2017
DOI: 10.1103/physrevb.96.085302
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Charged excitons in monolayer WSe2 : Experiment and theory

Abstract: Charged excitons, or X ± -trions, in monolayer transition metal dichalcogenides have binding energies of several tens of meV. Together with the neutral exciton X 0 they dominate the emission spectrum at low and elevated temperatures. We use charge tunable devices based on WSe2 monolayers encapsulated in hexagonal boron nitride, to investigate the difference in binding energy between X + and X − and the X − fine structure. We find in the charge neutral regime, the X 0 emission accompanied at lower energy by a s… Show more

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Cited by 276 publications
(310 citation statements)
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“…The bright negative trion (X − ) and the dark negative trion (X − d ) generate the highest energy lines in the electron-doped ML. The observed fine structure splitting of the bright negative trion confirms the high quality of our sample [31]. All measured energies agree well with previous reports on excitonic states in WSe 2 MLs encapsulated with h-BN [34,35,53,54].…”
Section: Gate-dependent Photoluminescencesupporting
confidence: 91%
“…The bright negative trion (X − ) and the dark negative trion (X − d ) generate the highest energy lines in the electron-doped ML. The observed fine structure splitting of the bright negative trion confirms the high quality of our sample [31]. All measured energies agree well with previous reports on excitonic states in WSe 2 MLs encapsulated with h-BN [34,35,53,54].…”
Section: Gate-dependent Photoluminescencesupporting
confidence: 91%
“…The excitations discussed above have been proposed previously on the basis of model calculations [24,32]. Employing ab initio methods [28,29], we are now able to provide a quantitative prediction of the energy and relative ordering of these excitations, treating dark and bright excitons and is observed 30 meV above.…”
Section: Dark Excitations In Monolayer Transition Metal Dichalcogenidesmentioning
confidence: 79%
“…3(c)] lattices with a lattice constant a. Here we consider ∆ 0 = 0, which corresponds to a wavelength λ ∼ (700 − 800) nm in state-of-the-art TMD setups [46,47]. We choose θ such that the cross section of the Gaussian beam is small enough and does not exceed the size of the WC.…”
Section: Optical Readoutmentioning
confidence: 99%