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Knowledge Base

The function mie3ds12 can be used to calculate the scattered far field of any (non-magnetic) material embedded in any ambient dielectric material. The function returns the scattering functions S1 and S2. The scattered far field can be calculated by

 

Where E|| is the field in the scattering plane and E is the field orthogonal to the scattering plane. The scattering plane is defined by the incident and scattered directions. The angle θ is the angle within the scattering plane (with respect to the incident angle) and the angle φ is the angle between the incident electric field and the scattering plane.

 

 

Note:

This script command was introduced in the 2017a R5 release.

 

Supported Product: FDTD, MODE, INTERCONNECT, DEVICE

 

References:

[1] Bohren C.F. and D.R. Huffman, “Absorption and Scattering of Light by Small Particles”, John Wiley, New York, NY, 1983.

[2] Documentation of Mätzler C. “MATLAB Functions for Mie Scattering and Absorption, Version 2”, IAP Res. Rep. No. 2002-11, August, 2002.

 

Syntax

Description

S = mie3ds12(u,m,x);

The result Q is a struct which contains quantities S1, S2 which has dimensions NxM where N is the length of u and M is the length of x.

 

The arguments are:

u: this is cos(q)

m: the ratio of the refractive index of the sphere to the refractive index of the ambient dielectric medium. This quantity may be complex-valued because the refractive index of the sphere may be complex. This quantity should either have a singleton value, or be the same length of x for dispersive media.

x: the size parameter which is defined as 2*pi*r/lambda0*n1 where lambda0 is the free space wavelength, r is the sphere radius and n1 is the real-valued refractive index of the ambient medium.

S = mie3ds12(u,m,x,nmax);

nmax : the maximum number of orders to calculate for the mie coefficients. The default value is 0, and in this case the nmax = ceil(x+4*x^(1/3))+2. There is typically no need to modify the default value.

 

Example

For example, lets calculate field in XY and YZ planes for 500nm light that is incident along the y axis, polarized along the z axis.

# input parameters

n1 = 1;

n2 = 1.5;

lambda0 = 500e-9;

radius = 500e-9;

# calculate m,x and call mie3ds12

m = n2/n1;

x = 2*pi*radius/lambda0*n1;

theta = linspace(0,2*pi,1000);

S = mie3ds12(cos(theta),m,x);

 

k = 2*pi/lambda0 * n1;

R = 1; # radius of 1m

 

# XY plane: phi = 90, Etang = EP, Eperp = Ez = ES

phi = 90*pi/180;

Etang = exp(1i*k*R)/(-1i*k*R)*cos(phi)*S.S2;

Eperp = exp(1i*k*R)/(1i*k*R)*sin(phi)*S.S1;

polar(theta,abs(Etang),abs(Eperp),"","","XY plane");

legend("|EP|","|ES|");

 

# YZ plane: phi = 0, Etang = EP, Eperp = Ex = ES

phi = 0;

Etang = exp(1i*k*R)/(-1i*k*R)*cos(phi)*S.S2;

Eperp = exp(1i*k*R)/(1i*k*R)*sin(phi)*S.S1;

polar(theta,abs(Etang),abs(Eperp),"","","YZ plane");

legend("|EP|","|ES|");

 

 

See Also

mie3d, Mie3D example

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