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1997
DOI: 10.1002/prop.2190450203
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All-order Finiteness inN = 1 SYM Theories: Criteria and Applications

Abstract: As a motivation, we first recall the possible connection of electric‐magnetic duality to finiteness in N = 1 super‐Yang‐Mills theories (SYM). Then, we present the criterion for all‐order finiteness (i.e., vanishing of the β‐functions at all orders) in N = 1 SYM. Finally, we apply this finiteness criterion to an SU(5) SGUT. The latter turns out to be all‐order finite if one imposes additional symmetries.

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Cited by 50 publications
(47 citation statements)
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“…The most impressive aspect of the RGI relations is that they are valid to all orders of perturbation theory, a fact that can be realized by exploring the uniqueness of these relations at 1-loop level [1]. Besides this we can also find RGI relations that guarantee finiteness to every order in perturbation theory [10,11].…”
Section: Introductionmentioning
confidence: 94%
“…The most impressive aspect of the RGI relations is that they are valid to all orders of perturbation theory, a fact that can be realized by exploring the uniqueness of these relations at 1-loop level [1]. Besides this we can also find RGI relations that guarantee finiteness to every order in perturbation theory [10,11].…”
Section: Introductionmentioning
confidence: 94%
“…One of the impressive aspects of the RGI relations is that their validity can be guaranteed to all-orders in perturbation theory by studying the uniqueness of the resulting relations at one-loop, as was proven [25,26] in the early days of the program of reduction of couplings [25][26][27][28][29][30]. Even more impressive is the fact that it is possible to find RGI relations among couplings guaranteeing finiteness to all-orders in perturbation theory [31][32][33][34][35].…”
Section: Jhep08(2018)150mentioning
confidence: 99%
“…It is based on (a) the structure of the supercurrent in N = 1 SUSY gauge theory [67][68][69] and on (b) the non-renormalization properties of N = 1 chiral anomalies [26,27,66,70,71]. Details on the proof can be found in [27,66] and further discussion in [26,28,[70][71][72]. Here, following mostly [72], we present a comprehensible sketch of the proof.…”
Section: Finiteness In N = 1 Supersymmetric Gauge Theoriesmentioning
confidence: 99%
“…The vanishing of the gauge β function at one loop, β (1) g , is equivalent to the vanishing of the R current anomaly (28). The vanishing of the anomalous dimensions at one loop implies the vanishing of the Yukawa coupling β functions at that order.…”
mentioning
confidence: 99%