Calculations/Time-Series-Analyzer/computeAndcompareRIN.m

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% Script to compute the Relative Intensity Noise of a laser by recording the y-t signal
% by Mathias Neidig in 2012
% modified for DyLab use by Karthik in 2024
% The RIN is defined as
%
% RIN = 10* log10 [Single-sided power spectrum density / (average power)]
%
% and is given in [RIN] = dB/Hz
clear all
close all
%% Set the directory where the data is
dirDCData = 'C:\\Users\\Karthik\\Documents\\GitRepositories\\Calculations\\Time-Series-Analyzer\\Time-Series-Data\\20240915\\After_AOD\\DC_Coupling\\';
dirACData = 'C:\\Users\\Karthik\\Documents\\GitRepositories\\Calculations\\Time-Series-Analyzer\\Time-Series-Data\\20240915\\After_AOD\\AC_Coupling\\';
%% Load the files which contain: - the DC coupled y-t signal to obtain the averaged power
% - the AC coupled y-t signal to obtain the fluctuations
% - the AC coupled y-t signal with the beam blocked to obtain the background fluctuations
%------------------------------------------------------------------------- %
bgsignal = load( [ dirACData '20240915_Background_AC'] ); %
dcsignal = load( [ dirDCData '20240915_5V_1.1Mod_DC_PID_Inactive'] ); %
acsignal_1 = load( [ dirACData '20240915_5V_1.1Mod_AC_PID_Inactive'] ); %
acsignal_2 = load( [ dirACData '20240915_5V_1.1Mod_AC_PID_Active'] ); %
label_0 = 'Background'; %
label_1 = 'Power = 5 V, Modulation = 1.1 V, PID Inactive'; %
label_2 = 'Power = 5 V, Modulation = 1.1 V, PID Active'; %
%------------------------------------------------------------------------- %
%% Read out the important parameters
dcdata = dcsignal.A;
acdata_1 = acsignal_1.A;
acdata_2 = acsignal_2.A;
bgdata = bgsignal.A;
N = length(dcdata); % #samples
f_s = 1/dcsignal.Tinterval; % Sample Frequency
delta_f = f_s/N; % step size in frequency domain
delta_t = 1/f_s; % time step
%% Custom Control Parameters
% Choose smoothing parameter; has to be odd
%----------------%
span = 21; %
%----------------%
%% Computes the RIN
% compute the average power (voltage^2)
average_P = mean(dcdata.*dcdata);
% compute the power spectrum density FFT(A) x FFT*(A)/N^2 of the source & the bg
psd_src_1 = fft(acdata_1) .* conj(fft(acdata_1))/N^2;
psd_src_2 = fft(acdata_2) .* conj(fft(acdata_2))/N^2;
psd_bg = fft(bgdata) .* conj(fft(bgdata))/N^2;
% converts the psd to the single-sided psd --> psd is symmetric around zero --> omit
% negative frequencies and put the power into the positive ones --> spsd
for i = 1 : N/2+1
if i>1
spsd_src_1(i) = 2*psd_src_1(i);
spsd_src_2(i) = 2*psd_src_2(i);
spsd_bg(i) = 2*psd_bg(i);
else
spsd_src_1(i) = psd_src_1(i);
spsd_src_2(i) = psd_src_2(i);
spsd_bg(i) = psd_bg(i);
end
end
% smooths the spsd by doing a moving average
spsd_src_smooth_1 = smooth(spsd_src_1,span,'moving');
spsd_src_smooth_2 = smooth(spsd_src_2,span,'moving');
spsd_bg_smooth = smooth(spsd_bg, span,'moving');
% calculates the RIN given in dB/Hz; the factor delta_f is needed to convert from dB/bin into dB/Hz
spsd_src_smooth_rel_1 = spsd_src_smooth_1/(average_P*delta_f);
