Abstract

In this paper we explore practicable ways for self-consistent calculations of spectral functions from analytically continued functional renormalization group (aFRG) flow equations. As a particularly straightforward one we propose to include parametrizations of self-energies based on explicit analytic one-loop expressions. To exemplify this scheme we calculate the spectral functions of pion and sigma meson of the $O(4)$ model at vanishing temperature in the broken phase. Comparing the results with those from previous aFRG calculations, we explicitly demonstrate how self-consistency at all momenta fixes the tight relation between particle masses and decay thresholds. In addition, the two-point functions from our new semianalytic FRG scheme have the desired domain of holomorphy built in and can readily be studied in the entire cut-complex frequency plane, on physical as well as other Riemann sheets. This is very illustrative and allows, for example, to trace the flow of the resonance pole of the sigma meson across an unphysical sheet. In order to assess the limitations due to the underlying one-loop structure, we also introduce a fully self-consistent numerical scheme based on spectral representations with scale-dependent spectral functions. The most notable improvement of this numerically involved calculation is that it describes the three-particle resonance decay of an off-shell pion, ${\ensuremath{\pi}}^{*}\ensuremath{\rightarrow}\ensuremath{\sigma}\ensuremath{\pi}\ensuremath{\rightarrow}3\ensuremath{\pi}$. Apart from this further conceptual improvement, overall agreement with the results from the considerably simpler semianalytic one-loop scheme is very encouraging, however. The latter can therefore provide a sound and practicable basis for self-consistent calculations of spectral functions in more realistic effective theories for warm and dense matter.

Highlights

  • The properties of strong-interaction matter, i.e., matter subject to the strong force described by quantum chromodynamics (QCD), are in the focus of intense experimental and theoretical study worldwide

  • Comparing our results for the Oð4Þ model spectral functions from this new self-consistent scheme with those from a corresponding analytically continued functional renormalization group (aFRG) calculation that is built on the local potential approximation (LPA) truncation as in most previous aFRG applications, see e.g., [32,33,34,35,36,37,38,39,40], we explicitly demonstrate that the mismatch between pole masses and decay thresholds is thereby removed

  • On the left-hand side we show the spectral functions obtained from the LPA aFRG flow and SC1L flow for a small but finite value of ε 1⁄4 0.1 MeV

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Summary

INTRODUCTION

The properties of strong-interaction matter, i.e., matter subject to the strong force described by quantum chromodynamics (QCD), are in the focus of intense experimental and theoretical study worldwide. In order to avoid the peculiarities associated with gauge invariance and confinement in QCD, one thereby often employs universality and structurally simpler replacement theories to study static and dynamic critical phenomena These functional approaches are originally formulated in Euclidean spacetime which hampers the access to real-time quantities like spectral functions or transport coefficients due to the analytic continuation problem. As a first step to include self-energies beyond one-loop structure we describe a fully self-consistent numerical framework, based on spectral representations with scale dependent spectral functions, in Sec. VI, where we compare the fully selfconsistent with the SC1L results from the previous sections to assess the overall quality of the latter. Details on the explicit analytic expressions for the self-energy parametrizations and loop functions are provided together with other technicalities in several appendixes

THEORETICAL SETUP
Analytically continued LPA flows
UV conditions and numerical implementation
TWO-POINT FUNCTIONS AND SPECTRAL FUNCTIONS
ANALYTIC STRUCTURE IN THE COMPLEX PLANE
TOWARD FULLY SELF-CONSISTENT SPECTRAL FUNCTIONS
Self-consistent Euclidean flows
Self-consistent aFRG flows
Self-consistent aFRG results and comparison
SUMMARY AND OUTLOOK
Full Text
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