Abstract
In a qualitative study, the low-energy properties of the $\text{SO}\!\left(6\right)$-symmetric Quark-Meson-Diquark Model as an effective model for two-color Quantum Chromodynamics are investigated within the Functional Renormalization Group (FRG) approach. In particular, we compute the infrared scaling behavior of fluctuation-induced higher-derivative couplings of the linear Quark-Meson-Diquark Model and map the resulting renormalized effective action onto its nonlinear counterpart. The higher-derivative couplings of the nonlinear model, which we identify as the low-energy couplings of the Quark-Meson-Diquark Model, are therefore entirely determined by the FRG flow of their linear equivalents. This grants full access to their scaling behavior and provides insights into conceptual aspects of purely bosonic effective models, as they are treated within the FRG. In this way, the presented work is understood as an immediate extension of our recent advances in the $\text{SO}\!\left(4\right)$-symmetric Quark-Meson Model beyond common FRG approximations.
Highlights
In a series of recent publications [1,2,3], we presented a low-energy analysis of the quark-meson model (QMM), which was treated as a effective model of the fundamental theory of the strong interaction, quantum chromodynamics (QCD)
The low-energy limit and qualitative features of the IR dynamics of the SOð6Þ-symmetric quark-meson-diquark model (QMDM) have been addressed within the functional renormalization group (FRG) formalism
In order to determine the corresponding low-energy couplings, which have exclusively been generated from the FRG integration of quantum fluctuations, we considered a complete set of higherderivative interactions beyond traditional approximation schemes and transformed the linear effective action into a nonlinear pseudo-NambuGoldstone bosons (pNGBs)
Summary
In a series of recent publications [1,2,3], we presented a low-energy analysis of the (two-flavor) quark-meson model (QMM), which was treated as a (linear) effective model of the fundamental theory of the strong interaction, quantum chromodynamics (QCD). We expanded the effective action of the QMM up to (and including) fourth order in its bosonic field variables as well as their respective space-time derivatives. As a result of this analysis, the low-energy limit of the QMM naturally emerges from the FRG integration of quantum fluctuations by transforming the linear realization of the SOð4Þ symmetry (among the bosonic fields) into its nonlinear counterpart [2,14,15,16,17,18,19,20].
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