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Start implementation with laguerre polynomials.
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using QuantumOptics | ||
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function clenshaw_laguerre{T<:Number}(α::Int, x::Float64, a::Vector{T}) | ||
n = length(a)-1 | ||
ϕ1 = 1 + α - x | ||
if n==0 | ||
return a[1] | ||
elseif n==1 | ||
return a[1] + a[2]*ϕ1 | ||
end | ||
b2 = 0. | ||
b1 = 0. | ||
b0 = 0. | ||
@inbounds for k=n:-1:1 | ||
b2 = b1 | ||
b1 = b0 | ||
A = (2*k + ϕ1)/(k+1) | ||
B = -(k+1+α)/(k+2) | ||
b0 = a[k+1] + A*b1 + B*b2 | ||
end | ||
B1 = -(1 + α)/2 | ||
return a[1] + ϕ1*b0 + B1*b1 | ||
end | ||
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function clenshaw_wigner{T<:Number}(α::Int, x::Float64, a::Vector{T}) | ||
n = length(a)-1 | ||
ϕ1 = -(α+1-x)/sqrt(α+1) | ||
if n==0 | ||
return a[1] | ||
elseif n==1 | ||
return a[1] + a[2]*ϕ1 | ||
end | ||
b2 = 0. | ||
b1 = 0. | ||
b0 = 0. | ||
@inbounds for k=n:-1:1 | ||
b2 = b1 | ||
b1 = b0 | ||
A = -(2*k + 1 + α - x)/sqrt((k+α+1)*(k+1)) | ||
B = -sqrt((k+1+α)*(k+1)/((k+2)*(α+k+2))) | ||
b0 = a[k+1] + A*b1 + B*b2 | ||
end | ||
B1 = -sqrt((α+1)/(2*(α+2))) | ||
return a[1] + ϕ1*b0 + B1*b1 | ||
end | ||
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α = 1 | ||
x = 0.3 | ||
# n = 3 | ||
# a = zeros(Float64, n+1) | ||
# a[end] = 1 | ||
# a = [0.4, 0.3, 0.1, 0.7] | ||
# println(clenshaw_laguerre(α, x, a)) | ||
# L0(α, x) = 1. | ||
# L1(α, x) = -x + α + 1. | ||
# L2(α, x) = x^2/2 - (α+2)*x + (α+2)*(α+1)/2 | ||
# L3(α, x) = -x^3/6 + (α+3)*x^2/2 - (α+2)*(α+3)*x/2 + (α+1)*(α+2)*(α+3)/6 | ||
# # println(L3(α, x)) | ||
# println(a[1]*L0(α, x)+ a[2]*L1(α, x) + a[3]*L2(α, x) + a[4]*L3(α, x)) | ||
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a_wigner = [0, 0, 1] | ||
a_laguerre = [(-1)^n*sqrt(factorial(α)*factorial(n)/factorial(α+n))*a_wigner[n+1] for n=0:length(a_wigner)-1] | ||
r1 = clenshaw_wigner(α, x, a_wigner) | ||
r2 = clenshaw_laguerre(α, x, a_laguerre) | ||
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println(r1) | ||
println(r2) | ||
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function wigner(rho, x, y) | ||
b = basis(rho) | ||
@assert isa(b, FockBasis) | ||
α = complex(x, y)/sqrt(2) | ||
w = complex(0.) | ||
coefficients = zeros(Complex128, b.N+1) | ||
for L=b.N:-1:0 | ||
D = diag(rho.data, L) | ||
for n=0:b.N-L | ||
D[n+1] *= (-1)^n*sqrt(factorial(n)/factorial(L+n)) | ||
end | ||
if L==0 | ||
coefficients[L+1] = clenshaw_laguerre(L, abs2(2*α), D) | ||
else | ||
coefficients[L+1] = 2*clenshaw_laguerre(L, abs2(2*α), D) | ||
end | ||
end | ||
println("coeffs: ", coefficients) | ||
exp(-2*abs2(α))/pi*real(QuantumOptics.polynomials.horner(coefficients, 2*α)) | ||
end | ||
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function wigner2(rho, x, y) | ||
b = basis(rho) | ||
@assert isa(b, FockBasis) | ||
α = complex(x, y)/sqrt(2) | ||
w = complex(0.) | ||
coefficients = zeros(Complex128, b.N+1) | ||
@inbounds for L=b.N:-1:0 | ||
D = diag(rho.data, L) | ||
fac = 1. | ||
for n=0:b.N-L | ||
D[n+1] *= fac | ||
fac *= -sqrt((n+1)/(L+n+1)) | ||
end | ||
if L==0 | ||
coefficient = clenshaw_laguerre(L, abs2(2*α), D) | ||
else | ||
coefficient = 2*clenshaw_laguerre(L, abs2(2*α), D) | ||
end | ||
w = coefficient + w*(2*α)/sqrt(L+1) | ||
end | ||
exp(-2*abs2(α))/pi*real(w) | ||
end | ||
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function wigner3(rho, x, y) | ||
b = basis(rho) | ||
@assert isa(b, FockBasis) | ||
α = complex(x, y)/sqrt(2) | ||
