Conference on Lasers and Electro-Optics 2019
DOI: 10.1364/cleo_at.2019.jth5c.6
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Ultrafast Transition from Intra- to Interlayer Exciton Phases in a Van Der Waals Heterostructure

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Cited by 4 publications
(4 citation statements)
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“…Thus, we find roughly a = 9.2 Å and b = 3.1 Å. It may be noted that a model describing van der Waals heterostructures as homogeneous material slabs separated by vacuum regions has recently successfully explained exciton binding energies in such geometries [40]. For MoS 2 and other TMDs, the barrier for conduction band electrons can be estimated as the vacuum level relative to the conduction band minimum, i.e., the electron affinity V 0 ≈ 3.8 eV [41].…”
Section: Structuresupporting
confidence: 62%
“…Thus, we find roughly a = 9.2 Å and b = 3.1 Å. It may be noted that a model describing van der Waals heterostructures as homogeneous material slabs separated by vacuum regions has recently successfully explained exciton binding energies in such geometries [40]. For MoS 2 and other TMDs, the barrier for conduction band electrons can be estimated as the vacuum level relative to the conduction band minimum, i.e., the electron affinity V 0 ≈ 3.8 eV [41].…”
Section: Structuresupporting
confidence: 62%
“…or by using means like strong magnetic field [66,67] , and unusual experimental geometries [68] . From the perspective of dynamics, the ability of optical spectroscopy to probe only 'bright' transitions leads to sparse mapping in momentum-space of various scattering processes of charge-carriers and excitons (e.g., two bright excitons that are perturbed at the beginning and the end of charge-transfer process [69] , or some internal excitations of these excitons [70] ). Figure 4a illustrates the distributions of these various excitonic states across the BZ and highlights the distributions and dynamic processes that momentum-resolved spectroscopy can effectively investigate.…”
Section: Virtues Of Momentum-resolved Versus Optical Characterization...mentioning
confidence: 99%
“…The interlayer excitons (IXs) are formed by bound pairs of electrons and holes spatially separated in two different two-dimensional (2D) semiconductor materials of van der Waals heterostructures (vdWHs) [1][2][3][4][5][6][7][8][9][10][11][12], such as those in 2D transition metal dichalcogenides (TMDC) bilayer with a type-II band alignment. The spatial separation between the electron and hole allows achieving long IX lifetimes, orders of magnitude longer than lifetimes of intralayer excitons in TMDC monolayers [8,11,[13][14][15][16][17][18]. This longer lifetime, combined with the large binding energy, has enabled the exploration of the rich many-body physics of IX and their applications in tunable photonic and optoelectronic devices [8,17,[19][20][21][22].…”
Section: Introductionmentioning
confidence: 99%