Index: /THZ_filters/2016_THz_FILTER_calculation/MF1.m
===================================================================
--- /THZ_filters/2016_THz_FILTER_calculation/MF1.m	(revision 733)
+++ /THZ_filters/2016_THz_FILTER_calculation/MF1.m	(revision 733)
@@ -0,0 +1,41 @@
+   clear all; close all; clc
+%inductive grating
+%phys. const
+c=299792458;%speed of light, m/s
+sigma=1.45e+6*1e-7*c*c;%stainless steel conductivity, [s]
+j=0;
+nu_filter=[20 23 24 25 26 27 30 40 50].*1e+9;
+nu=(0.001:0.01:1000)*1e+11;
+for f=nu_filter
+j=j+1;
+lamb0=c/f;
+ratio=0.02;%a/g ratio
+omega0=(1-0.27*(ratio));
+g=lamb0*omega0;
+a=ratio*g;%wire width
+
+
+
+disp(['g=' num2str(g*1e+3) 'mm a=' num2str(a*1e+3) 'mm nu=' num2str((1-0.27*ratio)*c/g*1e-9) ' GHz'])
+disp(['g=' num2str(round(g*1e+6)*1e-3) 'mm a=' num2str(round(a*1e+6)*1e-3) 'mm nu=' num2str((1-0.27*ratio)*c/g*1e-9) ' GHz'])
+disp(['Plate=' num2str(round(g*1e+6)*1e-3-2*round(a*1e+6)*1e-3) ' mm and ' num2str(round(1000/(round(g*1e+6)*1e-3))/10) ' squares on line'])
+disp(['  '])
+omega=nu*g/c;
+lamb=g./omega;
+eta=1/(1-2*ratio);
+R=eta./2.*sqrt(c./lamb./sigma);
+Om=lamb0./lamb-lamb./lamb0;
+ Z0=(2*log(csc(a*pi/(2*g))));
+t2=(R.^2+(Z0./Om).^2)./((1+R).^2+(Z0./Om).^2);
+
+
+semilogy(nu/1e+9,t2,'color',rand([1 3]),'linew',2)
+
+hold on
+end
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity')
+legend('20 GHz','23 GHz','24 GHz','25 GHz','26 GHz','27 GHz','30 GHz','40 GHz','50 GHz')
+grid on
+xlim([10 100])
Index: /THZ_filters/2017_THz_FILTER/Advantage_of_usage_double_filter.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/Advantage_of_usage_double_filter.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/Advantage_of_usage_double_filter.m	(revision 733)
@@ -0,0 +1,53 @@
+   clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=90;
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+Thet=pi/180*0;
+SPlam=c/50e+9;
+figure
+hold on
+for cc=1:length(SPlam)
+
+a=1e-4;
+b=1e-4;
+g=(SPlam(cc)+4*a+2*b)/2.27;
+disp(['g=' num2str(round(g*1e+4)/10) ' a=' num2str(a*1e+3) ' b=' num2str(b*1e+3) ' Freq=' num2str(round(c/SPlam(cc)*1e-9)) 'GHz' ])
+
+d=g/2;
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:20e+10;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+   Stot3= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)*S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+
+   Stot2= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+    Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt)=abs(1./Stot(2,2))^2;
+TTE2(cnt)=abs(1./Stot2(2,2))^2;
+TTE3(cnt)=abs(1./Stot3(2,2))^2;
+
+TTM(cnt)=abs(1./Stot(4,4))^2;
+end
+plot(FreqArr*1e-9,TTE,'-b','linew',2)
+plot(FreqArr*1e-9,TTE2,'-k','linew',2)
+plot(FreqArr*1e-9,TTE3,'-r','linew',2)
+
+end
+%  Ttot=sin(Thetp).^2.*TTE+cos(Thetp).^2.*TTM;
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('Cross filter 50GHz')
+legend('Single filter','Double filter','Triple filter')
Index: /THZ_filters/2017_THz_FILTER/OverlapCorrections.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/OverlapCorrections.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/OverlapCorrections.m	(revision 733)
@@ -0,0 +1,73 @@
+clear all; close all; clc
+phi=-10:0.1:10;%azimutal angle deg
+ dthet=-10:0.1:10;%polar angle deg, (shift from optic axis of the mirror)
+FWHM=[];
+
+lefts=[];
+rights=[];
+shift=3
+ for Thet=((48:7:125)+shift)
+
+
+
+for c=1:length(dthet)
+Lamb=6*(1-cos((Thet+dthet(c))/180*pi));
+R=Lamb/2;%focal spot (Abbe diffraction limit)
+r=1;%detector radius
+d=50.8*sqrt(tan(phi/180*pi).^2+tan(dthet(c)/180*pi).^2);
+A=@(x,y)x^2*acos(y./x)-y.*sqrt(x^2-y.^2);
+d1=(d.^2-r^2+R^2)./(2*d);
+d2=d-d1;
+Cs=A(R,d1)+A(r,d2);%sum of two lengthes
+
+Map(c,:)=real(Cs);
+end 
+figure
+contourf(dthet,phi,Map')
+xlabel('\Theta')
+ylabel('\phi')
+title(num2str(Thet))
+ FWHM=[FWHM,length(Map(101,(Map(101,:)>0.5*max(max(Map)))))*0.1];
+lefts=[lefts,find(Map(101,:)>0.5*max(max(Map)),1)];
+tmp=find(Map(101,:)>0.5*max(max(Map)));
+rights=[rights,tmp(end)];
+
+%  save(['map' num2str(Thet) '.mat'],'Map')
+ end
+ FWHM2=(rights-lefts+1)*0.1;
+R= (rights*0.1+((48:7:125)+shift)-10);
+L= (lefts*0.1+((48:7:125)+shift)-10);
+
+FreqR=3e+8./(6e-3*(1-cos(R/180*pi)));
+FreqL=3e+8./(6e-3*(1-cos(L/180*pi)));
+
+
+
+save freqp3.mat FreqR FreqL
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
Index: /THZ_filters/2017_THz_FILTER/S.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/S.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/S.m	(revision 733)
@@ -0,0 +1,14 @@
+%Filter matrix
+function Sn1n2=S(freq, Thet, g, a, b, n1, n2)
+c=299792458;
+a1=1e-4;
+A1=0.53;
+
+lamr=2.27*g-4*a-2*b;%resonant wavelength
+lamr=lamr*sqrt((n1^2+n2^2)/2);%used only in Omega
+Omega=lamr*freq/c-c./(lamr*freq);
+
+Y=1./(a1-1i.*g*A1./(lamr.*Omega));
+ YTM=Y.*cos(Thet);%TM % some problem of mixind TE and TM
+ YTE=Y./cos(Thet);%TE
+ Sn1n2=(1/(2*n1)).*[-YTE+(n1+n2) -YTE+(n1-n2) 0 0; YTE+(n1-n2) YTE+(n1+n2) 0 0; 0 0 -YTM+(n1+n2) -YTM+(n1-n2); 0 0 YTM+(n1-n2) YTM+(n1+n2) ];
Index: /THZ_filters/2017_THz_FILTER/T.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/T.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/T.m	(revision 733)
@@ -0,0 +1,5 @@
+%propagation matrix
+function Tmtx=T(freq,loss,d,n)
+c=299792458;
+
+Tmtx=exp(-loss*d).*[exp(-2*pi*1i*freq*d*n/c) 0 0 0;0 exp(2*pi*1i*freq*d*n/c) 0 0 ; 0 0 exp(-2*pi*1i*freq*d*n/c) 0; 0 0 0 exp(2*pi*1i*freq*d*n/c)];
Index: /THZ_filters/2017_THz_FILTER/Test_filters.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/Test_filters.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/Test_filters.m	(revision 733)
@@ -0,0 +1,81 @@
+   clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=90;
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+Thet=pi/180*0;
+% 48:7:125
+% SPlam=(6e-3*(1-cos(( 48:7:125)/180*pi)));
+% SPlam=c/2.99855e+9;
+SPlam=c./([ 20 24 27  30  32 34 37   40  50  66  94 ]*1e+9);
+color=colormap(jet(length(SPlam)));
+figure(1)
+hold on
+FreqArr=1e+9:1e+8:300e+9;
+
+sigma24=0.11e+9;
+gauss24=1/sqrt(2*pi*sigma24^2)*exp(-(FreqArr-24e+9).^2./(2*sigma24^2));
+% plot(FreqArr*1e-9,gauss24./max(gauss24),'-k','linew',2)
+sigma35=0.11e+9;
+gauss35=1/sqrt(2*pi*sigma35^2)*exp(-(FreqArr-32e+9).^2./(2*sigma35^2));
+for cc=1:length(SPlam)
+
+a=1e-4;
+b=1e-4;
+g=(SPlam(cc)+4*a+2*b)/2.27;
+disp(['g=' num2str(round(g*1e+4)/10) ' a=' num2str(a*1e+3) ' b=' num2str(b*1e+3) ' Freq=' num2str(round(c/SPlam(cc)*1e-9)) 'GHz' ])
+
+d=g/2;
+loss=0;
+c=3e+8;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+    Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt)=abs(1./Stot(4,4))^2;
+end
+plot(FreqArr*1e-9,TTE,'color',color(end-cc+1,:),'linew',2)
+
+Trans24(cc)=sum(TTE.*gauss24*1e+8);
+Trans35(cc)=sum(TTE.*gauss35*1e+8);
+legendInfo{cc} = ['\lambda= ' num2str(round(SPlam(cc)*1e+4)*1e-1) ' mm']; % or whatever is appropriate
+
+end
+% Ttot=sin(Thetp).^2.*TOP+cos(Thetp).^2.*TIP;
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('Cross filters, a=b=0.1 mm')
+legend(legendInfo,'location','northwest')
+
+ set(gca,'xscale','log')
+ xlim([1 200])
+figure
+hold on
+plot(c./SPlam*1e-9,Trans24,'-or','linew',2)
+plot(c./SPlam*1e-9,Trans35,'-ok','linew',2)
+grid on
+
+set(gca,'fontsize',16)
+xlabel('Filter frequency, [GHz]')
+ylabel('Transmission, [1]')
+title('Cross filters')
+legend('24 GHz','35 GHz','location','northeast')
+
+Trans32=Trans35
+% save dataT.mat Trans24 Trans35
+save dataT32.mat Trans32
+
+
+
Index: /THZ_filters/2017_THz_FILTER/Test_filters_ab.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/Test_filters_ab.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/Test_filters_ab.m	(revision 733)
@@ -0,0 +1,77 @@
+   clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=90;
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+Thet=pi/180*0;
+FreqGHz=50;
+Aarr=[0.1 0.5 1 2 3 5 ]*1e-3;
+color=colormap(jet(length(Aarr)));
+figure(1)
+hold on
+FreqArr=1e+9:1e+8:400e+9;
+sigma24=0.11e+9;
+gauss24=1/sqrt(2*pi*sigma24^2)*exp(-(FreqArr-24e+9).^2./(2*sigma24^2));
+% plot(FreqArr*1e-9,gauss24./max(gauss24),'-k','linew',2)
+sigma35=0.11e+9;
+gauss35=1/sqrt(2*pi*sigma35^2)*exp(-(FreqArr-32e+9).^2./(2*sigma35^2));
+for cc=1:length(Aarr)
+
+a=Aarr(cc);
+b=Aarr(cc);
+g=(c/(FreqGHz*1e+9)+4*a+2*b)/2.27;
+disp(['g=' num2str(round(g*1e+4)/10) ' a=' num2str(a*1e+3) ' b=' num2str(b*1e+3) ' Freq=' num2str(FreqGHz) 'GHz' ])
+d=g/2;
+loss=0;
+c=3e+8;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+    Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt)=abs(1./Stot(4,4))^2;
+end
+plot(FreqArr*1e-9,TTE,'color',color(end-cc+1,:),'linew',2)
+
+Trans24(cc)=sum(TTE.*gauss24*1e+8);
+Trans35(cc)=sum(TTE.*gauss35*1e+8);
+legendInfo{cc} = ['a=b= ' num2str(Aarr(cc)*1e+3) ' mm']; % or whatever is appropriate
+
+end
+% Ttot=sin(Thetp).^2.*TOP+cos(Thetp).^2.*TIP;
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('Cross filters (50 GHz)')
+legend(legendInfo,'location','northeast')
+
+figure
+hold on
+plot(Aarr*1e+3,Trans24,'-or','linew',2)
+plot(Aarr*1e+3,Trans35,'-ok','linew',2)
+grid on
+
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('a (b), [mm]')
+ylabel('Transmission, [1]')
+title('Cross filters (50 GHz)')
+legend('24 GHz','35 GHz','location','northwest')
+
+Trans24ab =Trans24(1:end-1);
+Trans35ab =Trans35(1:end-1);
+Trans32ab =Trans35(1:end-1);
+
+% save dataTab.mat Trans24ab Trans35ab
+save dataTab32.mat Trans32ab
+
Index: /THZ_filters/2017_THz_FILTER/Untitled Folder/cross_filter_double2.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/Untitled Folder/cross_filter_double2.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/Untitled Folder/cross_filter_double2.m	(revision 733)
@@ -0,0 +1,46 @@
+ clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=0;
+
+a1=1e-4;
+A1=0.53;
