Laser pulse amplification and dispersion compensation in an effectively extended optical cavity containing Bose-Einstein condensates

TL;DR

This paper proposes a laser pulse amplification method using Bose-Einstein condensates inside an optical cavity to compensate dispersion and increase pulse energy, analyzing the effects of slow light propagation and atom interactions.

Contribution

It introduces a novel pulse amplification scheme employing Bose-Einstein condensates for dispersion compensation and evaluates its efficiency and limitations.

Findings

Optimal amplification time is around 0.3 ms.

Amplification factor can reach approximately 100.

Bandwidth limits affect the minimum pulse width that can be amplified.

Abstract

We review and critically evaluate our proposal of a pulse amplification scheme based on two Bose-Einstein condensates inside the resonator of a mode-locked laser. Two condensates are used for compensating the group velocity dispersion. Ultraslow light propagation through the condensate leads to a considerable increase in the cavity round-trip delay time, lowers the effective repetition rate of the laser, and hence scales up the output pulse energy. It has been recently argued that atom-atom interactions would make our proposal even more efficient. However, neither in our original proposal nor in the case of interactions, limitations due to heating of the condensates by optical energy absorption were taken into account. Our results show that there is a critical time of operation, $~0.3$ ms, for the optimal amplification factor, which is in the order of $\sim 10^2$ at effective condensate lengths in the order of $\sim 50$ $\mu$m. The bandwidth limitation of the amplifier on the minimum temporal width of the pulse that can be amplified with this technique is also discussed.