spac, sigmaz=sb_par.sigmaz,t_offs=sb_par.t_offs, filling_pattern_file=sb_par.filling_pattern_file, Dt=Dt, t_end=t_end,
#~ beam_long_prof_file=sb_par.beam_long_prof_file, Dh_beam_field=sb_par.Dh_beam_field, chamb=chamb, sigmax=sb_par.sigmax, sigmay=sb_par.sigmay,
#~ x_beam_pos = sb_par.x_beam_pos, y_beam_pos = sb_par.y_beam_pos, save_beam_field_file_as=sb_par.save_beam_field_file_as,
#~ flag_secodary_beam = True, t_primary_beam = beamtim.t,
#~ Nx=sb_par.Nx, Ny=sb_par.Ny, nimag=sb_par.nimag, progress_mapgen_file = (progress_path+('_mapgen_sec_%d'%ii))))
if switch_model==0 or switch_model=='ECLOUD':
sey_mod=SEY_model_ECLOUD(Emax,del_max,R0)
elif switch_model==1 or switch_model=='ACC_LOW':
sey_mod=SEY_model_acc_low_ene(Emax,del_max,R0)
elif switch_model=='ECLOUD_nunif':
sey_mod=SEY_model_ECLOUD_non_unif(chamb, Emax,del_max,R0)
elif switch_model=='cos_low_ene':
sey_mod=SEY_model_cos_le(Emax,del_max,R0)
elif switch_model=='flat_low_ene':
sey_mod=SEY_model_flat_le(Emax,del_max,R0)
flag_seg = (flag_hist_impact_seg==1)
impact_man=imc.impact_management(switch_no_increase_energy, chamb, sey_mod, E_th, sigmafit, mufit,
Dx_hist, scrub_en_th, Nbin_En_hist, En_hist_max, thresh_low_energy=thresh_low_energy, flag_seg=flag_seg)
if track_method == 'Boris':
dynamics=dynB.pusher_Boris(Dt, B0x, B0y, B0z, \
B_map_file, fact_Bmap, Bz_map_file,N_sub_steps=N_sub_steps)
#~ elif track_method == 'StrongBdip':
#~ dynamics=dyndip.pusher_dipole_magnet(Dt,B)
#~ elif track_method == 'StrongBgen':
#~ dynamics=dyngen.pusher_strong_B_generalized(Dt, B0x, B0y, \
#~ B_map_file, fact_Bmap, B_zero_thrhld)
else:
raise ValueError("""track_method should be 'Boris' - others are not implemented in the PyHEADTAIL module""")
if init_unif_flag==1:
MP_e.add_uniform_MP_distrib(Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif)
spacech_ele.flag_decimate = False
self.MP_e = MP_e
self.dynamics = dynamics
self.impact_man = impact_man
self.spacech_ele = spacech_ele
self.save_ele_distributions_last_track = False
self.save_ele_potential_and_field = False
self.save_ele_MP_position = False
self.save_ele_MP_velocity = False
self.save_ele_MP_size = False
self.init_x = self.MP_e.x_mp.copy()
self.init_y = self.MP_e.y_mp.copy()
self.init_z = self.MP_e.z_mp.copy()
self.init_vx = self.MP_e.vx_mp.copy()
self.init_vy = self.MP_e.vy_mp.copy()
self.init_vz = self.MP_e.vz_mp.copy()
self.init_nel = self.MP_e.nel_mp.copy()
self.init_N_mp = self.MP_e.N_mp
import os, sys
BIN = os.path.expanduser("../../")
sys.path.append(BIN)
import numpy as np
import matplotlib.pyplot as pl
import gen_photoemission_class as gp
import geom_impact_ellip as gie
import MP_system as mps
file_to_test = 'inv_cdf_phem_ang_distrib.mat'
# generate a chamber
chamb = gie.ellip_cham_geom_object(x_aper=2e-2, y_aper=1e-2)
# Build object used by pyecloud
ob = gp.photoemission_from_file(inv_CDF_all_photoem_file=file_to_test,
chamb=chamb,
resc_fac=1.,
energy_distribution='gaussian',
e_pe_sigma=3.,
e_pe_max=10.,
k_pe_st=1.,
out_radius=10e-2,
photoelectron_angle_distribution='cosine_3D',
beamtim=None,
flag_continuous_emission=False)
N_mp_test = 100000
def __init__(self,
L_ecloud,
slicer,
Dt_ref,
pyecl_input_folder='./',
flag_clean_slices=False,
slice_by_slice_mode=False,
space_charge_obj=None,
**kwargs):
print 'PyECLOUD Version 5.5.3'
print 'PyHEADTAIL module'
print 'Initializing ecloud from folder: ' + pyecl_input_folder
self.slicer = slicer
self.Dt_ref = Dt_ref
self.L_ecloud = L_ecloud
self.pyecl_input_folder = pyecl_input_folder
self.kwargs = kwargs
b_par, x_aper, y_aper, B,\
gas_ion_flag, P_nTorr, sigma_ion_MBarn, Temp_K, unif_frac, E_init_ion,\
Emax, del_max, R0, E_th, sigmafit, mufit,\
Dt, t_end, lam_th, t_ion, N_mp_max,\
N_mp_regen, N_mp_after_regen, fact_split, fact_clean, nel_mp_ref_0,\
Nx_regen, Ny_regen, Nvx_regen, Nvy_regen, Nvz_regen,regen_hist_cut,\
N_mp_regen_low,\
Dt_sc, Dh_sc, t_sc_ON,Dx_hist,r_center, scrub_en_th,\
progress_path, logfile_path, flag_movie, flag_sc_movie,\
Dt_En_hist, Nbin_En_hist,En_hist_max, \
photoem_flag, inv_CDF_refl_photoem_file, k_pe_st, refl_frac, alimit, e_pe_sigma,\
e_pe_max,x0_refl, y0_refl, out_radius, \
switch_model, switch_no_increase_energy, thresh_low_energy, save_mp_state_time_file, \
init_unif_flag, Nel_init_unif, E_init_unif, x_max_init_unif, x_min_init_unif, y_max_init_unif, y_min_init_unif,\
chamb_type, filename_chm, flag_detailed_MP_info, flag_hist_impact_seg,\
track_method, B0x, B0y, B0z, B_map_file, Bz_map_file, N_sub_steps, fact_Bmap, B_zero_thrhld,\
N_mp_soft_regen, N_mp_after_soft_regen,\
flag_verbose_file, flag_verbose_stdout,\
flag_presence_sec_beams, sec_b_par_list, phem_resc_fac, dec_fac_secbeam_prof, el_density_probes, save_simulation_state_time_file,\
x_min_hist_det, x_max_hist_det, y_min_hist_det, y_max_hist_det, Dx_hist_det, dec_fact_out, stopfile, sparse_solver, B_multip,\
PyPICmode, filename_init_MP_state,\
init_unif_edens_flag, init_unif_edens, E_init_unif_edens,\
x_max_init_unif_edens, x_min_init_unif_edens, y_max_init_unif_edens, y_min_init_unif_edens, flag_assume_convex,\
f_telescope, target_grid, N_nodes_discard, N_min_Dh_main = \
read_parameter_files_pyhdtl(pyecl_input_folder)
for attr in kwargs.keys():
print 'Ecloud init. From kwargs: %s = %s' % (attr,
repr(kwargs[attr]))
tmpattr = kwargs[attr]
exec('%s=tmpattr' % attr)
#pyeclsaver=pysav.pyecloud_saver(logfile_path)
if switch_model == 'ECLOUD_nunif':
flag_non_unif_sey = 1
else:
flag_non_unif_sey = 0
if chamb_type == 'ellip':
chamb = ellip_cham_geom_object(x_aper,
y_aper,
flag_verbose_file=flag_verbose_file)
elif chamb_type == 'polyg' or chamb_type == 'polyg_cython':
import geom_impact_poly_fast_impact as gipfi
chamb = gipfi.polyg_cham_geom_object(
filename_chm,
flag_non_unif_sey,
flag_verbose_file=flag_verbose_file,
flag_verbose_stdout=flag_verbose_stdout,
flag_assume_convex=flag_assume_convex)
elif chamb_type == 'polyg_numpy':
raise ValueError("chamb_type='polyg_numpy' not supported anymore")
#~ chamb=gip.polyg_cham_geom_object(filename_chm, flag_non_unif_sey,
#~ flag_verbose_file=flag_verbose_file, flag_verbose_stdout=flag_verbose_stdout)
elif chamb_type == 'rect':
