Initial commit
new file: Copy_of_Exz_with_hamamatsu.m new file: Exz_mod.m new file: Exz_with_hamamatsu.m new file: GS.m new file: MRAF.m new file: MRAF_8bit.bmp new file: PSF of spherical aberration/Exz.m new file: PSF of spherical aberration/Thumbs.db new file: PSF of spherical aberration/josaa-12-10-2136.pdf new file: PSF of spherical aberration/josaa-12-2-325.pdf new file: PSF of spherical aberration/main.m new file: "PSF of spherical aberration/\351\207\215\350\246\201psf\346\226\207\347\214\256.pdf" new file: Spherical_aberration_SiminCao.m new file: gen_m.m new file: gen_rectangle.m new file: hamamatsu.m new file: m.tif new file: m2.tif new file: photo/50-30.BMP new file: photo/8bit_50-30.BMP new file: photo/8bit_ellipse.BMP new file: photo/convert_8bit.exe new file: photo/ellipse.BMP new file: rect_MRAF_SiminCao.m new file: rectangle.tif new file: size/.vscode/settings.json new file: size/black_c_20THSize_4f_1.064lamda.bmp new file: size/black_c_30THSize_4f_61.064lamda.bmp new file: size/black_output.bmp new file: size/black_rect_30THSize_4f_1.064lamda.bmp new file: size/black_rect_30THSize_4f_6_1.064lamda.bmp new file: size/c_20THSize_4f_1.064lamda.bmp new file: size/c_20THSize_4f_1.064lamda_resize.bmp new file: size/c_30THSize_4f_61.064lamda.bmp new file: size/c_30THSize_4f_61.064lamda_resize.bmp new file: size/noisy_output.bmp new file: size/output.bmp new file: size/rect_30THSize_4f_1.064lamda.bmp new file: size/rect_30THSize_4f_1.064lamda_resize.bmp new file: size/rect_30THSize_4f_6_1.064lamda.bmp new file: size/rect_30THSize_4f_6_1.064lamda_resize.bmp new file: size/resize_4.7z new file: size/resize_black.7z new file: size/size copy.py new file: size/size.py new file: size/wave.7z new file: sp.m new file: to8bit.m new file: trans_8bit.zip new file: wavef/A.bmp new file: wavef/B_linear.bmp new file: wavef/PHA SID230828-2003.csv new file: wavef/PHA_bilinear_1280_1024.csv new file: wavef/PHA_bilinear_reversal.csv new file: wavef/PHA_output_1280_1024.csv new file: wavef/Untitled-1.py new file: wavef/filled.bmp new file: wavef/from PIL import Image.py new file: wavef/matrix_filled.csv new file: wavef/output.bmp new file: wavef/output.csv new file: wavef/output2.bmp new file: wavef/pha_wavef copy.py new file: wavef/pha_wavef.py new file: wavef/pha_wavef_step.py new file: wavef/wavef.zip new file: wavef/xy_values.csv new file: "wavef/\346\226\260\345\273\272\346\226\207\344\273\266\345\244\271/matrix.csv" new file: "wavef/\346\226\260\345\273\272\346\226\207\344\273\266\345\244\271/matrix_filled.csv"
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wxchen
87
rect_MRAF_SiminCao.m
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87
rect_MRAF_SiminCao.m
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%MARF algorithm for the generation of Holograms of arbitrary designed beam shape
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close all
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clear all
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clc
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m=0.5;%mixing parameter when iterating,if m=1,then it is totally GS algorithm 混合参数进行迭代时,如果m = 1,那么它是完全GS算法
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row=1280;%resolution of DOE in x direction
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column=1024;%resolution of DOE in y direction
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[x,y]=meshgrid(1:row,1:column);
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R=0.0003;%curvature of quadratic phase profile 二次相轮廓的曲率
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Alpha=0.5;%aspect ratio of quadratic phase profile 二次相轮廓的长宽比
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Phase=zeros(column,row);%initial phase 初始相位i
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K1=zeros(column,row);
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for j=1:row
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for k=1:column
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K1(k,j)=4*R*(Alpha*(j-row/2)^2+(1-Alpha)*(k-column/2)^2);%initial quadratic phase 最初的二次相
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Phase(k,j)=mod(K1(k,j),2*pi);
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end
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end
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figure,imshow(mod(Phase.*255./(2*pi),256),[0 255]);
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%初始相位图计算
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F=0.04; %矩形光斑区域占相位图比例
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w=F*row;
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h=w*30/50; %矩形长w,宽h
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for j=1:row
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for k=1:column
