Erratum: Matching conditions and duality inN=1 SUSY gauge theories in the conformal window [Phys. Rev. D53, 4526 (1996)]

Superconformal flavor simplified

“…In the very weakly-coupled limit, m/Λ c is suppressed as e −8π 2 / N g 2 * and hence we expect the mixing angle sin α ≪ 1. On the other hand, it is important to note that approaching this weakly-coupled (Banks-Zaks) limit [65,66] requires being at very large N, and none of the models considered in the present work are at sufficiently large N so as to really approach this limit.…”

Mass spectra in $${\mathcal {N}}=1$$ N = 1 SQCD with additional colorless but flavored fields

“…the dual gauge coupling a(μ = Q ) = N c α(μ = Q )/2π is sufficiently close to its small frozen value, δ = [a * − a(μ ∼ Q )]/a * 1, and δ is neglected everywhere below in comparison with 1 for simplicity (and the same for the Yukawa coupling a f = N c α f /2π ), see [3] and the appendix therein). The fixed point value of the dual gauge coupling is a * 7b o /3N c 1 [13,14].…”

“…, where for the non-perturbative term we use the form proposed in [1] 14) in which A is the auxiliary field. From (8.13) and (8.14), the hybrids 12 , 21 are massless, the baryons B 2 , B 2 are light (the pion masses increased due to their mixing with the fions).…”

Aspects of Supersymmetric Field Theories

“…Ref. [3] for a related discussion. Along the RG flow, the j R µ current in the T µ supermultiplet is a linear combination of a conserved part, together with a violated part, j R µ = j R,cons µ + j R,viol µ .…”