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On Landau-Khalatnikov-Fradkin transformation in quenched QED3

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arxiv 2305.17775 v1 pith:DL5OIR2F submitted 2023-05-28 hep-th

classification hep-th
keywords correctionsgaugefour-looplandau-khalatnikov-fradkinmasslessperturbativepropagatorquenched
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We present the results of studies [1,2] of the gauge covariance of the massless fermion propagator in three-dimensional quenched quantum electrodynamics in the framework of dimensional regularization in d=3-2\ep. Assuming the finiteness of the perturbative expansion, i.e. existence of the limit \ep \to 0, it was shown in [1] that exactly for d=3 all odd perturbative coefficients, starting from the third order, must be equal to zero in any gauge. To test this, in Ref. [2] we calculated three- and four-loop corrections to the massless fermionic propagator. Three-loop corrections are finite and gauge-invariant, while four-loop corrections have singularities. The terms depending on the gauge parameter are completely determined by the lower orders in accordance with the Landau-Khalatnikov-Fradkin transformation.

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  1. Landau-Khalatnikov-Fradkin Transformations in Quantum Electrodynamics: For Perturbation Theory and Dynamical Mass Generation

    hep-ph 2025-02 conditional novelty 5.0 of 10

    The gauge-dependent parts of the QED fermion propagator at two loops are derived in QED3 and QED4 via Landau-Khalatnikov-Fradkin transformations, and a representative dynamical mass solution is shown to have gauge-ind...

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