Random lasing



Transition from sub-threshold emission to diffusive random laser to coherent random laser.


Database on random lasers with nonresonant feedback
(Partial listing- work in progress)

When optical gain is added to a medium with a random variation in its refractive index, a fascinating synergy of coherent amplification and multiple scattering occurs within the medium. The result is a drastic change in the emission characteristics of the system, which originates from the novel gain dynamics realized by the inhomogeneous structure. Ballistic propagation of light within the medium (that would occur in absence of the structure) is completely inhibited by the varying refractive index, and the light is made to undergo a Gaussian random walk that approximates a diffusion-like propagation while concomitantly undergoing optical amplification. Unlike a regular laser, the mode that eventually supersedes the emission is not chosen by any geometric resonance, but rather by the gain profile. The spectral profile narrows by roughly an order of magnitude. Refer to the figure, which shows the green profile collapsing in bandwidth to yield the blue profile.

Further to this behaviour, a dependence on two parameters is observed, namely, the degree of disorder, and the gain cross-section. When the two parameters are just right, the emission undergoes a transition from incoherent to coherent, and the spectrum further narrows by another order of magnitude, creating ultranarrow lasing modes. This is the critical regime of random lasing, which is realised by a combination of several factors occurring simultaneously, namely, mode competition, local pockets of ultrahigh gain, finite size effects and so on. All these factors, in turn, are realized solely by the disorder. Refer once again to the figure wherein the red profile depicts the ultranarrow modes.

At a critical degree of disorder, the diffusive modes of light are also inhibited by mesoscopic interferences within the system, and the transport comes to a halt. This manifests as closed-loop random paths inside the medium within regions that harbour exponentially decaying optical wavefunctions, known as Anderson localized modes, at the resonant frequencies. Again, these resonances are strictly mesoscopic, and not geometric. When gain is introduced over such a loop, it excessively amplifies the resonant frequency, which results in the occurrence of ultranarrow modes.

Light amplification in random media is a rich field of physics, wherein the above-mentioned and more phenomena have been observed. The physics is of interest to optics specialists, condensed-matter physicists, statistical physicists alike. We study this field through sophisticated experiments, coupled with advanced modelling techniques based on Monte Carlo methods of photon propagation, and finite difference time domain simulations. In fact, we were the first ones to apply a three-dimensional Gaussian random walk model to random lasing, which explained a few of the spectral features. We subsequently improvised this model to explain the ultranarrow lasing modes.

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