diff options
author | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-05-13 15:35:26 -0400 |
---|---|---|
committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-05-13 15:58:56 -0400 |
commit | d1b62466d81b164656588ac1c55acff15ee9ea43 (patch) | |
tree | cce78f90b0768361c4a268b946848842e1e47456 /axial/cav.m | |
download | optics_toolkit-d1b62466d81b164656588ac1c55acff15ee9ea43.tar.gz optics_toolkit-d1b62466d81b164656588ac1c55acff15ee9ea43.zip |
initial
The optics_toolkit code taken from
http://mercury.pr.erau.edu/~greta9a1/downloads/index.html
the older version is also available at mathwork web site
http://www.mathworks.com/matlabcentral/fileexchange/15459-basic-paraxial-optics-toolkit
Diffstat (limited to 'axial/cav.m')
-rw-r--r-- | axial/cav.m | 136 |
1 files changed, 136 insertions, 0 deletions
diff --git a/axial/cav.m b/axial/cav.m new file mode 100644 index 0000000..9e2fe34 --- /dev/null +++ b/axial/cav.m @@ -0,0 +1,136 @@ +function [qrefl,qtrans,qcav,prefl,ptrans,pcav]=cav(qin,l,m,lambda,L,R1,R2,r1,r2,l1,l2,n_iter,varargin)
+% Propagates a Gaussian beam through a cavity.
+% The function returns the q-factors of the reflected beam, the transmitted
+% beam and the cavity beam at the first mirror. Also returns the reflected,
+% transmitted and intracavity field amplitudes. (Notation: prefl,ptrans,pcav
+% refer to the complex field amplitudes from each bounce, not power. Thus the
+% total transmitted power, for example, is Ptransmitted = epsilon0*abs(sum(ptrans))^2.
+%
+% AUTHOR: Andri M. Gretarsson, 2003.
+% LAST MODIFIED: 2007 by AMG.
+%
+% SYNTAX: [qrefl,qtrans,qcav,prefl,ptrans,pcav]=...
+% cav(qin,l,m,lambda,L,R1,R2,r1,r2,l1,l2,n_iter <,n,Lmirr,pin>);
+%
+% INPUT VARIABLES
+% ---------------
+% R1,R2 = Radii of curvature of the end mirrors. Positive if mirror is
+% concave as seen from inside the cavity, negative otherwise.
+% (Sides facing outwards are assumed to be flat.) R1 corresponds
+% to the input mirror and R2 to the end mirror.
+%
+% FIGURE:
+%
+% Input beam Input mirror End Mirror Transmitted beam
+% -----------------|(==============)|- - - - - - - - - - -
+% Cavity beam
+%
+% Note: Reflected beam is in same location as the Input beam but
+% travels in the opposite direction (away from the cavity).
+%
+% L = Cavity length
+% l,m = TEM_lm Gaussian mode incidnet on the cavity.
+% lambda = wavelength
+% qin = q of the incoming beam immediately before the input optic
+% outward facing side (assumed flat).
+% r1 = Reflectoin coefficient (fraction of field _amplitude_ reflected) of input mirror.
+% r2 = Reflection coefficient of end mirror.
+% l1 = Loss coefficient for a single pass through the input mirror.
+% (Fraction of field _amplitude_ lost.)
+% l2 = Loss coefficient for a single pass through the end mirror.
+% (Fraction of field _amplitude_ lost.)
+% n_iter = Number of iterations (cavity traversals) to calculate.
+% n = Optional: 1x3 vector of indices of ref. of: mirror substrates,
+% cavity medium, external medium.
+% Default is n=[1.46,1,1].
+% Lmirr = Optional: 1x2 vector of mirror thicknesses (on the optic
+% axis). First value corresponds to the input mirror, second to
+% the end mirror. Default: Lmirr=[0,0].
+% pin = Amplitude factor of the beam entering the cavity
+%
+% NOTES: In the current version, antireflective coatings on the outside
+% faces (flat faces) of the mirrors are assumed to be perfect. This could
+% be improved in future versions. Also, the reflectivity and transmissivity
+% of the coatings are assumed to be the same for light incident from
+% either the substrate side or cavity side of the coating. Clearly, this
+% could be improved also.
+%
+%--------------------------------------------------------------------------
+% SYNTAX: [qrefl,qtrans,qcav,prefl,ptrans,pcav]=...
