Nothing
require(uniaxialOptics)
#plot conoscopy figures for some typical LC cells
#5CB LC films between ITO coated glass
glass <- 1.52^2 + 0.0i
ito <- 3.8 + 0.08i
nz <- 48 #divide lc into sublayers
d <- 30e-6 #lc layer thickness
eolc <- 1.52^2 + 0i
eelc <- 1.68^2 + 0i
di <- c(0,30e-9)
ei <- c(glass,ito)
numap <- asin(.55/1.52) #50X refracted by glass
#CCD plot function
ccdf <- function(lc,main) {
ccd <- conorect.lc(633e-9,lc,eolc, eelc, di, ei, rev(di), rev(ei),
nx=96,ny=96,pmin=0,pmax=numap)
image((ccd$crossed[,,1]),col=grey.colors(64,start=0,end=1),axes=FALSE,
main=main)
}
par(mfrow=c(2,3))
#han cell
#note that the lc profiles can be computed by
#the fucntion lc_switching_seqeunce in package
#Ericksen-Leslie, but are done on the cheap here.
lch <- list(depthz=c(0.5,rep(1,nz-2),0.5) * d/nz,
tilt=matrix(seq(0,pi/2,l=nz),ncol=1),
twist=matrix(seq(0,0,l=nz),ncol=1))
ccdf(lch,"HAN cell" )
#planar cell
lcp <- list(depthz=c(0.5,rep(1,nz-2),0.5) * d/nz,
tilt=matrix(seq(pi/2,pi/2,l=nz),ncol=1),
twist=matrix(seq(0,0,l=nz),ncol=1))
ccdf(lcp,"Planar homogeneous cell")
#pi/16 slab cell
lctn <- list(depthz=c(0.5,rep(1,nz-2),0.5) * d/nz,
tilt=matrix(seq(pi/16,pi/16,l=nz),ncol=1),
twist=matrix(seq(0,0,l=nz),ncol=1))
ccdf(lctn,expression(pi/16 * " slab cell"))
#homeotropic cell
lcht <- list(depthz=c(0.5,rep(1,nz-2),0.5) * d/nz,
tilt=matrix(seq(0,0,l=nz),ncol=1),
twist=matrix(seq(0,0,l=nz),ncol=1))
ccdf(lcht,"Homeotropic cell")
#pi/32midplane symettric cell
lcs <- list(depthz=c(0.5,rep(1,nz-2),0.5) * d/nz,
tilt=matrix( ifelse(1:nz > nz/2, pi/32, -pi/32),ncol=1),
twist=matrix(seq(0,0,l=nz),ncol=1))
ccdf(lcs,expression(pi/16 * " midplane symmetric cell"))
#tn cell
lctn <- list(depthz=c(0.5,rep(1,nz-2),0.5) * d/nz,
tilt=matrix(seq(pi/2,pi/2,l=nz),ncol=1),
twist=matrix(seq(0,pi/2,l=nz),ncol=1))
ccdf(lctn,"twisted cell")
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