diff options
author | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-05-16 16:09:53 -0400 |
---|---|---|
committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-05-16 16:09:53 -0400 |
commit | 5ae2b91ddda5583c8a24a28eb136ee08585a7125 (patch) | |
tree | 7a2eaeed3f2d246e0cc2c3feaa8a94c2f96be914 | |
parent | 24b48105c1c4ed1dcd3a0de68df91d7003b2789c (diff) | |
download | beam_reshape-5ae2b91ddda5583c8a24a28eb136ee08585a7125.tar.gz beam_reshape-5ae2b91ddda5583c8a24a28eb136ee08585a7125.zip |
addition of exact diffraction calculation
-rw-r--r-- | beam_intensity_at_point_from_image.m | 35 | ||||
-rw-r--r-- | demo_diffraction_on_a_disk.m | 43 | ||||
-rw-r--r-- | diffracted_image_at_target.m | 20 | ||||
-rw-r--r-- | gauss_diffraction_on_aperture.m | 28 | ||||
-rw-r--r-- | mask_transparency.m | 7 | ||||
-rw-r--r-- | show_diffraction.m | 29 |
6 files changed, 149 insertions, 13 deletions
diff --git a/beam_intensity_at_point_from_image.m b/beam_intensity_at_point_from_image.m new file mode 100644 index 0000000..f305d16 --- /dev/null +++ b/beam_intensity_at_point_from_image.m @@ -0,0 +1,35 @@ +function intensity=beam_intensity_at_point_from_image(x,y,z, img, xpos, ypos, lambda) + +[Ny,Nx] = size(img); + +xim=linspace(xpos(1), xpos(end), Nx); +yim=linspace(ypos(1), ypos(end), Ny); + +[ind_x, ind_y] = meshgrid(1:Nx, 1:Ny); +[rvec_x, rvec_y] = meshgrid(xim-x, yim-y); % rvec_x and rvec_y are matrices of Ny x Nx +rvec_z=z+rvec_x*0; % to get same matrix size as rvec_x and rvec_y + +dist=sqrt(rvec_x.^2+rvec_y.^2+rvec_z.^2); + + +E_ampl = img ./dist .* exp(1i*2*pi.*dist./lambda); + +% simple case: far field - Fraunhofer limit + +E_tot= (sum(E_ampl(:))); +intensity = E_tot*conj(E_tot); + +%%%% Below is exact case: Fresnel diffraction +%kvec_x= rvec_x./dist; +%kvec_y= rvec_y./dist; +%kvec_z= rvec_z./dist; +% +%Ex= E_ampl * kvec_x; +%Ey= E_ampl * kvec_y; +%Ez= E_ampl * kvec_z; +%% summing all E field components +%Ex_tot = sum (Ex(:)); +%Ey_tot = sum (Ey(:)); +%Ez_tot = sum (Ez(:)); +%intensity = Ex_tot*conj(Ex_tot) + Ey_tot*conj(Ey_tot) + Ez_tot*conj(Ez_tot); + diff --git a/demo_diffraction_on_a_disk.m b/demo_diffraction_on_a_disk.m new file mode 100644 index 0000000..49c2aff --- /dev/null +++ b/demo_diffraction_on_a_disk.m @@ -0,0 +1,43 @@ +% light wavelength +lambda=795e-9; % Rb D1 line + +% set up mask (source image) +Nx_s=301; +Ny_s=301; +img_source=zeros(Ny_s,Nx_s); + +src_size = 1.0*12.5e-3; +xpos_s=linspace( -src_size, src_size, Nx_s); +ypos_s=linspace( -src_size, src_size, Ny_s); + +[xmesh,ymesh]=meshgrid(xpos_s,ypos_s); +w=0.0014*3/2; +R=1; +z_before_mask=LaguerreGaussianE([0,0,q_(w,R,lambda),lambda],xmesh,ymesh,'cart'); + +% disk mask +mask_R = (w*0.33); +mask = mask_transparency(xmesh,ymesh, mask_R); + +% resulting field after mask +img_source= z_before_mask .