# -*- coding: utf-8 -*-
r"""
.. _slitDiffraction:

Slit diffraction with undulator source
--------------------------------------

This example shows wave diffraction of an undulator beam on a square slit. The
calculations were done for (1) a monochromatic beam with zero electron beam
emittance and (2) a finite energy band beam with the real electron emittance of
Petra III ring. The resulted images are compared with experimentally measured
ones [Zozulya_Sprung]_.

Notice that vertical stripes are less pronounced in the complete calculations
because the horizontal emittance is much larger than the vertical one.

.. [Zozulya_Sprung] A. Zozulya and M. Sprung, measured at P10 beamline,
    DESY Photon Science (2014) unpublished.

+-------+------------------------+------------------------+------------------------+--------+
| slit  |     ray tracing,       |     diffraction,       |     diffraction,       |  |exp| |
| size  |     zero emittance     |     zero emittance     |     real emittance     |        |
| (µm²) |                        |                        |                        |        |
+=======+========================+========================+========================+========+
|100×100|     |slit_r0_100|      |     |slit_w0_100|      |     |slit_wr_100|      | |e100| |
+-------+------------------------+------------------------+------------------------+--------+
|150×150|     |slit_r0_150|      |     |slit_w0_150|      |     |slit_wr_150|      | |e150| |
+-------+------------------------+------------------------+------------------------+--------+
|200×200|     |slit_r0_200|      |     |slit_w0_200|      |     |slit_wr_200|      | |e200| |
+-------+------------------------+------------------------+------------------------+--------+
|300×300|     |slit_r0_300|      |     |slit_w0_300|      |     |slit_wr_300|      | |e300| |
+-------+------------------------+------------------------+------------------------+--------+

.. |exp| replace:: exp P10
.. |slit_r0_100| imagezoom:: _images/slit_r0_100.*
.. |slit_r0_150| imagezoom:: _images/slit_r0_150.*
.. |slit_r0_200| imagezoom:: _images/slit_r0_200.*
.. |slit_r0_300| imagezoom:: _images/slit_r0_300.*

.. |slit_w0_100| imagezoom:: _images/slit_w0_100.*
.. |slit_w0_150| imagezoom:: _images/slit_w0_150.*
.. |slit_w0_200| imagezoom:: _images/slit_w0_200.*
.. |slit_w0_300| imagezoom:: _images/slit_w0_300.*

.. |slit_wr_100| imagezoom:: _images/slit_wr_100.*
.. |slit_wr_150| imagezoom:: _images/slit_wr_150.*
.. |slit_wr_200| imagezoom:: _images/slit_wr_200.*
.. |slit_wr_300| imagezoom:: _images/slit_wr_300.*

.. |e100| imagezoom:: _images/slit_e_100.*
   :loc: upper-right-corner
.. |e150| imagezoom:: _images/slit_e_150.*
   :loc: upper-right-corner
.. |e200| imagezoom:: _images/slit_e_200.*
   :loc: upper-right-corner
.. |e300| imagezoom:: _images/slit_e_300.*
   :loc: upper-right-corner

"""
__author__ = "Roman Chernikov", "Konstantin Klementiev"
__date__ = "08 Mar 2016"

import os, sys; sys.path.append(os.path.join('..', '..', '..'))  # analysis:ignore
# sys.path.append(r"/media/sf_Ray-tracing")
# import time
#import matplotlib as mpl
#mpl.use('Agg')
import xrt.backends.raycing as raycing
import xrt.backends.raycing.sources as rs
import xrt.backends.raycing.screens as rsc
import xrt.backends.raycing.apertures as ra
import xrt.backends.raycing.run as rr
import xrt.plotter as xrtp
import xrt.runner as xrtr
import xrt.backends.raycing.waves as rw
import numpy as np

R0 = 44000
mynrays = 1e6

slitDx = 0.1
slitDz = 0.1

SCRx = 1
SCRz = 1
dE = 0.5

#nrep = 160
#nrep = 1000
nrep = 1

E0 = 7900
eMinRays = E0 - dE
eMaxRays = E0 + dE

kwargs = dict(
    period=29., n=172,
    eE=6.08, eI=0.1,  # eEspread=0.001,
    eEpsilonX=0., eEpsilonZ=0.,
    #eEpsilonX=1, eEpsilonZ=0.01,
    betaX=1.20, betaZ=3.95,
    filamentBeam=True,
    uniformRayDensity=True,
    xPrimeMax=(slitDx/R0)*1e3, zPrimeMax=(slitDz/R0)*1e3,
    targetE=[E0, 3],
    eMin=eMinRays,
    eMax=eMaxRays)

prefix = 'far{0:02.0f}m-E0{1:4.0f}-'.format(R0*1e-3, E0)
if kwargs['eEpsilonX'] == 0:
    suffix = "_zeroEmittance"
else:
    suffix = "_realEmittance"

imcnst = 164

imSizeX = imcnst
imSizeZ = imcnst
xBins = imcnst
zBins = imcnst
xppb = 1
zppb = 1
imSize = imcnst
eBins = 16
eppb = 10
xfactor = 1.
zfactor = 1.
screenName = '-plane'
xlimits = [-0.175, 0.175]
zlimits = [-0.175, 0.175]
xName = '$x$'
zName = '$z$'
unit = "mm"

dx = (xlimits[1] - xlimits[0]) / float(xBins)
xmesh = np.linspace((xlimits[0] + dx/2) / xfactor,
                    (xlimits[1] - dx/2) / xfactor, xBins)
dz = (zlimits[1] - zlimits[0]) / float(zBins)
zmesh = np.linspace((zlimits[0] + dz/2) / zfactor,
                    (zlimits[1] - dz/2) / zfactor, zBins)


