Significant Enhancement in THz Emission and Piezoelectricity in Atomically Thin Nb-Doped MoS2Click to copy article linkArticle link copied!
- Neetesh DhakarNeetesh DhakarFemtosecond Spectroscopy and Nonlinear Photonics Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, IndiaMore by Neetesh Dhakar
- Pin ZhaoPin ZhaoSchool of Advanced Materials Science and Engineering, Sungkyunkwan University, Suwon 16419, Republic of KoreaMore by Pin Zhao
- Hyeon Yeong LeeHyeon Yeong LeeSchool of Advanced Materials Science and Engineering, Sungkyunkwan University, Suwon 16419, Republic of KoreaMore by Hyeon Yeong Lee
- Sang-Woo KimSang-Woo KimDepartment of Materials Science and Engineering, Yonsei University, Seoul 03722, Republic of KoreaCenter for Human-oriented Triboelectric Energy Harvesting, Yonsei University, Seoul 03722, Republic of KoreaMore by Sang-Woo Kim
- Brijesh KumarBrijesh KumarSmart Materials and Photonics Laboratory, Department of Physics, University of Lucknow, Lucknow 226007, IndiaMore by Brijesh Kumar
- Sunil Kumar*Sunil Kumar*E-mail: [email protected]Femtosecond Spectroscopy and Nonlinear Photonics Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi 110016, IndiaMore by Sunil Kumar
Abstract
A significantly enhanced THz radiation generation from femtosecond photoexcited MoS2 layers due to Nb-doping is reported here. Different microscopic mechanisms involved in the THz photocurrent generation vary in their relative contributions in the two cases of photoexcitation, i.e., above and below the electronic bandgap of the layers. For a moderate Nb-doping level of just ∼0.05%, we have observed a multifold enhancement in the THz emission for the case of the above bandgap excitation, which is, though, nearly 1.5 times for the case of the below bandgap excitation of the monolayer MoS2. Alongside the difference in THz generation efficiency, the THz pulse polarity is also reversed at the above bandgap excitation of the Nb-doped layers, consequent to the reversed surface depletion field. Except for a slightly smaller difference in the THz enhancement factor, all the observations are reproducible in the bilayers as well to imply a weaker inversion symmetry and reduced screening of the surface depletion field due to Nb-doping. Furthermore, we employed pristine MoS2 and Nb-doped MoS2 monolayers to fabricate piezoelectric nanogenerator devices. Like enhancement in the ultrafast THz emission, the piezoelectric performance of the nanogenerator, fabricated with the Nb-doped MoS2 monolayer is also increased by a similar factor.
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