As in the previous problem the quartz plate introduces a phase difference `delta` between the `O & E` components. When `delta = pi//2` (modulo `pi`) the resultant wave is circularly polarized. In this case intensity is independent of the rotation of the rear prism. Now
`delta = (2pi)/(lambda) (n_(e) - n_(0)) d`
`= (2pi)/(lambda)0.009 xx 0.5 xx 10^(-3) m`
`= (9pi)/(lambda),lambda`in `mu m`
For `lambda = 0.50mu m. delta = 18 pi`. The relevent values of `delta` have to be shosen in the form
`(k +(1)/(2))pi`. For `k = 17, 16, 15` we get
`lambda = 0.5143mum, 0.5435mu m` and `0.806 mu m`
These are the values f `lambda` which lie between `0.50 mu m` and `0.60mum`.