Cosmetic changes.
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@ -30,16 +30,16 @@ DyMagneticMoment = 9.93*9.274009994E-24;
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%% Bogoliubov excitation spectrum for quasi-2D dipolar gas with QF correction
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AtomNumber = 1E5; % Total atom number in the system
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wz = 2*pi*72.4; % Trap frequency in the tight confinement direction
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lz = sqrt(PlanckConstantReduced/(Dy164Mass*wz)); % Defining a harmonic oscillator length
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as = 102.515*BohrRadius; % Scattering length
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Trapsize = 7.5815; % Trap is assumed to be a box of finite extent , given here in units of the harmonic oscillator length
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wz = 2 * pi * 72.4; % Trap frequency in the tight confinement direction
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lz = sqrt(PlanckConstantReduced/(Dy164Mass * wz)); % Defining a harmonic oscillator length
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as = 102.515 * BohrRadius; % Scattering length
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Trapsize = 7.5815 * lz; % Trap is assumed to be a box of finite extent , given here in units of the harmonic oscillator length
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alpha = 0; % Polar angle of dipole moment
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phi = 0; % Azimuthal angle of momentum vector
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MeanWidth = 5.7304888515*lz; % Mean width of Gaussian ansatz
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MeanWidth = 5.7304888515 * lz; % Mean width of Gaussian ansatz
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k = linspace(0, 3e6, 1000); % Vector of magnitudes of k vector
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AtomNumberDensity = AtomNumber / (Trapsize * lz)^2; % Areal density of atoms
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AtomNumberDensity = AtomNumber / Trapsize^2; % Areal density of atoms
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add = VacuumPermeability*DyMagneticMoment^2*Dy164Mass/(12*pi*PlanckConstantReduced^2); % Dipole length
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eps_dd = add/as; % Relative interaction strength
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gs = 4 * pi * PlanckConstantReduced^2/Dy164Mass * as; % Contact interaction strength
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