论文标题
$ f $ - 电子和磁性订购效果在镍lanio $ _2 $和ndnio $ _2 $:类似铜的$ 3D_ {x^2-y^2} $ band的出色角色
$f$-electron and magnetic ordering effects in nickelates LaNiO$_2$ and NdNiO$_2$: remarkable role of the cuprate-like $3d_{x^2-y^2}$ band
论文作者
论文摘要
最近在掺杂的无限层镍中发现超导性的发现使人们更加普遍地了解高温超导性的性质。母体复合ndnio $ _ {2} $的低能电子结构,电子相关性在驱动超导性中的作用以及丘比特和镍镍之间可能的关系仍然是空的问题。在这里,通过比较LANIO $ _2 $和NDNIO $ _2 $在无参数的密度功能框架内,全电子第一原理框架中,我们揭示了塑造Pristine ndnio $ _2 $ _2 $的角色nd 4 $ f $ electron。除了4 $ f $ - 电子的效果外,LANIO $ _2 $和NDNIO $ _2 $之间的电子结构之间的相似之处很强。 ND 4 $ F $和NI 3 $ D $轨道之间的杂交显示可显着修改各种磁状态的费米表面。相比之下,磁有序阶段之间的竞争主要取决于ni $ d_ {x2-y2} $ band的差距,因此,Lanio $ _2 $和NDNIO $ _2 $中的基础状态证明与Cuprates的相似之处。发现$ d-p $的拆分量要大得多,而Intralayer 3 $ d $ ion-exchange耦合的镍含量与粉结酸盐相比更小。我们的现场哈伯德$ u $的估计值与丘比特中的估计值相似,但是发现Hund耦合$ j_h $的值对ND磁矩很敏感。 ndnio $ _2 $中的Exchange耦合$ j $仅是Curpates中的一半,这可以解释为什么镍中的$ T_C $与Cutrates一样大。
Recent discovery of superconductivity in the doped infinite-layer nickelates has renewed interest in understanding the nature of high-temperature superconductivity more generally. The low-energy electronic structure of the parent compound NdNiO$_{2}$, the role of electronic correlations in driving superconductivity, and the possible relationship betweeen the cuprates and the nickelates are still open questions. Here, by comparing LaNiO$_2$ and NdNiO$_2$ systematically within a parameter-free density functional framework, all-electron first-principles framework, we reveal the role Nd 4$f$ electrons in shaping the ground state of pristine NdNiO$_2$. Strong similarities are found between the electronic structures of LaNiO$_2$ and NdNiO$_2$, except for the effects of the 4$f$-electrons. Hybridization between the Nd 4$f$ and Ni 3$d$ orbitals is shown to significantly modify the Fermi surfaces of various magnetic states. In contrast, the competition between the magnetically ordered phases depends mainly on the gaps in the Ni $d_{x2-y2}$ band, so that the ground state in LaNiO$_2$ and NdNiO$_2$ turns out to be striking similarity to that of the cuprates. The $d-p$ band-splitting is found to be much larger while the intralayer 3$d$ ion-exchange coupling is smaller in the nickelates compared to the cuprates. Our estimated value of the on-site Hubbard $U$ is similar to that in the cuprates, but the value of the Hund's coupling $J_H$ is found to be sensitive to the Nd magnetic moment. The exchange coupling $J$ in NdNiO$_2$ is only half as large as in the curpates, which may explain why $T_c$ in the nickelates is half as large as the cuprates.