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Displacement Operator Formalism for Renormalization and Gauge Dependence to All Orders

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arxiv hep-ph/0501259 v1 pith:I7F5AFA7 submitted 2005-01-27 hep-ph

classification hep-ph
keywords formalismfunctionsgreenrenormalizedordersrenormalizationdependencedisplacement
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We present a new method for determining the renormalization of Green functions to all orders in perturbation theory, which we call the displacement operator formalism, or the D-formalism, in short. This formalism exploits the fact that the renormalized Green functions may be calculated by displacing by an infinite amount the renormalized fields and parameters of the theory with respect to the unrenormalized ones. With the help of this formalism, we are able to obtain the precise form of the deformations induced to the Nielsen identities after renormalization, and thus derive the exact dependence of the renormalized Green functions on the renormalized gauge-fixing parameter to all orders. As a particular non-trivial example, we calculate the gauge-dependence of $\tan\beta$ at two loops in the framework of an Abelian Higgs model, using a gauge-fixing scheme that preserves the Higgs-boson low-energy theorem for off-shell Green functions. Various possible applications and future directions are briefly discussed.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Renormalisation Group Invariants from Scaling and Non-overlapping Symmetries

    hep-th 2026-05 unverdicted novelty 6.0 of 10

    Scaling and non-overlapping global symmetries produce RGIs for bilinear operators to all loops via scale-invariant field directions, demonstrated in non-SUSY models including the 2HDM.

  2. Linearized renormalization

    hep-th 2025-05 conditional novelty 6.0 of 10

    For super-renormalizable scalar theories, the first-order change of the renormalized effective action under parameter variations is written with finitely many graphs built from full propagators and vertices, with no r...

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