| IPSF_Vectorial_1Int(na, wl, n1, n2, r, z, d, ang,deltaZ)
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function [r z I] = IPSF_Vectorial_1Int(na, wl, n1, n2, r, z, d, ang,deltaZ)
[r z] = meshgrid(r,z);
if n2 < n1
a = asin(n2./n1);
else
a = asin(na/n1);
end
k = (2*pi)/wl;
I0 = quadv(@E0field,0,a);
I1 = quadv(@E1field,0,a);
I2 = quadv(@E2field,0,a);
I = abs(I0).^2 + 4 .* abs(I1).^2 .* (cos(ang)).^2 + abs(I2).^2 + 2 .* cos(2 .* ang) .* real(I0 .* conj(I2));
function E0 = E0field(th1)
% Theta 2 from snells law
th2 = asin((n1.*sin(th1))./n2);
% Abberation Function
% Phi=0;
%Phi =deltaZ.* sin(th1).^2;
Phi = -d.*(n1.*cos(th1)-n2.*cos(th2))+deltaZ.*(1-cos(th1));
% Fresnel coefficients
[ts tp] = FresnelCoeff(th1, th2);
% Electric Field
E0 = (cos(th1).^(1/2)) .* sin(th1) .* (ts + tp .* cos(th2)) .* besselj(0, k .* r .* n1 .* sin(th1)) .* exp(-i .* k .* Phi - i.* k .* z .* n2 .* cos(th2));
end
function E1 = E1field(th1)
% Theta 2 from snells law
th2 = asin((n1.*sin(th1))./n2);
% Abberation Function
% Phi=0;
%Phi =deltaZ.* sin(th1).^2;
Phi = -d.*(n1.*cos(th1)-n2.*cos(th2))+deltaZ.*(1-cos(th1));
% Fresnel coefficients
[ts tp] = FresnelCoeff(th1, th2);
% Electric Field
E1 = (cos(th1).^(1/2)) .* sin(th1) .* (tp .* sin(th2)) .* besselj(1, k .* r .* n1 .* sin(th1)) .* exp(-i .* k .* Phi - i.* k .* z .* n2 .* cos(th2));
end
function E2 = E2field(th1)
% Theta 2 from snells law
th2 = asin((n1.*sin(th1))./n2);
% Abberation Function
% Phi=0;
% Phi =deltaZ.* sin(th1).^2;
Phi = -d.*(n1.*cos(th1)-n2.*cos(th2))+deltaZ.*(1-cos(th1));
% Fresnel coefficients
[ts tp] = FresnelCoeff(th1, th2);
% Electric Field
E2 = (cos(th1).^(1/2)) .* sin(th1) .* (ts - tp .* cos(th2)) .* besselj(2, k .* r .* n1 .* sin(th1)) .* exp(-i .* k .* Phi - i.* k .* z .* n2 .* cos(th2));
end
end
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