* mask; +%img_source= z_before_mask; + + +% set up target image +Nx_t=101; +Ny_t=101; +img_t=zeros(Ny_t,Nx_t); +tgt_size = 2*12.5e-3; +xpos_t=linspace( -tgt_size, tgt_size, Nx_t); +ypos_t=linspace( -tgt_size, tgt_size, Ny_t); +z_t=10; + + +% generating image of the mask accounting the diffraction +tic; % start timer +img_t=diffracted_image_at_target(img_source, xpos_s, ypos_s, img_t, xpos_t, ypos_t, z_t, lambda); +toc % show evaluation time + +% plot source and target images +show_diffraction(img_source, xpos_s, ypos_s, img_t, xpos_t, ypos_t); diff --git a/diffracted_image_at_target.m b/diffracted_image_at_target.m new file mode 100644 index 0000000..afc92fd --- /dev/null +++ b/diffracted_image_at_target.m @@ -0,0 +1,20 @@ +function img_target = diffracted_image_at_target(img_source, xpos_s, ypos_s, image_target, xpos_t, ypos_t, z_t, lambda) + +[Ny,Nx]=size(image_target); + +xim_t=linspace(xpos_t(1), xpos_t(end), Nx); +yim_t=linspace(ypos_t(1), ypos_t(end), Ny); + +img_target=zeros(Ny, Nx); + +for i=1:Nx + for k=1:Ny + intensity = beam_intensity_at_point_from_image(xim_t(i), yim_t(k), z_t, img_source, xpos_s, ypos_s, lambda); + img_target(k,i) = intensity; + end +end + + + + + diff --git a/gauss_diffraction_on_aperture.m b/gauss_diffraction_on_aperture.m index 6f72e85..bd962f6 100644 --- a/gauss_diffraction_on_aperture.m +++ b/gauss_diffraction_on_aperture.m @@ -7,7 +7,6 @@ % the magnitude of the coefficients of the various modes in the
% decomposition.
-
ploton=[1 0];
overlaponly=0; showfigure=0;
@@ -16,14 +15,16 @@ clear domain; screensize=0.0125;
nptsr=500;
nptstheta=100;
-accuracy=0.001;
-n=30;
+accuracy=0.0001;
+n=50;
+
+
[rmesh,thetamesh,xmesh,ymesh]=polarmesh([0,screensize,nptsr],[0 2*pi nptstheta],'lin');
domain(:,:,1)=rmesh; domain(:,:,2)=thetamesh;
-w=0.002;
-R=-1e3;
+w=0.0014*3/2;
+R=1;
lambda=0.795e-6;
q=q_(w,R,lambda);
@@ -33,8 +34,9 @@ deltax=0; deltay=0;
wfactor=1;
-mask_R = (w/2);
-mask = 1.0*((xmesh.^2+ymesh.^2) > mask_R^2);
+mask_R = (w*0.33);
+mask = mask_transparency( xmesh, ymesh, mask_R );
+
%mask = 1.0;
if overlaponly
@@ -51,7 +53,7 @@ if overlaponly return
end
-z_before_mask=LaguerreGaussianE([0,0,q_(w*wfactor,R,lambda),lambda],xmesh+deltax,ymesh+deltay,'cart');
+z_before_mask=LaguerreGaussianE([0,0,q_(w,R,lambda),lambda],xmesh+deltax,ymesh+deltay,'cart');
zin=mask.*z_before_mask;
clear tmat tmat_in
tmat_in(1:n,1,1)=1;
@@ -111,7 +113,7 @@ if length(ploton)>=2 & ploton(2)==1 end
figure(3)
-z_test=LaguerreGaussianE([30,0,q_(w*wfactor,R,lambda),lambda],xmesh+deltax,ymesh+deltay,'cart');
