def build_beamline():
beamLine = raycing.BeamLine(alignE=10000)
beamLine.Wiggler = rsources.Wiggler(bl=beamLine,
name=r"Flat-Top Wiggler",
center=[0, 0, 0],
nrays=500000,
eE=2.9,
eI=0.25,
eEpsilonX=18.1,
eEpsilonZ=0.0362,
betaX=9.1,
betaZ=2.8,
xPrimeMax=0.3,
zPrimeMax=0.005,
eMin=9995,
eMax=10005,
K=35,
period=150,
n=11)
beamLine.Generic_DCM = roes.DCM(bl=beamLine,
name=r"Generic DCM",
center=[0, 25300, 0],
bragg=[10000],
material=Si111,
material2=Si111,
cryst2perpTransl=6.5023)
beamLine.Aperture = rapts.RectangularAperture(bl=beamLine,
name=r"Aperture",
center=[0, 28300, r"auto"],
opening=[-10, 10, -0.1, 0.1])
beamLine.FSM = rscreens.Screen(bl=beamLine,
name=r"FSM",
center=[0, 30650, r"auto"])
return beamLine
def build_beamline(nrays=1e4,
hkl=(1, 1, 1),
stripe='Si',
eMinRays=2400,
eMaxRays=45000):
filterDiamond = rm.Material('C', rho=3.52, kind='plate')
if stripe.startswith('S'):
materialVCM = stripeSi
materialVFM = stripeSiO2
elif stripe.startswith('I'):
materialVCM = stripeIr
materialVFM = stripeIr
else:
raise ('Don' 't know the mirror material')
height = 0
beamLine = raycing.BeamLine(azimuth=0, height=height)
wigglerToStraightSection = 0
xWiggler = wigglerToStraightSection * beamLine.sinAzimuth
yWiggler = wigglerToStraightSection * beamLine.cosAzimuth
# rs.WigglerWS(
# beamLine, name='SoleilW50', center=(xWiggler, yWiggler, height),
# nrays=nrays, period=50., K=8.446, n=39, eE=3., eI=0.5,
# eSigmaX=48.66, eSigmaZ=6.197, eEpsilonX=0.263, eEpsilonZ=0.008,
# eMin=50, eMax=60050, eMinRays=eMinRays, eMaxRays=eMaxRays, eN=2000,
# xPrimeMax=0.22, zPrimeMax=0.06, nx=40, nz=10)
rs.Wiggler(beamLine,
name='SoleilW50',
center=(xWiggler, yWiggler, height),
nrays=nrays,
period=50.,
K=8.446,
n=39,
eE=3.,
eI=0.5,
eSigmaX=48.66,
eSigmaZ=6.197,
eEpsilonX=0.263,
eEpsilonZ=0.008,
eMin=eMinRays,
eMax=eMaxRays,
xPrimeMax=0.22,
zPrimeMax=0.06)
beamLine.fsm0 = rsc.Screen(beamLine, 'FSM0', (0, 15000, height))
beamLine.feFixedMask = ra.RectangularAperture(
beamLine, 'FEFixedMask', (0, 15750, height),
('left', 'right', 'bottom', 'top'), [-3.15, 3.15, -0.7875, 0.7875])
beamLine.fsmFE = rsc.Screen(beamLine, 'FSM-FE', (0, 16000, height))
beamLine.filter1 = roe.Plate(beamLine,
'Filter1', (0, 23620, height),
pitch=math.pi / 2,
limPhysX=(-9., 9.),
limPhysY=(-4., 4.),
surface='diamond 60 $\mu$m',
material=filterDiamond,
t=0.06,
alarmLevel=0.)
if stripe.startswith('I'):
beamLine.filter2 = roe.Plate(beamLine,
'Filter2', (0, 23720, height),
pitch=math.pi / 2,
limPhysX=(-9., 9.),
limPhysY=(-4., 4.),
surface='diamond 0.4 mm',
material=filterDiamond,
t=0.4,
alarmLevel=0.)
