A Michelson interferometer uses a monochromatic light source with vacuum wavelength λ. Light from the source is split into two paths by a half-mirror (beam splitter). Path 1 has a fixed mirror M1, and Path 2 has a movable mirror M2 placed on a smooth horizontal floor with mass M. The movable mirror M2 is connected to a light spring with spring constant k and can oscillate horizontally.
Furthermore, the movable mirror M2 and the space it moves in are completely immersed in a long narrow tank filled with a transparent liquid of absolute refractive index n. (The half-mirror and fixed mirror M1 are in air, with refractive index 1.)
In the initial state, the movable mirror M2 is at rest near the natural length of the spring, and the detector observes interference fringes of a certain brightness.
A bullet of mass m flies horizontally at speed v0 and embeds completely into the back of the movable mirror M2 (perfectly inelastic collision). The collision time is extremely short, so immediately after the collision, M2 (with the bullet) acquires velocity V and begins oscillating in the liquid. The resistance of the liquid is negligible.
When the movable mirror M2 oscillates, the optical path length of Path 2 changes continuously, causing the interference fringes at the detector to change periodically (fringe shift). Find the maximum frequency fmax (number of fringe changes per second) observed at the detector during this oscillation.
Assume the speed of light is incomparably larger than the speeds of the bullet and mirror, so Doppler wavelength changes are negligible. Only changes in optical path difference need to be considered.
Compute fmax in units of MHz (106 Hz) and give the answer as a positive integer equal to the value multiplied by 100.