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# -*- coding: utf-8 -*-
"""
__author__ = "Konstantin Klementiev", "Roman Chernikov"
__date__ = "2017-02-01"
Created with xrtQook
"""
import numpy as np
import sys
import os, sys; sys.path.append(os.path.join('..', '..')) # analysis:ignore
import xrt.backends.raycing.sources as rsources
import xrt.backends.raycing.screens as rscreens
import xrt.backends.raycing.materials as rmats
import xrt.backends.raycing.oes as roes
# import xrt.backends.raycing.apertures as rapts
import xrt.backends.raycing.run as rrun
import xrt.backends.raycing as raycing
import xrt.plotter as xrtplot
import xrt.runner as xrtrun
Emin, Emax = 8998, 9002
crystalSi01 = rmats.CrystalSi(
t=0.1,
hkl=[1, 1, 1],
useTT=True,
# calcBorrmann='TT',
geom=r"Laue reflected")
def build_beamline():
beamLine = raycing.BeamLine()
beamLine.geometricSource01 = rsources.GeometricSource(
bl=beamLine,
name=None,
center=[0, 0, 0],
nrays=1000,
distE=r"flat",
dx=0.001, dz=0.001,
dxprime=0, dzprime=0,
energies=[Emin, Emax])
beamLine.screen02 = rscreens.Screen(
bl=beamLine,
center=[0, 10000, 0])
beamLine.lauePlate01 = roes.BentLaueCylinder(
# beamLine.lauePlate01 = roes.LauePlate(
bl=beamLine,
name=None,
center=[0, 10000, 0],
pitch=0.0,
R=1e4,
crossSection='parabolic',
material=crystalSi01,
targetOpenCL='auto')
beamLine.screen01 = rscreens.Screen(
bl=beamLine,
name=None,
center=[0.0, 20000, 0.0])
return beamLine
def run_process(beamLine):
geometricSource01beamGlobal01 = beamLine.geometricSource01.shine()
screen02beamLocal01 = beamLine.screen02.expose(
beam=geometricSource01beamGlobal01)
lauePlate01beamGlobal01, lauePlate01beamLocal01 = beamLine.lauePlate01.reflect(
beam=geometricSource01beamGlobal01)
screen01beamLocal01 = beamLine.screen01.expose(
beam=lauePlate01beamGlobal01)
outDict = {
'geometricSource01beamGlobal01': geometricSource01beamGlobal01,
'lauePlate01beamGlobal01': lauePlate01beamGlobal01,
'lauePlate01beamLocal01': lauePlate01beamLocal01,
'screen01beamLocal01': screen01beamLocal01,
'screen02beamLocal01': screen02beamLocal01}
return outDict
rrun.run_process = run_process
def align_beamline(beamLine, energy):
geometricSource01beamGlobal01 = rsources.Beam(nrays=2)
geometricSource01beamGlobal01.a[:] = 0
geometricSource01beamGlobal01.b[:] = 1
geometricSource01beamGlobal01.c[:] = 0
geometricSource01beamGlobal01.x[:] = 0
geometricSource01beamGlobal01.y[:] = 0
geometricSource01beamGlobal01.z[:] = 0
geometricSource01beamGlobal01.E[:] = energy
geometricSource01beamGlobal01.state[:] = 1
tmpy = beamLine.screen02.center[1]
newx = beamLine.screen02.center[0]
newz = beamLine.screen02.center[2]
beamLine.screen02.center = (newx, tmpy, newz)
print("screen02.center:", beamLine.screen02.center)
screen02beamLocal01 = beamLine.screen02.expose(
beam=geometricSource01beamGlobal01)
tmpy = beamLine.lauePlate01.center[1]
newx = beamLine.lauePlate01.center[0]
newz = beamLine.lauePlate01.center[2]
beamLine.lauePlate01.center = (newx, tmpy, newz)
print("lauePlate01.center:", beamLine.lauePlate01.center)
braggT = crystalSi01.get_Bragg_angle(energy)
alphaT = 0 if beamLine.lauePlate01.alpha is None else beamLine.lauePlate01.alpha
lauePitch = 0
print("bragg, alpha:", np.degrees(braggT), np.degrees(alphaT), "degrees")
braggT += -crystalSi01.get_dtheta(energy, alphaT)
if crystalSi01.geom.startswith('Laue'):
lauePitch = 0.5 * np.pi
print("braggT:", np.degrees(braggT), "degrees")
