Landau-Fermi liquids in disguise

M. Fabrizio
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Abstract

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, coherent `quasiparticles` do exist also approaching a Luttinger surface in compressible interacting electron systems. Thermodynamic and dynamic properties of such `quasiparticles` are just those of conventional ones. For instance, they yield well defined quantum oscillations in Luttinger's 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.
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伪装的朗多-费米液体
在相互作用电子的周期系统中,费米曲面和卢廷格曲面分别是指零能量和零温度下单粒子格林函数在布里渊区内的极点和零点位置。解析性质上的这种差异是在费米表面附近出现定义良好的准粒子的基础,而在卢廷格表面附近则假定不存在准粒子,在卢廷格表面,单粒子的态密度在零能量下消失。我们在这里表明,与这种普遍看法相反,在可压缩相互作用的电子系统中,相干的“准粒子”也确实存在于接近卢廷格表面的地方。这种“准粒子”的热力学和动力学性质和传统粒子一样。例如,它们在卢廷格表面产生了定义良好的量子振荡,在温度比热中产生了线性振荡,考虑到物理电子状态密度的消失,这是惊人的,但实际上在强相关材料中并不罕见。
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