2020
DOI: 10.1103/physrevb.102.085304
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Many-body theory of the optical conductivity of excitons and trions in two-dimensional materials

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Cited by 48 publications
(99 citation statements)
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“…Figure 5 c shows the energy splitting between and as a function of the gate voltage and the Fermi energy level. We found that the splitting between the two transitions increases linearly with the doping level of the device, as predicted and observed in previous literature for exciton and trion transitions [ 30 , 33 , 34 ], following the equation where is the splitting between exciton and trion transitions; is the binding energy of ; is the Fermi energy, which is proportional to the back-gate voltage; and c is the slope of the linear fit, predicted to have a value of [ 33 ].…”
Section: Resultssupporting
confidence: 89%
“…Figure 5 c shows the energy splitting between and as a function of the gate voltage and the Fermi energy level. We found that the splitting between the two transitions increases linearly with the doping level of the device, as predicted and observed in previous literature for exciton and trion transitions [ 30 , 33 , 34 ], following the equation where is the splitting between exciton and trion transitions; is the binding energy of ; is the Fermi energy, which is proportional to the back-gate voltage; and c is the slope of the linear fit, predicted to have a value of [ 33 ].…”
Section: Resultssupporting
confidence: 89%
“…The error estimation is discussed in the ESI. † The influence of the many-body excitonic state, [34][35][36] which has traditionally been called trion, has been neglected as they are negligible at room temperature and intrinsic electron doping levels. 37,38 In fact, one single Lorentzian reproduces the static spectrum accurately, without the need of including a second Lorentzian to model the trion which is observed in low temperature photoluminescence experiments.…”
Section: Resultsmentioning
confidence: 99%
“…The large binding energy of excitons in TMDs as compared to other microcavity semiconductors such as quantum-wells [32][33][34], combined with the possibility to control the electron density in the different valleys, opens up exciting new venues to explore Bose-Fermi mixtures in a hybrid light-matter setting [35][36][37]. This has stimulated a number of studies regarding the properties electron-exciton mixtures and their coupling to light [38][39][40][41][42][43][44][45][46][47][48]. In particular, the emergence of new quasiparticles, the so-called Fermipolaron-polaritons have been observed [49].…”
Section: Introductionmentioning
confidence: 99%