Daily Overview: Today’s highlights focus on deepening the understanding of the electronic structure of mixed Ruddlesden-Popper nickelates. In [1], polarization-resolved electronic Raman scattering was employed to probe the density wave state of La₃Ni₂O₇ single crystals, revealing momentum-selective anisotropic electronic correlations and confirming the coexistence of spin density wave gaps with two different coupling strengths, thereby providing a microscopic foundation for understanding the emergence of nickelate superconductivity under pressure. In [2], magnetotransport measurements on compressively strained La₂SmNi₂O₇ thin films directly observed the coexistence of antiferromagnetic spin fluctuations and superconductivity at low temperatures. The unique “Mexican hat”-shaped magnetoresistance behavior reveals a novel relationship between fluctuations and superconductivity, offering key experimental evidence for elucidating the pairing mechanism of nickelate superconductivity. arXiv submission processing window: 2026-02-08 14:41 to 2026-02-08 14:47 UTC.
1. Anisotropic Electronic Correlations in the Spin Density Wave State of La$_3$Ni$_2$O$_7$
- Relevance Score:
5.9071 - Authors: Ge He, Jun Shen, Shiyu Xie, Haotian Zhang, Mengwu Huo, Jun Shu, Deyuan Hu, Xiaoxiang Zhou, Yanmin Zhang, Lei Qin, Liangxin Qiao, Hengjie Liu, Chuansheng Hu, Xijie Dong, Dengjing Wang, Jun Liu, Wei Hu, Jie Yuan, Yajun Yan, Zeming Qi, Kui Jin, Zengyi Du, Meng Wang, Donglai Feng
- Link: http://arxiv.org/abs/2602.07998v1
- Paper page: Anisotropic Electronic Correlations in the Spin Density Wave State of La₃Ni₂O₇
Summary: Using polarization-resolved electronic Raman scattering measurements on high-quality La₃Ni₂O₇ single crystals, we observe a pronounced, symmetry-dependent spectral weight redistribution across the density-wave transition below 150 K: the B₁g channel exhibits an asymmetric peak, while the B₂g channel shows a symmetric broad peak, corresponding to electronic excitations near the X/Y points of the Brillouin zone and along the diagonal directions, respectively. Quantitative analysis extracts two sets of SDW gap values, with the B₁g channel gap approximately 37.5–40.4 meV (2Δ/kBTc ≈ 5.5–5.9) and the B₂g channel gap about 23.0 meV (2Δ/kBTc ≈ 3.4), indicating intermediate-to-strong coupling for the former and weak coupling for the latter. This momentum-selective anisotropic coupling strength cannot be explained by simple weak-coupling nesting theory, revealing that the unconventional SDW originates from anisotropic electronic correlations. The temperature dependence of the gap is significantly weaker than mean-field expectations, and the isotropy of the B₂g channel along with the weak anisotropy of the B₁g channel further support the coexistence of two distinct coupling mechanisms. This work establishes the electronic characteristics of the SDW in La₃Ni₂O₇, providing a microscopic foundation for understanding the emergence of high-temperature superconductivity in nickelates under pressure.
2. Coexistence of Antiferromagnetic Spin Fluctuations and Superconductivity in La2SmNi2O7 Thin Films
- Relevance Score:
5.3786 - Authors: Minhui Xu, Yibo Wang, Jia Liu, Long Cheng, Shuyin Li, Shuaishuai Yin, Xu Zheng, Lixin Yu, Aidi Zhao, Xiaolong Li, Jiandi Zhang, Xiaofang Zhai
- Affiliations: University of Chinese Academy of Sciences, Chinese Academy of Sciences, ShanghaiTech University
- Link: http://arxiv.org/abs/2602.07994v1
Summary: In compressively strained La₂SmNi₂O₇ thin films, the coexistence of antiferromagnetic spin fluctuations and superconductivity is directly observed through magnetotransport measurements. The films exhibit high-quality epitaxial structures with an orthorhombic oxygen octahedral rotation pattern. Below the superconducting onset temperature, a characteristic “Mexican hat”-shaped magnetoresistance emerges under in-plane magnetic fields: a negative magnetoresistance in the low-field regime, attributed to the suppression of antiferromagnetic fluctuations and consequent reduction in scattering; and a positive magnetoresistance in the high-field regime, resulting from the Zeeman effect disrupting superconducting fluctuations. By defining a crossover field B* to quantify the strength of antiferromagnetic fluctuations, it is found that B* decreases with increasing temperature and vanishes near the superconducting onset temperature, a behavior distinctly different from that of high-temperature cuprate superconductors. These experimental results not only confirm the coexistence of antiferromagnetic fluctuations and superconductivity but also reveal a direct and novel relationship between them, providing crucial experimental evidence for understanding the pairing mechanism in nickelate superconductors.