Higher-derivative mathcal{N}=1 and mathcal{N}=2 supersymmetric Maxwell-Chern-Simons theories at one loop in superspace
Pith reviewed 2026-05-09 17:29 UTC · model grok-4.3
The pith
Higher-derivative supersymmetric Maxwell-Chern-Simons theories in N=1 and N=2 superspace have their one-loop effective potentials computed explicitly in closed form via background field quantization.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The effective potential is obtained in closed form and expressed in terms of the roots of polynomial functions.
Load-bearing premise
The higher-derivative operator, a polynomial of arbitrary degree in the d'Alembertian, can be introduced exclusively in the gauge sector while preserving the supersymmetry and allowing consistent background field quantization in the higher-derivative R_ξ gauge.
read the original abstract
We define a higher-derivative generalization of Maxwell-Chern-Simons theory in $\mathcal{N}=1$ and $\mathcal{N}=2$ superspaces. In particular, the chosen higher-derivative operator is a polynomial function of the d'Alembertian of arbitrary degree, and it is introduced exclusively in the gauge sector. The main goal is to explicitly compute the one-loop quantum corrections to the superfield effective potential for these theories. This is carried out by means of background field quantization in a higher-derivative $R_\xi$ gauge. The effective potential is obtained in closed form and expressed in terms of the roots of polynomial functions.
Editorial analysis
A structured set of objections, weighed in public.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Supersymmetry is preserved by the higher-derivative operator introduced only in the gauge sector.
- domain assumption Background field quantization in the higher-derivative R_ξ gauge is valid and yields a gauge-independent effective potential.
discussion (0)
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