import geom_impact_rect_fast_impact as girfi
chamb = girfi.rect_cham_geom_object(
x_aper,
y_aper,
flag_verbose_file=flag_verbose_file,
flag_verbose_stdout=flag_verbose_stdout)
else:
raise ValueError(
'Chamber type not recognized (choose: ellip/rect/polyg)')
MP_e = MPs.MP_system(N_mp_max,
nel_mp_ref_0,
fact_split,
fact_clean,
N_mp_regen_low,
N_mp_regen,
N_mp_after_regen,
Dx_hist,
Nx_regen,
Ny_regen,
Nvx_regen,
Nvy_regen,
Nvz_regen,
regen_hist_cut,
chamb,
N_mp_soft_regen=N_mp_soft_regen,
N_mp_after_soft_regen=N_mp_after_soft_regen)
if sparse_solver == 'klu':
print '''sparse_solver: 'klu' no longer supported --> going to PyKLU'''
sparse_solver = 'PyKLU'
if space_charge_obj is not None:
spacech_ele = space_charge_obj
else:
spacech_ele = scc.space_charge(chamb,
Dh_sc,
Dt_sc=Dt_sc,
sparse_solver=sparse_solver,
PyPICmode=PyPICmode,
f_telescope=f_telescope,
target_grid=target_grid,
N_nodes_discard=N_nodes_discard,
N_min_Dh_main=N_min_Dh_main)
if switch_model == 0 or switch_model == 'ECLOUD':
sey_mod = SEY_model_ECLOUD(Emax, del_max, R0)
elif switch_model == 1 or switch_model == 'ACC_LOW':
sey_mod = SEY_model_acc_low_ene(Emax, del_max, R0)
elif switch_model == 'ECLOUD_nunif':
sey_mod = SEY_model_ECLOUD_non_unif(chamb, Emax, del_max, R0)
elif switch_model == 'cos_low_ene':
sey_mod = SEY_model_cos_le(Emax, del_max, R0)
elif switch_model == 'flat_low_ene':
sey_mod = SEY_model_flat_le(Emax, del_max, R0)
flag_seg = (flag_hist_impact_seg == 1)
impact_man = imc.impact_management(switch_no_increase_energy,
chamb,
sey_mod,
E_th,
sigmafit,
mufit,
Dx_hist,
scrub_en_th,
Nbin_En_hist,
En_hist_max,
thresh_low_energy=thresh_low_energy,
flag_seg=flag_seg)
if track_method == 'Boris':
dynamics=dynB.pusher_Boris(Dt, B0x, B0y, B0z, \
B_map_file, fact_Bmap, Bz_map_file,N_sub_steps=N_sub_steps)
#~ elif track_method == 'StrongBdip':
#~ dynamics=dyndip.pusher_dipole_magnet(Dt,B)
#~ elif track_method == 'StrongBgen':
#~ dynamics=dyngen.pusher_strong_B_generalized(Dt, B0x, B0y, \
#~ B_map_file, fact_Bmap, B_zero_thrhld)
elif track_method == 'BorisMultipole':
import dynamics_Boris_multipole as dynmul
dynamics = dynmul.pusher_Boris_multipole(Dt=Dt,
N_sub_steps=N_sub_steps,
B_multip=B_multip)
else:
raise ValueError(
"""track_method should be 'Boris' or 'BorisMultipole' - others are not implemented in the PyEC4PyHT module"""
)
if init_unif_flag == 1:
print "Adding inital %.2e electrons to the initial distribution" % Nel_init_unif
MP_e.add_uniform_MP_distrib(Nel_init_unif, E_init_unif,
x_max_init_unif, x_min_init_unif,
y_max_init_unif, y_min_init_unif)
if init_unif_edens_flag == 1:
print "Adding inital %.2e electrons/m^3 to the initial distribution" % init_unif_edens
MP_e.add_uniform_ele_density(n_ele=init_unif_edens,
E_init=E_init_unif_edens,
x_max=x_max_init_unif_edens,
x_min=x_min_init_unif_edens,
y_max=y_max_init_unif_edens,
y_min=y_min_init_unif_edens)
if filename_init_MP_state != -1 and filename_init_MP_state is not None:
print "Adding inital electrons from: %s" % filename_init_MP_state
MP_e.add_from_file(filename_init_MP_state)
self.x_beam_offset = 0.
