2021
DOI: 10.1016/j.pquantelec.2021.100343
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Recent advances and applications of random lasers and random fiber lasers

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Cited by 144 publications
(80 citation statements)
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References 429 publications
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“…In spite of the lower quality of FASnI 3 on PET, the values of ASE/RL thresholds found in the present work (1.5/3 µJ cm −2 ) are still remarkably lower than values reported for other semiconductor materials. For example, a typical RL threshold of ≈1 mJ cm −2 is usually reported for dyes [ 13,15 ] or colloidal quantum dots, [ 60,62 ] in both cases prepared as thin films on rigid substrates. In the case of LPs, the threshold of RL is reduced down to 1–10 µJ cm −2 in the case of thin films deposited on rigid substrates, [ 41,42,44,45,63,64 ] but it increases up to 0.1–1 mJ cm −2 for similar films on flexible ones (polyimide, Ni foam).…”
Section: Ase and Lasing In Flexible Waveguidesmentioning
confidence: 99%
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“…In spite of the lower quality of FASnI 3 on PET, the values of ASE/RL thresholds found in the present work (1.5/3 µJ cm −2 ) are still remarkably lower than values reported for other semiconductor materials. For example, a typical RL threshold of ≈1 mJ cm −2 is usually reported for dyes [ 13,15 ] or colloidal quantum dots, [ 60,62 ] in both cases prepared as thin films on rigid substrates. In the case of LPs, the threshold of RL is reduced down to 1–10 µJ cm −2 in the case of thin films deposited on rigid substrates, [ 41,42,44,45,63,64 ] but it increases up to 0.1–1 mJ cm −2 for similar films on flexible ones (polyimide, Ni foam).…”
Section: Ase and Lasing In Flexible Waveguidesmentioning
confidence: 99%
“…Moreover, the use of nontoxic materials to be in contact with human skin or tissues should also be a requirement for the potential biomedical applications of this sort of future optoelectronic/photonic sensing devices. [ 13–16 ] Fortunately, lead‐free perovskites (LFP) have opened promising routes for such a new generation of ecofriendly optical sources, [ 17 ] as an alternative to the lead halide perovskite (LP) families. Nevertheless, although LPs have been consolidated as excellent optical gain materials for traditional resonators [ 18–21 ] or random lasing (RL), [ 22 ] the use of LFPs for developing lasers or optical amplifiers is still at its infancy.…”
Section: Introductionmentioning
confidence: 99%
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“…Random lasers, different from conventional lasers that are based on cavity mirror feedback, are generated by multiple light scattering associated with a disordered optically gain medium. [1][2][3] Owning to the advantages of random lasers such as simplicity, small size and low spatial coherence, [4][5][6] such lasers have been extensively studied in various fields including speckle-free imaging, [4,7] super-resolution spectroscopy, [8] information security, [9] sensing, [10,11] and biomedical. [12] Nevertheless, controlling the emission wavelength of random lasers is still challenging due to the absence of optical cavity, which limits their applications in some fields such as medical detection, [13] photonic crystals, [14,15] and high-precision sensors.…”
Section: Introductionmentioning
confidence: 99%
“…RFLs are the quasi one-dimensional realization 5 of random lasers (RLs), a class of disordered photonic systems proposed early in 1968 but unambiguously demonstrated only in 1994, as reviewed in 6 . RLs differ from conventional lasers as their operation does not require a conventional optical cavity.…”
mentioning
confidence: 99%