summaryrefslogtreecommitdiff
path: root/liouville.m
diff options
context:
space:
mode:
Diffstat (limited to 'liouville.m')
-rw-r--r--liouville.m14
1 files changed, 8 insertions, 6 deletions
diff --git a/liouville.m b/liouville.m
index 4c78557..4ce714c 100644
--- a/liouville.m
+++ b/liouville.m
@@ -1,4 +1,5 @@
1;
+clear all;
t0 = clock (); % we will use this latter to calculate elapsed time
@@ -30,14 +31,15 @@ kappa_p =zeros(1,N_detun_steps+1);
kappa_m =zeros(1,N_detun_steps+1);
detun_step=(detuning_p_max-detuning_p_min)/N_detun_steps;
+% now we create Liouville indexes list
+[N, rhoLiouville_w, rhoLiouville_r, rhoLiouville_c]=unfold_density_matrix(Nlevels,Nfreq);
+rhoLiouville=zeros(N,1);
% calculate E_field independent properties of athe atom
% to be used as sub matrix templates for Liouville operator matrix
[L0m, polarizability_m]=L0_and_polarization_submatrices( ...
- Nlevels*Nlevels, ...
- H0, g_decay, g_dephasing, dipole_elements, ...
- E_field, ...
- modulation_freq, rhoLiouville_w, rhoLiouville_r, rhoLiouville_c ...
+ Nlevels, ...
+ H0, g_decay, g_dephasing, dipole_elements ...
);
for detuning_p_cntr=1:N_detun_steps+1;
wp0=w12;
@@ -77,8 +79,8 @@ for detuning_p_cntr=1:N_detun_steps+1;
%rho_d=rhoOfFreq(rhoLiouville, 3, Nlevels, Nfreq); % drive frequency
%rho_m=rhoOfFreq(rhoLiouville, 4, Nlevels, Nfreq); % opposite sideband frequency
- kappa_p(detuning_p_cntr)=sucseptibility(2, rhoLiouville, dipole_elements, Nlevels, Nfreq);
- %kappa_m(detuning_p_cntr)=sucseptibility(4, rhoLiouville, dipole_elements, Nlevels, Nfreq);
+ kappa_p(detuning_p_cntr)=susceptibility(2, rhoLiouville, dipole_elements, Nlevels, Nfreq);
+ %kappa_m(detuning_p_cntr)=susceptibility(4, rhoLiouville, dipole_elements, Nlevels, Nfreq);
detuning_freq(detuning_p_cntr)=detuning_p;
%kappa_p_re=real(kappa_p);