def build_beamline(nrays=mynrays):
    beamLine = raycing.BeamLine()
    beamLine.source = rs.Undulator(beamLine, nrays=nrays, **kwargs)
    beamLine.fsm0 = rsc.Screen(beamLine, 'FSM0', (0, R0, 0))
    beamLine.slit = ra.RectangularAperture(
        beamLine, 'squareSlit', [0, R0, 0], ('left', 'right', 'bottom', 'top'),
        [-slitDx, slitDx, -slitDz, slitDz])

    beamLine.fsm1 = rsc.Screen(beamLine, 'FSM1', [0, R0, 0])
    return beamLine


def run_process(beamLine):
    area = ((beamLine.slit.opening[3] - beamLine.slit.opening[2]) *
            (beamLine.slit.opening[1] - beamLine.slit.opening[0]))
    waveOnScreen = beamLine.fsm1.prepare_wave(beamLine.slit, xmesh, zmesh)

    beamSource = None
    repeats = 1
    for repeat in range(repeats):
#alternative one (old):
#        beamSource = beamLine.source.shine(
#            accuBeam=beamSource, fixedEnergy=E0)
#        beamFSM0 = beamLine.fsm0.expose(beamSource)
#        slitLocal = beamLine.slit.propagate(beamSource)
#        beamFSM1 = beamLine.fsm1.expose(beamSource)
#        slitLocal.area = area
#        rw.diffract(slitLocal, waveOnScreen)
#alternative two (new):
        waveOnSlit = beamLine.slit.prepare_wave(beamLine.source, mynrays)
        beamSource = beamLine.source.shine(accuBeam=beamSource,
                                           fixedEnergy=E0, wave=waveOnSlit)
        beamFSM0 = beamLine.fsm0.expose(beamSource)
        beamLine.slit.propagate(beamSource)
        beamFSM1 = beamLine.fsm1.expose(beamSource)
        waveOnSlit.area = area
        rw.diffract(waveOnSlit, waveOnScreen)

        if waveOnScreen.diffract_repeats == 0:
            break
        if repeats > 1:
            print('wave repeats: {0} of {1} done'.format(repeat+1, repeats))

    outDict = {'beamSource': beamSource,
               'beamFSM0': beamFSM0,
               'beamFSM1': beamFSM1,
               'waveOnScreen': waveOnScreen
               }
    return outDict
rr.run_process = run_process


def define_plots(beamLine):
    plots = []

    plot = xrtp.XYCPlot(
        'beamFSM0', aspect='auto',
        xaxis=xrtp.XYCAxis(xName, unit, bins=xBins, ppb=xppb),
        yaxis=xrtp.XYCAxis(zName, unit, bins=zBins, ppb=zppb),
        caxis=xrtp.XYCAxis('energy', 'eV', bins=eBins, ppb=eppb),
        title='1-BeamSource')
    plot.baseName = plot.title + suffix
    plots.append(plot)

    plot = xrtp.XYCPlot(
        'beamFSM1', aspect='auto',
        xaxis=xrtp.XYCAxis(xName, unit, bins=xBins, ppb=xppb),
        yaxis=xrtp.XYCAxis(zName, unit, bins=zBins, ppb=zppb),
        caxis=xrtp.XYCAxis('energy', 'eV', bins=eBins, ppb=eppb),
        title='2-Screen Rays')
    plot.baseName = plot.title + suffix
    plots.append(plot)

    plot = xrtp.XYCPlot(
        'waveOnScreen', aspect='auto',
        xaxis=xrtp.XYCAxis(xName, unit, bins=xBins, ppb=xppb),
        yaxis=xrtp.XYCAxis(zName, unit, bins=zBins, ppb=zppb),
        caxis=xrtp.XYCAxis('energy', 'eV', bins=eBins, ppb=eppb),
        title='3-Screen Wave')
    plot.baseName = plot.title + suffix
    plots.append(plot)
    return plots


def plot_generator(plots, beamLine):
    for dS in [slitDx]:
        beamLine.slit.opening[0] = -dS/2
        beamLine.slit.opening[1] = dS/2
        beamLine.slit.opening[2] = -dS/2
        beamLine.slit.opening[3] = dS/2
        beamLine.slit.set_optical_limits()

        dX = 3.7
        beamLine.fsm1.center[1] = R0+dX*1000
        for plot in plots:
            plot.ax2dHist.locator_params(nbins=4)
            plot.xaxis.fwhmFormatStr = '%.2f'
            plot.yaxis.fwhmFormatStr = '%.2f'
            plot.xaxis.limits = xlimits
            plot.yaxis.limits = zlimits
            plot.caxis.limits = [eMinRays, eMaxRays]
            plot.caxis.offset = (eMinRays + eMaxRays) / 2
            plot.fluxFormatStr = '%.2p'
            plot.saveName =\
                plot.baseName +\
                ", slit {0:.2f} mm at {1} m, screen at {2} m.png".\
                format(2*dS, R0/1000, dX)
#            plot.persistentName = plot.saveName + '.pickle'
        yield


def main():
    beamLine = build_beamline()
    plots = define_plots(beamLine)
    xrtr.run_ray_tracing(plots, repeats=nrep, beamLine=beamLine, processes=1,
                         generator=plot_generator)

# this is necessary to use multiprocessing in Windows, otherwise the new Python
# contexts cannot be initialized:
if __name__ == '__main__':
    main()
