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Background Fields Meet the Heat Kernel: Gauge Invariance and RGEs without diagrams

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
abstract

We introduce a new method that exploits the combination of the Heat Kernel (HK) and Background Field Method to compute gauge-invariant and gauge parameter-independent quantities such as the effective potential, anomalous dimensions, and renormalization group equations. In contrast to currently employed techniques, these results are obtained exclusively from the dynamics of the background fields, without relying on supplementary input from, e.g., traditional diagrammatic calculations. This is achieved by a consistent treatment of open and closed derivatives in the HK expansions. In this way, we compute the standard quantities such as $\beta$ functions and their gauge-parameter independence when background fields are on-shell. We demonstrate this formalism for instructive examples such as Scalar QED and Yukawa theory. Full results for the bosonic part of the Standard Model provide further validation of our approach.

fields

hep-ph 2

years

2026 2

representative citing papers

Polyakov Loops Tame Phase Transitions

hep-ph · 2026-07-07 · conditional · novelty 6.0

Polyakov loop contributions to the thermal effective potential soften electroweak phase transitions, disfavoring first-order transitions and suppressing gravitational-wave signals.

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Showing 2 of 2 citing papers.

  • Polyakov Loops Tame Phase Transitions hep-ph · 2026-07-07 · conditional · none · ref 70 · internal anchor

    Polyakov loop contributions to the thermal effective potential soften electroweak phase transitions, disfavoring first-order transitions and suppressing gravitational-wave signals.

  • Higher-dimensional operators and Polyakov loop in hot Scalar QED from the heat kernel hep-ph · 2026-06-08 · unverdicted · none · ref 43 · internal anchor

    Computes dimension-six operators in finite-temperature massive scalar QED via heat kernel methods and evaluates their combined effect with the Polyakov loop on first-order phase transition thermodynamics.