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| author | Eugeniy E. Mikhailov <evgmik@gmail.com> | 2020-09-25 09:04:00 -0400 |
|---|---|---|
| committer | Eugeniy E. Mikhailov <evgmik@gmail.com> | 2020-09-25 09:04:00 -0400 |
| commit | 0a88292ffb9018a08b212a0f10031550a54c19cd (patch) | |
| tree | fa8cedfc7b2350c2ad43b9670ce2d117ac733f6f /compass_circ_output_results.m | |
| parent | 22fe474995db0894edaf4bfb1b73023f3af1d3ec (diff) | |
| download | multi_mode_eit-0a88292ffb9018a08b212a0f10031550a54c19cd.tar.gz multi_mode_eit-0a88292ffb9018a08b212a0f10031550a54c19cd.zip | |
better name for variable
Diffstat (limited to 'compass_circ_output_results.m')
| -rw-r--r-- | compass_circ_output_results.m | 14 |
1 files changed, 12 insertions, 2 deletions
diff --git a/compass_circ_output_results.m b/compass_circ_output_results.m index 627ead7..b2c7a04 100644 --- a/compass_circ_output_results.m +++ b/compass_circ_output_results.m @@ -1,7 +1,7 @@ 1; -load '/tmp/total_relative_transmission_vs_phi.mat' ; +load '/tmp/total_relative_transmission_vs_theta.mat' ; % let's create sideband transmission vs angle vectors % 1st of all we need to create matrix instead of a vector @@ -11,7 +11,7 @@ load '/tmp/total_relative_transmission_vs_phi.mat' ; N_detunings=length(detuning_freq); N_angles=length(thetas); -transmission_matrix=reshape(total_relative_transmission_vs_phi, N_detunings, N_angles); +transmission_matrix=reshape(total_relative_transmission_vs_theta, N_detunings, N_angles); % the last sideband is not in two-photon resonance % we use it as a reference for background transmission @@ -54,4 +54,14 @@ legend(labels); hold off; +figure(2) +j=4; k= 3; +j=2; k= 7; +% plotting parametric line of a sideband amplitude (j) vs another one (k) +plot(zoom_factor*(transmission_matrix(j,:)), zoom_factor*(transmission_matrix(k,:))) +xlabel( labels{j}); +ylabel( labels{k}); +title('One sideband amplitude vs another for different angles theta, between B-field and light propagation direction'); + + % vim: ts=2:sw=2:fdm=indent |