beamLine.vcm = roe.SimpleVCM(beamLine,
'VCM', [0, 25290, height],
surface=('Si', ),
material=(materialVCM, ),
limPhysX=(-15., 15.),
limPhysY=(-680., 680.),
limOptX=(-6, 6),
limOptY=(-670., 670.),
R=5.0e6,
pitch=2e-3,
alarmLevel=0.)
beamLine.fsmVCM = rsc.Screen(beamLine, 'FSM-VCM', (0, 26300, height))
beamLine.dmm = roe.DCM(
beamLine,
'DMM',
[0, 27060, height],
surface=('mL1', ),
material=(mL, ),
material2=(mL, ),
limPhysX=(-12, 12),
limPhysY=(-150, 150),
cryst2perpTransl=20,
cryst2longTransl=100,
limPhysX2=(-12, 12),
limPhysY2=(-200, 200),
# targetOpenCL='auto',
targetOpenCL='CPU',
alarmLevel=0.05)
beamLine.BSBlock = ra.RectangularAperture(beamLine,
'BSBlock', (0, 29100, height),
('bottom', ), (22, ),
alarmLevel=0.)
beamLine.slitAfterDCM = ra.RectangularAperture(
beamLine,
'SlitAfterDCM', (0, 29200, height), ('left', 'right', 'bottom', 'top'),
[-7, 7, -2, 2],
alarmLevel=0.5)
beamLine.fsmDCM = rsc.Screen(beamLine, 'FSM-DCM', (0, 29400, height))
beamLine.vfm = roe.SimpleVFM(beamLine,
'VFM', [0, 30575, height],
surface=('SiO2', ),
material=(materialVFM, ),
limPhysX=(-20., 20.),
limPhysY=(-700., 700.),
limOptX=(-10, 10),
limOptY=(-700, 700),
positionRoll=math.pi,
R=5.0e6,
r=40.77,
alarmLevel=0.2)
beamLine.slitAfterVFM = ra.RectangularAperture(
beamLine,
'SlitAfterVFM', (0, 31720, height), ('left', 'right', 'bottom', 'top'),
[-7, 7, -2, 2],
alarmLevel=0.5)
beamLine.fsmVFM = rsc.Screen(beamLine, 'FSM-VFM', (0, 32000, height))
beamLine.ohPS = ra.RectangularAperture(beamLine,
'OH-PS', (0, 32070, height),
('left', 'right', 'bottom', 'top'),
(-20, 20, 25, 55),
alarmLevel=0.2)
beamLine.slitEH = ra.RectangularAperture(
beamLine,
'slitEH', (0, 43000, height), ('left', 'right', 'bottom', 'top'),
[-20, 20, -7, 7],
alarmLevel=0.5)
beamLine.fsmSample = rsc.Screen(beamLine, 'FSM-Sample', (0, 45863, height))
return beamLine
def run(case):
myBalder = raycing.BeamLine(azimuth=0, height=0)
kwargs = dict(name='SoleilW50',
center=(0, 0, 0),
period=50.,
K=8.446,
n=39,
eE=3.,
eI=0.5,
eSigmaX=48.66,
eSigmaZ=6.197,
eEpsilonX=0.263,
eEpsilonZ=0.008,
eMin=50,
eMax=eMax * 1e3 + 50,
xPrimeMax=0.2,
zPrimeMax=0.05,
eN=2000,
nx=20,
nz=10)
kwargs['distE'] = 'BW'
source = rs.Wiggler(myBalder, **kwargs)
E = np.mgrid[source.E_min:(source.E_max + 0.5 * source.dE):source.dE]
I0 = source.intensities_on_mesh()[0]
flux = I0.sum(axis=(1, 2)) * source.dTheta * source.dPsi
fig = plt.figure(figsize=(10, 6))
fig.suptitle(u'Integrated {0}'.format(case) +
u' beam flux into 0.4$\\times$ 0.1 mrad$^2$',
fontsize=14)
# fig.subplots_adjust(right=0.88)
ax = fig.add_subplot(111)
ax.set_xlabel(r'energy (keV)')
if case == 'monochromatic':
