Li Yidian, Cao Yantao, Liu Liangyang, Peng Pai, Lin Hao, Pei Cuiying, Zhang Mingxin, Wu Heng, Du Xian, Zhao Wenxuan, Zhai Kaiyi, Zhang Xuefeng, Zhao Jinkui, Lin Miaoling, Tan Pingheng, Qi Yanpeng, Li Gang, Guo Hanjie, Yang Luyi, Yang Lexian
State Key Laboratory of Low Dimensional Quantum Physics, Department of Physics, Tsinghua University, Beijing 100084, China.
Key Lab for Magnetism and Magnetic Materials of the Ministry of Education, Lanzhou University, Lanzhou 730000, China; Songshan Lake Materials Laboratory, Dongguan 523808, China.
Sci Bull (Beijing). 2025 Jan 30;70(2):180-186. doi: 10.1016/j.scib.2024.10.011. Epub 2024 Oct 17.
In addition to the pressurized high-temperature superconductivity, bilayer and trilayer nickelate superconductors LaNiO (n = 2 and 3) exhibit many intriguing properties at ambient pressure, such as orbital-dependent electronic correlation, non-Fermi liquid behavior, and density-wave transitions. Here, using ultrafast reflectivity measurement, we observe a drastic difference between the ultrafast dynamics of the bilayer and trilayer nickelates at ambient pressure. We observe a coherent phonon mode in LaNiO involving the collective vibration of La, Ni, and O atoms, which is absent in LaNiO. Temperature-dependent relaxation time diverges near the density-wave transition temperature of LaNiO, while it is inversely proportional to the temperature in LaNiO above ∼150 K, suggesting a non-Fermi liquid behavior of LaNiO. Moreover, we estimate the electron-phonon coupling constants to be 0.05-0.07 and 0.12-0.16 for LaNiO and LaNiO, respectively, suggesting a relatively minor role of electron-phonon coupling in the electronic properties of LaNiO at ambient pressure. The relevant microscopic interaction and dynamic information are essential for further studying the interplay between superconductivity and density-wave transitions in nickelate superconductors.
除了高压高温超导性外,双层和三层镍酸盐超导体LaNiO(n = 2和3)在常压下还表现出许多有趣的特性,如轨道相关的电子关联、非费米液体行为和密度波转变。在此,我们利用超快反射率测量,观察到双层和三层镍酸盐在常压下超快动力学之间的显著差异。我们在LaNiO中观察到一种涉及La、Ni和O原子集体振动的相干声子模式,而在LaNiO中不存在这种模式。与温度相关的弛豫时间在LaNiO的密度波转变温度附近发散,而在LaNiO中高于约150 K时它与温度成反比,这表明LaNiO具有非费米液体行为。此外,我们估计LaNiO和LaNiO的电子-声子耦合常数分别为0.05 - 0.07和0.12 - 0.16,这表明在常压下电子-声子耦合在LaNiO的电子性质中作用相对较小。相关的微观相互作用和动力学信息对于进一步研究镍酸盐超导体中超导性与密度波转变之间的相互作用至关重要。