极限下量子临界金属的不稳定性

Petter Saterskog
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引用次数: 0

摘要

我们研究了一个2+1维的模型,该模型由$N_f$费米子组成的费米曲面耦合到量子临界点附近的标量涨落。$N_f\rightarrow0$极限允许我们非摄动地计算费米子相关函数的长程行为。我们用它来计算在零和有限温度下,具有零和有限阶参数间隙的不同量子cps附近的电荷、自旋和对磁化率。当涨落抹去费米子准粒子时,我们发现涨落的总体效应导致了增强的配对。我们还发现,在T=0时,在有限区间的序参量涨落间隙内,涨落诱导自旋和电荷密度波不稳定。我们恢复了在$N_f\rightarrow0$限制中被抑制的图的一个子集,所有具有最多2个顶点的内部费米子环的图,并发现这不会改变相关器的远程行为,除了在qcp处。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Instabilities of quantum critical metals in the limit $N_f\rightarrow0$
We study a model in 2+1 dimensions composed of a Fermi surface of $N_f$ flavors of fermions coupled to scalar fluctuations near quantum critical points (QCPs). The $N_f\rightarrow0$ limit allows us to non-perturbatively calculate the long-range behavior of fermion correlation functions. We use this to calculate charge, spin and pair susceptibilities near different QCPs at zero and finite temperatures, with zero and finite order parameter gaps. While fluctuations smear out the fermionic quasiparticles, we find QCPs where the overall effect of fluctuations leads to enhanced pairing. We also find QCPs where the fluctuations induce spin and charge density wave instabilities for a finite interval of order parameter fluctuation gaps at $T=0$. We restore a subset of the diagrams suppressed in the $N_f\rightarrow0$ limit, all diagrams with internal fermion loops with at most 2 vertices, and find that this does not change the long-range behavior of correlators except right at the QCPs.
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