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if j>row/2-w/2&j<row/2+w/2&k>column/2-h/2&k<column/2+h/2
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Photo(k,j)=255;
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else
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Photo(k,j)=0;
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end
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end
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end
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A=Photo;%target pattern
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goals=double(A);%target pattern
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figure(),surfc(x,y,goals), title('Target intensity distribution'), colormap jet, axis equal, axis tight, view([45, 45]), shading interp
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SigRegion=((x-(row+1)/2).^2+(y-(column+1)/2).^2)./(2*w).^2; %信号区域尺寸是2w大小
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SigRegion(SigRegion<=1)=1;
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SigRegion(SigRegion>1)=0;
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A0=exp(-((x-row/2).^2+(y-column/2).^2)./(750^2));%Gaussian incident光斑大小该如何设置？
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Efficiency=[];%diffraction efficiency
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Accuracy=[];%accuracy of the generated laser pattern
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tic %tic/toc配合使用来计时
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h=waitbar(0,'Caculating ...');
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index=0;
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loop=100;%times of iterative
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for k=1:loop
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f=exp(1i.*Phase).*A0;
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f1=fftshift(fft2((fftshift(f))));
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f1=f1.*sqrt(sum(sum(abs(A0).^2))/sum(sum(abs(f1).^2)));
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% Factor=sqrt(sum(sum(abs(A0).^2))/sum(sum(abs(f1).^2)));
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% disp(Factor)
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f2=(m*sqrt(goals.*SigRegion)+(1-m)*abs(f1.*~SigRegion)).*exp(1i.*(angle(f1)));
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f3=fftshift(ifft2(ifftshift(f2)));
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Phase=angle(f3);
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Efficiency=[Efficiency sum(sum(abs(f1.*goals./255).^2))/sum(sum(abs(f1).^2))];
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fTarget=abs(f1).*goals./255;
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goals_u=1-((max((fTarget(:))))^2-(min((fTarget(fTarget~=0))))^2)./((max((fTarget(:))))^2+(min((fTarget(fTarget~=0))))^2); %均匀性计算
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Accuracy=[Accuracy goals_u];
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index=index+1;
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waitbar(index./loop); %进度条
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end
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close(h); %关闭进度条
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toc
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Intensity=abs(f1).^2./sum(sum(abs(f1).^2))*100000;
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figure(),surfc(x,y,Intensity), title('Simulated intensity distribution'), colormap jet, axis equal, axis tight, view([45, 45]), shading interp;
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figure(),imshow(abs(f1),[])
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figure,plot(Efficiency,'*'),title('efficiency');%Efficiency varies with iterative
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figure,plot(Accuracy,'*'),title('accuracy');%Accuracy varies with iterative
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Phase=Phase-min(min(Phase));
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Phase=mod(Phase,2*pi);
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hologram=round(Phase.*255./(2.*pi));
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figure(),imshow(hologram,[0 255]);
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imwrite(uint8(hologram),'MRAF.bmp');
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% Addition=zeros(1080,420);
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% hologramStandard=[Addition hologram Addition];
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% figure,imshow(hologramStandard,[]);
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% imwrite(uint8(hologram),'E:\CGH\MRAF\letter\APL\apl30点\holo\L1920_03.bmp');
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