self.y_beam_offset = 0.
if 'x_beam_offset' in kwargs.keys():
self.x_beam_offset = kwargs['x_beam_offset']
if 'y_beam_offset' in kwargs.keys():
self.y_beam_offset = kwargs['y_beam_offset']
# initialize proton density probes
self.save_ele_field_probes = False
self.x_probes = -1
self.y_probes = -1
self.Ex_ele_last_track_at_probes = -1
self.Ey_ele_last_track_at_probes = -1
if 'probes_position' in kwargs.keys():
self.save_ele_field_probes = True
self.probes_position = kwargs['probes_position']
self.N_probes = len(self.probes_position)
self.x_probes = []
self.y_probes = []
for ii_probe in xrange(self.N_probes):
self.x_probes.append(probes_position[ii_probe]['x'])
self.y_probes.append(probes_position[ii_probe]['y'])
self.x_probes = np.array(self.x_probes)
self.y_probes = np.array(self.y_probes)
self.N_tracks = 0
spacech_ele.flag_decimate = False
self.MP_e = MP_e
self.dynamics = dynamics
self.impact_man = impact_man
self.spacech_ele = spacech_ele
self.save_ele_distributions_last_track = False
self.save_ele_potential_and_field = False
self.save_ele_potential = False
self.save_ele_field = False
self.save_ele_MP_position = False
self.save_ele_MP_velocity = False
self.save_ele_MP_size = False
self.track_only_first_time = False
self.init_x = self.MP_e.x_mp[:self.MP_e.N_mp].copy()
self.init_y = self.MP_e.y_mp[:self.MP_e.N_mp].copy()
self.init_z = self.MP_e.z_mp[:self.MP_e.N_mp].copy()
self.init_vx = self.MP_e.vx_mp[:self.MP_e.N_mp].copy()
self.init_vy = self.MP_e.vy_mp[:self.MP_e.N_mp].copy()
self.init_vz = self.MP_e.vz_mp[:self.MP_e.N_mp].copy()
self.init_nel = self.MP_e.nel_mp[:self.MP_e.N_mp].copy()
self.init_N_mp = self.MP_e.N_mp
self.flag_clean_slices = flag_clean_slices
self.slice_by_slice_mode = slice_by_slice_mode
if self.slice_by_slice_mode:
self.track = self._track_in_single_slice_mode
self.finalize_and_reinitialize = self._finalize_and_reinitialize
me = 9.10938356e-31
switch = 2
sey_mod = ECL.SEY_model_ECLOUD(Emax=332.,
del_max=1.8848,
R0=0.7,
E_th=35.,
mufit=1.6636,
secondary_angle_distribution='cosine_3D',
sigmafit=1.0828,
switch_no_increase_energy=switch,
thresh_low_energy=1.)
chamb = ellip_cham_geom_object(1., 1., flag_verbose_file=False)
impact_management_object = impact_management(chamb=chamb,
sey_mod=sey_mod,
Dx_hist=.1,
scrub_en_th=25.,
Nbin_En_hist=100,
En_hist_max=3000,
flag_seg=False,
cos_angle_width=0.05,
flag_cos_angle_hist=True)
cos_theta_test = np.linspace(0., 1., 10)
E_0_single = 35.
E_impact_eV_test = E_0_single
n_rep = 100000
alpha = 0.9
