In the figure shown in $YDSE$, a parallel beam of light is incident on the slits from a medium of refractive index $n_1$. The wavelength of light in this medium is $\lambda_1$. $A$ transparent slab of thickness $t$ and refractive index $n_3$ is placed in front of one slit. The medium between the screen and the plane of the slits is $n_2$. The phase difference between the light waves reaching point $O$ (symmetrical, relative to the slits) is:

  • A
    $\frac{2\pi}{n_1 \lambda_1} (n_3 - n_2) t$
  • B
    $\frac{2\pi}{\lambda_1} (n_3 - n_2) t$
  • C
    $\frac{2\pi n_1}{n_2 \lambda_1} \left( \frac{n_3}{n_2} - 1 \right) t$
  • D
    $\frac{2\pi n_1}{\lambda_1} (n_3 - n_1) t$

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