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Erratum: Superconducting instability in non-Fermi liquids [Phys. Rev. B 94, 115138 (2016)]

Ipsita Mandal
Phys. Rev. B 109, 079902 – Published 29 February 2024

Abstract

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  • Received 8 February 2024

DOI:https://doi.org/10.1103/PhysRevB.109.079902

©2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Article Text

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Original Article

Superconducting instability in non-Fermi liquids

Ipsita Mandal
Phys. Rev. B 94, 115138 (2016)
Issue

Vol. 109, Iss. 7 — 15 February 2024

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Images

  • Figure 7
    Figure 7

    The contourplots of the two fixed points (ṼS*) of βV as functions of d and m. The intersection of the white areas in the two density plots corresponds to regions where no perturbative fixed point exists. The dashed black (red) curve (line) represents d=dc(d=d̃c) in each plot.

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  • Figure 8
    Figure 8

    The contourplot of the second root obtained from βV=0, representing a fixed point value ṼS*, as a function of m and d. Here we have enlarged the region around m=1. The dashed black line represents d=dc.

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  • Figure 9
    Figure 9

    The representative RG flows in the various regions of the (d,m) plane. The black dots represent the finite fixed points when they exist. The contour shading conveys the magnitudes of the flow vector (ṼSl,ẽl) in different regions.

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