+
+
+Thet=pi/180*0;
+garr=(0:0.05:1)*4e-3;
+for cnt2=1:length(garr)
+g=4e-3;
+a=garr(cnt2);;
+b=1e-4;
+d=g/2;
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:4e+11;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+%  Stot= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+  Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt2,cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt2,cnt)=abs(1./Stot(4,4))^2;
+end
+end
+% Ttot=sin(Thetp).^2.*TOP+cos(Thetp).^2.*TIP;
+% figure
+% 
+% semilogy(FreqArr,TTE,'k')
+% hold on
+% 
+% semilogy(FreqArr,TTM,'r')
+figure
+[hc,hc]=contourf(FreqArr*1e-9,garr,TTE);
+set(hc,'LineStyle','none');
+colorbar
+3e+8./(6e-3*(1-cos((48:7:125)/180*pi)))*1e-9
+
+
Index: /THZ_filters/2017_THz_FILTER/Untitled Folder/cross_filter_double3.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/Untitled Folder/cross_filter_double3.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/Untitled Folder/cross_filter_double3.m	(revision 733)
@@ -0,0 +1,51 @@
+ clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=0;
+
+a1=1e-4;
+A1=0.53;
+
+g=4e-3;
+
+
+Thet=pi/180*0;
+garr=(0:0.05:0.5)*g;
+parr=(0:0.05:0.5)*g;
+for cnt3=1:length(parr)
+
+for cnt2=1:length(garr)
+a=garr(cnt2);
+b=parr(cnt3);
+d=g/2;
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:1e+11;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+%  Stot= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+  Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt2,cnt3,cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt2,cnt3,cnt)=abs(1./Stot(4,4))^2;
+end
+end
+end
+% Ttot=sin(Thetp).^2.*TOP+cos(Thetp).^2.*TIP;
+% figure
+% 
+% semilogy(FreqArr,TTE,'k')
+% hold on
+% 
+% semilogy(FreqArr,TTM,'r')
+
+xslice = garr(1:4:end); 
+yslice = parr(1:4:end); 
+zslice = 1e+9;
+slice(garr,parr,FreqArr,TTE,xslice,yslice,zslice)
+shading flat
+
Index: /THZ_filters/2017_THz_FILTER/cross_filter.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/cross_filter.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/cross_filter.m	(revision 733)
@@ -0,0 +1,46 @@
+   clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=90;
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+Thet=pi/180*0;
+SPlam=c/2.99855e+9;
+figure
+hold on
+for cc=1:length(SPlam)
+
+a=1e-4;
+b=1e-4;
+g=(SPlam(cc)+4*a+2*b)/2.27;
+disp(['g=' num2str(round(g*1e+4)/10) ' a=' num2str(a*1e+3) ' b=' num2str(b*1e+3) ' Freq=' num2str(round(c/SPlam(cc)*1e-9)) 'GHz' ])
+
+d=g/2;
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:1e+10;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+  % Stot= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+    Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt)=abs(1./Stot(4,4))^2;
+end
+plot(FreqArr*1e-9,TTE,'-k','linew',2)
+
+end
+%  Ttot=sin(Thetp).^2.*TTE+cos(Thetp).^2.*TTM;
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('Single cross filter 3GHz')
Index: /THZ_filters/2017_THz_FILTER/cross_filter_2d_g.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/cross_filter_2d_g.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/cross_filter_2d_g.m	(revision 733)
@@ -0,0 +1,66 @@
+ clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=0;
+
+a1=1e-4;
+A1=0.53;
+
+
+Thet=pi/180*0;
+darr=(0:0.05:8)*1e-3;
+for cnt2=1:length(darr)
+g=2.9e-3;
+a=1e-4;
+b=1e-4;
+d=darr(cnt2);
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:1e+11;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+ Stot= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+%  Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt2,cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt2,cnt)=abs(1./Stot(4,4))^2;
+end
+end
+% Ttot=sin(Thetp).^2.*TOP+cos(Thetp).^2.*TIP;
+% figure
+% 
+% semilogy(FreqArr,TTE,'k')
+% hold on
+% 
+% semilogy(FreqArr,TTM,'r')
+figure
+[hc,hc]=contourf(FreqArr*1e-9,darr/g,TTE);
+set(hc,'LineStyle','none');
+colorbar
+
+set(gca,'fontsize',16)
+ylabel('d/g, [1]')
+xlabel('Frequency, [GHz]')
+title('Double cross filter transmissivity')
+
+% 3e+8./(6e-3*(1-cos((48:7:125)/180*pi)))*1e-9
+% 
+% 
+% for cnt2=1:length(darr)
+% 
+% Px=(TTE(cnt2,:));
+% fwm(cnt2)=length(Px(Px>0.5*max(Px)));
+% Px2=(TTE(cnt2,1:600));
+% 
+% fwhm(cnt2)=length(Px2(Px2>0.5));
+% 
+% end
+% figure
+% hold on
+% plot(darr,fwm)
+% plot(darr,fwhm,'k')
+
Index: /THZ_filters/2017_THz_FILTER/cross_filter_CLIO.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/cross_filter_CLIO.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/cross_filter_CLIO.m	(revision 733)
@@ -0,0 +1,111 @@
+   clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=90;
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+Thet=pi/180*0;
+Ang=48:7:125;
+ SPlam=(6e-3*(1-cos(( Ang)/180*pi)));
+color=colormap(jet(length(SPlam)));
+
+
+figure(1)
+hold on
+for cc=1:length(SPlam)
+
+a=1e-4;
+b=1e-4;
+g=(SPlam(cc)+4*a+2*b)/2.27;
+disp(['g=' num2str(round(g*1e+4)/10) ' a=' num2str(a*1e+3) ' b=' num2str(b*1e+3) ' Freq=' num2str(round(c/SPlam(cc)*1e-9)) 'GHz' ])
+
+ d=g/2;
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:4e+11;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+    Stot= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+%     Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt)=abs(1./Stot(4,4))^2;
+end
+ plot(FreqArr*1e-9,TTE,'color',color(cc,:),'linew',2)
+% [~,pks]=findpeaks(TTE);
+%  Px=TTE(1:round((pks(2)+pks(1))/2));
+[~,mxp]=max(TTE);
+ Px=TTE(1:round(1.9*mxp));
+fwhm(cc)=length(Px(Px>0.5))*1e+8;
+legendInfo{cc} = ['\lambda= ' num2str(round(SPlam(cc)*1e+4)*1e-1) ' mm']; % or whatever is appropriate
+load freq.mat
+Frange=(FreqArr>FreqR(cc))&(FreqArr<FreqL(cc));
+FilterFiltering(cc)=sum(TTE(Frange))/sum(Frange);
+load freqm3.mat
+Frange=(FreqArr>FreqR(cc))&(FreqArr<FreqL(cc));
+FilterFilteringm3(cc)=sum(TTE(Frange))/sum(Frange);
+load freqp3.mat
+Frange=(FreqArr>FreqR(cc))&(FreqArr<FreqL(cc));
+FilterFilteringp3(cc)=sum(TTE(Frange))/sum(Frange);
+end
+% Ttot=sin(Thetp).^2.*TOP+cos(Thetp).^2.*TIP;
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('Cross filters')
+% legend(legendInfo,'location','northwest')
+
+
+% plot(FreqArr*1e-9,TTM,'r')
+
+FreqGHz=3e+8./SPlam*1e-9;
+% FreqR=3e+8./(6e-3*(1-cos(( Ang-3)/180*pi)))
+% FreqL=3e+8./(6e-3*(1-cos(( Ang+3)/180*pi)))
+
+for k=1:length(FreqGHz)
+    
+%     plot([FreqGHz(k) FreqGHz(k)],[0 1],'k','linew',2) 
+%     plot([FreqR(k) FreqR(k)]*1e-9,[0 1],'color',color(k,:),'linew',1) 
+%     plot([FreqL(k) FreqL(k)]*1e-9,[0 1],'color',color(k,:),'linew',1) 
+%    plot([FreqR2(k) FreqR2(k)]*1e-9,[0 1],'color',color(k,:),'linew',1) 
+%    plot([FreqL2(k) FreqL2(k)]*1e-9,[0 1],'color',color(k,:),'linew',1) 
+
+end
+%  set(gca,'xscale','log')
+
+% % figure
+% % plot(FreqGHz,fwhm./FreqGHz*1e-9,'-or')
+
+figure
+hold on
+plot(FreqR(1:11)*1e-9,FreqL(2:12)*1e-9)
+plot(1:150,1:150,'r')
+
+xlim([0 150])
+ylim([0 150])
+grid on
+
+
+figure
+hold on
+
+plot(FreqGHz,FilterFiltering,'-or','linew',2)
+plot(FreqGHz,FilterFilteringm3,'-ok','linew',2)
+plot(FreqGHz,FilterFilteringp3,'-ob','linew',2)
+ylim([0 1])
+xlim([30 155])
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Cut ratio, [1]')
+legend('Correct position','-3^o shift','+3^o shift','location','southwest')
Index: /THZ_filters/2017_THz_FILTER/expresult.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/expresult.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/expresult.m	(revision 733)
@@ -0,0 +1,54 @@
+clear all; close all;
+Freq=[20 24 27 30 32 34 37 40 50 66 94];
+ap=[0.1 0.5 1 2 3];
+L35=[32 71 117 201 267 203 111 101 31 13 9]/301;
+R35=[35 81 127 221 277 213 119 113 43 25 17]/313;
+La35=[31 69 85 145 147]/301;
+Ra35=[43 79 95 155 157]/313;
+L24=[111 269 171 133 115 111 91 89 69 51 57]/281;
+R24=[121 277 181 143 125 123 103 103 79 61 67]/293;
+La24=[69 93 95 135 167]/281;
+Ra24=[73 103 105 149 177]/293;
+
+T35=(R35+L35)/2;
+ET35=(R35-L35)/2;
+T35a=(Ra35+La35)/2;
+ET35a=(Ra35-La35)/2;
+
+T24=(R24+L24)/2;
+ET24=(R24-L24)/2;
+T24a=(Ra24+La24)/2;
+ET24a=(Ra24-La24)/2;
+load dataT.mat
+load dataT32.mat
+load dataTab32.mat
+load dataTab.mat
+figure(1)
+hold on
+errorbar(Freq,T24,ET24,'-.r','linew',2)
+errorbar(Freq,T35,ET35,'-.k','linew',2)
+plot(Freq, Trans24,'-^r','linew',2)
+plot(Freq, Trans35,'-^k','linew',2)
+plot(Freq, Trans32,'-^b','linew',2)
+
+grid on
+set(gca,'fontsize',16)
+legend(' Exp. 24 GHz','Exp. 35 GHz','Calc. 24 GHz','Calc. 35 GHz','Calc. 32 GHz')
+xlabel('Filter frequency, [GHz]')
+ylabel('Transmission, [1]')
+title('Cross filters')
+
+figure(2)
+hold on
+errorbar(ap,T24a,ET24a,'-.r','linew',2)
+errorbar(ap,T35a,ET35a,'-.k','linew',2)
+plot(ap, Trans24ab,'-^r','linew',2)
+plot(ap, Trans35ab,'-^k','linew',2)
+plot(ap, Trans32ab,'-^b','linew',2)
+
+grid on
+set(gca,'fontsize',16)
+legend(' Exp. 24 GHz','Exp. 35 GHz','Calc. 24 GHz','Calc. 35 GHz','Calc. 32 GHz','location','northwest')
+xlabel('a (b), [mm]')
+ylabel('Transmission, [1]')
+title('Cross filters (50 GHz)')
Index: /THZ_filters/2017_THz_FILTER/readme.txt
===================================================================
--- /THZ_filters/2017_THz_FILTER/readme.txt	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/readme.txt	(revision 733)
@@ -0,0 +1,10 @@
+Test_filters.m -- calculation of filters with fixed a and b for different frequencies for test sources
+Test_filters_ab.m -- fixed filter frequency and change a&b
+S.m T.m -- required files for matrix calculation
+freq.mat -- data with aperture limits
+OverlapCorrections.m -- take apperture limits
+cross_filter_2d_g.m -- dependence from second filter position
+cross_filter.m - 3GHz filter 
+cross_filter_CLIO.m -- calculation for small filters
+
+test_param.m and test_param_2d_ab.m plot figures for report showing the behawiour of fwhm of T from change of a and b.
