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-rw-r--r--faraday/output_faraday_results_vs_B.m59
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diff --git a/faraday/output_faraday_results_vs_B.m b/faraday/output_faraday_results_vs_B.m
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+function psr_rad=output_faraday_results_vs_B()
+load '/tmp/xi_vs_B.mat' ;
+
+Er=(1+I*xi_right)*E_field_pos_freq.right;
+El=(1+I*xi_left) *E_field_pos_freq.left;
+
+Ex=(Er+El)/sqrt(2);
+Ey=I*(Er-El)/sqrt(2);
+
+%extra rotation to compensate rotation due to ellipticity
+% actually no need for it since x-polarization shifts by positive phase
+% and y-pol by negative phase
+%el_rot=0*psi_el;
+%Ex=cos(el_rot)*Ex-sin(el_rot)*Ey;
+%Ey=sin(el_rot)*Ex+cos(el_rot)*Ey;
+
+Ipos=(abs(Ey).^2)/2;
+Ineg=(abs(Ex).^2)/2;
+
+figure(1);
+hold off;
+plot(detuning_freq, real(xi_left-xi_right), '-');
+title("differential real xi");
+xlabel("two photon detuning (MHz)");
+
+figure(2);
+hold off;
+plot(detuning_freq, imag(xi_left-xi_right), '-');
+title("differential imag xi");
+xlabel("two photon detuning (MHz)");
+
+figure(3);
+hold off;
+plot(detuning_freq, real(xi_left), '-', detuning_freq, real(xi_right), '-');
+title("real xi");
+xlabel("two photon detuning (MHz)");
+
+figure(4);
+hold off;
+plot(detuning_freq, imag(xi_left), '-', detuning_freq, imag(xi_right), '-');
+title("imag xi");
+xlabel("two photon detuning (MHz)");
+
+figure(5);
+hold off;
+I_probe=E_field_probe^2;
+psr_rad=(Ipos-Ineg)/(2*I_probe);
+plot(detuning_freq, psr_rad, '-');
+subt_str=sprintf("Laser Rabi freq normalized to upper state decay %.3f, ellipticity %.1f degree, \n B field ground level splitting %.3f Gauss", I_probe, psi_el*180/pi, B_field);
+title(cstrcat("BPD normilized PSR signal at F_g=2 to F_e=1,2.\n ",subt_str) );
+xlabel("two photon detuning (MHz)");
+ylabel("PSR (radians)");
+
+print("psr_vs_detuning.ps");
+
+fname= sprintf("psr_vs_detuning_Fg=2toFe=1,2_Ip=%.3f_el_%.1f_B=%.3fG.mat", I_probe, psi_el*180/pi,B_field);
+save(fname,'detuning_freq', 'psr_rad');
+
+return;