Issue 17, 2022

Recent progress and prospects of random lasers using advanced materials

Abstract

Random lasers (RLs) are a particular class of optical devices. In a random laser, the optical feedback is provided by scattering media rather than by an optical cavity, as for traditional lasers. Such unique configuration leads to lasers with low spatial coherence and renders RLs attractive in the fields such as speckle-free imaging, sensing, and light therapy. The random laser generation depends on the gain and disordered scattering medium to obtain feedback and optical amplification. Therefore, the properties of the gain and scattering materials had particular importance for random lasers. The advancement of disordered nanostructure-based optical devices for photonic applications may further facilitate distinct and novel functionalities in RLs. However, the applicability of RLs has been restricted due to emission in random directions, polarization and wavelength tunability difficulties, and intense competition of modes. This review will discuss the recent progress and prospects of random lasers using advanced materials to address these limitations for RLs. Finally, some applications of RLs, including medical and diagnostics, photonic devices, sensors, and display technology, will be briefly reviewed.

Graphical abstract: Recent progress and prospects of random lasers using advanced materials

Article information

Article type
Review Article
Submitted
26 Febr. 2022
Accepted
03 Jūl. 2022
First published
06 Jūl. 2022
This article is Open Access
Creative Commons BY license

Mater. Adv., 2022,3, 6687-6706

Recent progress and prospects of random lasers using advanced materials

N. Padiyakkuth, S. Thomas, R. Antoine and N. Kalarikkal, Mater. Adv., 2022, 3, 6687 DOI: 10.1039/D2MA00221C

This article is licensed under a Creative Commons Attribution 3.0 Unported Licence. You can use material from this article in other publications without requesting further permissions from the RSC, provided that the correct acknowledgement is given.

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