Resistive anisotropy in the charge density wave phase of Kagome superconductor CsV3Sb5 thin films
arXiv:2412.02469 · doi:10.1063/5.0232533
Abstract
We investigate the resistive anisotropy in CsV3Sb5 thin films within the charge density wave phase. Using a device structure with twelve electrodes symmetrically distributed in a circular shape, we measure the resistivity anisotropy by varying the current direction. A twofold resistivity anisotropy modulated by temperature is found, which is fully consistent with the electronic nematicity in CsV3Sb5, that is, the spontaneous rotational symmetry breaking by electronic degree of freedom. Additionally, the resistivity anisotropy also shows modest changes by applying magnetic fields, implying the possible chiral charge orders with time-reversal symmetry breaking. These findings provide deep insights into the correlated electronic states in Kagome materials and highlight the unique properties of CsV3Sb5 in the two-dimensional regime.
13 pages
References in corpus (14)
- Theory of Intertwined Orders in High Temperature Superconductors
- CsVSb: a topological kagome metal with a superconducting ground state
- Unconventional Fermi surface instabilities in the Kagome Hubbard Model
- Superconductivity in the kagome metal KVSb
- Topological Insulators and Nematic Phases from Spontaneous Symmetry Breaking in 2D Fermi Systems with a Quadratic Band Crossing
- Formation of a Nematic Fluid at High Fields in Sr3Ru2O7
- Superconductivity and normal-state properties of kagome metal RbV3Sb5 single crystals
- Unusual competition of superconductivity and charge-density-wave state in a compressed topological kagome metal
- Doped Kagome System as Exotic Superconductor
- Highly-robust reentrant superconductivity in CsV3Sb5 under pressure
- Tuning Inelastic Light Scattering via Symmetry Control in 2D Magnet CrI
- Anisotropic superconducting properties of Kagome metal CsV3Sb5
- Carrier Injection and Manipulation of Charge-Density Wave in Kagome Superconductor CsV3Sb5
- Chiral spin density wave order on frustrated honeycomb and bilayer triangle lattice Hubbard model at half-filling