2019
DOI: 10.1103/physrevlett.123.097403
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Interaction-Induced Shubnikov–de Haas Oscillations in Optical Conductivity of Monolayer MoSe2

Abstract: We report polarization-resolved resonant reflection spectroscopy of a charge-tunable atomically-thin valley semiconductor hosting tightly bound excitons coupled to a dilute system of fully spin-and valley-polarized holes in the presence of a strong magnetic field. We find that exciton-hole interactions manifest themselves in hole-density dependent, Shubnikov-de Haas-like oscillations in the energy and line broadening of the excitonic resonances. These oscillations are evidenced to be precisely correlated with … Show more

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Cited by 67 publications
(41 citation statements)
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“…They find the reduced mass equal to 0.268 V : . A few more recent works also reported inter-Landau-level transitions in doped hBNencapsulated monolayer WSe2 [274][275][276] and MoSe2 277 . Notably, the reduced masses are also determined in a more consistent fashion by analyzing the energy shifts of the excitons in the low-field limit (diamagnetic shift).…”
Section: Landau Quantization and Rydberg Spectroscopymentioning
confidence: 93%
“…They find the reduced mass equal to 0.268 V : . A few more recent works also reported inter-Landau-level transitions in doped hBNencapsulated monolayer WSe2 [274][275][276] and MoSe2 277 . Notably, the reduced masses are also determined in a more consistent fashion by analyzing the energy shifts of the excitons in the low-field limit (diamagnetic shift).…”
Section: Landau Quantization and Rydberg Spectroscopymentioning
confidence: 93%
“…Concurrently, the exciton resonance evolves into a repulsive polaron (RP) (see Supplementary Information S1). The strong sensitivity of the RP resonance energy to changes in electron density renders it an ideal spectroscopic tool for sensing the electron density n in the same layer 24,25 . The strain induced resonance energy difference between X top and X bot , ensuring different energies for the corresponding RP top and RP bot , together with the much weaker sensitivity of RP top (RP bot ) on electron density n b (n t ) in the bottom (top) layer, allows us to determine the charging configuration of the two layers simultaneously.…”
Section: Charge Configuration Detection By Exciton-polaron Spectmentioning
confidence: 99%
“…To explain experiments in which both the valley Zeeman effect and LLs are important [8,17], one needs to find a general approach to take into account the two effects on an equal-footing framework. However, in many cases, the above theories are patched together in an ad hoc fashion to interpret transport and optical measurements in the literature [8,[17][18][19]. Specifically, the LLs obtained from the massive Dirac fermion model are further shifted by an additive Zeeman term, which is obtained from one of the models that deduced an expression for the Zeeman term without the LL effect.…”
Section: Introductionmentioning
confidence: 99%