Valentina Salazar
3 years ago
1 changed files with 69 additions and 0 deletions
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clear; |
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% Elementary constants |
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c = 299792458; %Speed of light [m/s] |
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h = 6.626070040e-34; %Planck constant [J/Hz] |
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hbar = h/2/pi; |
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u0 = 4*pi*1e-7; %Vacuum permeability [N/A^2] |
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e0 = 1/u0/(c^2); %Vacuum permittivity [A^2*s^4/kg/m^3] |
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qe = 1.6021766208e-19; %Elementary charge [C] |
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G = 6.67408e-11; %Gravitational constant [m^3/kg/s^2] |
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kB = 1.38064852e-23; %Boltzmann constant [J/K] |
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me = 9.10938356e-31; %Electron rest mass [kg] |
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mp = 1.672621898e-27; %Proton mass [kg] |
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uB = qe*hbar /2/me; %Bohr magneton [J/T] |
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uN = qe*hbar /2/mp; %Nuclear magnton [J/T] |
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alpha = u0*qe^2*c/(2*h); %Fine structure constant |
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u = 1.660539040e-27; %Atomic mass unit [kg] |
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a0 = 4*pi*e0*hbar^2/me/qe^2; %Bohr radius [m] |
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Ry = 13.605693009; %Rydberg energy [eV] |
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%Dysprosium properties |
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mDy = 164*u; %Dysprosium mass [kg] |
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abuDy164 = 0.2826; %Dy164 abundance |
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Polar1064 = 193*4*pi*e0*a0^3; %Dynamical polarizability of Dy for 1064 and 532 [A^2s^4/kg] |
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Polar532 = 350*4*pi*e0*a0^3; |
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%Laser properties |
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lambda = 532e-9; %Laser wavelength [m] |
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k = 2*pi/lambda; %Wave number of laser [m^-1] |
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P0 = 10; %Power [W] |
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%Coordinate rotation y-axis for E1 |
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theta= 4/180*pi; %Half angle between the beams |
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x = linspace(-3000,3000,1501)*1e-6; %Definition of coordinate System |
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y = 0; |
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z = linspace(-300,300,1501)*1e-6; |
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[X,Z]=meshgrid(x,z); |
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xt= X.*cos(theta)+Z.*sin(theta); |
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yt = y; |
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zt= -X.*sin(theta)+Z.*cos(theta); |
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%Gaussian beam propagating in xt direction |
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w0 = 90e-6; %Beam waist at x=xt=0 (center of the trap) |
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xr = pi*w0.^2/lambda; %Rayleigh length i xt-direction |
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wxt = w0.*sqrt(1+(xt./xr).^2); %Radius to 1/e |
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P = P0/2; |
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E0 = sqrt(2*P./(pi*wxt.^2*c*e0)); %Electric field at time 0 , x=-f origin |
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E1 = E0*w0./wxt.*exp(-(zt.^2+yt.^2)./wxt.^2).*exp(-1i*k.*xt); %Electric field 1 |
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%Coordinate rotation y-axis for E2 |
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theta= -theta; %Half angle between the beams |
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xt= X.*cos(theta)+Z.*sin(theta); |
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yt = y; |
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zt= -X.*sin(theta)+Z.*cos(theta); |
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E2 = E0*w0./wxt.*exp(-(zt.^2+yt.^2)./wxt.^2).*exp(-1i*k.*xt); %Electric field 1 |
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%Interference of the two beams |
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Itot = abs(E1+E2).^2 ; %Intensity of the interference pattern |
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figure |
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imagesc(x,z,Itot) |
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set(gca,'YDir','normal') |
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