+z_test=LaguerreGaussianE([100,0,q_(w,R,lambda),lambda],xmesh+deltax,ymesh+deltay,'cart');
h=pcolor(xmesh,ymesh,abs(z_test).^2); set(h,'edgecolor','none'); axis square; colorbar; drawnow; shg;
title('high order LG');
@@ -119,8 +121,8 @@ title('high order LG'); figure(4)
[rmesh,thetamesh,xmesh,ymesh]=polarmesh([0,screensize/10,nptsr],[0 2*pi nptstheta],'lin');
domain(:,:,1)=rmesh; domain(:,:,2)=thetamesh;
-mask = 1.0*((xmesh.^2+ymesh.^2) > mask_R^2);
-z_before_mask_magn=LaguerreGaussianE([0,0,q_(w*wfactor,R,lambda),lambda],xmesh+deltax,ymesh+deltay,'cart');
+mask = mask_transparency( xmesh, ymesh, mask_R );
+z_before_mask_magn=LaguerreGaussianE([0,0,q_(w,R,lambda),lambda],xmesh+deltax,ymesh+deltay,'cart');
zin_magn=mask.*z_before_mask_magn;
zout_magn=recompose(domain,'lg',coeffs,[q,lambda,accuracy]);
subplot(221);
@@ -142,8 +144,8 @@ figure(5) clear mask domain;
[rmesh,thetamesh,xmesh,ymesh]=polarmesh([0,screensize/5,nptsr],[0 2*pi 2],'lin');
domain(:,:,1)=rmesh; domain(:,:,2)=thetamesh;
-mask = 1.0*((xmesh.^2+ymesh.^2) > mask_R.^2);
-z_before_mask_magn=LaguerreGaussianE([0,0,q_(w*wfactor,R,lambda),lambda],xmesh,ymesh,'cart');
+mask = mask_transparency( xmesh, ymesh, mask_R );
+z_before_mask_magn=LaguerreGaussianE([0,0,q_(w,R,lambda),lambda],xmesh,ymesh,'cart');
zin_magn=mask.*z_before_mask_magn;
zout_magn=recompose(domain,'lg',coeffs,[q,lambda,accuracy]);
diff --git a/mask_transparency.m b/mask_transparency.m new file mode 100644 index 0000000..0a858bd --- /dev/null +++ b/mask_transparency.m @@ -0,0 +1,7 @@ +function mask = mask_transparency( xmesh, ymesh, mask_R )
+% mask_R is the radius of the aperture
+
+% solid disk mask
+mask = 1.0*((xmesh.^2+ymesh.^2) > mask_R^2);
+
+end
diff --git a/show_diffraction.m b/show_diffraction.m new file mode 100644 index 0000000..3421b0f --- /dev/null +++ b/show_diffraction.m @@ -0,0 +1,29 @@ +function show_diffraction(img_source, xpos_s, ypos_s, img_target, xpos_t, ypos_t) + +[Ny_s,Nx_s] = size(img_source); +[Ny_t,Nx_t] = size(img_target); + +% plot mask image +figure(1); +x_s=linspace(xpos_s(1), xpos_s(end), Nx_s); +y_s=linspace(ypos_s(1), ypos_s(end), Ny_s); +imagesc(x_s,y_s, abs(img_source).^2); +colorbar; colormap('gray'); +xlabel('x (m)'); +ylabel('y (m)'); +title('mask image'); + +% plot diffraction image +figure(2); +x_t=linspace(xpos_t(1), xpos_t(end), Nx_t); +y_t=linspace(ypos_t(1), ypos_t(end), Ny_t); +% I use gamma correction due to luck of the display dynamic range +% pixel brightness correction, display dependent +%gamma=1/4; +gamma=1; +imagesc(x_t, y_t, (abs(img_target).^2).^(gamma)); +colorbar; colormap('gray'); +xlabel('x (m)'); +ylabel('y (m)'); +title('target image'); + |