Abstract

We discuss the signature of the anomalous breaking of the superconformal symmetry in $\mathcal{N}=1$ super Yang Mills theory, mediated by the Ferrara-Zumino hypercurrent ($\mathcal{J}$) with two vector ($\mathcal V$) supercurrents $(\mathcal{JVV})$ and its manifestation in the anomaly action, in the form of anomaly poles. This allows to investigate in a unified way both conformal and chiral anomalies. The analysis is performed in parallel to the Standard Model, for comparison. We investigate, in particular, massive deformations of the $\mathcal{N}=1$ theory and the spectral densities of the anomaly form factors which are extracted from the components of this correlator. In this extended framework it is shown that all the anomaly form factors are characterized by spectral densities which flow with the mass deformation. In particular, the continuum contributions from the two-particle cuts of the intermediate states turn into into poles in the zero mass limit, with a single sum rule satisfied by each component. Non anomalous form factors, instead, in the same anomalous correlators, are characterized by non-integrable spectral densities. These tend to uniform distributions as one moves towards the conformal point, with a clear dual behaviour. As in a previous analysis of the dilaton pole of the Standard Model, also in this case the poles can be interpreted as signaling the exchange of a composite dilaton/axion/dilatino (ADD) multiplet in the effective Lagrangian.[...]

Highlights

  • Dilaton fields are expected to play a very important role in the dynamics of the early universe and are present in almost any model which attempts to unify gravity with the ordinary gauge interactions

  • In case of gauging of these currents, as in superconformal theories coupled to gravity, we show that the cancellation of the corresponding anomalies requires either a vanishing β function or the inclusion of an extra gravitational sector which effectively sets the residue at the anomaly poles of the gauged currents to vanish

  • As in the AV V case, this composite state should be identified with the anomaly pole of the related anomaly correlator (the T V V diagram, with T the energy momentum tensor (EMT)), at least at the level of the 1-particle irreducible (1PI) anomaly effective action [11]

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Summary

Introduction

Dilaton fields are expected to play a very important role in the dynamics of the early universe and are present in almost any model which attempts to unify gravity with the ordinary gauge interactions (see for instance [1]). As in the AV V case, this composite state should be identified with the anomaly pole of the related anomaly correlator (the T V V diagram, with T the energy momentum tensor (EMT)), at least at the level of the 1-particle irreducible (1PI) anomaly effective action [11] Considerations of this nature brings us to the conclusion that the effective massless Nambu-Goldstone modes which should appear as a result of the existence of global anomalies, should be looked for in specific perturbative form factors under special kinematical limits. Radiative nature of the breaking of a certain global symmetry, as in the case of the anomaly, does not guarantee the massless nature of these modes, which could acquire a nonzero mass The extension of this analysis to the superconformal case is interesting in view of recent results concerning the derivation of the superconformal anomaly action for the Goldstone supermultiplet in a theory where conformal symmetry is spontaneously broken [13].

Anomalies and anomaly poles
Sum rules
The T V V and AV V vertices in an ordinary gauge theory
Theoretical framework
The perturbative expansion in the component formalism
The supercorrelator in the on-shell and massless case
The chiral multiplet contribution
The vector multiplet contribution
The supercorrelator in the on-shell and massive case
The flavor chiral symmetries and the Konishi anomaly
Mass deformations and the spectral densities flow
The analytic structure of Φ2
10 Constraining the flow: scaling behaviour and sum rules
11.1 The extra pole of QCD
11.2 T V V and the two spectral flows of the electroweak theory
11.3 The non-transverse AV V correlator
11.4 Cancellations in the supersymmetric case
13 Conclusions and perspectives
A Scalar integrals
B Electroweak form factors for the T V V
D Polology
E Feynman rules
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