1984
DOI: 10.1016/0370-2693(84)90311-3
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Anomalous supersymmetry transformation of some composite operators in SQCD

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Cited by 324 publications
(292 citation statements)
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“…The correction terms in the superconformal currents are linear in P and generate linear dilaton in the asymptotic region. (Alternatively, one can obtain the whole current superfield by cancelling the Konishi anomaly [16] associated to the axial anomaly.) We find that the central charge is 5) which coincides with the central charge of the level k SL(2, R)/ U(1) Kazama-Suzuki model.…”
Section: Jhep08(2001)045mentioning
confidence: 99%
See 1 more Smart Citation
“…The correction terms in the superconformal currents are linear in P and generate linear dilaton in the asymptotic region. (Alternatively, one can obtain the whole current superfield by cancelling the Konishi anomaly [16] associated to the axial anomaly.) We find that the central charge is 5) which coincides with the central charge of the level k SL(2, R)/ U(1) Kazama-Suzuki model.…”
Section: Jhep08(2001)045mentioning
confidence: 99%
“…The equation (4.10) is a (1 + 1)-dimensional version of the Konishi anomaly [16], and its detailed derivation is given in appendix C.…”
Section: Jhep08(2001)045mentioning
confidence: 99%
“…Above W 2 is the supersymmetric gauge field kinetic term (function of V), g is the holomorphic coupling constant and d 6 z and d 8 z include integration over the fermionic superspace variables. The main tool in deriving ∆a| N=1 is the use of the Konishi anomaly [13][14][15] which is also of use in deriving the NSVZ β-function e.g. [12] or the appendix of [10].…”
Section: N = 1 Supersymmetric Gauge Theorymentioning
confidence: 99%
“…This number has to be multiplied by by flavour and colour numbers: 2N f (two matter-field per flavour) and N c (the S U(N c ) Casimir of the adjoint representation). Finally ∆a is given by 2N f N c ν∆a| (13) γ UV,IR →δγ UV,IR . With (γ UV , γ IR ) = (0, γ * ) leads to (δγ UV , δγ IR ) = (−γ * , 0) and finally…”
Section: ∆A| N=1 From Dilaton Effective Action and Konishi Anomalymentioning
confidence: 99%
“…In short the familiar results for the renormalization of the trace of the supercurrent are assumed to hold in the spontaneous breaking domain wall case as well as in its absence [24], [29]. With a further renormalization of the supercurrent, denoted…”
Section: Radiative Correctionsmentioning
confidence: 99%