The change in the electronic structure of layered CuxIrTe2 has been characterized by transport and spectroscopic measurements, combined with first-principles calculations. The Cu-intercalation suppresses the monoclinic distortion, giving rise to the stabilization of the trigonal phase with superconductivity. Thermopower and Hall resistivity measurements suggest the multiband nature with hole and electron carriers for this system, which is masked by the predominance of the hole carriers enhanced by the interlayer hybridization in the trigonal phase. Rather than the instability of Ir d band, a subtle balance between the interlayer and intralayer Te-Te hybridizations is proposed as a main factor dominating the structural transition and the superconductivity.
The
control of acoustic phonons, which are the carriers of sound
and heat, has become the focus of increasing attention because of
a demand for manipulating the sonic and thermal properties of nanometric
devices. In particular, the photoacoustic effect using ultrafast optical
pulses has a promising potential for the optical manipulation of phonons
in the picosecond time regime. So far, its mechanism has been mostly
based on the commonplace thermoelastic expansion in isotropic media,
which has limited applicability. In this study, we investigate a conceptually
new mechanism of the photoacoustic effect involving a structural instability
that utilizes a transition-metal dichalcogenide VTe2 with
a ribbon-type charge-density-wave (CDW). Ultrafast electron microscope
imaging and diffraction measurements reveal the generation and propagation
of unusual acoustic waves in a nanometric thin plate associated with
optically induced instantaneous CDW dissolution. Our results highlight
the capability of photoinduced structural instabilities as a source
of coherent acoustic waves.
We investigate photo-induced lattice strains of a monoclinic VTe2 thin flake using ultrafast electron diffraction. After photoexcitation by a 190 fs pulse, we observe diffraction intensity oscillations with periods of 35 and 75 ps, which indicate coherent acoustic phonons of two distinct branches. The oscillations of and diffraction intensities have opposite signs, indicating the change of the diffraction angle due to the shear strain. By numerically simulating these diffraction intensities as a function of the monoclinic angle, we evaluate the amplitude of the photo-induced shear strain.
Topologically nontrivial materials host protected edge states associated with the bulk band inversion through the bulk-edge correspondence. Manipulating such edge states is highly desired for developing new functions and devices practically using their dissipation-less nature and spin-momentum locking. Here we introduce a transition-metal dichalcogenide VTe2, that hosts a charge density wave (CDW) coupled with the band inversion involving V3d and Te5p orbitals. Spin- and angle-resolved photoemission spectroscopy with first-principles calculations reveal the huge anisotropic modification of the bulk electronic structure by the CDW formation, accompanying the selective disappearance of Dirac-type spin-polarized topological surface states that exist in the normal state. Thorough three dimensional investigation of bulk states indicates that the corresponding band inversion at the Brillouin zone boundary dissolves upon the CDW formation, by transforming into anomalous flat bands. Our finding provides a new insight to the topological manipulation of matters by utilizing CDWs’ flexible characters to external stimuli.
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