Start Learning Free

Before You Begin

Question #43725

Difficulty: 8/10 | 🟢 Free

The Question

In a Young's Double Slit Experiment, a monochromatic light source of wavelength λ\lambda is used, and the two slits produce beams of equal intensity at the screen. A transparent dielectric slab of thickness tst_s is placed directly in front of one of the slits. The slab is subjected to a high-frequency electromagnetic field, which modulates its refractive index via the Kerr effect such that n(t)=n0+Δnsin⁡(ωt)n(t) = n_0 + \Delta n \sin(\omega t), where n0n_0 and Δn\Delta n are positive constants. The interference pattern is recorded by a slow detector with an integration time τ≫2πω\tau \gg \frac{2\pi}{\omega}. Which of the following expressions represents the visibility V=Imax−IminImax+IminV = \frac{I_{max} - I_{min}}{I_{max} + I_{min}} of the observed fringes?

[Given: 12π∫02πcos⁡(zsin⁡θ)dθ=J0(z)\frac{1}{2\pi} \int_{0}^{2\pi} \cos(z \sin \theta) d\theta = J_0(z) and 12π∫02πsin⁡(zsin⁡θ)dθ=0\frac{1}{2\pi} \int_{0}^{2\pi} \sin(z \sin \theta) d\theta = 0, where J0(z)J_0(z) is the zeroth-order Bessel function of the first kind.]

Options

  • A.

    ∣J0(2πλΔn ts)∣\left| J_0\left( \frac{2\pi}{\lambda} \Delta n \, t_s \right) \right|

  • B.

    ∣J0(πλΔn ts)∣\left| J_0\left( \frac{\pi}{\lambda} \Delta n \, t_s \right) \right|

  • C.

    cos⁡2(πλΔn ts)\cos^2\left( \frac{\pi}{\lambda} \Delta n \, t_s \right)

  • D.

    11

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Central Fringe Shift|Maxwell's Correction to Ampere's Law|Transverse Nature of EM Waves

Why This Question Is Tricky

Common Mistakes

Students often fall into the trap of treating interference patterns as static or assume that a high-frequency modulation simply shifts the central maximum back and forth without affecting the overall contrast (incorrectly concluding V=1).

They fail to recognize that a slow detector records the time-averaged intensity, not the instantaneous intensity.

By incorrectly averaging the phase ⟨ϕ(t)⟩\langle \phi(t) \rangle instead of the intensity ⟨cos⁡ϕ(t)⟩\langle \cos \phi(t) \rangle, they miss the Bessel function dependence entirely.

This question tests the fundamental wave optics principle that observable intensity is the time average of the squared superposition of waves, requiring students to correctly couple the optical path length to a time-dependent dielectric permittivity.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterWave Optics - Class 12
ConceptCentral Fringe Shift
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree