2017
DOI: 10.1088/2053-1583/2/4/044003
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Resonant Raman and photoluminescence spectra of suspended molybdenum disulfide

Abstract: Notes: 1 These authors contributed equally. AbstractRaman and photoluminescence (PL) measurements were performed on suspended and supported MoS2 up to 6 trilayers (TLs). The difference in the dielectric environment of suspended and supported MoS2 does not lead to large differences in the PL or Raman spectra.Most of the apparent difference in the PL intensity can be explained by the interference effect except for 1TL MoS2. The positions of the Raman peaks are not much different between suspended and supported M… Show more

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Cited by 41 publications
(56 citation statements)
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References 41 publications
(75 reference statements)
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“…The relative increase of the intensity of the A′ 1 /A 1g to the E′ / E g / E 1 2g can be attributed to increased out‐of‐plane motion of the sulfur atoms when free of substrate interactions. The red shift for both modes upon suspension of MoS 2 has previously been attributed to a release from residual substrate strain or doping . Previous reports have also suggested that this shift may be due to biaxial strain in MoS 2 as it “sags” over the holey area, and calculated a red‐shift rate of strain of −2.2 cm −1 /% for the A ′ 1 /A 1g mode and −5.2 cm −1 /% for the E′ / E g / E 1 2g mode in bilayer MoS 2 .…”
Section: Resultsmentioning
confidence: 80%
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“…The relative increase of the intensity of the A′ 1 /A 1g to the E′ / E g / E 1 2g can be attributed to increased out‐of‐plane motion of the sulfur atoms when free of substrate interactions. The red shift for both modes upon suspension of MoS 2 has previously been attributed to a release from residual substrate strain or doping . Previous reports have also suggested that this shift may be due to biaxial strain in MoS 2 as it “sags” over the holey area, and calculated a red‐shift rate of strain of −2.2 cm −1 /% for the A ′ 1 /A 1g mode and −5.2 cm −1 /% for the E′ / E g / E 1 2g mode in bilayer MoS 2 .…”
Section: Resultsmentioning
confidence: 80%
“…The red shift for both modes upon suspension of MoS 2 has previously been attributed to a release from residual substrate strain or doping. [24] Previous reports have also suggested that this shift may be due to biaxial strain in MoS 2 as it "sags" over the holey area, [25] and calculated a red-shift rate of strain of À2.2 cm À1 /% for the A 0 1 /A 1g mode and À5.2 cm À1 /% for the E 0 /E g /E 1 2g mode in bilayer MoS 2 . Using these values as benchmarks for this work results in an estimation of biaxial tensile strain for the suspended 2L MoS 2 presented here of $ 1.77% from the E 0 /E g /E 1 2g red-shift of $9.2 cm À1 , and $3.02% from the A 0 1 /A 1g red-shift of $6.7 cm À1 .…”
Section: Resultsmentioning
confidence: 89%
“…The breathing modes are almost invisible except for the highest excitation energies, which is similar to the case of MoS2. 12,47 Since inter-layer vibrations are dominated by chalcogen to chalcogen interactions, no enhancement of shear and breathing modes at the A exciton state For resonance studies, normalization was carried out to extract the intrinsic resonance effects. First, the Raman intensities are normalized by the intensity of the Si Raman peak at 520 cm -1 for each excitation energy to correct for the efficiency of the detection system.…”
Section: Resultsmentioning
confidence: 99%
“…The performance of devices based on 2D heterostructures can also be improved by optimizing light absorption in the stack by coupling plasmonic nanoantennae or microcavities to the structures [14][15][16]. In 2D materials, there is another convenient way to enhance light coupling by modifying the layer structure and the dielectric surroundings of the device with a suitable substrate [17][18][19][20][21][22].…”
mentioning
confidence: 99%