spsd_src_smooth_rel_2 = spsd_src_smooth_2/(average_P*delta_f);
spsd_bg_smooth_rel = spsd_bg_smooth /(average_P*delta_f);
RIN_src_smooth_1 = 10*log10(spsd_src_smooth_rel_1);
RIN_src_smooth_2 = 10*log10(spsd_src_smooth_rel_2);
RIN_bg_smooth = 10*log10(spsd_bg_smooth_rel);
% creates an array for the frequencies up to half the sampling frequency
f = f_s/2 * linspace(0,1,N/2+1);
f_smooth = smooth(f,span,'moving');
%
% Calculates the shot noise limit of the used PD given the wavelength of the light source and
% incident average power
PlanckConstant = 6.62607015E-34;
SpeedOfLight = 299792458;
WavelengthOfLaserLight = 1064E-9;
FrequencyOfLaserLight = SpeedOfLight / WavelengthOfLaserLight;
QuantumEfficiencyOfPD = 1;
AverageIncidentPower = 0.001; % (in W)
ShotNoiseLimit = 10*log10((2 * PlanckConstant * FrequencyOfLaserLight) / (QuantumEfficiencyOfPD * AverageIncidentPower));
%% Plots the RIN
% Plots the RIN vs frequency
f_ = clf;
figure(f_);
set(gcf,'Position',[100 100 950 750])
semilogx(f_smooth, RIN_bg_smooth, LineStyle = "-", Color = [.7 .7 .7])
hold on
semilogx(f_smooth,RIN_src_smooth_1,'r-')
semilogx(f_smooth,RIN_src_smooth_2,'b-')
ax = gca(f_);
ax.XAxis.FontSize = 14;
ax.YAxis.FontSize = 14;
xlabel('Frequency [Hz]', FontSize=16)
ylabel('RIN [dBc/Hz]', FontSize=16)
xlim([10 5E6]);
ylim([-140 -25]);
title('\bf Intensity noise of Arm 1 of the ODT as measured by an Out-of-loop PD', FontSize=14)
legend(label_0, label_1, label_2, 'Location','NorthWest', FontSize=12);
grid on
% optional: save the picture without editing wherever you want
%------------------------------------------%
% saveas(f_,'FileName','png'); %
%------------------------------------------%
%%
compute_eFoldingTime(f_smooth, spsd_src_smooth_rel_2, 100, 1000, label_2)
%%
compute_eFoldingTime(f_smooth, spsd_src_smooth_rel_2, 1000, 5000, label_2)
%%
function compute_eFoldingTime(faxis, Skk, fstart, fend, data_str)
% computes the energy e-folding time: time to increase the energy by a factor e in sec.
[~,idx_ini] = min(abs(faxis-(2 * fstart))); % Find closest index for 2*fstart
[~,idx_fin] = min(abs(faxis-(2 * fend))); % Find closest index for 2*fend
Skk = Skk(idx_ini:idx_fin); % Slice Skk array
freqs = linspace(fstart, fend, length(Skk));
% Calculate e-folding time
e_folding_time = arrayfun(@(idx) 1 / (pi^2 * freqs(idx)^2 * Skk(idx)), 1:length(freqs));
% Plotting
figure('Position', [100, 100, 1200, 800]);
semilogx(freqs, e_folding_time, 'r', 'LineWidth', 2, 'DisplayName', data_str);
hold on;
grid on;
set(gca, 'GridLineStyle', '-'); % Thin grid lines
% Create gridlines for multiples of 10
x_multiples_of_10 = 10.^floor(log10(min(freqs(freqs > 0))):log10(max(freqs(freqs > 0))));
for val = x_multiples_of_10
xline(val, 'k-', 'LineWidth', 2); % Thick lines for multiples of 10
end
legend('show', 'Location', 'southwest', 'FontSize', 12);
xlabel('Frequency [Hz]', 'FontSize', 14);
ylabel('$T_e$ [s]', 'Interpreter', 'latex', 'FontSize', 14);
title(sprintf('Lower Bound= %.5f s', min(e_folding_time)), 'FontSize', 14);
set(gca, 'XScale', 'log');
set(gca, 'FontSize', 12);
hold off;
end