2011
DOI: 10.1016/j.nuclphysb.2011.06.018
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Derivation of the exact NSVZ β-function in SQED, regularized by higher derivatives, by direct summation of Feynman diagrams

Abstract: For N = 1 supersymmetric quantum electrodynamics, regularized by higher derivatives, a method for summation of all Feynman diagrams defining the βfunction is presented. Using this method we prove that the β-function is given by an integral of a total derivative, which can be easily calculated. It is shown that surviving terms give the exact NSVZ β-function. The results are compared with the explicit three-loop calculation.

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Cited by 86 publications
(188 citation statements)
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“…The integrals defining the three-loop β-function are presented, for example, in Ref. [55]. They were obtained in [47], but a more compact form for writing them was proposed later.…”
Section: (This Expression Is Written In the Euclidean Space After Tmentioning
confidence: 99%
“…The integrals defining the three-loop β-function are presented, for example, in Ref. [55]. They were obtained in [47], but a more compact form for writing them was proposed later.…”
Section: (This Expression Is Written In the Euclidean Space After Tmentioning
confidence: 99%
“…With the higher covariant derivative regularization the NSVZ relation was derived for the Abelian supersymmetric theories in all orders for the renormalization group (RG) functions defined in terms of the bare coupling constant [34,35] (which are scheme-independent for a fixed regularization [36]). The RG functions defined in the standard way in terms of the renormalized coupling constant [37] satisfy the NSVZ relation only in the NSVZ scheme which in this case can be constructed in all orders by imposing simple boundary conditions on the renormalization constants [20,36].…”
Section: Jhep05(2016)014mentioning
confidence: 99%
“…The main feature of quantum corrections, which allows to do this, is the factorization of integrals for the β-function (defined in terms of the bare coupling constant) into integrals of (double) total derivatives in the momentum space in the limit of the vanishing external momentum [38,39]. In the Abelian case this has been proved in all orders [34,35] and confirmed by explicit calculations in the three-loop approximation [40]. Using a similar method it has been proved that the integrals for the Adler D-function [41] (defined in terms of the bare coupling constant) in N = 1 supersymmetric QCD are also integrals of double total derivatives in all orders.…”
Section: Jhep05(2016)014mentioning
confidence: 99%
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