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Abstract
Research on charge-density-wave (CDW) ordered transition-metal dichalcogenides continues to unravel new states of quantum matter correlated to the intertwined lattice and electronic degrees of freedom. Here, we report an inelastic x-ray scattering investigation of the lattice dynamics of the canonical CDW compound 2H-TaSe2 complemented by angle-resolved photoemission spectroscopy and density functional perturbation theory. Our results rule out the formation of a central-peak without full phonon softening for the CDW transition in 2H-TaSe2 and provide evidence for a novel precursor region above the CDW transition temperature TCDW, which is characterized by an overdamped phonon mode and not detectable in our photoemission experiments. Thus, 2H-TaSe2 exhibits structural before electronic static order and emphasizes the important lattice contribution to CDW transitions. Our ab-initio calculations explain the interplay of electron-phonon coupling and Fermi surface topology triggering the CDW phase transition and predict that the CDW soft phonon mode promotes emergent superconductivity near the pressure-driven CDW quantum critical point.
The authors study the charge-density-wave (CDW) compound 2H-TaSe2 by inelastic x-ray scattering combined with photoemission spectroscopy. They find evidence for a precursor region above the CDW transition temperature, which is characterized by an overdamped phonon mode and is not detectable by photoemission.
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1 Karlsruhe Institute of Technology, Institute for Quantum Materials and Technologies, Karlsruhe, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874); Chongqing University, College of Physics, Chongqing, P. R. China (GRID:grid.190737.b) (ISNI:0000 0001 0154 0904)
2 Karlsruhe Institute of Technology, Institute for Quantum Materials and Technologies, Karlsruhe, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874)
3 Université de Fribourg, Département de Physique and Fribourg Center for Nanomaterials, Fribourg, Switzerland (GRID:grid.8534.a) (ISNI:0000 0004 0478 1713)
4 Université de Fribourg, Département de Physique and Fribourg Center for Nanomaterials, Fribourg, Switzerland (GRID:grid.8534.a) (ISNI:0000 0004 0478 1713); Universidade de São Paulo, São Paulo, Instituto de Física, São Paulo, Brazil (GRID:grid.11899.38) (ISNI:0000 0004 1937 0722)
5 Argonne National Laboratory, Advanced Photon Source, Lemont, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)
6 Kiel University, Institute of Experimental and Applied Physics and KiNSIS, Kiel, Germany (GRID:grid.9764.c) (ISNI:0000 0001 2153 9986); Kiel University, Ruprecht Haensel Laboratory, Kiel, Germany (GRID:grid.9764.c) (ISNI:0000 0001 2153 9986)
7 Kiel University, Institute of Experimental and Applied Physics and KiNSIS, Kiel, Germany (GRID:grid.9764.c) (ISNI:0000 0001 2153 9986); Kiel University, Ruprecht Haensel Laboratory, Kiel, Germany (GRID:grid.9764.c) (ISNI:0000 0001 2153 9986); Deutsches Elektronen-Synchrotron DESY, Ruprecht Haensel Laboratory, Hamburg, Germany (GRID:grid.7683.a) (ISNI:0000 0004 0492 0453)
8 Argonne National Laboratory, Materials Science Division, Lemont, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)