Index: /THZ_filters/2017_THz_FILTER/results.txt
===================================================================
--- /THZ_filters/2017_THz_FILTER/results.txt	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/results.txt	(revision 733)
@@ -0,0 +1,31 @@
+g=2.9 a=0.1 b=0.1 Freq=50GHz
+g=4 a=0.5 b=0.5 Freq=50GHz
+g=5.3 a=1 b=1 Freq=50GHz
+g=7.9 a=2 b=2 Freq=50GHz
+g=10.6 a=3 b=3 Freq=50GHz
+g=15.9 a=5 b=5 Freq=50GHz
+
+g=6.9 a=0.1 b=0.1 Freq=20GHz
+g=5.8 a=0.1 b=0.1 Freq=24GHz
+g=5.2 a=0.1 b=0.1 Freq=27GHz
+g=4.7 a=0.1 b=0.1 Freq=30GHz
+g=4.4 a=0.1 b=0.1 Freq=32GHz
+g=4.1 a=0.1 b=0.1 Freq=34GHz
+g=3.8 a=0.1 b=0.1 Freq=37GHz
+g=3.6 a=0.1 b=0.1 Freq=40GHz
+g=2.9 a=0.1 b=0.1 Freq=50GHz
+g=2.3 a=0.1 b=0.1 Freq=66GHz
+g=1.7 a=0.1 b=0.1 Freq=94GHz
+
+g=1.1 a=0.1 b=0.1 Freq=151GHz
+g=1.4 a=0.1 b=0.1 Freq=117GHz
+g=1.7 a=0.1 b=0.1 Freq=94GHz
+g=2 a=0.1 b=0.1 Freq=78GHz
+g=2.3 a=0.1 b=0.1 Freq=66GHz
+g=2.6 a=0.1 b=0.1 Freq=57GHz
+g=2.9 a=0.1 b=0.1 Freq=50GHz
+g=3.2 a=0.1 b=0.1 Freq=45GHz
+g=3.5 a=0.1 b=0.1 Freq=40GHz
+g=3.9 a=0.1 b=0.1 Freq=37GHz
+g=4.1 a=0.1 b=0.1 Freq=34GHz
+g=4.4 a=0.1 b=0.1 Freq=32GHz
Index: /THZ_filters/2017_THz_FILTER/test_param.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/test_param.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/test_param.m	(revision 733)
@@ -0,0 +1,51 @@
+   clear all; close all; clc
+%% Double Cross filter 
+n1=1;
+n2=1;
+n=1;%ref. indx of media between filters
+Thetp=90;
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+Thet=pi/180*0;
+SPlam=c/50e+9;
+aar=[0.01 0.1 1 2 5]*1e-3;
+color=colormap(jet(length(aar)));
+
+figure
+hold on
+for cc=1:length(aar)
+
+b=aar(cc);
+a=1e-4;
+g=(SPlam+4*a+2*b)/2.27;
+disp(['g=' num2str(round(g*1e+4)/10) ' a=' num2str(a*1e+3) ' b=' num2str(b*1e+3) ' Freq=' num2str(round(c/SPlam*1e-9)) 'GHz' ])
+
+d=g/2;
+loss=0;
+c=3e+8;
+FreqArr=1e+9:1e+8:2e+11;
+for cnt=1:length(FreqArr)
+
+freq=FreqArr(cnt);
+
+  % Stot= S(freq, Thet, g, a, b, n1, n2)*T(freq,loss,d,n)* S(freq, Thet, g, a, b, n1, n2);
+    Stot=  S(freq, Thet, g, a, b, n1, n2);
+
+TTE(cnt)=abs(1./Stot(2,2))^2;
+TTM(cnt)=abs(1./Stot(4,4))^2;
+end
+ plot(FreqArr*1e-9,TTE,'color',color(cc,:),'linew',2)
+legendInfo{cc} = ['b= ' num2str(aar(cc)*1e+3) ' mm']; % or whatever is appropriate
+
+end
+%  Ttot=sin(Thetp).^2.*TTE+cos(Thetp).^2.*TTM;
+grid on
+set(gca,'fontsize',16)
+% set(gca,'xscale','log')
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('Single cross filter 50GHz')
+legend(legendInfo,'location','northeast')
Index: /THZ_filters/2017_THz_FILTER/test_param_2d_ab.m
===================================================================
--- /THZ_filters/2017_THz_FILTER/test_param_2d_ab.m	(revision 733)
+++ /THZ_filters/2017_THz_FILTER/test_param_2d_ab.m	(revision 733)
@@ -0,0 +1,34 @@
+   clear all; close all; clc
+%% Double Cross filter 
+
+a1=1e-4;
+A1=0.53;
+
+c=299792458;
+SPlam=c/100e+9;
+aar=(0.1:0.2:5)*1e-3;
+bar=(0.1:0.2:5)*1e-3;
+
+
+for cc=1:length(aar)
+for ck=1:length(bar)
+
+a=aar(cc);
+b=bar(ck);
+g=(SPlam+4*a+2*b)/2.27;
+
+FreqArr=1e+9:1e+8:2e+11;
+for cnt=1:length(FreqArr)
+Stot=  S(FreqArr(cnt), 0, g, a, b, 1, 1);
+TTE(cnt)=abs(1./Stot(2,2))^2;
+end
+Rez(cc,ck)=sum(TTE>0.5)*1e+8;
+end
+end
+[hC hC] =contourf(aar*1e+3,bar*1e+3,Rez'.*1e-9)
+ set(hC,'LineStyle','none');
+colorbar
+set(gca,'fontsize',16)
+xlabel('a, [mm]')
+ylabel('b, [mm]')
+title('100 GHz, FWHM of transmittance, [GHz]')
Index: /THZ_filters/CrossReport/Report.aux
===================================================================
--- /THZ_filters/CrossReport/Report.aux	(revision 733)
+++ /THZ_filters/CrossReport/Report.aux	(revision 733)
@@ -0,0 +1,62 @@
+\relax 
+\providecommand\hyper@newdestlabel[2]{}
+\providecommand\HyperFirstAtBeginDocument{\AtBeginDocument}
+\HyperFirstAtBeginDocument{\ifx\hyper@anchor\@undefined
+\global\let\oldcontentsline\contentsline
+\gdef\contentsline#1#2#3#4{\oldcontentsline{#1}{#2}{#3}}
+\global\let\oldnewlabel\newlabel
+\gdef\newlabel#1#2{\newlabelxx{#1}#2}
+\gdef\newlabelxx#1#2#3#4#5#6{\oldnewlabel{#1}{{#2}{#3}}}
+\AtEndDocument{\ifx\hyper@anchor\@undefined
+\let\contentsline\oldcontentsline
+\let\newlabel\oldnewlabel
+\fi}
+\fi}
+\global\let\hyper@last\relax 
+\gdef\HyperFirstAtBeginDocument#1{#1}
+\providecommand\HyField@AuxAddToFields[1]{}
+\providecommand\HyField@AuxAddToCoFields[2]{}
+\citation{cros}
+\citation{cros}
+\citation{cros}
+\citation{cros}
+\providecommand\tcolorbox@label[2]{}
+\select@language{english}
+\@writefile{toc}{\select@language{english}}
+\@writefile{lof}{\select@language{english}}
+\@writefile{lot}{\select@language{english}}
+\@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}{section.1}}
+\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Cross-mesh filters layout (from \cite  {cros})\relax }}{1}{figure.caption.1}}
+\providecommand*\caption@xref[2]{\@setref\relax\@undefined{#1}}
+\newlabel{cfy}{{1}{1}{Cross-mesh filters layout (from \cite {cros})\relax }{figure.caption.1}{}}
+\@writefile{toc}{\contentsline {section}{\numberline {2}Matrix methods}{1}{section.2}}
+\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Equivalent circuit of cross filter (from \cite  {cros})\relax }}{2}{figure.caption.2}}
+\newlabel{ecc}{{2}{2}{Equivalent circuit of cross filter (from \cite {cros})\relax }{figure.caption.2}{}}
+\newlabel{ta}{{3a}{2}{Change of transmissivity as function of geometrical parameter a \relax }{figure.caption.3}{}}
+\newlabel{sub@ta}{{a}{2}{Change of transmissivity as function of geometrical parameter a \relax }{figure.caption.3}{}}
+\newlabel{tb}{{3b}{2}{Change of transmissivity as function of geometrical parameter b\relax }{figure.caption.3}{}}
+\newlabel{sub@tb}{{b}{2}{Change of transmissivity as function of geometrical parameter b\relax }{figure.caption.3}{}}
+\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces \relax }}{2}{figure.caption.3}}
+\@writefile{toc}{\contentsline {section}{\numberline {3}Proposed experimental check of filter properties}{3}{section.3}}
+\newlabel{p1t}{{4a}{3}{Transmissivity functions for different test wavelengths\relax }{figure.caption.4}{}}
+\newlabel{sub@p1t}{{a}{3}{Transmissivity functions for different test wavelengths\relax }{figure.caption.4}{}}
+\newlabel{p1r}{{4b}{3}{Transmission for different filter with present sources\relax }{figure.caption.4}{}}
+\newlabel{sub@p1r}{{b}{3}{Transmission for different filter with present sources\relax }{figure.caption.4}{}}
+\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces First part of experiment: check transmission\relax }}{3}{figure.caption.4}}
+\newlabel{p2t}{{5a}{3}{Transmissivity functions for different filter parameters\relax }{figure.caption.5}{}}
+\newlabel{sub@p2t}{{a}{3}{Transmissivity functions for different filter parameters\relax }{figure.caption.5}{}}
+\newlabel{p2r}{{5b}{3}{Transmission for different filter with present sources\relax }{figure.caption.5}{}}
+\newlabel{sub@p2r}{{b}{3}{Transmission for different filter with present sources\relax }{figure.caption.5}{}}
+\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces Second part of experiment: check filters parameters dependence\relax }}{3}{figure.caption.5}}
+\@writefile{toc}{\contentsline {section}{\numberline {4}Multiple filters}{4}{section.4}}
+\newlabel{ond}{{6a}{4}{Transmissivity function of single, double and triple cross filters\relax }{figure.caption.6}{}}
+\newlabel{sub@ond}{{a}{4}{Transmissivity function of single, double and triple cross filters\relax }{figure.caption.6}{}}
+\newlabel{gg}{{6b}{4}{Change of transmissivity function for double cross filters as function of filters separation\relax }{figure.caption.6}{}}
+\newlabel{sub@gg}{{b}{4}{Change of transmissivity function for double cross filters as function of filters separation\relax }{figure.caption.6}{}}
+\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces Multiple filters\relax }}{4}{figure.caption.6}}
+\bibcite{cros}{1}
+\@writefile{toc}{\contentsline {section}{\numberline {5}CLIO filters}{5}{section.5}}
+\@writefile{lof}{\contentsline {figure}{\numberline {7}{\ignorespaces Transmissivity functions of cross filters for Smith-Purcell experiment at CLIO.\relax }}{5}{figure.caption.7}}
+\newlabel{clioT}{{7}{5}{Transmissivity functions of cross filters for Smith-Purcell experiment at CLIO.\relax }{figure.caption.7}{}}
+\@writefile{lof}{\contentsline {figure}{\numberline {8}{\ignorespaces Impact of detectors shift on fraction of measured radiation with double cross filters\relax }}{5}{figure.caption.8}}
+\newlabel{err}{{8}{5}{Impact of detectors shift on fraction of measured radiation with double cross filters\relax }{figure.caption.8}{}}
Index: /THZ_filters/CrossReport/Report.log
===================================================================
--- /THZ_filters/CrossReport/Report.log	(revision 733)
+++ /THZ_filters/CrossReport/Report.log	(revision 733)
@@ -0,0 +1,1241 @@
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+   defining Unicode char U+011D (decimal 285)
+   defining Unicode char U+011E (decimal 286)
+   defining Unicode char U+011F (decimal 287)
