2018
DOI: 10.1039/c8ra03436b
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Interlayer coupling and the phase transition mechanism of stacked MoS2/TaS2 heterostructures discovered using temperature dependent Raman and photoluminescence spectroscopy

Abstract: a Ultrathin 1T (tetragonal)-TaS 2 and monolayer MoS 2 heterostructures were prepared to study their phase transition (PT) mechanisms and band structure modulation. The temperature dependency of photoluminescence (PL) and Raman spectra was utilized to study interlayer coupling and band structure.The PL results indicate that the band structure of MoS 2 /TaS 2 heterostructures undergoes a sharp change at 214 K. This is attributed to the PT of 1T-TaS 2 from a Mott insulator state to a metastable state. In addition… Show more

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Cited by 9 publications
(8 citation statements)
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“…The solid, dashed, and dotted lines in figure 4(a) are the spectra before H 2 exposure, after exposure at 523 K and 22 Pa, and after exposure at 523 K and 100 Pa, respectively, where the reaction chamber was evacuated after 20 min of H 2 adsorption. Four large peaks can be observed near 102, 243, 306, and 374 cm −1 , as well as other small peaks consistent with the previously reported Raman peaks for 1T-TaS 2 [19,[32][33][34][35][36][37]. Among these peaks, those around 102 and 243 cm −1 were attributed to the zone center modes, which emerge as a consequence of zone folding caused by the lattice modulation of CCDW ordering [33].…”
Section: Resultssupporting
confidence: 87%
“…The solid, dashed, and dotted lines in figure 4(a) are the spectra before H 2 exposure, after exposure at 523 K and 22 Pa, and after exposure at 523 K and 100 Pa, respectively, where the reaction chamber was evacuated after 20 min of H 2 adsorption. Four large peaks can be observed near 102, 243, 306, and 374 cm −1 , as well as other small peaks consistent with the previously reported Raman peaks for 1T-TaS 2 [19,[32][33][34][35][36][37]. Among these peaks, those around 102 and 243 cm −1 were attributed to the zone center modes, which emerge as a consequence of zone folding caused by the lattice modulation of CCDW ordering [33].…”
Section: Resultssupporting
confidence: 87%
“…As shown in Figure 4 e,f, the photoluminescence peak position, corresponding to the direct excitonic transition energy in MoS 2 /WSe 2 , is affected by temperature variations. An increasing temperature causes a redshift in the PL peak, indicating a reduction in the energy gap of the heterostructure [ 37 ]. This energy gap refers to the energy of the lowest allowable exciton state, which corresponds to the energy required to create an electron–hole pair in the system.…”
Section: Resultsmentioning
confidence: 99%
“…Many phase-change heterostructures reported in literature are based on two-dimensional chalcogenide materials as a phase-change switchable interlayer due to their easy transfer and stacking according to device design. Heterostructures based on crystalline three-dimensional materials such as VO 2 and La 1– x Sr x MnO 3 highly rely on lattice-matched substrates and are not free-standing, limiting their adaptability to a wider range of applications.…”
Section: Phase-change Heterostructurementioning
confidence: 99%