Karnaukhov Igor N
G.V. Kurdyumov Institute for Metal Physics, 36 Vernadsky Boulevard, 03142, Kiev, Ukraine.
Sci Rep. 2021 Mar 12;11(1):5842. doi: 10.1038/s41598-021-85317-z.
Using mean field approach, we provide analytical and numerical solution of the symmetric Anderson lattice for arbitrary dimension at half filling. The symmetric Anderson lattice is equivalent to the Kondo lattice, which makes it possible to study the behavior of an electron liquid in the Kondo lattice. We have shown that, due to hybridization (through an effective field due to localized electrons) of electrons with different spins and momenta [Formula: see text] and [Formula: see text], the gap in the electron spectrum opens at half filling. Such hybridization breaks the conservation of the total magnetic momentum of electrons, the spontaneous symmetry is broken. The state of electron liquid is characterized by a large Fermi surface. A gap in the spectrum is calculated depending on the magnitude of the on-site Coulomb repulsion and value of s-d hybridization for the chain, as well as for square and cubic lattices. Anomalous behavior of the heat capacity at low temperatures in the gapped state, which is realized in the symmetric Anderson lattice, was also found.
使用平均场方法,我们给出了半填充时任意维度对称安德森晶格的解析解和数值解。对称安德森晶格等同于近藤晶格,这使得研究近藤晶格中电子液体的行为成为可能。我们已经表明,由于具有不同自旋和动量的电子[公式:见正文][公式:见正文]之间的杂化(通过局域电子产生的有效场),电子能谱在半填充时出现能隙。这种杂化破坏了电子总磁矩的守恒,自发对称性被打破。电子液体的状态由一个大的费米面表征。根据链、正方形晶格和立方晶格的在位库仑排斥强度以及s-d杂化值计算出能谱中的能隙。还发现了在对称安德森晶格中实现的能隙态低温下热容量的反常行为。