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+   defining Unicode char U+0121 (decimal 289)
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+   defining Unicode char U+012B (decimal 299)
+   defining Unicode char U+012C (decimal 300)
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+   defining Unicode char U+014C (decimal 332)
+   defining Unicode char U+014D (decimal 333)
+   defining Unicode char U+014E (decimal 334)
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+   defining Unicode char U+0152 (decimal 338)
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+   defining Unicode char U+015C (decimal 348)
+   defining Unicode char U+015D (decimal 349)
+   defining Unicode char U+015E (decimal 350)
+   defining Unicode char U+015F (decimal 351)
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+   defining Unicode char U+0161 (decimal 353)
+   defining Unicode char U+0162 (decimal 354)
+   defining Unicode char U+0163 (decimal 355)
+   defining Unicode char U+0164 (decimal 356)
+   defining Unicode char U+0165 (decimal 357)
+   defining Unicode char U+0168 (decimal 360)
+   defining Unicode char U+0169 (decimal 361)
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+   defining Unicode char U+016B (decimal 363)
+   defining Unicode char U+016C (decimal 364)
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+   defining Unicode char U+016E (decimal 366)
+   defining Unicode char U+016F (decimal 367)
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+   defining Unicode char U+0172 (decimal 370)
+   defining Unicode char U+0173 (decimal 371)
+   defining Unicode char U+0174 (decimal 372)
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+   defining Unicode char U+01D0 (decimal 464)
+   defining Unicode char U+01D1 (decimal 465)
+   defining Unicode char U+01D2 (decimal 466)
+   defining Unicode char U+01D3 (decimal 467)
+   defining Unicode char U+01D4 (decimal 468)
+   defining Unicode char U+01E2 (decimal 482)
+   defining Unicode char U+01E3 (decimal 483)
+   defining Unicode char U+01E6 (decimal 486)
+   defining Unicode char U+01E7 (decimal 487)
+   defining Unicode char U+01E8 (decimal 488)
+   defining Unicode char U+01E9 (decimal 489)
+   defining Unicode char U+01EA (decimal 490)
+   defining Unicode char U+01EB (decimal 491)
+   defining Unicode char U+01F0 (decimal 496)
+   defining Unicode char U+01F4 (decimal 500)
+   defining Unicode char U+01F5 (decimal 501)
+   defining Unicode char U+0218 (decimal 536)
+   defining Unicode char U+0219 (decimal 537)
+   defining Unicode char U+021A (decimal 538)
+   defining Unicode char U+021B (decimal 539)
+   defining Unicode char U+01E02 (decimal 7682)
+   defining Unicode char U+01E03 (decimal 7683)
+   defining Unicode char U+200C (decimal 8204)
+   defining Unicode char U+2013 (decimal 8211)
+   defining Unicode char U+2014 (decimal 8212)
+   defining Unicode char U+2018 (decimal 8216)
+   defining Unicode char U+2019 (decimal 8217)
+   defining Unicode char U+201A (decimal 8218)
+   defining Unicode char U+201C (decimal 8220)
+   defining Unicode char U+201D (decimal 8221)
+   defining Unicode char U+201E (decimal 8222)
+   defining Unicode char U+2030 (decimal 8240)
+   defining Unicode char U+2031 (decimal 8241)
+   defining Unicode char U+2039 (decimal 8249)
+   defining Unicode char U+203A (decimal 8250)
+   defining Unicode char U+2423 (decimal 9251)
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+   defining Unicode char U+00A0 (decimal 160)
+   defining Unicode char U+00A1 (decimal 161)
+   defining Unicode char U+00A3 (decimal 163)
+   defining Unicode char U+00AD (decimal 173)
+   defining Unicode char U+00B8 (decimal 184)
+   defining Unicode char U+00BF (decimal 191)
+   defining Unicode char U+00C5 (decimal 197)
+   defining Unicode char U+00C6 (decimal 198)
+   defining Unicode char U+00D8 (decimal 216)
+   defining Unicode char U+00DF (decimal 223)
+   defining Unicode char U+00E6 (decimal 230)
+   defining Unicode char U+00EC (decimal 236)
+   defining Unicode char U+00ED (decimal 237)
+   defining Unicode char U+00EE (decimal 238)
+   defining Unicode char U+00EF (decimal 239)
+   defining Unicode char U+00F8 (decimal 248)
+   defining Unicode char U+0131 (decimal 305)
+   defining Unicode char U+0141 (decimal 321)
+   defining Unicode char U+0142 (decimal 322)
+   defining Unicode char U+0152 (decimal 338)
+   defining Unicode char U+0153 (decimal 339)
+   defining Unicode char U+0174 (decimal 372)
+   defining Unicode char U+0175 (decimal 373)
+   defining Unicode char U+0176 (decimal 374)
+   defining Unicode char U+0177 (decimal 375)
+   defining Unicode char U+0218 (decimal 536)
+   defining Unicode char U+0219 (decimal 537)
+   defining Unicode char U+021A (decimal 538)
+   defining Unicode char U+021B (decimal 539)
+   defining Unicode char U+2013 (decimal 8211)
+   defining Unicode char U+2014 (decimal 8212)
+   defining Unicode char U+2018 (decimal 8216)
+   defining Unicode char U+2019 (decimal 8217)
+   defining Unicode char U+201C (decimal 8220)
+   defining Unicode char U+201D (decimal 8221)
+)
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+   defining Unicode char U+00A7 (decimal 167)
+   defining Unicode char U+00B6 (decimal 182)
+   defining Unicode char U+00B7 (decimal 183)
+   defining Unicode char U+2020 (decimal 8224)
+   defining Unicode char U+2021 (decimal 8225)
+   defining Unicode char U+2022 (decimal 8226)
+)
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+   defining Unicode char U+00A9 (decimal 169)
+   defining Unicode char U+00AA (decimal 170)
+   defining Unicode char U+00AE (decimal 174)
+   defining Unicode char U+00BA (decimal 186)
+   defining Unicode char U+02C6 (decimal 710)
+   defining Unicode char U+02DC (decimal 732)
+   defining Unicode char U+200C (decimal 8204)
+   defining Unicode char U+2026 (decimal 8230)
+   defining Unicode char U+2122 (decimal 8482)
+   defining Unicode char U+2423 (decimal 9251)
+))
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Index: /THZ_filters/CrossReport/Report.out
===================================================================
--- /THZ_filters/CrossReport/Report.out	(revision 733)
+++ /THZ_filters/CrossReport/Report.out	(revision 733)
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+\BOOKMARK [1][-]{section.1}{Introduction}{}% 1
+\BOOKMARK [1][-]{section.2}{Matrix methods}{}% 2
+\BOOKMARK [1][-]{section.3}{Proposed experimental check of filter properties}{}% 3
+\BOOKMARK [1][-]{section.4}{Multiple filters}{}% 4
+\BOOKMARK [1][-]{section.5}{CLIO filters}{}% 5
Index: /THZ_filters/CrossReport/Report.tex
===================================================================
--- /THZ_filters/CrossReport/Report.tex	(revision 733)
+++ /THZ_filters/CrossReport/Report.tex	(revision 733)
@@ -0,0 +1,247 @@
+\documentclass[12pt,a4paper,titlepage]{article}
+\usepackage{graphicx}
+\usepackage{hyperref}
+\usepackage[left=2cm,right=2cm,top=1cm,bottom=2cm]{geometry}
+\usepackage[utf8]{inputenc}
+\usepackage[english]{babel}
+\usepackage{wrapfig}
+%\pagestyle{empty}
+\usepackage{graphicx}
+\usepackage{caption}
+\usepackage{float}
+\usepackage{subcaption}
+\usepackage{epstopdf}
+\usepackage{amsmath}
+\usepackage{tcolorbox}
+\graphicspath{{pics/}}
+
+\begin{document}
+\begin{center}
+\Huge Cross Filters
+\end{center}
+
+\begin{flushright}
+Khodnevych Vitalii\\
+Nicolas Delerue
+\end{flushright}
+
+
+
+%\begin{figure}[!htb]
+%\begin{subfigure}{.5\textwidth}
+%  \centering
+%  \includegraphics[width=\linewidth]{wiki.PNG}
+%  \caption{Inductive and capacitive mesh filters (image source: wikipedia)}
+%  \label{meshp}
+%\end{subfigure}
+%\begin{subfigure}{.5\textwidth}
+%
+%  \centering
+%  \includegraphics[width=0.8\linewidth]{CAM01213.jpg}
+%  \caption{Manufactured THz filters of 20, 30 and 50 GHz}  
+%  \label{manfilt}
+%  \end{subfigure}
+%\caption{Mesh filters}
+%\end{figure}%
+\section{Introduction}
+\begin{figure}[!htb]
+\centering
+\includegraphics[width=0.8\linewidth]{cross.png}
+\caption{Cross-mesh filters layout (from \cite{cros})}  
+\label{cfy}
+\end{figure}
+  
+  Cross filters layout is presented on figure \ref{cfy}. Characteristic sizes (g,a,b) determine filtering frequency and width of transmissivity function. On resonant wavelength $$\lambda_r=2.27g-4a-2b$$  transmission is zero for capacitive filter and one for inductive cross-mesh filter. \par 
+  We will be interested only by inductive filters.  Characteristic impedance in this case is: $$Y(f)=\frac{1}{a_1\pm i\frac{gA_1}{\lambda_r\Omega(f)}}$$
+  where $a_1=0.0001$ is metal loss parameter and $A_1=0.53$ is bandwidth parameter.  Normalized frequency is $$\Omega(f)=\frac{\lambda_rf}{c}-\frac{c}{\lambda_rf}$$
+ \section{Matrix methods}
+ To determine the transmittance and reflectance of cross filters  matrix method is used. Systems with several filters will be reduced simple matrix multiplication.  Filter scattering matrix depends only on the impedance of equivalent circuit (see fig. \ref{ecc}).