+% cav(qin,l,m,lambda,L,R1,R2,r1,r2,l1,l2,n_iter <,n,Lmirr,pin>);
+%--------------------------------------------------------------------------
+
+if ( nargin>=13 && ~isempty(varargin{1}) ), n=varargin{1}; else n=[1.46,1,1]; end
+if ( nargin>=14 && ~isempty(varargin{2}) ), Lmirr=varargin{2}; else Lmirr=[0,0]; end
+if ( nargin>=15 && ~isempty(varargin{3}) ), pin=varargin{3}; else pin=1; end
+
+nsubs=n(1);
+ncav=n(2);
+noutside=n(3);
+L1=Lmirr(1);
+L2=Lmirr(2);
+
+% Variable initialization
+t1 = sqrt(1-r1^2-l1^2);
+t2 = sqrt(1-r2^2-l2^2);
+qrefl = zeros(n_iter,1); qcav = zeros(n_iter,1); qtrans = zeros(n_iter,1);
+prefl = zeros(n_iter,1); pcav = zeros(n_iter,1); ptrans = zeros(n_iter,1);
+% #cav -> immediately inside input mirror travelling towards end mirror
+% #refl -> immediately outside input mirror (outside cavity) travelling towards laser
+% #trans-> immediately outside end mirror (outside cavity) travelling away from cavity
+
+% Note the poor notation for field amplitudes throughout: prefl, pcav,
+% etc. The letter p does NOT mean power in this case!
+
+% Commonly used quantitites
+freeL = free(L,ncav);
+freeL1 = free(L1,nsubs);
+freeL2 = free(L2,nsubs);
+mirrR1 = mirr(R1); % input mirror
+mirrR2 = mirr(R2); % end mirror
+% mirrR1phase=exp(i*2*pi*(nsubs*L1/lambda-floor(nsubs*L1/lambda)));
+% mirrR2phase=exp(i*2*pi*(nsubs*L2/lambda-floor(nsubs*L2/lambda)));
+% tripphase=exp(i*2*pi*(ncav*L/lambda-floor(ncav*L/lambda)));
+mirrR1phase=exp(i*2*pi*(nsubs*L1/lambda));
+mirrR2phase=exp(i*2*pi*(nsubs*L2/lambda));
+tripphase=exp(i*2*pi*(ncav*L/lambda));
+
+% Prompt reflection
+[qrefl(1),prefl(1)]= prop(qin,...
+ fdie(nsubs,noutside)*freeL1*mirr(-R1)*freeL1*fdie(noutside,nsubs),...
+ [l,m],-r1*mirrR1phase^2*pin);
+
+qcav(1)=i*1; pcav(1)=0;
+qtrans(1)=i*1; pcav(1)=0;
+
+% First entry into cavity
+[qcav(2),pcav(2)] = prop(qin,...
+ sdie(-R1,nsubs,ncav)*freeL1*fdie(noutside,nsubs),...
+ [l,m],t1*mirrR1phase*pin);
+
+% First transmission through end mirror
+[qtrans(2),ptrans(2)] = prop(qcav(2),...
+ fdie(nsubs,noutside)*freeL2*sdie(R2,ncav,nsubs)*freeL,...
+ [l,m],t2*tripphase*mirrR2phase*pcav(2));
+
+% First round trip leakage through input mirror
+[qrefl(2),prefl(2)] = prop(qcav(2),...
+ fdie(nsubs,noutside)*freeL1*sdie(R1,ncav,nsubs)*freeL*mirrR2*freeL,...
+ [l,m],t1*r2*mirrR1phase*tripphase^2*pcav(2));
+
+for s = 3:n_iter+2
+
+ [qcav(s),pcav(s)] = prop(qcav(s-1),...
+ mirrR1*freeL*mirrR2*freeL,...
+ [l,m],r1*r2*tripphase^2*pcav(s-1));
+
+ [qtrans(s),ptrans(s)] = prop(qcav(s),...
+ fdie(nsubs,noutside)*freeL2*sdie(R2,ncav,nsubs)*freeL,...
+ [l,m], t2*tripphase*mirrR2phase*pcav(s));
+
+ [qrefl(s),prefl(s)] = prop(qcav(s),...
+ fdie(nsubs,noutside)*freeL1*sdie(R1,ncav,nsubs)*freeL*mirrR2*freeL,...
+ [l,m],t1*r2*mirrR1phase*tripphase^2*pcav(s));
+
+
+end
|