ax.set_ylabel(r'flux (ph/s/(Si111 DCM bw)')
else:
ax.set_ylabel(r'flux (ph/s/0.1%bw)')
if case == 'monochromatic':
refl = stripePt.get_amplitude(E, np.sin(1e-3))
ras = refl[0]
ax2 = ax.twinx()
rI = (abs(ras)**2)**2
ax2.plot(E * 1e-3, rI, '-b', lw=2)
ax2.set_ylabel('reflectivity of two Pt mirrors at 1 mrad', color='b')
ax2.set_ylim(0, 1)
fluxRes = flux * 2e-4 * 1e3 * rI
else:
fluxRes = flux
ax.plot(E * 1e-3, fluxRes, '-r', lw=2, label='wiggler')
ax.set_ylim(0, None)
ax.set_xlim(0, eMax)
saveName = 'fluxBalder-{0}'.format(case)
fig.savefig(saveName + '.png')
wb = xlwt.Workbook()
ws = wb.add_sheet('flux')
ws.write(0, 0, "energy (eV)")
if case == 'monochromatic':
ws.write(0, 1, "flux (ph/s/(Si111 DCM bw)")
else:
ws.write(0, 1, "flux (ph/s/0.1%bw)")
for ie, (e, f) in enumerate(zip(E, fluxRes)):
ws.write(ie + 1, 0, e)
ws.write(ie + 1, 1, f)
wb.save(saveName + '.xls')
plt.show()
def build_beamline(nrays=raycing.nrays, eMinRays=550, eMaxRays=30550):
x0, y0 = -30095.04, -30102.65 # straight section center
xFar, yFar = -59999.67, -198.017
height = 1400.
azimuth = np.arctan2(xFar - x0, yFar - y0)
stripeSi = rm.Material('Si', rho=2.33)
stripeRh = rm.Material('Rh', rho=12.41)
stripePt = rm.Material('Pt', rho=21.45)
si111_1 = rm.CrystalSi(hkl=(1, 1, 1), tK=-171+273.15)
si311_1 = rm.CrystalSi(hkl=(3, 1, 1), tK=-171+273.15)
si111_2 = rm.CrystalSi(hkl=(1, 1, 1), tK=-140+273.15)
si311_2 = rm.CrystalSi(hkl=(3, 1, 1), tK=-140+273.15)
filterDiamond = rm.Material('C', rho=3.52, kind='plate')
beamLine = raycing.BeamLine(azimuth=azimuth, height=height)
wigglerToStraightSection = 645.0
xWiggler = x0 + wigglerToStraightSection * beamLine.sinAzimuth
yWiggler = y0 + wigglerToStraightSection * beamLine.cosAzimuth
rs.Wiggler(beamLine, name='MPW80', center=(
xWiggler, yWiggler, height),
nrays=nrays, period=80., K=13, n=12, eE=3., eI=0.4,
eSigmaX=200, eSigmaZ=15, eEpsilonX=4.3, eEpsilonZ=0.043,
eMin=eMinRays, eMax=eMaxRays,
xPrimeMax=1.5, zPrimeMax=0.25)
# rs.GeometricSource(beamLine, 'Source', (xWiggler, yWiggler, height),
# nrays=nrays, distE='flat', energies=(2000, 25000),
# polarization='horizontal')
sampleToStraightSection = 36554.1
beamLine.xSample = x0 + sampleToStraightSection * beamLine.sinAzimuth
beamLine.ySample = y0 + sampleToStraightSection * beamLine.cosAzimuth
beamLine.feFixedMask = ra.RectangularAperture(
beamLine, 'FEFixedMask', (-36876.69, -23321.01, height),
('left', 'right', 'bottom', 'top'), [-8.3, 8.3, -2.35, 2.35])
beamLine.fePhotonShutter = ra.RectangularAperture(
beamLine, 'FEPhotonShutter', (-37133.37, -23064.33, height),
('left', 'right', 'bottom', 'top'), [-10.5, 10.5, -8.0, 8.0],
alarmLevel=0.)
