Fabrizio Michele
International School for Advanced Studies (SISSA), Via Bonomea 265, 34136, Trieste, Italy.
Nat Commun. 2022 Mar 23;13(1):1561. doi: 10.1038/s41467-022-29190-y.
In periodic systems of interacting electrons, Fermi and Luttinger surfaces refer to the locations within the Brillouin zone of poles and zeros, respectively, of the single-particle Green's function at zero energy and temperature. Such difference in analytic properties underlies the emergence of well-defined quasiparticles close to a Fermi surface, in contrast to their supposed non-existence close to a Luttinger surface, where the single-particle density-of-states vanishes at zero energy. We here show that, contrary to such common belief, dispersive 'quasiparticles' with infinite lifetime do exist also close to a pseudo-gapped Luttinger surface. Thermodynamic and dynamic properties of such 'quasiparticles' are just those of conventional ones. For instance, they yield well-defined quantum oscillations in Luttinger surface and linear-in-temperature specific heat, which is striking given the vanishing density of states of physical electrons, but actually not uncommon in strongly correlated materials.
在相互作用电子的周期系统中,费米面和卢廷格面分别指的是在零能量和温度下,单粒子格林函数在布里渊区中极点和零点的位置。这种解析性质的差异是靠近费米面处明确准粒子出现的基础,与之形成对比的是,在靠近卢廷格面处它们被认为不存在,因为在那里单粒子态密度在零能量处消失。我们在此表明,与这种普遍看法相反,具有无限寿命的色散“准粒子”在靠近赝能隙卢廷格面处也确实存在。这种“准粒子”的热力学和动力学性质与传统准粒子的性质相同。例如,它们在卢廷格面产生明确的量子振荡以及与温度成线性关系的比热,鉴于物理电子态密度为零,这一点很引人注目,但实际上在强关联材料中并不罕见。