Elastoresistivity in the incommensurate charge density wave phase of BaNi(AsP)
arXiv:2207.02462 · doi:10.1038/s41535-022-00525-8
Abstract
Electronic nematicity, the breaking of the crystal lattice rotational symmetry by the electronic fluid, is a fascinating quantum state of matter. Recently, BaNiAs has emerged as a promising candidate for a novel type of nematicity triggered by charge fluctuations. In this work, we scrutinize the electronic nematicity of BaNi(AsP) with using electronic transport measurements under strain. We report a large elastoresistance coefficient that is maximized at a temperature slightly higher than the first-order triclinic transition, and that corresponds to the recently discovered tetragonal-to-orthorhombic transition. The reported elastoresistance does not follow the typical Curie-Weiss form observed in iron-based superconductors but has a much sharper temperature dependence with a finite elastoresistance onsetting only together with a strong enhancement of the incommensurate charge density wave of the material. Consequently, the elastoresistance and the associated orthorhombic distortion appears here as a property of this incommensurate charge density wave. Finally, we report and track the hysteretic behavior seen in the resistance versus strain sweeps and interpret its origin as the pinning of orthorhombic domains. Our results revise the understanding of the interplay between nematicity, charge density waves and structural distortions in this material.
10 pages, 5 figures. Supplementary materials available on request
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- Spectral Evidence for Unidirectional Charge Density Wave in Detwinned BaNiAs
- The high-pressure phase diagram of BaNiAs: unconventional charge-density-waves and structural phase transitions
- Strong electron-phonon coupling in BaSrNiAs
- I-centered vs F-centered orthorhombic symmetry and negative thermal expansion of the charge density wave of EuAl2Ga2
- Chemical pressure tuning of competing orders in
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- Reaching Quantum Critical Point by Adding Non-magnetic Disorder in Single Crystals of Superconductor
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