Apr 25, 2024
2:15pm - 2:30pm
Room 445, Level 4, Summit
Zhaoyu Liu1,Yue Shi1,Qianni Jiang1,Elliott Rosenberg1,Jonathan DeStefano1,Jinjin Liu2,Chaowei Hu1,Yuzhou Zhao1,Zhiwei Wang2,Yugui Yao2,David Graf3,Pengcheng Dai4,Jihui Yang1,Xiaodong Xu1,Jiun-Haw Chu1
University of Washington1,Beijing Institute of Technology2,National High Magnetic Field Laboratory3,Rice University4
Zhaoyu Liu1,Yue Shi1,Qianni Jiang1,Elliott Rosenberg1,Jonathan DeStefano1,Jinjin Liu2,Chaowei Hu1,Yuzhou Zhao1,Zhiwei Wang2,Yugui Yao2,David Graf3,Pengcheng Dai4,Jihui Yang1,Xiaodong Xu1,Jiun-Haw Chu1
University of Washington1,Beijing Institute of Technology2,National High Magnetic Field Laboratory3,Rice University4
Ever since the discovery of the charge density wave (CDW) transition in the kagome metal CsV<sub>3</sub>Sb<sub>5</sub>, the nature of its symmetry breaking is under intense debate. While evidence suggests that the rotational symmetry is already broken at the CDW transition temperature (T<sub>CDW</sub>), an additional electronic nematic instability well below T<sub>CDW</sub> was reported based on the diverging elastoresistivity coefficient in the anisotropic channel (m<sub>E2g</sub>). Verifying the existence of a nematic transition below T<sub>CDW</sub> is not only critical for establishing the correct description of the CDW order parameter, but also important for understanding the low-temperature superconductivity. Here, we report elastoresistivity measurements of CsV<sub>3</sub>Sb<sub>5</sub> using three different techniques probing both isotropic and anisotropic symmetry channels. Contrary to previous reports, we find the anisotropic elastoresistivity coefficient m<sub>E2g</sub> is temperature-independent except for a step jump at T<sub>CDW</sub>. The absence of nematic fluctuations is further substantiated by measurements of the elastocaloric effect, which show no enhancement associated with nematic susceptibility. On the other hand, the symmetric elastoresistivity coefficient m<sub>A1g</sub> increases below T<sub>CDW</sub>, reaching a peak value of 90 at T<sup><span style="font-size:10.8333px">*</span></sup>=20 K. Our results strongly indicate that the phase transition at T<sup>*</sup><span style="font-size:10.8333px"> </span>is not nematic in nature and the previously reported diverging elastoresistivity is due to the contamination from the A<sub>1g</sub> channel.