2002
DOI: 10.1103/physrevb.66.073106
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Charge-density wave and three-dimensional Fermi surface in1TTaSe2studied by photoemission spectroscopy

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Cited by 40 publications
(28 citation statements)
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“…This is generally associated with two mechanisms: first, electrons are injected into previously unoccupied d-states, increasing the electron density on Mo and nesting the Fermi surface simultaneously, and second, the electron density is spatially modulated accompanied by a periodic lattice distortion (PLD) with complicated ionic patterns featured by reduced symmetry. Different from the electron self-modulation in such CDW materials as NbSe 2 , TiSe 2 and TaSe 2 [56][57][58], the modulation of electron density in Li-intercalated MoS 2 requires outer electron injection and depends on the symmetry of host matrix (1T or 2H). It is shown here that the Peierls instability exists also in the Li-intercalated 2H-MoS 2 , which results in the formation of a CDW weaker than that in the 1T counterpart.…”
Section: Formation and Stabilization Of Cdw After LI Intercalationmentioning
confidence: 99%
“…This is generally associated with two mechanisms: first, electrons are injected into previously unoccupied d-states, increasing the electron density on Mo and nesting the Fermi surface simultaneously, and second, the electron density is spatially modulated accompanied by a periodic lattice distortion (PLD) with complicated ionic patterns featured by reduced symmetry. Different from the electron self-modulation in such CDW materials as NbSe 2 , TiSe 2 and TaSe 2 [56][57][58], the modulation of electron density in Li-intercalated MoS 2 requires outer electron injection and depends on the symmetry of host matrix (1T or 2H). It is shown here that the Peierls instability exists also in the Li-intercalated 2H-MoS 2 , which results in the formation of a CDW weaker than that in the 1T counterpart.…”
Section: Formation and Stabilization Of Cdw After LI Intercalationmentioning
confidence: 99%
“…In this paper, we will report on a study of the CDW phase transition in 1T-TaSe 2 between a commensurate phase (C-phase, q C = 0.225a* + 0.07b*) and an incommensurate phase (IC-phase, q IC = 0.278b*) induced by the fs-laser excitation. Theoretical analysis of the topology of the Fermi surface suggests that CDW in the IC-phase can be connected by the modulation wave vector as predicted by Peierls model [13][14], however, the nature of the C-phase and CDW transitions, is still under debate [15][16][17][18].…”
mentioning
confidence: 99%
“…In previous literatures, it is demonstrated that the layered 1T-TaSe 2 crystals contain numerous of remarkable structural and physical phenomena in correlation with CDW and superconductivity [20][21][22]. 1T-TaSe 2 materials have a quasi-two-dimensional structure consisting of planes of hexagonally arranged Ta atoms, sandwiched by two Se layers coordinating the central Ta atom in an octahedral arrangement [15]. The structural modulations in association with CDW states occur dominantly in the a-b plane which depends evidently on the temperature and chemical compositions [21].…”
mentioning
confidence: 99%
“…The layered compounds tend to have flat cleavage surfaces which are suitable for angleresolved photoemission spectroscopy (ARPES) measurements, and the three-dimensional electronic structures can be observed by sweeping photon energy for ARPES. For example, the ARPES study on the classical 1T-TaSe 2 system has shown that the large Se-Se interaction between the layers and the strong covalency between the Ta 5d and Se 4p orbitals provide three-dimensional Fermi surfaces which play important roles in the charge density wave formation [1]. In the case of Fe-based superconductors, the origin of the spin and orbital order in the parent materials is still controversial and the three-dimensional multi-band Fermi surfaces observed by ARPES are key ingredients to understand the spin and orbital instabilities as well as the nodeless and nodal superconducting states [2].…”
mentioning
confidence: 99%