+  \begin{figure}[!htb]
+\centering
+\includegraphics[width=0.4\linewidth]{cross2.png}
+\caption{Equivalent circuit of cross filter (from \cite{cros})}  
+\label{ecc}
+\end{figure}
+
+Incident wave $a_1$ and reflected wave $b_1$ on the l.h.s. relate to the wave amplitudes $a_2,\ b_2$ on r.h.s. by following matrix:
+
+\begin{equation}
+\begin{pmatrix} b_1 \\ a_1 \end{pmatrix}
+= 
+\begin{pmatrix} S_{11} & S_{12}\\ S_{21} & S_{22} \end{pmatrix}
+\begin{pmatrix} b_2 \\ a_2 \end{pmatrix} 
+\end{equation}
+If $a_2=0$, transmission coefficient $$t=\frac{b_2}{a_1}=\frac{1}{S_{22}}$$. By applying Kirchoff's laws we could find $S_{ij}$ elements:
+\begin{equation}
+S= 
+\begin{pmatrix} -\frac{Y(f)}{2}+1 & -\frac{Y(f)}{2}\\ \frac{Y(f)}{2} & \frac{Y(f)}{2}+1 \end{pmatrix}
+\end{equation}
+As Y is frequency-dependent, so transmittance also will be frequency dependent.\par 
+In case of series of elements, we multiply  scattering matrix  of each element $S_{total}=...S_3S_2S_1$. Transport matrix (in medium between filters):
+\begin{equation}
+T= 
+\begin{pmatrix} e^{-\frac{2\pi ifd}{c}} & 0\\ 0 & e^{\frac{2\pi ifd}{c}} \end{pmatrix}
+\end{equation}
+where d is distance between filters. In case of repetitive system of several filters $S_{total}=...S_3T_{32}S_2T_{21}S_1$. Transmission coefficient in this case calculated from $S_{total}$ matrix.\par 
+In calculation code also taken into account change of refractive index from medium to medium (in case filter is grown on substrate), angle of incident wave fall, loss of propagation between filters, polarization angle of incident wave.\par
+Change of transmissivity as function of geometrical parameters a and b are presented on figures \ref{ta} and \ref{tb}.
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{a_T.eps}
+  \caption{Change of transmissivity as function of geometrical parameter a }
+  \label{ta}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{b_T.eps}
+  \caption{Change of transmissivity as function of geometrical parameter b}
+  \label{tb}
+  \end{subfigure}
+\caption{}
+\end{figure}%
+
+
+%\begin{figure}[!htb]
+%\begin{subfigure}{.5\textwidth}
+%  \centering
+%  \includegraphics[width=\linewidth]{10.eps}
+%  \caption{}
+%  \label{}
+%\end{subfigure}
+%%\begin{subfigure}{.5\textwidth}
+%%
+%%  \centering
+%%  \includegraphics[width=\linewidth]{30.eps}
+%%  \caption{•}  
+%%  \label{}
+%%  \end{subfigure}
+%  \begin{subfigure}{.5\textwidth}
+%
+%  \centering
+%  \includegraphics[width=\linewidth]{50.eps}
+%  \caption{}
+%  \label{}
+%\end{subfigure}
+%%\begin{subfigure}{.5\textwidth}
+%%
+%%  \centering
+%%  \includegraphics[width=\linewidth]{100.eps}
+%%  \caption{•}  
+%%  \label{}
+%%  \end{subfigure}
+%\caption{}
+%\end{figure}%
+\newpage
+\clearpage
+\section{Proposed experimental check of filter properties}
+ETALON project at LAL have two RF sources: on 24 and 35 GHz. They will be used to check properties of cross filters. For this purpose we design 16 filters. Experiment will consist from two parts:
+\begin{itemize}
+\item Check transmissivity of filters as function of filter frequency (see \ref{p1t} and \ref{p1r} )
+\item Check transmissivity of filters as function of a,b parameters for fixed filter frequency (see \ref{p2t} and \ref{p2r} )
+\end{itemize}
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{TFp1T.eps}
+  \caption{Transmissivity functions for different test wavelengths}
+  \label{p1t}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{TFp1R.eps}
+  \caption{Transmission for different filter with present sources}  
+  \label{p1r}
+  \end{subfigure}
+\caption{First part of experiment: check transmission}
+\end{figure}%
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{TFp2T.eps}
+  \caption{Transmissivity functions for different filter parameters}
+  \label{p2t}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{TFp2R.eps}
+  \caption{Transmission for different filter with present sources}  
+  \label{p2r}
+  \end{subfigure}
+\caption{Second part of experiment: check filters parameters dependence}
+\end{figure}%
+
+\newpage
+\clearpage
+\section{Multiple filters}
+To decrease tails of transmissivity functions possible to use several cross filters. On figure \ref{ond} is shown transmissivity for single, double and triple filters. Double filters significantly decrease  tails but produce narrow window in region far from resonant frequency. Triple filters didn't give big effect, but require more filters in realization. So we will use double cross filters. \par 
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{sdt.eps}
+  \caption{Transmissivity function of single, double and triple cross filters}
+  \label{ond}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{dcft.eps}
+  \caption{Change of transmissivity function for double cross filters as function of filters separation}  
+  \label{gg}
+  \end{subfigure}
+\caption{Multiple filters}
+\end{figure}%
+Question which arise is at which optimal distance put second filter with respect to first one. We find (see \ref{gg}) that when filters separation is equal half of g parameter, transmissivity function have best characteristics.
+\newpage
+\clearpage
+\section{CLIO filters}
+Using matrix method for calculation cross filters we could calculate double structure filters for Smith-Purcell experiment at CLIO. Filter size is 3x3 cm. Filter separation is equal half of g parameter. Frequency of filters are calculated for current setup ($7^o$ detector separation, 6 mm grating). Transmissivity functions are presented on figure \ref{clioT}.\par 
+\begin{figure}[!htb]
+\centering
+\includegraphics[width=1\linewidth]{clio.eps}
+\caption{Transmissivity functions of cross filters for Smith-Purcell experiment at CLIO.}  
+\label{clioT}
+\end{figure}
+Usage of filters give big advantages for experiment, as it significantly cut background components of the signal.  But it's also require precise alignment. Shift of detector mount with respect to grating base cause decrease of signal (as detector then aligned on other frequency and filters stay at designed). As wavelengths  of Smith-Purcell radiation are distributed by cosine law, shift of setup in one or other side is not same (see fig. \ref{err}). To estimate this effect we calculate the ratio of transmitted fraction of radiation with and without filter. Integration borders are determined by acceptance of detection system (25mm OAP + pyrodetector). Result of this calculation presented on figure \ref{err}. We conclude that even with error of detector system mount, we still should detect more than 90\% of emitted radiation.
+\begin{figure}[!htb]
+\centering
+\includegraphics[width=0.5\linewidth]{Error.eps}
+\caption{Impact of detectors shift on fraction of measured radiation with double cross filters}  
+\label{err}
+\end{figure}
+
+
+
+
+
+
+
+
+
+
+
+
+
+\begin{thebibliography}{9}
+
+
+
+\bibitem{cros}
+  Benjamin Hooberman
+  \emph{Everything You Ever Wanted to Know About Frequency-Selective Surface Filters but Were Afraid to Ask}, May 2005
+  
+
+\end{thebibliography}
+
+
+
+
+
+
+
+\end{document}
Index: /THZ_filters/Doc/Report.aux
===================================================================
--- /THZ_filters/Doc/Report.aux	(revision 733)
+++ /THZ_filters/Doc/Report.aux	(revision 733)
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+\relax 
+\providecommand\hyper@newdestlabel[2]{}
+\providecommand\HyperFirstAtBeginDocument{\AtBeginDocument}
+\HyperFirstAtBeginDocument{\ifx\hyper@anchor\@undefined
+\global\let\oldcontentsline\contentsline
+\gdef\contentsline#1#2#3#4{\oldcontentsline{#1}{#2}{#3}}
+\global\let\oldnewlabel\newlabel
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+\AtEndDocument{\ifx\hyper@anchor\@undefined
+\let\contentsline\oldcontentsline
+\let\newlabel\oldnewlabel
+\fi}
+\fi}
+\global\let\hyper@last\relax 
+\gdef\HyperFirstAtBeginDocument#1{#1}
+\providecommand\HyField@AuxAddToFields[1]{}
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+\citation{mesh}
+\providecommand\tcolorbox@label[2]{}
+\select@language{english}
+\@writefile{toc}{\select@language{english}}
+\@writefile{lof}{\select@language{english}}
+\@writefile{lot}{\select@language{english}}
+\@writefile{toc}{\contentsline {section}{\numberline {1}Mesh filters}{1}{section.1}}
+\providecommand*\caption@xref[2]{\@setref\relax\@undefined{#1}}
+\newlabel{meshp}{{1a}{1}{Inductive and capacitive mesh filters (image source: wikipedia)\relax }{figure.caption.1}{}}
+\newlabel{sub@meshp}{{a}{1}{Inductive and capacitive mesh filters (image source: wikipedia)\relax }{figure.caption.1}{}}
+\newlabel{manfilt}{{1b}{1}{Manufactured THz filters of 20, 30 and 50 GHz\relax }{figure.caption.1}{}}
+\newlabel{sub@manfilt}{{b}{1}{Manufactured THz filters of 20, 30 and 50 GHz\relax }{figure.caption.1}{}}
+\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Mesh filters\relax }}{1}{figure.caption.1}}
+\newlabel{}{{2a}{1}{First set of filters with 5x5 cm size\relax }{figure.caption.2}{}}
+\newlabel{sub@}{{a}{1}{First set of filters with 5x5 cm size\relax }{figure.caption.2}{}}
+\newlabel{}{{2b}{1}{Second set of filters with 10x10 cm size\relax }{figure.caption.2}{}}
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+\newlabel{35g}{{4b}{2}{Transmissivity of filters for 35 GHz source\relax }{figure.caption.4}{}}
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Index: /THZ_filters/Doc/Report.log
===================================================================
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Index: /THZ_filters/Doc/Report.out
===================================================================
--- /THZ_filters/Doc/Report.out	(revision 733)
+++ /THZ_filters/Doc/Report.out	(revision 733)
@@ -0,0 +1,2 @@
+\BOOKMARK [1][-]{section.1}{Mesh filters}{}% 1
+\BOOKMARK [1][-]{section.2}{Experimental check of filter properties}{}% 2
Index: /THZ_filters/Doc/Report.tex
===================================================================
--- /THZ_filters/Doc/Report.tex	(revision 733)
+++ /THZ_filters/Doc/Report.tex	(revision 733)
@@ -0,0 +1,199 @@
+\documentclass[12pt,a4paper,titlepage]{article}
+\usepackage{graphicx}
+\usepackage{hyperref}
+\usepackage[left=2cm,right=2cm,top=1cm,bottom=2cm]{geometry}
+\usepackage[utf8]{inputenc}
+\usepackage[english]{babel}
+\usepackage{wrapfig}
+%\pagestyle{empty}
+\usepackage{graphicx}
+\usepackage{caption}
+\usepackage{float}
+\usepackage{subcaption}
+\usepackage{epstopdf}
+
+\usepackage{tcolorbox}
+\graphicspath{{pics/}{newpics/}}
+
+\begin{document}
+\begin{center}
+\Huge Mesh Filters
+\end{center}
+
+\begin{flushright}
+Khodnevych Vitalii\\
+Nicolas Delerue
+\end{flushright}
+Precise measurements of beam profile with Smith-Purcell radiation require precise measurements of spectrum. To filter background signal from Smith-Purcell radiation we will use inductive mesh filters. Detector unit at each angle will have its own filter, which correspond to emitted wavelength of Smith-Purcell radiation.
