Wang Yuxuan, Abanov Artem, Altshuler Boris L, Yuzbashyan Emil A, Chubukov Andrey V
Department of Physics and Institute for Condensed Matter Theory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA.
Department of Physics, Texas A&M University, College Station, Texas 77843, USA.
Phys Rev Lett. 2016 Oct 7;117(15):157001. doi: 10.1103/PhysRevLett.117.157001. Epub 2016 Oct 5.
Near a quantum-critical point in a metal strong fermion-fermion interaction mediated by a soft collective boson gives rise to incoherent, non-Fermi liquid behavior. It also often gives rise to superconductivity which masks the non-Fermi liquid behavior. We analyze the interplay between the tendency to pairing and fermionic incoherence for a set of quantum-critical models with effective dynamical interaction between low-energy fermions. We argue that superconducting T_{c} is nonzero even for strong incoherence and/or weak interaction due to the fact that the self-energy from dynamic critical fluctuations vanishes for the two lowest fermionic Matsubara frequencies ω_{m}=±πT. We obtain the analytic formula for T_{c}, which reproduces well earlier numerical results for the electron-phonon model at vanishing Debye frequency.
在金属中,靠近量子临界点时,由软集体玻色子介导的强费米子 - 费米子相互作用会导致非相干的非费米液体行为。它通常还会引发超导性,而超导性会掩盖非费米液体行为。我们针对一组具有低能费米子间有效动态相互作用的量子临界模型,分析配对倾向与费米子非相干性之间的相互作用。我们认为,即使对于强非相干性和/或弱相互作用,超导转变温度(T_{c})也不为零,这是因为对于两个最低的费米子马氏频率(\omega_{m}=±\pi T),动态临界涨落的自能消失。我们得到了(T_{c})的解析公式,该公式很好地再现了德拜频率为零时电子 - 声子模型的早期数值结果。