beamLine.feMovableMaskLT = ra.RectangularAperture(
beamLine, 'FEMovableMaskLT', (-38979.62, -21218.07, height),
('left', 'top'), [-10, 3.], alarmLevel=0.5)
beamLine.feMovableMaskRB = ra.RectangularAperture(
beamLine, 'FEMovableMaskRB', (-39262.47, -20935.23, height),
('right', 'bottom'), [10, -3.], alarmLevel=0.5)
beamLine.filter1 = roe.Plate(
beamLine, 'Filter1',
(-42740.918, -17456.772, height), pitch=np.pi/2,
limPhysX=(-20., 20.), limPhysY=(-9., 9.),
surface=('diamond 90 $\mu$m',), material=(filterDiamond,), t=0.09,
targetOpenCL=targetOpenCL,
alarmLevel=0.)
beamLine.fsm1 = rsc.Screen(
beamLine, 'DiamondFSM1', (-42920.68, -17277.01, height),
compressX=1./2.44)
beamLine.vcm = roe.VCM(
beamLine, 'VCM', [-43819.49, -16378.20, height],
surface=('Rh', 'Si', 'Pt'), material=(stripeRh, stripeSi, stripePt),
limPhysX=(-53., 53.), limPhysY=(-655., 655.),
limOptX=((-47., -15.5, 16.), (-16., 15.5, 47.)),
limOptY=((-650., -655., -650.), (650., 655., 650.)),
R=5.0e6,
jack1=[-43328.05, -16869.64, 973.0732],
jack2=[-44403.38, -15964.02, 973.0732],
jack3=[-44233.68, -15794.31, 973.0732],
tx1=[0.0, -695.], tx2=[0.0, 705.75],
targetOpenCL=targetOpenCL,
alarmLevel=0.)
beamLine.fsm2 = rsc.Screen(
beamLine, 'NormalFSM2', (-44745.34, -15452.36, height),
compressX=1./2.44)
beamLine.dcm = roe.DCMOnTripodWithOneXStage(
beamLine, 'DCM',
[-45342.09, -14855.6, 1415.], surface=('Si311', 'Si111'),
material=(si311_1, si111_1), material2=(si311_2, si111_2),
limPhysX=((-51.1, 6.1), (-6.1, 51.1)), limPhysY=(-30., 30.),
cryst2perpTransl=20., cryst2longTransl=95.,
limPhysX2=((8.6, -48.6), (48.6, -8.6)), limPhysY2=(-90., 90.),
jack1=[-45052.88, -15079.04, 702.4973],
jack2=[-44987.82, -14490.02, 702.4973],
jack3=[-45576.85, -14555.08, 702.4973],
targetOpenCL=targetOpenCL,
alarmLevel=0.)
beamLine.fsm3 = rsc.Screen(
beamLine, 'DiamondFSM3', (-46625.89, -13571.81, height),
compressX=1./2.44)
beamLine.BSBlock = ra.RectangularAperture(
beamLine, 'BSBlock',
(-45988.52, -14209.17, height), ('bottom',), (22,), alarmLevel=0.)
beamLine.slitAfterDCM_LR = ra.RectangularAperture(
beamLine, 'SlitAfterDCM_LR', (-46095.65, -14102.04, height),
('left', 'right'), [-25.0, 25.0], alarmLevel=0.5)
beamLine.slitAfterDCM_BT = ra.RectangularAperture(
beamLine, 'SlitAfterDCM_BT', (-46107.67, -14090.02, height),
('bottom', 'top'), [27.0, 77.0], alarmLevel=0.5)
foilsZActuatorOffset = 0
beamLine.xbpm4foils = ra.SetOfRectangularAperturesOnZActuator(
beamLine, 'XBPM4foils', (-46137.73, -14059.97, height),
(u'Cu5µm', u'Al7µm', u'Al0.8µm', 'top-edge'),
(1344.607 + foilsZActuatorOffset, 1366.607 + foilsZActuatorOffset,
1388.607 + foilsZActuatorOffset, 1400. + foilsZActuatorOffset),
(45, 45, 45), (8, 8, 8), alarmLevel=0.)