+\section{Mesh filters}
+Metal-mesh filters are filters made from metal meshes (see fig. \ref{meshp}). They working diapason is from far infrared to submilimeter regions of the electro-magnetic spectrum. We use inductive mesh filters. That's mean that they are band-pass filters. Transmissivity function is presented on figure \ref{trans}. Using Ulrich’s \cite{mesh} theory we calculate mesh parameters (period, thickness of wire(strip); see fig. \ref{meshp}) for certain frequencies. Example of manufactured filters present on figure \ref{manfilt}.
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{wiki.PNG}
+  \caption{Inductive and capacitive mesh filters (image source: wikipedia)}
+  \label{meshp}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=0.8\linewidth]{CAM01213.jpg}
+  \caption{Manufactured THz filters of 20, 30 and 50 GHz}  
+  \label{manfilt}
+  \end{subfigure}
+\caption{Mesh filters}
+\end{figure}%
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{Trans5.eps}
+  \caption{First set of filters with 5x5 cm size}
+  \label{}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{Trans10.eps}
+  \caption{Second set of filters with 10x10 cm size}  
+  \label{}
+  \end{subfigure}
+\caption{Transmissivity functions of inductive mesh filters}
+  \label{trans}
+\end{figure}%
+
+
+
+
+\section{Experimental check of filter properties}
+To test filters we use setup, as present on figure \ref{exper}. We test filters with two GHz sources: GDO-2510F on 24GHz and SOL-3510-28-G1 on 35 GHz. Setup consist of source (S), chopper with frequency 25 Hz (result dont depend from chopper speed), filter frame (F) with or without filter, and detector (D) with connected Horn anthena (A).
+\begin{figure}[!htb]
+  \centering
+  \includegraphics[width=0.7\linewidth]{CAM01210b.jpg}
+  \caption{Experimental setup: S - GHz source, C - chopper (25 Hz), F - frame for filter, A - Gain Horm Anthena (GHA-28), D - detector (DET-28S)}
+  \label{exper}
+\end{figure}%
+To acquire the signal we use RTM 2054 Oscilloscope. We measure peak-to-peak voltage (Vpp) on detector. \par 
+Order of measurements was following: measure Vpp without filter; install filter and measure Vpp with filter. Ratio with and without of Vpp gives Trasmissivity for current filter.\par 
+Due to big wavelength position of parts of experimental setup play big role. For example some inroduce of some part could change diffraction pattern and signal on detector could increase or decrease. This will be discussed later.\par 
+We make few sets of measurement in different configuration of experimental setup (see fig \ref{24g}). Result of measurements strongly depend from position on line of experimental tools (detector, filter etc).
+We make three sets of measurements (Data set 3) for 24 GHz source (see fig. \ref{24g}) and conclude, that they are quite reproducible for current setup. Also we make measurements with and without horn anthena for 35 GHz source (see fig. \ref{35g}). Change of results was caused by diffraction in plane of detectors anthena and necessity of usage near-field approach.\par
+
+ 
+
+
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{BigF24.eps}
+  \caption{Transmissivity of filters for 24 GHz source}
+  \label{24g}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{BigF35.eps}
+  \caption{Transmissivity of filters for 35 GHz source}
+  \label{35g}
+  \end{subfigure}
+\caption{Experimental results}
+\end{figure}%
+
+To understand effect of diffraction, we change filter frame position wiht step 0.5 and measure transmissivity for filters. Results are presented on figure \ref{map}. We clearly see that pattern with me measure repeat with step equal of half source wavelength. We find from this data that corresponding source frequency equal $2.34\pm0.24$ GHz with given in documentation of source 24 GHz. On figure \ref{Tmap} present transmissivity of filters form maximum to minimum. Why transmissivity is changing is not clear yet.
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{BigMAP.eps}
+  \caption{}
+  \label{map}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{BigF24Difr.eps}
+  \caption{}
+  \label{Tmap}
+  \end{subfigure}
+\caption{Experimental results: Trasmissivity as function of filter position}
+\end{figure}%
+
+To be able avoid diffraction effects we construct other setup, where we place components as close, as possible to each other. Also we install 1 inch tube in between chopper and filter. \par 
+\begin{figure}[!htb]
+  \centering
+  \includegraphics[width=0.7\linewidth]{CAM01236.jpg}
+  \caption{Experimental setup \#2}
+  \label{}
+\end{figure}%
+
+Due to unknown spectral characteristics of detector and both sources, we could not compare experimental results with our calculation, but can assume gaussian spectrum of the source and flat frequency sensitivity of detector.
+With new setup we repeat measurement for both sets of filters and and both sources we have. Results are present on figures \ref{compB} and fig. \ref{compS}. We still don't have good agreement with 20-50 GHz filters (see fig. \ref{compB}), which was caused due to near-field effects, we suspect.\par
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{Bg24.eps}
+  \caption{}
+  \label{}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{Bg35.eps}
+  \caption{}
+  \label{}
+  \end{subfigure}
+\caption{Experimental results: big filters}
+  \label{compB}
+\end{figure}%
+
+
+
+But we have good agreement of calculation and experiment for other set of filters (see fig. \ref{compS}). With small correction of filter impedance, agreement even better for both sources.
+
+
+
+
+\begin{figure}[!htb]
+\begin{subfigure}{.5\textwidth}
+  \centering
+  \includegraphics[width=\linewidth]{Sm24.eps}
+  \caption{}
+  \label{}
+\end{subfigure}
+\begin{subfigure}{.5\textwidth}
+
+  \centering
+  \includegraphics[width=\linewidth]{Sm35.eps}
+  \caption{}
+  \label{}
+  \end{subfigure}
+\caption{Experimental results: small filters}
+  \label{compS}
+
+\end{figure}%
+\newpage
+\section*{Conclusion}
+Experimental check of filter properties gives good agreement between calculation and data for small filters.% Difference in experiment and calculation for big filters (20-50 GHz) could be caused by the long wavelength for which filters was designed or too small a/g ratio. For small filters data  and experiment agreed, 
+So this code could be used for calculation filters for Smith-Purcell experiment at CLIO.
+
+\begin{thebibliography}{9}
+
+\bibitem{mesh}
+  R. Ulrich,
+  \emph{Far-infrared properties of metallic mesh and its complement-
+ary structure}, Infrared Physics, Vol. 7, pp. 37-55, Pergamon Press Ltd.
+1967, Printed in Great Britain.
+  
+
+\end{thebibliography}
+
+
+
+
+
+
+
+\end{document}
Index: /THZ_filters/Experiment results/AllMeasurements.m
===================================================================
--- /THZ_filters/Experiment results/AllMeasurements.m	(revision 733)
+++ /THZ_filters/Experiment results/AllMeasurements.m	(revision 733)
@@ -0,0 +1,42 @@
+%All measurements
+close all; clear all
+Freq=[20 23 24 25 26 27 30 40 50];
+Vpp0=[101.6 104.00 108 113.6 122.4 114.4 104.6 87.2 88.]/145.6;
+Vpp1=[116.8 124.0 120.0 126.4 133.6 124.8 115.2 100 97.6]./[153.6 150.4 148.8 147.2 145.2 145.6 144.8 144.8 143.2];
+Vpp0a=[113.6 122.4 118.4 124.0 129.6 124 115.2 98.4 96.0]./[148.8 147.2 145.6 144.0 144.0 143.2 142.4 141.6 142.4];
+Vpp1a=[114.4 124.8 116.8 126.4 132.8 124.8 112.4 96.0 92.8]./[148.0 145.6 144.8 144.8 144.0 144.0 143.2 143.2 143.2];
+Vpp=[Vpp1; Vpp0a; Vpp1a];
+Vppx=([198 230 226 218 242 254 256 208 224]-16)./([248 248 244 246 244 244 242 244 244]-16);
+
+figure
+hold on
+plot(Freq,Vppx,'-*r','linew',2)
+plot(Freq,Vpp0,'-*k','linew',2)
+
+errorbar(Freq,mean(Vpp),std(Vpp),'-ob','linew',2)
+set(gca,'fontsize',16)
+grid on
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('GDO-2510, 24 [GHz]')
+ legend('Data set 1','Data set 2','Data set 3','location','southeast')
+ylim([0 1.2])
+
+
+
+
+% Vpp2=[106.4 104.8 109.6 105.6 104.8 110.4 105.8 114.4 117.6];
+Vpp3=[112.8 108.8 111.2 107.2 108.0 112.8 107.2 117.6 118.4]./[122.4 121.6 120.8 120.0 120.0 120.0 120.0 119.2 119.2];
+Vpp4=[53.8 52.8 55.2 48.0 51.2 55.2 45.6 58.4 60.8]./[68 66.4 65.6 65.6 65.6 65.6 65.6 65.6 65.6];
+figure
+hold on
+% plot(Freq,Vpp2)
+grid on
+plot(Freq,Vpp3,'-or','linew',2)
+plot(Freq,Vpp4,'-ok','linew',2)
