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February 4, 2020 06:56
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# Order parameter for a Bose-Einstein condensate with a lattice of | |
# seven vortices | |
using LinearAlgebra, BandedMatrices, Optim, Arpack | |
g = 10/sqrt(2); Ω=0.55*sqrt(2) | |
Nc = 116.24 | |
h = 0.2/2^(1/4); N = 110 | |
C = g*Nc/h^2 # Optim sets norm(ψ) = 1 | |
y = h/2*(1-N:2:N-1); x = y'; z = x .+ 1im*y | |
V = r² = abs2.(z) | |
ψ = Complex.(exp.(-r²/2)/√π) | |
ψ = z.^7 .*ψ./sqrt(1 .+ r²).^7 | |
# jitter to include L ≠ 7 components | |
ψ += (0.1*randn(N,N) + 0.1im*randn(N,N)).*abs.(ψ) | |
ψ ./= norm(ψ) | |
# Finite difference matrices. ∂ on left is ∂y, ∂' on right is ∂x | |
function op(stencil, mid = (length(stencil)+1)÷2) | |
diags = [i-mid=>fill(stencil[i],N-abs(i-mid)) for i = keys(stencil)] | |
BandedMatrix(Tuple(diags), (N,N)) | |
end | |
∂ = (1/h).*op([-1/60, 3/20, -3/4, 0, 3/4, -3/20, 1/60]) | |
∂² = (1/h^2).*op([1/90, -3/20, 3/2, -49/18, 3/2, -3/20, 1/90]) | |
# Minimise the energy | |
# | |
# E(ψ) = -∫ψ*∇²ψ/2 + V|ψ|²+g/2·|ψ|⁴-Ω·ψ*Jψ | |
# | |
# The GPE functional L(ψ) is the gradient required by Optim. | |
L(ψ) = -(∂²*ψ+ψ*∂²)/2+V.*ψ+C*abs2.(ψ).*ψ-1im*Ω*(y.*(ψ*∂')-x.*(∂*ψ)) | |
Ham(ψ) = -(∂²*ψ+ψ*∂²)/2+V.*ψ+C/2*abs2.(ψ).*ψ-1im*Ω*(y.*(ψ*∂')-x.*(∂*ψ)) | |
E(xy) = sum(conj.(togrid(xy)).*Ham(togrid(xy))) |> real | |
grdt!(buf,xy) = copyto!(buf, L(togrid(xy))[:]) | |
togrid(xy) = reshape(xy, size(z)) | |
# Precondition for potential energy. Give up near the origin, where | |
# kinetic energy dominates and dividing by V ≈ 0 would make things worse. | |
P = Diagonal(sqrt.(1 .+ V[:].^2)) | |
result1 = optimize(E, grdt!, ψ[:], | |
ConjugateGradient(manifold=Sphere()), | |
Optim.Options(iterations = 10000, allow_f_increases=true) | |
) | |
ψ₁ = togrid(result1.minimizer) |
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