BaDElPh Highlights
- BaDElPh Highlights
- Tuning the topological and magnetic properties of TIs
- Ferrimagnetism in graphene
- Anomalies at the DP in graphene
- CDW & Kondo effect in a Dirac semimetal
- QWS on bilayer graphene
- Flat band in graphene
- Antiferromagnetic TI
- MoS2 on Gr/Ir(111)
- EAL of low-energy electrons in solids
- SC in few-monolayer MgB2
- SOC induced gap in graphene
- Li-doped black phosphorous
- Rashba coupling amplification in BaNiS2
- High-quality graphene
- EPC and SC in graphene
- Surface-enhanced CDW in UD Bi(2201)
- Origin of electron accumulation in In2O3
- Impurity state in H-Graphene
- Gap and orbital character in Ba(FeCo)2As2
- Surface-umklapp at an organic-metal interface
- Quasiparticles at the Mott transition in V2O3
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Kramers NL in the CDW state of YTe3
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YTe3, a nonmagnetic quasi-two-dimensional chalcogenide, exhibits an incommensurate CDW state below 334 K. Using ARPES and DFT, we establish that YTe3 is a CDW-induced Kramers nodal line (KNL) metal, a recently proposed topological state of matter. Two mutually orthogonal CDW domains, each exhibiting a unidirectional and similar qCDW, is revealed from both LEED and STM, while the noncentrosymmetric crystal structure has been established by x-ray crystallography and Raman spectroscopy. DFT calculated bands provides excellent agreement with ARPES when the contributions from both the twin domains are considered. The CDW gap is barely visible in the Fermi surface (FS) of YTe3 because of the twin domains. Nevertheless, the gap could be identified by comparing with the FS measured at high temperature (345 K) in the non-CDW state. The bands calculated using DFT with SOC show a KNL along Σ resulting from the crossings between the bilayer split main and shadow bands dispersing perpendicular to the KNL. |
The KNL exists only in the CDW phase where shadow bands are present and the inversion symmetry is broken. Thus, our work establishes that YTe3 is a CDW-driven KNL metal. Retrieve article S. Sarkar, J. Bhattacharya, P. Bhakuni, D. Jangra, P. Sadhukhan, R. Batabyal, C.D. Malliakas, M. Bianchi, D. Curcio, S. Roy, A. Pariari, S. Barman, M. Balal, G. Di Santo, L. Petaccia, D.Y. Chung, Y. Wang, V.G. Sathe, P. Mandal, M.G. Kanatzidis, Ph. Hofmann, A. Chakrabarti, S.R. Barman, Phys. Rev. B 113, 035129 (2026). doi: 10.1103/ld4p-hl13 |
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