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Condensed Matter > Strongly Correlated Electrons

arXiv:2403.02322v5 (cond-mat)
[Submitted on 4 Mar 2024 (v1) , last revised 10 Sep 2025 (this version, v5)]

Title: Stable non-Fermi liquid fixed point at the onset of incommensurate $2k_F$ charge density wave order

Title: 在非共格$2k_F$电荷密度波序开始时的稳定非费米液体固定点

Authors:Ipsita Mandal
Abstract: We consider the emergence of a non-Fermi liquid fixed point in a two-dimensional metal, at the onset of a quantum phase transition from a Fermi liquid state to an incommensurate charge density wave (CDW) ordered phase. The momentum of the CDW boson is centred at the wavevector $ \boldsymbol{ \mathcal Q} $, which connects a single pair of antipodal points on the Fermi surface with antiparallel tangent vectors. We employ the dimensional regularization technique in which the co-dimension of the Fermi surface is extended to a generic value, while keeping the dimension of the Fermi surface itself fixed at one. Although the system is strongly coupled at dimension $d=2$, the interactions become marginal at the upper critical dimension $d=d_c$, whose value is found to be $ 5/2$. Using a controlled perturbative expansion in the parameter $\epsilon = d_c - d $, we compute the critical exponents of the stable infrared fixed point characterizing the quantum critical point. The scalings of the original theory are determined by setting $\epsilon =1/2$, where the fermion self-energy is seen to scale with the frequency with a fractional power law of $2/3$, which is the telltale signature of a typical non-Fermi liquid phase.
Abstract: 我们考虑在二维金属中出现非费米液体固定点,这是从费米液体状态到不共线电荷密度波(CDW)有序相的量子相变开始时的现象。 CDW玻色子的动量集中在波矢$ \boldsymbol{ \mathcal Q} $上,该波矢连接费米面上的一对相对点,并具有反平行的切向量。 我们采用维数正则化技术,其中费米面的余维数被扩展到一个通用值,同时保持费米面本身的维度固定为一。 尽管系统在维度$d=2$处是强耦合的,但在上临界维度$d=d_c$处相互作用变得边缘,其值被发现为$ 5/2$。 通过参数$\epsilon = d_c - d $的受控微扰展开,我们计算了表征量子临界点的稳定红外固定点的临界指数。 原始理论的标度由设置$\epsilon =1/2$确定,其中费米子自能被看到与频率呈分数幂律的标度,其幂指数为$2/3$,这是典型非费米液体相的特征标志。
Comments: In the published version, a singularity relevant for the UV was erroneously considered in the RG flow equations in the IR. This arxiv version includes the corrected results, showing that the number of coupling constant(s) is one (rather than two). The corrigendum has been published as Nucl. Phys. B 1018, 117047 (2025)
Subjects: Strongly Correlated Electrons (cond-mat.str-el) ; Superconductivity (cond-mat.supr-con); High Energy Physics - Theory (hep-th)
Cite as: arXiv:2403.02322 [cond-mat.str-el]
  (or arXiv:2403.02322v5 [cond-mat.str-el] for this version)
  https://doi.org/10.48550/arXiv.2403.02322
arXiv-issued DOI via DataCite
Journal reference: Nucl. Phys. B 1005, 116586 (2024)
Related DOI: https://doi.org/10.1016/j.nuclphysb.2024.116586
DOI(s) linking to related resources

Submission history

From: Ipsita Mandal [view email]
[v1] Mon, 4 Mar 2024 18:55:12 UTC (240 KB)
[v2] Tue, 23 Apr 2024 01:46:11 UTC (217 KB)
[v3] Tue, 11 Jun 2024 19:07:13 UTC (236 KB)
[v4] Sun, 14 Jul 2024 12:00:38 UTC (236 KB)
[v5] Wed, 10 Sep 2025 13:28:04 UTC (213 KB)
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