Returns the fraction of transmitted power to each physical grating orders for a given simulation. Results are normalized such that the sum of all the orders is equal to 1. To convert these values into fractions of the source power, multiply by the the transmission script function.
3D simulations: Data is returned in a NxMxP matrix where N,M are the number of grating orders, and P is the number of frequency points.
2D simulations: Data is returned in a NxP matrix where N is the number of grating orders, and P is the number of frequency points.
Syntax 
Description 

out = grating("monitorname",f, index, direction ); 
Returns the strength of all physical grating orders from monitorname. 
Parameter 
Default value 
Type 
Description 


monitorname 
required 
string 
name of the monitor from which far field is calculated 

f 
optional 
1 
vector 
Index of the desired frequency point. This can be a single number or a vector. Multithreaded projection to allow multiple frequency points to be calculated simultaneously was introduced in R2016b. 
index 
optional 
value at monitor center 
number 
The index of the material to use for the projection. 
direction 
optional 
direction of max power flow 
number 
Direction: this can be +1 or 1. 
The following table summarizes how to interpret the coordinate vector properties for various monitor orientations.
Monitor orientation 
Monitor surface normal 
'N', 'ux', 'gratingn', 'gratingperiod1', 'gratingu1', 'gratingbloch1', correspond to 
'M', 'uy', 'gratingm', 'gratingperiod2', 'gratingu2', 'gratingbloch2' correspond to 
XY plane 
Z 
x axis 
y axis 
XZ plane 
Y 
x axis 
z axis 
YZ plane 
X 
y axis 
z axis 
Example
This 2D example plots the relative strength of the grating orders.
mname="T"; # monitor name theta=gratingangle(mname); # angle of each grating order G=grating(mname); # power to each order (fraction of transmitted power) plot(theta,G,"theta (deg)","relative power","grating orders","plot points");
This 3D example calculates various grating quantities.
mname="T"; # monitor name N=gratingn(mname); # grating order numbers M=gratingm(mname); u1=gratingu1(mname); # grating unit vectors (can be converted to theta,phi) u2=gratingu2(mname); G=grating(mname); # power to each order (fraction of transmitted power) T=transmission(mname); # total power transmitted through monitor (fraction of source power) # Print all grating orders to prompt. Results will sum to 1. # Then normalize grating results to the injected source power. ?G; # grating results ?G*T; # normalized to source power # find strength and direction of 0,0 grating order nx=find(N,0); # find 0th grating order ny=find(M,0); # find 0th grating order ?"Grating order 0,0 strength: " + num2str( G(nx,ny) ); ?"Grating order 0,0 direction: Ux=" +num2str(u1(nx)) + " Uy=" +num2str(u2(ny)); # image all grating orders, using log scale image(u1,u2,G,"ux","uy","Grating order strength","logplot");
Calculate the zeroth grating order transmission from a monitor that recorded multiple frequency points. The grating function operates on one frequency point at a time, so a for loop is required.
mname="T"; # monitor name f=getdata(mname,"f"); # get frequency vector T=transmission(mname); # get total transmission G00 = matrix(length(f)); # initialize matrix # get 0,0 grating order for each frequency for (i=1:length(T)) { N=gratingn(mname,i); # grating order numbers M=gratingm(mname,i); temp=grating("T2",i); G00(i) = temp(find(N,0),find(M,0)); # select 0,0 grating order } plot(c/f*1e6,T,G00*T,"wavelength (um)","power"); legend("total transmission","0,0 grating transmission");
See Also
List of commands , gratingn , gratingperiod1 , gratingbloch1 , gratingu1 , gratingangle , gratingpolar , gratingvector