Atomically thin yellow pearl: an impetus for thermal nonlinear optical effect assisted continuous wave random lasing

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dc.contributor.author Mandal, Nabarun
dc.contributor.author Pramanik, Ashim
dc.contributor.author Dey, Arindam
dc.contributor.author Kumbhakar, Pathik
dc.contributor.author Kochat, Vidya
dc.contributor.author Gautam, Abhay Raj Singh
dc.contributor.author Glavin, Nicholas
dc.contributor.author Roy, Ajit K.
dc.contributor.author Ajayan, P. M.
dc.contributor.author Tiwary, Chandra Sekhar
dc.coverage.spatial United States of America
dc.date.accessioned 2022-10-07T13:27:06Z
dc.date.available 2022-10-07T13:27:06Z
dc.date.issued 2022-09
dc.identifier.citation Mandal, Nabarun; Pramanik, Ashim; Dey, Arindam; Kumbhakar, Pathik; Kochat, Vidya; Gautam, Abhay Raj Singh; Glavin, Nicholas; Roy, Ajit K.; Ajayan, P. M. and Tiwary, Chandra Sekhar, "Atomically thin yellow pearl: an impetus for thermal nonlinear optical effect assisted continuous wave random lasing", arXiv, Cornell University Library, DOI: arXiv:2209.13295, Sep. 2022. en_US
dc.identifier.uri https://arxiv.org/abs/2209.13295
dc.identifier.uri https://repository.iitgn.ac.in/handle/123456789/8196
dc.description.abstract Above cryogenic temperatures, random laser (RL) emission under continuous wave (CW) optical pumping is often challenging for materials having plenty of lattice defects. Thus, intensive care is required while fabricating the RL device. Synthesis of 2D materials having unique functionality at the atomic limit is necessary for use in such devices. In this work, defects-free 2D yellow pearl (2D-YP) has been synthesized from bulk south sea pearl using liquid-phase exfoliation (LPE) technique. Thereafter, 2D-YP has been employed as passive scatterer to achieve CW pumped RL emission from a conventional gain molecule, i.e., Rhodamine B (RhB). Compared to other semiconductor (TiO2) and 2D (Graphene and h-BN) passive scatterers, ~25 times improvement in gain volume is observed for the disordered system consisting of RhB and 2D-YP, i.e., 2D-YP@RhB, which is found to be due to the formation of a large refractive index gradient, as induced by the thermal nonlinear optical (NLO) interaction. Hence, incoherent RL (ic-RL) emission ~591 nm is reported for 2D-YP@RhB at a lowest threshold input pump power and a linewidth of 65 mW and 3 nm, respectively. Additionaly, a clear transition from ic-RL to mode tunable coherent RL (c-RL) emission is also possible by altering the configuration of the 2D-YP@RhB container. Therefore, the newly designed Van der Waals heterostructure, i.e., 2D-YP with intrinsic photon trapping capability may pave an avenue towards developing future exciting optoelectronic devices.
dc.description.statementofresponsibility by Nabarun Mandal, Ashim Pramanik, Arindam Dey, Pathik Kumbhakar, Vidya Kochat, Abhay Raj Singh Gautam, Nicholas Glavin, Ajit K. Roy, P. M. Ajayan and Chandra Sekhar Tiwary
dc.language.iso en_US en_US
dc.publisher Cornell University Library en_US
dc.subject 2D-YP en_US
dc.subject LPE en_US
dc.subject Conventional gain molecule en_US
dc.subject Optoelectronic devices en_US
dc.subject Random laser en_US
dc.title Atomically thin yellow pearl: an impetus for thermal nonlinear optical effect assisted continuous wave random lasing en_US
dc.type Pre-Print Archive en_US
dc.relation.journal arXiv


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