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Third‐Order Nonlinear Optical Modulation in MoS<sub>2</sub> Nanosheets in the Presence of CdSe and CdSe/V<sub>2</sub>O<sub>5</sub> Quantum Dots

Srinivasa Rao KondaDepartment of Physics Indian Institute of Technology Ropar Rupnagar Punjab 140001 IndiaPuspendu BarikGPL Photonics Laboratory State Key Laboratory of Luminescence Science and Technology Changchun Institute of Optics Fine Mechanics and Physics Chinese Academy of Sciences Changchun Jilin 130033 ChinaSubhash C. SinghThe Institute of Optics University of Rochester Rochester NY 14627 USAMottamchetty VenkateshDepartment of Physics and Astronomy Aarhus University Ny Munkegade 120 Aarhus C 8000 DenmarkAmit SrivasthavaDepartment of Physics TDPG College VBS Purvanchal University Jaunpur 222001 IndiaR. A. GaneevDepartment of Optics and Spectroscopy Voronezh State University Voronezh 394006 RussiaS. Venugopal RaoSchool of Physics &amp; DIA‐CoE (formerly ACRHEM) University of Hyderabad Hyderabad Telangana 500046 IndiaChunlei GuoThe Institute of Optics University of Rochester Rochester NY 14627 USAWei LiGPL Photonics Laboratory State Key Laboratory of Luminescence Science and Technology Changchun Institute of Optics Fine Mechanics and Physics Chinese Academy of Sciences Changchun Jilin 130033 China
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Abstract

Abstract Embedding semiconductor quantum dots (QDs) into a 2D transition metal dichalcogenide (TMDCs) can significantly modulate the electronic charge transfer and, hence, the nonlinear optical (NLO) properties of the TMDCs. However, the influence of strong interactions within 2D nanostructure‐QDs composites on their third‐order NLO responses has not been explored thus far. The third‐order NLO characteristics of few‐layered MoS 2 nanosheets embedded with CdSe and CdSe/V 2 O 5 QDs are studied using 35‐fs pulses at 400 and 800 nm excitations. It is observed that an alteration of the third‐order NLO properties in MoS 2 occurs in the presence of QDs. Notably, the MoS 2 ‐QDs hybrid system exhibits a significant modulation in third‐order nonlinearities, with a substantial multi‐fold increase in the figure of merit in the presence of core CdSe QDs and suppression with passivated CdSe/V 2 O 5 QDs. These findings strongly indicate that QD‐based hybrid systems with charge transfer channels probably enhance carrier mobility and enable tunable electron transfer dynamics, which can emerge as a viable strategy for tailoring third‐order NLO properties in TMDCs, positioning these hybrid materials as promising candidates for optoelectronic applications.

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