beamLine.vfm = roe.DualVFM(
beamLine, 'VFM', [-47491.364, -12706.324, 1449.53],
surface=('Rh', 'Pt'), material=(stripeRh, stripePt),
limPhysX=(-56., 56.), limPhysY=(-714., 714.),
limOptX=((1., -46.), (46., -4.)),
limOptY=((-712., -712.), (712., 712.)),
positionRoll=np.pi, R=5.0e6,
r1=70., xCylinder1=23.5, hCylinder1=3.7035,
r2=35.98, xCylinder2=-25.0, hCylinder2=6.9504,
jack1=[-46987.20, -13210.49, 1272.88],
jack2=[-48062.53, -12304.87, 1272.88],
jack3=[-47892.83, -12135.16, 1272.88],
tx1=[0.0, -713.], tx2=[0.0, 687.75],
targetOpenCL=targetOpenCL,
alarmLevel=0.2)
beamLine.fsm4 = rsc.Screen(
beamLine, 'DiamondFSM4', (-48350.17, -11847.53, height),
compressX=1./2.44)
beamLine.ohPSFront = ra.RectangularAperture(
beamLine, 'OH-PS-FrontCollimator', (-48592.22, -11605.47, height),
('left', 'right', 'bottom', 'top'), (-23., 23., 30.48, 79.92),
alarmLevel=0.2)
beamLine.ohPSBack = ra.RectangularAperture(
beamLine, 'OH-PS-BackCollimator', (-48708.19, -11489.51, height),
('left', 'right', 'bottom', 'top'), (-23., 23., 31.1, 81.1),
alarmLevel=0.)
beamLine.eh100To40Flange = ra.RoundAperture(
beamLine, 'eh100To40Flange', [-53420.63, -6777.058, height], 19.,
alarmLevel=0.)
eh100To40FlangeToslit = 1159.
slitX = beamLine.eh100To40Flange.center[0] +\
eh100To40FlangeToslit * np.sin(azimuth)
slitY = beamLine.eh100To40Flange.center[1] +\
eh100To40FlangeToslit * np.cos(azimuth)
beamLine.slitEH = ra.RectangularAperture(
beamLine, 'slitEH', (slitX, slitY, height),
('left', 'right', 'bottom', 'top'), [-5, 5, -2.5, 2.5], alarmLevel=0.5)
beamLine.fsmAtSample = rsc.Screen(
beamLine, 'FocusAtSample',
(beamLine.xSample, beamLine.ySample, height))
return beamLine
betaX=9.,
betaZ=2.,
eMax=eMax,
xPrimeMax=thetaMax * 1e3,
zPrimeMax=psiMax * 1e3,
distE='BW')
if case == 'Veritas':
kwargs['period'] = 48.
kwargs['n'] = 81
kwargs['K'] = 4.51
if case == 'Hippie':
kwargs['period'] = 53.
kwargs['n'] = 73
kwargs['K'] = 5.28
sourceW = rs.Wiggler(**kwargs)
energy = np.linspace(100., eMax, eN)
theta = np.linspace(-1, 1, 101) * thetaMax
psi = np.linspace(-1, 1, 101) * psiMax
# theta = np.linspace(-1, 1, 15) * thetaMax
# psi = np.linspace(-1, 1, 15) * psiMax
dtheta, dpsi = theta[1] - theta[0], psi[1] - psi[0]
I0W = sourceW.intensities_on_mesh(energy, theta, psi)[0]
fluxW = I0W.sum(axis=(1, 2)) * dtheta * dpsi
dE = energy[1] - energy[0]
power = fluxW.sum() * dE * SIE0 * 1e3
print('total power = {} W'.format(power))
cumpower = np.cumsum(fluxW) * dE * SIE0 * 1e3 / power
ind = np.argwhere(cumpower > 0.5)[0]
y1, y2 = cumpower[ind - 1], cumpower[ind]
x1, x2 = energy[ind - 1], energy[ind]