w = complex(0.) | ||
@inbounds for L=b.N:-1:0 | ||
D = diag(rho.data, L) | ||
if L==0 | ||
coefficient = clenshaw_wigner(L, abs2(2*α), D) | ||
else | ||
coefficient = 2*clenshaw_wigner(L, abs2(2*α), D) | ||
end | ||
w = coefficient + w*(2*α)/sqrt(L+1) | ||
end | ||
exp(-2*abs2(α))/pi*real(w) | ||
end | ||
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function clenshaw_wigner2(N::Int, α::Int, x::Float64, a::Matrix{Complex128}) | ||
# n = length(a)-1 | ||
n = N-α | ||
ϕ1 = -(α+1-x)/sqrt(α+1) | ||
if n==0 | ||
return a[1, α+1] | ||
elseif n==1 | ||
return a[1, α+1] + a[2, α+2]*ϕ1 | ||
end | ||
f0 = sqrt(float((n+α)*(n))) | ||
f1 = 1. | ||
f0_ = 1/f0 | ||
f1_ = 1. | ||
b2 = complex(0.) | ||
b1 = complex(0.) | ||
b0 = a[n+1, α+n+1] | ||
@inbounds for k=n-1:-1:1 | ||
b2 = b1 | ||
b1 = b0 | ||
A = -(2*k + 1 + α - x)*f0_ | ||
B = -f0*f1_ | ||
f1 = f0 | ||
f1_ = f0_ | ||
f0 = sqrt((k+α)*k) | ||
f0_ = 1/f0 | ||
b0 = a[k+1, α+k+1] + A*b1 + B*b2 | ||
end | ||
B1 = -sqrt((α+1)/(2*(α+2))) | ||
return a[1, α+1] + ϕ1*b0 + B1*b1 | ||
end | ||
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function clenshaw_wigner3(N::Int, α::Int, x::Float64, a::Matrix{Complex128}) | ||
# n = length(a)-1 | ||
n = N-α | ||
ϕ1 = -(α+1-x)/sqrt(α+1) | ||
if n==0 | ||
return a[1, α+1] | ||
elseif n==1 | ||
return a[1, α+1] + a[2, α+2]*ϕ1 | ||
end | ||
f0 = sqrt(float((n+α-1)*(n-1))) | ||
f1 = sqrt(float((n+α)*n)) | ||
f0_ = 1/f0 | ||
f1_ = 1/f1 | ||
b2 = complex(0.) | ||
b1 = a[n+1, α+n+1] | ||
A = -(2*n-1+α-x)/f1 | ||
b0 = a[n, α+n] + A*b1 | ||
@inbounds for k=n-2:-1:1 | ||
b2 = b1 | ||
b1 = b0 | ||
A = -(2*k + 1 + α - x)*f0_ | ||
B = -f0*f1_ | ||
f1 = f0 | ||
f1_ = f0_ | ||
f0 = sqrt((k+α)*k) | ||
f0_ = 1/f0 | ||
b0 = a[k+1, α+k+1] + A*b1 + B*b2 | ||
end | ||
B1 = -sqrt((α+1)/(2*(α+2))) | ||
return a[1, α+1] + ϕ1*b0 + B1*b1 | ||
end | ||
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function wigner4(rho, x, y) | ||
b = basis(rho) | ||
@assert isa(b, FockBasis) | ||
N = b.N::Int | ||
α = complex(x, y)/sqrt(2) | ||
abs2α = abs2(2*α) | ||
w = complex(0.) | ||
coefficient = complex(0.) | ||
@inbounds for L=N:-1:1 | ||
coefficient = 2*clenshaw_wigner2(N, L, abs2α, rho.data) | ||
w = coefficient + w*(2*α)/sqrt(L+1) | ||
end | ||
coefficient = clenshaw_wigner2(N, 0, abs2α, rho.data) | ||
w = coefficient + w*(2*α) | ||
exp(-2*abs2(α))/pi*real(w) | ||
end | ||
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x = 2 | ||
y = 0 | ||
b = FockBasis(200) | ||
rho = DenseOperator(b) | ||
rho.data[1,3] = 1im | ||
rho = dm(coherentstate(b, 2)) | ||
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# @code_warntype wigner4(rho, x, y) | ||
# @code_warntype clenshaw_wigner2(3, 2, 1., rho.data) | ||
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# w = wigner2(rho, x, y) | ||
# println("wigner=", w) | ||
w = wigner3(rho, x, y) | ||
println("wigner=", w) | ||
w = wigner4(rho, x, y) | ||
println("wigner=", w) | ||
@time w = wigner2(rho, x, y) | ||
@time w = wigner2(rho, x, y) | ||
@time w = wigner3(rho, x, y) | ||
@time w = wigner3(rho, x, y) | ||
@time w = wigner4(rho, x, y) | ||
@time w = wigner4(rho, x, y) | ||
# println("wigner=", w) | ||
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function f1(N, rho, x, y) | ||
for i=1:N | ||
wigner4(rho, x, y) | ||
end | ||
end | ||
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@time f1(10000, rho, 1., 1.) | ||
@time f1(10000, rho, 1., 1.) | ||
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Profile.clear() | ||
@profile f1(10000, rho, 1., 1.) |