2019
DOI: 10.1103/physrevb.99.205420
|View full text |Cite
|
Sign up to set email alerts
|

Magnetophotoluminescence of exciton Rydberg states in monolayerWSe2

Abstract: Monolayer WSe 2 hosts a series of exciton Rydberg states denoted by the principal quantum number n = 1, 2, 3, etc. While most research focuses on their absorption properties, their optical emission is also important but much less studied.Here we measure the photoluminescence from the 1s -5s exciton Rydberg states in ultraclean monolayer WSe 2 encapsulated by boron nitride under magnetic fields from -31 T to 31 T. The exciton Rydberg states exhibit similar Zeeman shifts but distinct diamagnetic shifts from each… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

4
45
0

Year Published

2019
2019
2022
2022

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 60 publications
(49 citation statements)
references
References 53 publications
4
45
0
Order By: Relevance
“…It needs to be checked if it is the case for the dark exciton in MoS2 as well. Finally, phonon replicas of dark excitons, for instance in Figure 9 are observed energetically below the dark excitons in monolayer WS2 and WSe2 on the basis of their observed g factors (either about 9 or 12), energetic locations, and valley polarization 177,179,180,209 . Therefore, magnetooptical spectroscopy has been crucial in the identification of PL peaks previously under debate 87,166,203 .…”
Section: Neutral 'Dark' Excitons In Tmdcsmentioning
confidence: 95%
See 1 more Smart Citation
“…It needs to be checked if it is the case for the dark exciton in MoS2 as well. Finally, phonon replicas of dark excitons, for instance in Figure 9 are observed energetically below the dark excitons in monolayer WS2 and WSe2 on the basis of their observed g factors (either about 9 or 12), energetic locations, and valley polarization 177,179,180,209 . Therefore, magnetooptical spectroscopy has been crucial in the identification of PL peaks previously under debate 87,166,203 .…”
Section: Neutral 'Dark' Excitons In Tmdcsmentioning
confidence: 95%
“…Δ is of the order of few meVs to a few 10s of meVs, while Δ ranges from about 150 meV to 500 meV [162][163][164][165] . Due to the specific sign of the conductionband splitting, the ground-state exciton in WS2, WSe2, and MoS2 is found to be optically "spin forbidden" or "dark" 87,162,[172][173][174][175][176][177][178][179][180][181]164,182,[165][166][167][168][169][170][171] (see Figure 2(b)). In MoSe2 and MoTe2, however, the ground-state exciton is an optically "bright" state due to a reversed conduction band splitting compared to the other three materials 165,[182][183][184][185] (Figure 2(b)).…”
Section: Zeeman Splittingmentioning
confidence: 99%
“…Electron-and exciton-phonon interaction results in pronounced sidebands in absorption and emission spectra, [5,6] controls resonant light scattering and impacts coherence generation. [7][8][9][10] The electron-phonon interaction serves as an efficient channel of the momentum and energy relaxation of charge carriers and excitons. [11][12][13] In general, polaron effects related to the coupling of the charge carriers with in-plane polarized phonons are important for the physics of TMDC monolayers.…”
Section: Introductionmentioning
confidence: 99%
“…They have direct band gap at two time-reversal valleys (K, K') [2,3], where spin-orbit coupling (SOC) splits each band into two subbands with opposite spins [4][5][6]. The electrons and holes can form tightly bound excitons at each valley [7][8][9][10][11][12][13][14]. If they come from bands with the same electron spin, they form bright excitons with efficient radiative recombination [ Fig.…”
mentioning
confidence: 99%