Direct Visualization of an Incommensurate Unidirectional Charge Density Wave in La$_4$Ni$_3$O$_{10}$

Mingzhe Li; Jiashuo Gong; Yinghao Zhu; Ziyuan Chen; Jiakang Zhang; Enkang Zhang; Yuanji Li; Ruotong Yin; Shiyuan Wang; Jun Zhao; Dong-Lai Feng; Zengyi Du; Ya-Jun Yan

paper

Direct Visualization of an Incommensurate Unidirectional Charge Density Wave in La $_{4}$ Ni $_{3}$ O $_{10}$

arXiv:2501.18885

Abstract

Superconductivity emerges in both La $_{3}$ Ni $_{2}$ O $_{7}$ and La $_{4}$ Ni $_{3}$ O $_{10}$ under high pressure by suppressing their density-wave transitions, but critical temperature (Tc) differs significantly between these two compounds. To gain deeper insights into the distinct superconducting states, it is essential to unravel the nature of the density-wave states at ambient pressure, a topic that remains largely unexplored. Here, using scanning tunneling microscopy/spectroscopy (STM/STS), we report the direct visualization of an incommensurate unidirectional charge density wave (CDW) in La $_{4}$ Ni $_{3}$ O $_{10}$ in real space. The density of states (DOS) is strongly depleted near $E_{F}$ , indicating the opening of a CDW gap of $2 I^ \approx 71$ meV, which is unfavorable for the formation of superconductivity at ambient pressure. We propose that the CDW arises from Fermi surface nesting, and is likely a subsidiary phase of a spin density wave. Compared to La $_{3}$ Ni $_{2}$ O $_{7}$ , the weaker electronic correlation in La $_{4}$ Ni $_{3}$ O $_{10}$ is likely one reason for the lower $T_{c}$ .

11 pages, 4 figures

Direct Visualization of an Incommensurate Unidirectional Charge Density Wave in La4​Ni3​O10​

Abstract

Direct Visualization of an Incommensurate Unidirectional Charge Density Wave in La $_{4}$ Ni $_{3}$ O $_{10}$