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SM ISO690:2012 MITIOGLU, Anatolie, ANGHEL, Sergiu, BALLOTTIN, Mariana, SUSHKEVICH, Konstantin, KULYUK, Leonid, CHRISTIANEN, Peter C.M.. Anomalous rotation of the linearly polarized emission of bright excitons in strained WSe2 monolayers under high magnetic fields. In: Physical Review B, 2019, vol. 99, p. 0. ISSN 2469-9950. DOI: https://doi.org/10.1103/PhysRevB.99.155414 |
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Physical Review B | |
Volumul 99 / 2019 / ISSN 2469-9950 /ISSNe 2469-9969 | |
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DOI:https://doi.org/10.1103/PhysRevB.99.155414 | |
Pag. 0-0 | |
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Rezumat | |
Linearly polarized microphotoluminescence (μ-PL) measurements of strained WSe2 monolayers in out-of-plane high magnetic fields are presented. At low temperature, a splitting of the bright exciton emission into two exciton components is observed, which is attributed to an in-plane uniaxial strain based on the full polarization dependence of the photoluminescence spectrum. High magnetic field measurements directly reveal a distinct evolution of the linear polarization and allows us to extract the valley coherence time constants (Ts2∗) for both exciton components. For the high-energy transition of the exciton, the valley coherence time ≃0.45 ps, closely matching Ts2∗ of an unstrained monolayer (≃0.34 ps). For the low-energy exciton, however, Ts2∗ is four times larger, ≃1.97 ps. This valley coherence time observed here may be explored for future valleytronic applications. |
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Cuvinte-cheie Landforms, Magnetic fields, Monolayers, Photoluminescence spectroscopy, polarization, Selenium compounds, temperature |
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At low temperature, a splitting of the bright exciton emission into two exciton components is observed, which is attributed to an in-plane uniaxial strain based on the full polarization dependence of the photoluminescence spectrum. High magnetic field measurements directly reveal a distinct evolution of the linear polarization and allows us to extract the valley coherence time constants (Ts2∗) for both exciton components. For the high-energy transition of the exciton, the valley coherence time ≃0.45 ps, closely matching Ts2∗ of an unstrained monolayer (≃0.34 ps). For the low-energy exciton, however, Ts2∗ is four times larger, ≃1.97 ps. 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