2016
DOI: 10.1002/adma.201602626
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Indirect Bandgap Puddles in Monolayer MoS2 by Substrate‐Induced Local Strain

Abstract: An unusually large bandgap modulation of 1.23-2.65 eV in monolayer MoS on a SiO /Si substrate is found due to the inherent local bending strain induced by the surface roughness of the substrate, reaching the direct-to-indirect bandgap transition. Approximately 80% of the surface area reveals an indirect bandgap, which is confirmed further by the degraded photoluminescence compared to that from suspended MoS .

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Cited by 136 publications
(131 citation statements)
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“…The MoS 2 value 0.1% is in good agreement with the additional strain found in Ref. 21 in the case of MoS 2 on SiO 2 . Since the subsequent optical band gap change is only in the order of 10 meV, such a dramatic shift in the A-peak position in MoS 2 is not expected.…”
supporting
confidence: 79%
“…The MoS 2 value 0.1% is in good agreement with the additional strain found in Ref. 21 in the case of MoS 2 on SiO 2 . Since the subsequent optical band gap change is only in the order of 10 meV, such a dramatic shift in the A-peak position in MoS 2 is not expected.…”
supporting
confidence: 79%
“…Moreover, the indirect band gap resonance was expected to be less luminescent than a direct process. Compared to the data presented here or ref., 32 our situation was quite different as the nanostructuring gave rise to a strong strain gradient and involved fewer processes, which increased the indirect gap response: 1) The consequences of the exciton funneling effect are not easily determined in this configuration and can favor indirect band gap processes. 2) Suspended MoS2 has a more intense photoluminescence signal than non-suspended and our suspended part was the stressed region.…”
Section: Resultsmentioning
confidence: 94%
“…One of the interesting properties of 2D materials is that they can be scaled down to atomic thickness. Strain is easily induced in a thin MoS 2 channel by both substrate surface roughness and/or the high‐ k deposition process, resulting in MoS bond bending . Since the conduction and valence bands of MoS 2 are mainly composed of the energy splitting of the Mo d orbital, the band tail states will be easily introduced, as schematically illustrated in Figure b.…”
Section: Introductionmentioning
confidence: 99%