Function References
FourierTools.conv
— Functionconv(u, v[, dims])
Convolve u
with v
over dims
dimensions with an FFT based method. Note, that this method introduces wrap-around artifacts without proper padding/windowing.
Arguments
u
is an array in real space.v
is the array to be convolved in real space as well.- Per default
ntuple(+, min(N, M)))
means that we perform the convolution over all dimensions of that array which has less dimensions. Ifdims
is an array with integers, we perform convolution only over these dimensions. Eg.dims=[1,3]
would perform the convolution over the first and third dimension. Second dimension is not convolved.
If u
and v
are both a real valued array we use rfft
and hence the output is real as well. If either u
or v
is complex we use fft
and output is hence complex.
Examples
1D with FFT over all dimensions. We choose v
to be a delta peak. Therefore convolution should act as identity.
julia> u = [1 2 3 4 5]
1×5 Array{Int64,2}:
1 2 3 4 5
julia> v = [0 0 1 0 0]
1×5 Array{Int64,2}:
0 0 1 0 0
julia> conv(u, v)
1×5 Matrix{Float64}:
4.0 5.0 1.0 2.0 3.0
2D with FFT with different dims
arguments.
julia> u = 1im .* [1 2 3; 4 5 6]
2×3 Matrix{Complex{Int64}}:
0+1im 0+2im 0+3im
0+4im 0+5im 0+6im
julia> v = [1im 0 0; 1im 0 0]
2×3 Matrix{Complex{Int64}}:
0+1im 0+0im 0+0im
0+1im 0+0im 0+0im
julia> conv(u, v)
2×3 Matrix{ComplexF64}:
-5.0+0.0im -7.0+0.0im -9.0+0.0im
-5.0+0.0im -7.0+0.0im -9.0+0.0im
FourierTools.ccorr
— Functionccorr(u, v[, dims]; centered=false)
Calculates the cross-correlation between u
and v
along dims
. centered=true
moves the output of the cross-correlation to the Fourier center.
If u
and v
are both a real valued array we use rfft
and hence the output is real as well. If either u
or v
is complex we use fft
and output is hence complex.
Per default the correlation is performed along min(ndims(u), ndims(v))
.
julia> ccorr([1,1,0,0], [1,1,0,0], centered=true)
4-element Vector{Float64}:
0.0
1.0
2.0
1.0
julia> ccorr([1,1,0,0], [1,1,0,0])
4-element Vector{Float64}:
2.0
1.0
0.0
1.0
julia> ccorr([1im,0,0,0], [0,1im,0,0])
4-element Vector{ComplexF64}:
0.0 + 0.0im
0.0 + 0.0im
0.0 + 0.0im
1.0 + 0.0im
julia> ccorr([1im,0,0,0], [0,1im,0,0], centered=true)
4-element Vector{ComplexF64}:
0.0 + 0.0im
1.0 + 0.0im
0.0 + 0.0im
0.0 + 0.0im
FourierTools.conv_psf
— Functionconv_psf(u, psf[, dims])
conv_psf
is a shorthand for conv(u,ifftshift(psf))
. For examples see conv
.
FourierTools.plan_conv
— Functionplan_conv(u, v [, dims]; kwargs...)
Pre-plan an optimized convolution for arrays shaped like u
and v
(based on pre-plan FFT) along the given dimenions dims
. dims = 1:ndims(u)
per default. The 0 frequency of u
must be located at the first entry.
We return two arguments: The first one is v_ft
(obtained by fft(v)
or rfft(v)
). The second return is the convolution function pconv
. pconv
itself has two arguments. pconv(u, v_ft=v_ft)
where u
is the object and v_ft
the v_ft. This function achieves faster convolution than conv(u, u)
. Depending whether u
is real or complex we do fft
s or rfft
s Additionally, it is possible to provide flags=FFTW.MEASURE
as kwargs
to change the planning of the FFT.
Examples
julia> u = [1 2 3 4 5]
1×5 Matrix{Int64}:
1 2 3 4 5
julia> v = [1 0 0 0 0]
1×5 Matrix{Int64}:
1 0 0 0 0
julia> v_ft, pconv = plan_conv(u, v);
julia> pconv(u, v_ft)
1×5 Matrix{Float64}:
1.0 2.0 3.0 4.0 5.0
julia> pconv(u)
1×5 Matrix{Float64}:
1.0 2.0 3.0 4.0 5.0
FourierTools.plan_conv_psf
— Functionplan_conv_psf(u, psf [, dims]; kwargs...) where {T, N}
plan_conv_psf
is a shorthand for plan_conv(u, ifftshift(psf))
. For examples see plan_conv
.
FourierTools.plan_conv_buffer
— Functionplan_conv_buffer(u, v [, dims]; kwargs...)
Similar to plan_conv
but instead uses buffers to prevent memory allocations. Not AD friendly!
FourierTools.plan_conv_psf_buffer
— Functionplan_conv_psf_buffer(u, psf [, dims]; kwargs...) where {T, N}
plan_conv_psf_buffer
is a shorthand for plan_conv_buffer(u, ifftshift(psf))
. For examples see plan_conv
.