1;
clear all; 
t0 = clock (); % we will use this latter to calculate elapsed time


% load useful functions;
useful_functions;

% some physical constants
useful_constants;

% load atom energy levels and decay description
%rb87_D1_line;
%four_levels_with_polarization;
%four_levels;
three_levels;
%two_levels;

% load EM field description
field_description;

%Nfreq=length(modulation_freq);



%tune probe frequency
detuning_p=0;
N_detun_steps=100;
%detuning_p_min=-B_field*gmg*4; % span  +/-4 Zeeman splitting
%detuning_p_max=-detuning_p_min;
detuning_freq=zeros(1,N_detun_steps+1);
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;

fprintf (stderr, "calculating atom properties\n");
fflush (stderr);
% calculate E_field independent properties of the atom
% to be used as sub matrix templates for Liouville operator matrix
[L0m, polarizability_m]=L0_and_polarization_submatrices( ...
		Nlevels, ...
		H0, g_decay, g_dephasing, dipole_elements ...
		);
elapsed_time = etime (clock (), t0);
fprintf (stderr, "elapsed time so far is %.3f sec\n",elapsed_time);
fflush (stderr);

global atom_properties;
atom_properties.L0m=L0m;
atom_properties.polarizability_m=polarizability_m;
atom_properties.dipole_elements=dipole_elements;

Ed=.1;     Edc=conj(Ed);
Ep=0.8*Ed;  Epc=conj(Ep);

%modulation_freq=[0,  wp, wd, -wp, -wd,  wp-wd, wd-wp];
E_field_drive   =[0,  0 , Ed,  0  , Edc, 0,     0    ];
E_field_probe   =[0,  Ep, 0 ,  Epc, 0  , 0,     0    ];
E_field_zero    =[0,  0 , 0 ,  0  , 0  , 0,     0    ];
E_field_lab.linear = E_field_zero + (1.00000+0.00000i)*E_field_probe  + (1.00000+0.00000i)*E_field_drive; 
E_field_lab.right  = E_field_zero + (0.00000+0.00000i)*E_field_probe  + (0.00000+0.00000i)*E_field_drive;
E_field_lab.left   = E_field_zero + (0.00000+0.00000i)*E_field_probe  + (0.00000+0.00000i)*E_field_drive;

% phi is angle between linear polarization and axis x
phi=pi*2/8;
% theta is angle between lab z axis (light propagation direction) and magnetic field axis (z')
theta=pi/2;
theta=0;

% we define light as linearly polarized 
E_field_lab.x=cos(phi)*E_field_lab.linear;
E_field_lab.y=sin(phi)*E_field_lab.linear;
E_field_lab.z=E_field_zero;

basis_transformation; % load subroutines
coord_transf_m =  lin2circ * oldlin2newlin(theta);
E_field.right  = coord_transf_m(1,1)*E_field_lab.x + coord_transf_m(1,2)*E_field_lab.y + coord_transf_m(1,3)*E_field_lab.z;
E_field.left   = coord_transf_m(2,1)*E_field_lab.x + coord_transf_m(2,2)*E_field_lab.y + coord_transf_m(2,3)*E_field_lab.z;
E_field.linear = coord_transf_m(3,1)*E_field_lab.x + coord_transf_m(3,2)*E_field_lab.y + coord_transf_m(3,3)*E_field_lab.z;


fprintf (stderr, "tuning laser in forloop to set conditions vs detuning\n");
fflush (stderr);

detuning_freq=[-.075, -.05, -.025, 0 , .025, .05 , .075, .1];

problem_cntr=1;
N_angle_steps=15;
min_angle=0; max_angle=pi/2; 
phis=min_angle:((max_angle-min_angle)/N_angle_steps):max_angle;
for phi=phis;
	for detuning_p_cntr=1:length(detuning_freq);
		% we define light as linearly polarized 
		% where phi is angle between light polarization and axis x
		E_field_lab.x=cos(phi)*E_field_lab.linear;
		E_field_lab.y=sin(phi)*E_field_lab.linear;
		E_field_lab.z=E_field_zero;
		% now we transfor x,y,z, to x',y', and z' with respect to magnetic field az z' axis
		coord_transf_m =  lin2circ * oldlin2newlin(theta);
		E_field.right  = coord_transf_m(1,1)*E_field_lab.x + coord_transf_m(1,2)*E_field_lab.y + coord_transf_m(1,3)*E_field_lab.z;
		E_field.left   = coord_transf_m(2,1)*E_field_lab.x + coord_transf_m(2,2)*E_field_lab.y + coord_transf_m(2,3)*E_field_lab.z;
		E_field.linear = coord_transf_m(3,1)*E_field_lab.x + coord_transf_m(3,2)*E_field_lab.y + coord_transf_m(3,3)*E_field_lab.z;

			wp0=w_pf1;
			wd=w_pf1-w_hpf_ground;
			detuning_p=detuning_freq(detuning_p_cntr);
			wp=wp0+detuning_p;
			wm=wd-(wp-wd);
			%modulation_freq=[0,  wp, wd, wm,   -wp, -wd, -wm,  wp-wd, wd-wp];
			modulation_freq=[0,  wp, wd, -wp,   -wd,  wp-wd, wd-wp];
			freq_index=freq2index(wp,modulation_freq);

			atom_field_problem.E_field          = E_field;
			atom_field_problem.modulation_freq  = modulation_freq;
			atom_field_problem.freq_index       = freq_index;

			problems_cell_array{problem_cntr}=atom_field_problem;
			problem_cntr++;


			%kappa_p(detuning_p_cntr)=susceptibility_steady_state_at_freq( atom_field_problem);
	endfor
endfor

save '/tmp/problem_definition.mat' problems_cell_array atom_properties  detuning_freq  theta;
fprintf (stderr, "now really hard calculations begin\n");
fflush (stderr);
% once we define all problems the main job is done here
%kappa_p=cellfun( @susceptibility_steady_state_at_freq, problems_cell_array);
%kappa_p=parcellfun(2, @susceptibility_steady_state_at_freq, problems_cell_array);
%[xi_linear, xi_left, xi_right]=parcellfun(2, @susceptibility_steady_state_at_freq, problems_cell_array);
total_absorption_vs_detuning=parcellfun(2, @total_field_absorption, problems_cell_array);

%save 'xi_vs_detuning.mat' detuning_freq xi_linear xi_left xi_right  ;
problem_cntr--;
save '/tmp/total_absorption_vs_detuning_and_angle_phi.mat' detuning_freq total_absorption_vs_detuning phis problem_cntr;

compass_output_results;

elapsed_time = etime (clock (), t0)

% vim: ts=2:sw=2:fdm=indent