Magnetic susceptibility measurements
8 条关联记录
8 条关联记录
本研究通过角分辨光电子能谱(ARPES)对无限层镍酸盐超导体 La0.8Ca0.2NiO2 及其母体 LaNiO2 薄膜的低能电子结构进行测量,利用改进的表面处理工艺首次在该体系中分辨出清晰的准粒子峰。在 La0.8Ca0.2NiO2 中,电子自能虚部与能量呈近似线性关系,其斜率从 (π/2, π/2) 到 (π, 0) 方向逐渐增大,显示出动量依赖的边际费米液体样散射特征。两种薄膜均表现出从对角线方向向反节点区域逐步抑制的低能谱权重,母体中的抑制更强,然而整个费米面上始终保留有限的费米能级谱权重,未见到能带前沿位移或背弯现象,表明不存在铜氧化物中典型的赝能隙。这些结果表明,动量选择性关联和边际费米液体样散射可以在无可检测赝能隙的情况下发生,为甄别高温超导正常态所必需的电子要素提供了关键基准,并暗示赝能隙并非必需,电荷转移能级和掺杂载流子轨道特征可能起着决定性作用。
1 条关联记录
1 条关联记录
3 条关联记录
9 条关联记录
该研究通过高压高温拉曼光谱和同步辐射红外反射光谱,系统研究了双层镍氧化物La₃Ni₂O₇在压力与温度下的结构相变与电子性质演变。拉曼测量证实了压力驱动的结构相变(从倾斜的Amam相到无倾斜的Fmmm或I4/mmm相),并观察到Fano线型出现,表明电子-声子耦合增强。高温数据揭示了该相变在常压下存在544 K的上限温度,完善了温压相图。红外反射率测量显示,相变伴随载流子密度提升近两个数量级,标志着从不良金属到良金属的交叉。实验建立了结构相变与电子性质强耦合的统一图像,超导性在约6-7 GPa处与无倾斜相的出现紧密相关,但高对称性与金属性本身不足以诱发超导,可能还需考虑密度波涨落等强电子关联效应。
The recent discovery of superconductivity in La3Ni2O7–δ with a transition temperature Tc close to 80 K at high pressures has attracted significant attention, due particularly to a possible density wave (DW) transition occurring near the superconducting dome. Identifying the type of DW order is crucial for understanding the origin of superconductivity in this system. However, owing to the presence of La4Ni3O10 and other intergrowth phases in La3Ni2O7–δ samples, extracting the intrinsic information from the La3Ni2O7 phase is challenging. In this study, we employed 139La nuclear quadrupole resonance (NQR) measurements to eliminate the influence of other structural phases in the sample and obtain microscopic insights into the DW transition in La3Ni2O7–δ. Below the DW transition temperature TDW ∼ 153 K, we observe a distinct splitting in the ±5/2 ↔ ±7/2 transition of the NQR resonance peak at the La(2) site, while only a line broadening is seen in the ±3/2 ↔ ±5/2 transition peak. Through further analysis of the spectra, we show that the line splitting is due to a unidirectional charge modulation. A magnetic line broadening is also observed below TDW, accompanied by a large enhancement of the spin-lattice relaxation rate, indicating the formation of magnetically ordered moments in the DW state. Our results suggest a simultaneous formation of charge- and spin-density wave orders in La3Ni2O7–δ, thereby offering critical insights into the electronic correlations in Ni-based superconductors.
该研究结合第一性原理计算、压力依赖的双轨道模型以及自洽FLEX和线性化Eliashberg方程,揭示了无限层La₀.₈Sr₀.₂NiO₂中压力增强且稳健超导的微观机制。结果表明,压力升高增大了动能尺度、降低了有效关联强度U/t、增强了层间杂化,并使空穴从La/Sr电荷库转移到关联的Ni区域;在低压下,动能尺度增大和体系趋近最佳中等耦合促进配对,而高压下压力诱导的自掺杂使体系进入过掺杂区,从而抑制超导,形成宽超导穹顶。尽管压缩使费米面显著三维化,与配对相关的自旋磁化率对q_z依赖较弱,仍主要在(π,π)附近出现峰值,因此Ni d_{x²-y²}主导的d波配对态在计算压力范围内保持稳定。这一受限的低能配对框架解释了该材料在兆巴级压缩下超导的异常稳健性。
该文针对双层镍酸盐La3Ni2O7中体态无节点能隙与点接触输运呈d波样特征之间的矛盾,在理论上假定由强层间反铁磁耦合驱动的层间配对为主导配对通道,并在两轨道紧束缚模型中引入层间与层内配对振幅以复现ARPES/STM的多能隙结构。作者指出,当点接触对两层耦合不均匀时,一个在层交换镜面对称下为奇的接触势可充当作用于层赝自旋的有效Zeeman场,从而在势垒区束缚随势垒宽度和强度移动的隙内Andreev态;在镜面本征基中,该势垒混合配对符号相反的镜面扇区并打开符号反转的Andreev通道。对La3Ni2O7顶部层势垒的模拟表明,其亚隙电导可重现通常被当作d波指纹的取向依赖零偏压电导峰及侧峰,说明无节点的层间配对态可模拟d波Andreev信号,为调和相互冲突的实验证据提供了自然图像。