loBeam = rsources.Beam(copyFrom=geometricSource01beamGlobal01)
raycing.global_to_virgin_local(
beamLine,
geometricSource01beamGlobal01,
loBeam,
center=beamLine.lauePlate01.center)
raycing.rotate_beam(
loBeam,
roll=-(beamLine.lauePlate01.positionRoll + beamLine.lauePlate01.roll),
yaw=-beamLine.lauePlate01.yaw,
pitch=0)
theta0 = np.arctan2(-loBeam.c[0], loBeam.b[0])
th2pitch = np.sqrt(1. - loBeam.a[0]**2)
targetPitch = np.arcsin(np.sin(braggT) / th2pitch) -\
theta0
targetPitch += alphaT + lauePitch
beamLine.lauePlate01.pitch = targetPitch
print("lauePlate01.pitch:", np.degrees(beamLine.lauePlate01.pitch), "degrees")
lauePlate01beamGlobal01, lauePlate01beamLocal01 = beamLine.lauePlate01.reflect(
beam=geometricSource01beamGlobal01)
print("Laue Plate exit point")
print(lauePlate01beamGlobal01.x, lauePlate01beamGlobal01.y,
lauePlate01beamGlobal01.z)
tmpy = beamLine.screen01.center[1]
newx = lauePlate01beamGlobal01.x[0] +\
lauePlate01beamGlobal01.a[0] * (tmpy - lauePlate01beamGlobal01.y[0]) /\
lauePlate01beamGlobal01.b[0]
newz = lauePlate01beamGlobal01.z[0] +\
lauePlate01beamGlobal01.c[0] * (tmpy - lauePlate01beamGlobal01.y[0]) /\
lauePlate01beamGlobal01.b[0]
beamLine.screen01.center = (newx, tmpy, newz)
print("screen01.center:", beamLine.screen01.center)
screen01beamLocal01 = beamLine.screen01.expose(
beam=lauePlate01beamGlobal01)
def define_plots():
plots = []
plot01 = xrtplot.XYCPlot(
beam=r"lauePlate01beamLocal01",
xaxis=xrtplot.XYCAxis(
label=r"x",
unit='$\mu$m',
fwhmFormatStr="%.1f",
bins=256,
ppb=1,
# factor=1000,
limits=[-5, 5]),
yaxis=xrtplot.XYCAxis(
label=r"y",
unit='$\mu$m',
fwhmFormatStr="%.1f",
# factor=1000,
bins=256,
ppb=1,
limits=[-50, 50]),
caxis=xrtplot.XYCAxis(
label=r"energy",
unit=r"eV",
bins=256,
ppb=1,
limits=[Emin, Emax]),
aspect=r"auto",
title=r"01 - Laue crystal Fooprint")
plots.append(plot01)
plot01a = xrtplot.XYCPlot(
beam=r"lauePlate01beamLocal01",
xaxis=xrtplot.XYCAxis(
label=r"y",
unit='$\mu$m',
fwhmFormatStr="%.1f",
# factor=1000,
bins=256,
ppb=1,
limits=[-50, 50]),
yaxis=xrtplot.XYCAxis(
label=r"z",
unit='$\mu$m',
fwhmFormatStr="%.1f",
bins=256,
ppb=1),
caxis=xrtplot.XYCAxis(
label=r"energy",
unit=r"eV",
bins=256,
ppb=1,
limits=[Emin, Emax]),
aspect=r"auto",
title=r"01a - Laue crystal depth profile")
plots.append(plot01a)
plot02 = xrtplot.XYCPlot(
beam=r"screen01beamLocal01",
xaxis=xrtplot.XYCAxis(
label=r"x",
fwhmFormatStr="%.1f",
bins=256,
ppb=1),
yaxis=xrtplot.XYCAxis(
label=r"z",
fwhmFormatStr="%.3f",
bins=256,
ppb=1),
caxis=xrtplot.XYCAxis(
label=r"energy",
unit=r"eV",
limits=[Emin, Emax],
bins=256,
ppb=1),
aspect=r"auto",
title=r"02 - screen")
plots.append(plot02)
plot03 = xrtplot.XYCPlot(
beam=r"screen02beamLocal01",
xaxis=xrtplot.XYCAxis(
label=r"x",
bins=256,
ppb=1,
unit='$\mu$m',
fwhmFormatStr="%.1f"),
yaxis=xrtplot.XYCAxis(
label=r"z",
bins=256,
ppb=1,
unit='$\mu$m',
fwhmFormatStr="%.1f"),
caxis=xrtplot.XYCAxis(
label=r"energy",
bins=256,
ppb=1,
unit=r"eV",
limits=[Emin, Emax]),
aspect=r"auto",
title=r"00 - Laue crystyal - incoming beam")
plots.append(plot03)
for plot in plots:
plot.saveName = plot.title + "R{0}m_t{1}mm.png".format(10, 0.1)
return plots
def main():
beamLine = build_beamline()
E0 = (Emin+Emax)*0.5
align_beamline(beamLine, E0)
plots = define_plots()
xrtrun.run_ray_tracing(
plots=plots,
repeats=10,
backend=r"raycing",
beamLine=beamLine)
if __name__ == '__main__':
main()
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