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#!/usr/bin/env python3
# /// script
# requires-python = ">=3.10"
# dependencies = ["bornagain>=25,<26"]
# ///
"""
Simulation of grating using very long boxes and cumulative 1D paracrystal order.
Monte-carlo integration is used to get rid of
large-particle form factor oscillations.
"""
import bornagain as ba
ba.require_versions("bornagain>=25,<26")
from bornagain import angstrom, deg, nm
def get_sample():
"""
A sample with a grating on a substrate,
modelled by very long boxes forming a 1D paracrystal.
"""
# Materials
particle_color = (0.86, 0.24, 0.18)
particle_mat = ba.RefractiveMaterial("Particle", particle_color, 6e-5, 2e-8)
substrate_color = (0.28, 0.57, 0.82)
substrate_mat = ba.RefractiveMaterial("Substrate", substrate_color, 6e-6, 2e-8)
vacuum = ba.Vacuum()
# Particles
box_length = 10000*nm
ff = ba.Box(10*nm, box_length, 10*nm)
particle = ba.Particle(particle_mat, ff)
particle_rotation = ba.RotationZ(45*deg)
particle.rotate(particle_rotation)
# Interference functions
layout = ba.Paracrystal1D(particle, 30*nm, 45*deg, 1/box_length, 1000*nm)
profile = ba.Profile1DGauss(4*nm)
layout.setProbabilityDistribution(profile)
# Layers
layer_1 = ba.Layer(vacuum)
layer_1.deposit2D(layout)
layer_2 = ba.Layer(substrate_mat)
# Sample
sample = ba.Sample()
sample.addLayer(layer_1)
sample.addLayer(layer_2)
return sample
def get_simulation(sample):
beam = ba.Beam(1e10, 1*angstrom, 0.2*deg)
n = 101
det = ba.SphericalDetector(n, -1*deg, 1*deg, n, 0, 2*deg)
simulation = ba.ScatteringSimulation(beam, sample, det)
simulation.options().setMonteCarloIntegration(True, 100, seed=0)
if not "__no_terminal__" in globals():
simulation.setTerminalProgressMonitor()
return simulation
if __name__ == '__main__':
sample = get_sample()
simulation = get_simulation(sample)
result = simulation.simulate()
ba.showSample3D(sample, sample_size=300*nm, seed=0)
ba.plot_datafield(result, intensity_min=1e-3, unit_aspect=1)
ba.plt.show()
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