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('SOL-35310, 35 [GHz]')
+legend('With GHA','Without GHA','location','southeast')
+ylim([0.5 1])
Index: /THZ_filters/Experiment results/Experiment2translationStage.m
===================================================================
--- /THZ_filters/Experiment results/Experiment2translationStage.m	(revision 733)
+++ /THZ_filters/Experiment results/Experiment2translationStage.m	(revision 733)
@@ -0,0 +1,63 @@
+clear all; close all; clc;
+
+F20=[91.2 96 99.2 100.8 99.2 96 92 89.6 88 90.4 88 89.6 90.4 93.6 98.4 104 105.6 104.8 100 96  92.8 92 92.8 92 92.8 93.6];
+F23=[100.8 104 105.6 104.8 104 100 97.6 96.8 94.4 92.8 91.2 95.2 100 105.6 108.8 111.2 111.2 108.8 104.8 103.2 100.8 97.6 95.2 96 99.2 103.2];
+F24=[96.8 100.8 104.8 105.6 105.6 104 101.6 99.2 96 95.2 96 96.8 98.4 102.4 108 111.2 112.8 112 110.4 105.6 100.8 99.2 98.4 98.4 100 102.4];
+F25=[107.2 111.2 114.4 117.6 116.8 115.2 110.4 107.2 102.4 100.8 103.2 105.6 108 112.8 117.6 122.4 124.8 124 121.6 116.8 110.4 107.2 106.4 106.4 109.6 111.2];
+F26=[104.8 108 110.4 109.6 108 104.8 103.2 102.4 100.8 100 99.2 100 104.8 111.2 115.2 117.6 118.4 114.4 111.2 110.4 109.6 108.0 104.8 103.2 106.4 110.4];
+F27=[107.2 113.6 116.8 116.0 113.6 110.4 106.4 101.6 98.4 96.8 97.6 100 104.8 112 117.6 122.4 122.4 120 114.4 108.8 104.8 103.2 102.4 103.2 104.8 108.8];
+F30=[104 110.4 113.6 115.2 113.6 111.2 106.2 101.6 97.6 94.4 96.0 100 105.6 111.2 117.6 120.8 120.8 119.2 115.2 109.6 104.8 102.4 101.6 102.4 104.0 109.6];
+F40=[109.6 117.6 120.0 116.8 112.8 106.8 99.2 95.2 91.2 88.8 91.2 97.6 106.4 116 124.2 124.8 121.6 117.6 110.4 104 98.4 95.2 95.2 98.4 104.8 112.0];
+F50=[99.2 107.2 109.6 106.4 100.8 92.0 84.0 80.8 78.4 77.6 78.4 86.4 96.0 107.2 112.8 115.2 110.4 104.0 96.0 88.8 84.0 84.0 84.8 88.8 96.0 103.2];
+Block=[23 17.8 17 21.4 26.6 34.6 42.0 46.8 46 44.8 41.2 35.6 28.8 20 15.4 16.0 20.6 27.2 35.6 43.8 46.8 46 42.8 37.2 28.4 20];
+Frame=[122.4 121.3 126.4 132.0 136 136.8 135.2 132.8 127.2 123.2 121.6 124.0 126.4 125.6 127.2 133.6 140.8 143.2 141.6 140.0 136.0 131.2 125.6 122.4 123.2 124];
+
+F=[F20; F23; F24; F25; F26; F27; F30; F40; F50];
+F=F-repmat(Block,[9 1]);
+Frame=Frame-Block;
+F=F./repmat(Frame,[9 1]);
+% F=F./repmat(F(4,:),[9 1]);
+nu_f=[20 23 24 25 26 27 30 40 50]
+Len=(0:25)*1/2;
+figure
+[hc hc]=contourf(Len, nu_f,F)
+set(hc,'edgecolor','none')
+colorbar
+set(gca,'fontsize',16)
+ylabel('Frequency, [GHz]')
+xlabel('Frame position, [mm]')
+title('Transmissivity, 24GHz')
+
+
+figure
+hold on
+cm=colormap(jet(8));
+for ii=1:8
+plot(nu_f,F(:,ii+1),'-^','color',cm(9-ii,:),'linew',2)
+end
+grid on
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+ legend('0.5 mm','1 mm','1.5 mm','2 mm','2.5 mm','3 mm','3.5 mm','4 mm','Location','northeast')
+title('24GHz source')
+xlim([19 66])
+
+
+Fi=pchip(1:26,F,1:0.1:26);
+for k=1:9
+for c=-50:50
+   R(c+51)=corr(Fi(k,1:(126-c+1))',Fi(k,(126+c-1):251)');
+end
+    [~,Rk(k)]=max(R);
+end
+% plot(nu_f,(Rk-50+126)/10)
+% hold on
+% plot(nu_f,ones(size(nu_f))*299/24)
+% ylim([12 13.5])
+299.792/mean((Rk-50+126)/10)% GHz
+299.792/mean((Rk-50+126)/10)^2*std((Rk-50+126)/10)% Error GHz
+
+% figure
+% errorbar(nu_f,mean(F,2),std(F'))
+% xlim([19 51])
Index: /THZ_filters/Experiment results/Experiment3.m
===================================================================
--- /THZ_filters/Experiment results/Experiment3.m	(revision 733)
+++ /THZ_filters/Experiment results/Experiment3.m	(revision 733)
@@ -0,0 +1,70 @@
+%Experiment N3
+close all; clear all; clc
+nu_f=[20 23 24 25 26 27 30 40 50];
+nu_f0=[37 53 75 124 186 368];
+F=[416 368 364 390 420 422 382 352 328]/438;
+F0=[350 230 180 104 60 24]/438;
+figure
+hold on
+plot(nu_f,F,'-ob')
+plot(nu_f0,F0,'-or')
+%%%
+
+F37=[74.9 74.4 81.33 83.06 75.6 83.3 90.74 80.42 79.78 75.7];
+F53=[63.8 58.6 61.2 57.2 69.7 50.2 94.4 52.01 88.2 54.73];
+F75=[51.5 35.7 47.13 43.57 53.47 30.16 64.12 41.9 52.5 35.53];
+F124=[33.1 10.79 11.06 24.49 11.35 17.22 12.3 25 14.7 21.6];
+F186=[11.38 4.3 9.15 21.64 7.89 6.7 10.3 24.4 13 25.3];
+F368=[2.6 0.5 0.9 2.12 2.24 2.3 2.8 1.26 7.17 1.68];
+Frame=[74.5 72.6 73.1 72.8 73.56 74.2 74.1];
+Fx=[mean(F37) mean(F53) mean(F75) mean(F124) mean(F186) mean(F368)];
+eFx=[std(F37) std(F53) std(F75) std(F124) std(F186) std(F368)];
+figure
+errorbar(nu_f0,Fx,eFx)
+
+
+F37=[79.2 119.3 85.7 93.2 79.4 88 89.7 81.8];
+F53=[40.7 38.5 51.2 48.3 47.1 34.6 47.5 53.5];
+F75=[42.3 23.6 45.6 22.2 30.9 15.2 29.8 25.4];
+F124=[18.5 8.18 17.4 16.7 6.15 9.84 7.0 7.5];
+F186=[7.8 11.4 9.5 6.4 4.8 4.1 4.9 4.5 ];
+F368=[11.03 3.57 5.36 5.7 7.1 2.53 4.5 2.3];
+Frame=[95.8 92.5 92.7 92.05 92 92.1];
+Fx=[mean(F37) mean(F53) mean(F75) mean(F124) mean(F186) mean(F368)];
+eFx=[std(F37) std(F53) std(F75) std(F124) std(F186) std(F368)];
+figure
+errorbar(nu_f0,Fx,eFx)
+%%%%
+F20=[89.1 84.8 83.2 81.2];
+F23=[72 71.4 70.3 72];
+F24=[67.7 71 70.5 72.7 ];
+F25=[74.5 74.6 74.2 74.2 ];
+F26=[81.7 82 81 82.4];
+F27=[88 84.2 87.8 88.5];
+F30=[77.6 77.4 76.6 79.7];
+F40=[61.3 60.21 60.9 62];
+F50=[66.2 66 67.3 66];
+Frame=[94.3 93.8 93 92.3 93.7 93.2 93.1];
+Fx=[mean(F20) mean(F23) mean(F24) mean(F25) mean(F26) mean(F27) mean(F30) mean(F40) mean(F50)]./mean(Frame);
+eFx=[std(F20) std(F23) std(F24) std(F25) std(F26) std(F27) std(F30) std(F40) std(F50)]./mean(Frame);
+figure
+errorbar(nu_f,Fx,eFx)
+
+F20=[94.7 95.4 96.2 94.2 ];
+F23=[ 90.3 93.3 87 86.6 ];
+F24=[ 87.6 91.6 88.4 89.5 ];
+F25=[87.7 88 88.3 87.5];
+F26=[85.2 83.9 83.1 84.6];
+F27=[84.9 83 80.5 77.3];
+F30=[82.6 82 83.3 85.5];
+F40=[87 89.5 89.2 88];
+F50=[91.4 94.2 94.8 90.7];
+Frame=[96.3 93.3 92.7 92 91.8 91.6 91 91.2];
+Fx=[mean(F20) mean(F23) mean(F24) mean(F25) mean(F26) mean(F27) mean(F30) mean(F40) mean(F50)]./mean(Frame);
+eFx=[std(F20) std(F23) std(F24) std(F25) std(F26) std(F27) std(F30) std(F40) std(F50)]./mean(Frame);
+figure
+errorbar(nu_f,Fx,eFx)
+
+
+
+
Index: /THZ_filters/Experiment results/MF_EXP.m
===================================================================
--- /THZ_filters/Experiment results/MF_EXP.m	(revision 733)
+++ /THZ_filters/Experiment results/MF_EXP.m	(revision 733)
@@ -0,0 +1,53 @@
+   clear all; close all; clc
+%inductive grating
+%phys. const
+c=299792458;%speed of light, m/s
+sigma=1.45e+6*1e-7*c*c;%stainless steel conductivity, [s]
+j=0;
+nu_filter=[20 23 24 25 26 27 30 40 50].*1e+9;
+nu=(0.001:0.01:100)*1e+9;
+F24i=[];
+sigma24=0.01e+9;
+gauss24=1/sqrt(2*pi*sigma24^2)*exp(-(nu-24e+9).^2./(2*sigma24^2));
+F35i=[];
+sigma35=1e+9;
+gauss35=1/sqrt(2*pi*sigma35^2)*exp(-(nu-35e+9).^2./(2*sigma35^2));
+color=colormap(jet(length(nu_filter)))
+for f=nu_filter
+j=j+1;
+lamb0=c/f;
+ratio=0.02;%a/g ratio
+omega0=(1-0.27*(ratio));
+g=lamb0*omega0;
+a=ratio*g;%wire width
+
+
+
+disp(['g=' num2str(g*1e+3) 'mm a=' num2str(a*1e+3) 'mm nu=' num2str((1-0.27*ratio)*c/g*1e-9) ' GHz'])
+disp(['g=' num2str(round(g*1e+6)*1e-3) 'mm a=' num2str(round(a*1e+6)*1e-3) 'mm nu=' num2str((1-0.27*ratio)*c/g*1e-9) ' GHz'])
+disp(['Plate=' num2str(round(g*1e+6)*1e-3-2*round(a*1e+6)*1e-3) ' mm and ' num2str(round(1000/(round(g*1e+6)*1e-3))/10) ' squares on line'])
+disp(['  '])
+omega=nu*g/c;
+lamb=g./omega;
+eta=1/(1-2*ratio);
+R=eta./2.*sqrt(c./lamb./sigma);
+Om=lamb0./lamb-lamb./lamb0;
+Z0=(2*log(csc(a*pi/(2*g))));
+% Z0=8;
+t2=(R.^2+(Z0./Om).^2)./((1+R).^2+(Z0./Om).^2);
+
+plot(nu/1e+9,t2,'color',color(end-j+1,:),'linew',2)
+F24i=[F24i,t2*gauss24'*1e+7];
+F35i=[F35i,t2*gauss35'*1e+7];
+
+hold on
+end
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity,[1]')
+legend('20 GHz','23 GHz','24 GHz','25 GHz','26 GHz','27 GHz','30 GHz','40 GHz','50 GHz','location','southeast')
+grid on
+xlim([10 100])
+ylim([0 1])
+
+
Index: /THZ_filters/Experiment results/MF_EXP2.m
===================================================================
--- /THZ_filters/Experiment results/MF_EXP2.m	(revision 733)
+++ /THZ_filters/Experiment results/MF_EXP2.m	(revision 733)
@@ -0,0 +1,53 @@
+   clear all; close all; clc
+%inductive grating
+%phys. const
+c=299792458;%speed of light, m/s
+ sigma=1.45e+6*1e-7*c*c;%stainless steel conductivity, [s]
+j=0;
+nu_filter=[37 53 75 124 186 368].*1e+9;
+nu=(0.0001:0.01:500)*1e+9;
+F24=[];
+F35=[];
+
+sigma24=1e+9;
+gauss24=1/sqrt(2*pi*sigma24^2)*exp(-(nu-24e+9).^2./(2*sigma24^2));
+sigma35=1e+9;
+gauss35=1/sqrt(2*pi*sigma35^2)*exp(-(nu-35e+9).^2./(2*sigma35^2));
+color=colormap(jet(length(nu_filter)))
+for f=nu_filter
+j=j+1;
+lamb0=c/f;
