2019
DOI: 10.1002/pssb.201900308
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Interlayer Excitons in Transition‐Metal Dichalcogenide Heterobilayers

Abstract: In heterobilayers consisting of different transition‐metal dichalcogenide (TMDC) monolayers, optically excited electron–hole pairs can be spatially separated into the adjacent layers due to a type‐II band alignment. However, they remain Coulomb correlated and form interlayer excitons (ILEs), which recombine radiatively. While these ILEs are observed in several TMDC material combinations, their characters and properties depend on the specific system. Herein, some of these peculiarities are demonstrated by compa… Show more

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Cited by 18 publications
(13 citation statements)
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References 62 publications
(91 reference statements)
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“…1c, we extract a dipole value with a lower bound of about 0.3 e•nm. In terms of order of magnitude, the large extracted dipole moments are very similar to results on interlayer excitons in MoSe 2 /WSe 2 heterobilayers using photoluminescence [5][6][7]26]. For comparison with other homobilayer systems, interlayer excitons have very different characteristics depending on the TMD material [27,28].…”
supporting
confidence: 76%
See 1 more Smart Citation
“…1c, we extract a dipole value with a lower bound of about 0.3 e•nm. In terms of order of magnitude, the large extracted dipole moments are very similar to results on interlayer excitons in MoSe 2 /WSe 2 heterobilayers using photoluminescence [5][6][7]26]. For comparison with other homobilayer systems, interlayer excitons have very different characteristics depending on the TMD material [27,28].…”
supporting
confidence: 76%
“…Zeeman splitting of interlayer excitons.-Magneto-optics is a powerful tool for line identification and transition energy tuning [26]. The A-intralayer exciton, which exhibits a negligible Stark shift, shows a negative Zeeman splitting of about 2 meV at B z = +9 T, which changes sign as the magnetic field direction is reversed in Fig.…”
mentioning
confidence: 97%
“…While the space indirect emission has been predicted 34,43,59 and experimentally measured to be at energies close to 1 eV, 33,34,64 the most common emission observed by µ-PL at energies between 1.55-1.6 eV was identified as a momentum-space indirect owing to the large lattice mismatch and the offset of energy levels. [26][27][28][29][30][31][32] This particular interlayer emission was demonstrated to possess a weak twist angle dependence and became undetectable when the temperature is decreased. 26 However, several factors made us consider a possible reassignment of the PL bands reported in this range.…”
Section: Discussionmentioning
confidence: 93%
“…26,[28][29][30] We note that we did not take into consideration the twisted angle since the emission at 1.6 eV was observed for all the angles studied in the previous works. 26,27 d-e) and (h-i), and 200 nm in (f) and (j). Pixel sizes: 100 nm in (e) and (i), 30 nm in (f), and 40 nm in (j).…”
Section: Resultsmentioning
confidence: 99%
“…The truly two dimensional nature of these 2D materials enables large quantum efficiencies, offers a straight-foward integration into existing photonic chip technology and offers a rich playground, in which to manipulate their electronic properties. Strain [19][20][21] , defects 22 and patterned dielectrics 23 affect electronic and optical properties much more significantly than in bulk materials, while heterobilayers 24,25 , moiré physics 26,27 , proximity-induced effects 28 and Janus monolayers 29 offer promising possibilities to tailor device properties.…”
Section: Introductionmentioning
confidence: 99%