The LMA approach implies that the layer is laterally divided into domains containing particles of the same size and shape and organized into a certain structure. In this approximation the domains are spatially separated and thus completely independent from each other.
The scattering intensity is incoherently summed over the domains with the corresponding weights.
# Structured particle layouts with different particle types
layout_1 = ba.RadialParacrystal(particle_1, 16.8*nm, 1000*nm)
layout_2 = ba.RadialParacrystal(particle_2, 22.8*nm, 1000*nm)
layout_1.setProbabilityDistribution(profile)
layout_2.setProbabilityDistribution(profile)
# Populate layer with weighted layouts
layer.addStruct(0.5, layout_1)
layer.addStruct(0.5, layout_2)
The DA approach implies that the particles share the common interference function but present there with their individual weights. There is still no coherence between different types of particles.
For ordered structures with multiple particle types, use a Mixture:
# Particle mixture
mix = ba.Mixture()
mix.addParticle(particle_1, 0.8)
mix.addParticle(particle_2, 0.2)
# Structured layout with mixture
layout = ba.RadialParacrystal(mix, 18*nm, 1000*nm)
layout.setProbabilityDistribution(profile)
layer.addStruct(layout)
For disordered case, particles are added directly to the layer:
layer.depositParticle(density_1, particle_1)
layer.depositParticle(density_2, particle_2)
Applicable only to radial paracrystal.
The SSCA approach introduces phase shift between different fractions
with the common interference function within the layout.
This is done by setting parameter kappa to 1 (it is 0 by default).
# Particle mixture
mix = ba.Mixture()
mix.addParticle(particle_1, 0.8)
mix.addParticle(particle_2, 0.2)
# Structured layout with mixture
layout = ba.RadialParacrystal(mix, 18*nm, 1000*nm)
layout.setProbabilityDistribution(profile)
layout.setKappa(1) # Enable SSCA
layer.addStruct(layout)
Scattering from a distribution of cylinders of two different sizes, positioned according to the radial paracrystal model.
The sample is made of cylinders deposited on a substrate.
The distribution of particles is made of:
The interference function is radial paracrystal with a peak distance of $18$ nm and a damping length of $1$ $\mu$m. (LMA: two radial paracrystals with a peak distances of $16.8$ and $22.8$ nm.)
The wavelength is equal to 0.1 nm.
The incident angles are $\alpha_i = 0.2 ^{\circ}$ and $\varphi_i = 0^{\circ}$.
The example below compares the scattering patterns of all three approximations.
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