+ratio=0.2;%a/g ratio
+omega0=(1-0.27*(ratio));
+g=lamb0*omega0;
+a=ratio*g;%wire width
+
+
+
+disp(['g=' num2str(g*1e+3) 'mm a=' num2str(a*1e+3) 'mm nu=' num2str((1-0.27*ratio)*c/g*1e-9) ' GHz'])
+disp(['g=' num2str(round(g*1e+6)*1e-3) 'mm a=' num2str(round(a*1e+6)*1e-3) 'mm nu=' num2str((1-0.27*ratio)*c/g*1e-9) ' GHz'])
+disp(['Plate=' num2str(round(g*1e+6)*1e-3-2*round(a*1e+6)*1e-3) ' mm and ' num2str(round(1000/(round(g*1e+6)*1e-3))/10) ' squares on line'])
+disp(['  '])
+omega=nu*g/c;
+lamb=g./omega;
+eta=1/(1-2*ratio);
+R=eta./2.*sqrt(c./lamb./sigma);
+Om=lamb0./lamb-lamb./lamb0;
+  Z0=(2*log(csc(a*pi/(2*g))));
+% Z0=2.5
+t2=(R.^2+(Z0./Om).^2)./((1+R).^2+(Z0./Om).^2);
+
+
+plot(nu/1e+9,t2,'color',color(end-j+1,:),'linew',2)
+F24=[F24,t2*gauss24'*1e+7];
+F35=[F35,t2*gauss35'*1e+7];
+
+hold on
+end
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+ legend('37 GHz','53 GHz','75 GHz','124 GHz','186 GHz','368 GHz','location','southeast')
+grid on
+xlim([10 500])
+
Index: /THZ_filters/Experiment results/MakePlots.m
===================================================================
--- /THZ_filters/Experiment results/MakePlots.m	(revision 733)
+++ /THZ_filters/Experiment results/MakePlots.m	(revision 733)
@@ -0,0 +1,125 @@
+%%plots
+close all; clear all; clc
+figure(2)
+hold on
+
+load smallFc.mat
+plot(nu_filter*1e-9,F24i,'-.ok','linew',2,'MarkerFaceColor','k')
+load smallF.mat
+plot(nu_filter*1e-9,F24i,'-.ob','linew',2,'MarkerFaceColor','b')
+F0=[350 230 180 104 60 24]/438;
+% plot(nu_filter*1e-9,F0,'-or','linew',2)
+
+F37=[79.2 119.3 85.7 93.2 79.4 88 89.7 81.8];
+F53=[40.7 38.5 51.2 48.3 47.1 34.6 47.5 53.5];
+F75=[42.3 23.6 45.6 22.2 30.9 15.2 29.8 25.4];
+F124=[18.5 8.18 17.4 16.7 6.15 9.84 7.0 7.5];
+F186=[7.8 11.4 9.5 6.4 4.8 4.1 4.9 4.5 ];
+F368=[11.03 3.57 5.36 5.7 7.1 2.53 4.5 2.3];
+Frame=[95.8 92.5 92.7 92.05 92 92.1];
+Fx=[mean(F37) mean(F53) mean(F75) mean(F124) mean(F186) mean(F368)]./mean(Frame);
+eFx=[std(F37) std(F53) std(F75) std(F124) std(F186) std(F368)]./mean(Frame);
+errorbar(nu_filter*1e-9,Fx,eFx,'^r','linew',2)
+grid on
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+ legend('Calc. Z_0=2.3', 'Calc. Z_0=1.9','Exp. data')
+grid on
+title('24GHz source')
+
+figure(3)
+hold on
+
+load smallFc.mat
+plot(nu_filter*1e-9,F35i,'-.ok','MarkerFaceColor','k','linew',2)
+load smallF.mat
+plot(nu_filter*1e-9,F35i,'-.ob','MarkerFaceColor','b','linew',2)
+
+% F0=[224 122 88 40 19.8 5.12]/215;
+% plot(nu_filter*1e-9,F0,'-or','linew',2)
+
+F37=[74.9 74.4 81.33 83.06 75.6 83.3 90.74 80.42 79.78 75.7];
+F53=[63.8 58.6 61.2 57.2 69.7 50.2 94.4 52.01 88.2 54.73];
+F75=[51.5 35.7 47.13 43.57 53.47 30.16 64.12 41.9 52.5 35.53];
+F124=[33.1 10.79 11.06 24.49 11.35 17.22 12.3 25 14.7 21.6];
+F186=[11.38 4.3 9.15 21.64 7.89 6.7 10.3 24.4 13 25.3];
+F368=[2.6 0.5 0.9 2.12 2.24 2.3 2.8 1.26 7.17 1.68];
+Frame=[74.5 72.6 73.1 72.8 73.56 74.2 74.1];
+Fx=[mean(F37) mean(F53) mean(F75) mean(F124) mean(F186) mean(F368)]./mean(Frame);
+eFx=[std(F37) std(F53) std(F75) std(F124) std(F186) std(F368)]./mean(Frame);
+
+errorbar(nu_filter*1e-9,Fx,eFx,'^r','linew',2)
+grid on
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+ legend('Calc. Z_0=2.3', 'Calc. Z_0=1.9','Exp. data')
+title('35GHz source')
+load bigF.mat
+
+
+
+figure(4)
+plot(nu_filter*1e-9,F24i,'-ok','linew',2)
+nu_f0=[37 53 75 124 186 368];
+F=[416 368 364 390 420 422 382 352 328]/438;
+F0=[350 230 180 104 60 24]/438;
+
+% Freq=[20 23 24 25 26 27 30 40 50];
+% Vpp0=[116.8 124.0 120.0 126.4 133.6 124.8 115.2 100 97.6]./[153.6 150.4 148.8 147.2 145.2 145.6 144.8 144.8 143.2];
+hold on
+% plot(Freq,Vpp0,'-ok')
+% plot(Freq,F,'-og')
+% % plot(nu_f0,F0,'-or')
+% ylim([0 1])
+F20=[89.1 84.8 83.2 81.2];
+F23=[72 71.4 70.3 72];
+F24=[67.7 71 70.5 72.7 ];
+F25=[74.5 74.6 74.2 74.2 ];
+F26=[81.7 82 81 82.4];
+F27=[88 84.2 87.8 88.5];
+F30=[77.6 77.4 76.6 79.7];
+F40=[61.3 60.21 60.9 62];
+F50=[66.2 66 67.3 66];
+Frame=[94.3 93.8 93 92.3 93.7 93.2 93.1];
+Fx=[mean(F20) mean(F23) mean(F24) mean(F25) mean(F26) mean(F27) mean(F30) mean(F40) mean(F50)]./mean(Frame);
+eFx=[std(F20) std(F23) std(F24) std(F25) std(F26) std(F27) std(F30) std(F40) std(F50)]./mean(Frame);
+errorbar(nu_filter*1e-9,Fx,eFx,'-.^r','linew',2)
+grid on
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+ legend('Prediction', 'Experiment','location','southeast')
+title('24GHz source')
+load bigF.mat
+ylim([0 1])
+
+
+figure(5)
+plot(nu_filter*1e-9,F35i,'-ok','linew',2)
+% Vpp3=[112.8 108.8 111.2 107.2 108.0 112.8 107.2 117.6 118.4]./[122.4 121.6 120.8 120.0 120.0 120.0 120.0 119.2 119.2];
+% Vpp4=[260 240 240 230 238 212 192 246 252]/226
+ hold on
+% plot(Freq,Vpp4,'-or')
+% plot(Freq,Vpp3,'-ok')
+F20=[94.7 95.4 96.2 94.2 ];
+F23=[ 90.3 93.3 87 86.6 ];
+F24=[ 87.6 91.6 88.4 89.5 ];
+F25=[87.7 88 88.3 87.5];
+F26=[85.2 83.9 83.1 84.6];
+F27=[84.9 83 80.5 77.3];
+F30=[82.6 82 83.3 85.5];
+F40=[87 89.5 89.2 88];
+F50=[91.4 94.2 94.8 90.7];
+Frame=[96.3 93.3 92.7 92 91.8 91.6 91 91.2];
+Fx=[mean(F20) mean(F23) mean(F24) mean(F25) mean(F26) mean(F27) mean(F30) mean(F40) mean(F50)]./mean(Frame);
+eFx=[std(F20) std(F23) std(F24) std(F25) std(F26) std(F27) std(F30) std(F40) std(F50)]./mean(Frame);
+errorbar(nu_filter*1e-9,Fx,eFx,'-.^r','linew',2)
+grid on
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+ legend('Prediction', 'Experiment','location','southeast')
+title('35GHz source')
+ylim([0 1.1])
Index: /THZ_filters/Experiment results/THzFilter.m
===================================================================
--- /THZ_filters/Experiment results/THzFilter.m	(revision 733)
+++ /THZ_filters/Experiment results/THzFilter.m	(revision 733)
@@ -0,0 +1,39 @@
+%Thz Filter
+close all; clear all
+Freq=[20 23 24 25 26 27 30 40 50];
+Vpp0=[101.6 104.00 108 113.6 122.4 114.4 104.6 87.2 88.]/145.6;
+Vpp1=[116.8 124.0 120.0 126.4 133.6 124.8 115.2 100 97.6]./[153.6 150.4 148.8 147.2 145.2 145.6 144.8 144.8 143.2];
+Vpp0a=[113.6 122.4 118.4 124.0 129.6 124 115.2 98.4 96.0]./[148.8 147.2 145.6 144.0 144.0 143.2 142.4 141.6 142.4];
+Vpp1a=[114.4 124.8 116.8 126.4 132.8 124.8 112.4 96.0 92.8]./[148.0 145.6 144.8 144.8 144.0 144.0 143.2 143.2 143.2];
+Vpp=[Vpp1; Vpp0a; Vpp1a];
+
+figure
+hold on
+% plot(Freq,Vpp0,'-ok')
+% plot(Freq,Vpp1,'-or','linew',2)
+% plot(Freq,Vpp0a,'-ok','linew',2)
+% plot(Freq,Vpp1a,'-ob','linew',2)
+errorbar(Freq,mean(Vpp),std(Vpp),'-or','linew',2)
+set(gca,'fontsize',16)
+grid on
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('GDO-2510, 24 [GHz]')
+% legend('Data set 1','Data set 2','Data set 3')
+ylim([0.5 1])
+
+% Vpp2=[106.4 104.8 109.6 105.6 104.8 110.4 105.8 114.4 117.6];
+Vpp3=[112.8 108.8 111.2 107.2 108.0 112.8 107.2 117.6 118.4]./[122.4 121.6 120.8 120.0 120.0 120.0 120.0 119.2 119.2];
+Vpp4=[53.8 52.8 55.2 48.0 51.2 55.2 45.6 58.4 60.8]./[68 66.4 65.6 65.6 65.6 65.6 65.6 65.6 65.6];
+figure
+hold on
+% plot(Freq,Vpp2)
+grid on
+plot(Freq,Vpp3,'-or','linew',2)
+plot(Freq,Vpp4,'-ok','linew',2)
+set(gca,'fontsize',16)
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('SOL-35310, 35 [GHz]')
+legend('With GHA','Without GHA','location','southeast')
+ylim([0.5 1])
Index: /THZ_filters/Experiment results/THzFilter2.m
===================================================================
--- /THZ_filters/Experiment results/THzFilter2.m	(revision 733)
+++ /THZ_filters/Experiment results/THzFilter2.m	(revision 733)
@@ -0,0 +1,15 @@
+%Experiment #2
+close all
+Freq=[20 23 24 25 26 27 30 40 50];
+Vpp1=([198 230 226 218 242 254 256 208 224]-16)./([248 248 244 246 244 244 242 244 244]-16);
+
+figure
+hold on
+plot(Freq,Vpp1,'-or','linew',2)
+
+set(gca,'fontsize',16)
+grid on
+xlabel('Frequency, [GHz]')
+ylabel('Transmissivity, [1]')
+title('GDO-2510, 24 [GHz]')
+ylim([0.5 1.1])
Index: /THZ_filters/Experiment results/readme.txt
===================================================================
--- /THZ_filters/Experiment results/readme.txt	(revision 733)
+++ /THZ_filters/Experiment results/readme.txt	(revision 733)
@@ -0,0 +1,13 @@
+MF_EXP.m -- big filter transmissivity
+MF_EXP2.m -- small filter transmissivity
+MF1.m -- original calculation
+
+
+THzFilter.m -- first measurements
+THzFilter2.m -- second measurements
+Experiment2TranslationStage.m -- second and half measurements
+Experiment3.m -- third try of measurements (exp data)
+AllMeasurements.m -- united measurements
+
+MakePlots.m -main plots with comparison
+
