2016
DOI: 10.1038/ncomms13552
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Raman signatures of inversion symmetry breaking and structural phase transition in type-II Weyl semimetal MoTe2

Abstract: Transition metal dichalcogenide MoTe2 is an important candidate for realizing the newly predicted type-II Weyl fermions, for which the breaking of the inversion symmetry is a prerequisite. Here we present direct spectroscopic evidence for the inversion symmetry breaking in the low-temperature phase of MoTe2 by systematic Raman experiments and first-principles calculations. We identify five lattice vibrational modes that are Raman-active only in the low-temperature noncentrosymmetric structure. A hysteresis is … Show more

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Cited by 130 publications
(170 citation statements)
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“…According to the previous works3334, the evolution of the Raman mode at near 130 cm −1 is a direct verification of the structural phase transition of MoTe 2 from high temperature β to low temperature Td phase. In addition, there are different Raman signals for β- and Td-phase at the range of 150~300 cm −1 .…”
Section: Resultsmentioning
confidence: 70%
“…According to the previous works3334, the evolution of the Raman mode at near 130 cm −1 is a direct verification of the structural phase transition of MoTe 2 from high temperature β to low temperature Td phase. In addition, there are different Raman signals for β- and Td-phase at the range of 150~300 cm −1 .…”
Section: Resultsmentioning
confidence: 70%
“…For cooling below 300 K, the intensity of peak E grows gradually with decreasing temperature, while the intensities of A and D slightly decrease. None of these modes, however, display large, abrupt changes characteristic of a first-order − phase transition as in the bulk crystal at ~250 K [31,32]. For heating close to 400 K, the intensities of all three peaks decrease, which could indicate the beginning of a transition into another phase different from both the and phases.…”
mentioning
confidence: 99%
“…We have followed the convention used by Zhang et al and labeled the phase peaks as A, D, and E in order of increasing energy [32]. The lower energy A peak has been assigned to a shear mode, while the activated as a consequence of inversion symmetry breaking in the orthorhombic state [31,32]. has been observed in other TMDC materials and could be due to a reduced interlayer force constant in few layer systems [33][34][35].…”
mentioning
confidence: 99%
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“…1 (b)). Above 250 K the 1T' structure transforms to the centrosymmetric monoclinic (space group P12/m1) 1T" structure [16] Raman spectroscopy and resistivity measurements indicate a structural phase transition at T* ∼ 257.5 K [18]. Details about the crystals growth and their characterization can be found in the Supplementary Information [19].…”
mentioning
confidence: 99%