Abstract

We discuss the only two viable realizations of fermion compositeness described by a calculable relativistic effective field theory consistent with unitarity, crossing symmetry and analyticity: chiral-compositeness vs goldstino-compositeness. We construct the effective theory of mathcal{N} Goldstini and show how the Standard Model can emerge from this dynamics. We present new bounds on either type of compositeness, for quarks and leptons, using dilepton searches at LEP, dijets at the LHC, as well as low-energy observables and precision measurements. Remarkably, a scale of compositeness for Goldstino-like electrons in the 2 TeV range is compatible with present data, and so are Goldstino-like first generation quarks with a compositeness scale in the 10 TeV range. Moreover, assuming maximal R-symmetry, goldstino-compositeness of both right- and left-handed quarks predicts exotic spin-1/2 colored sextet particles that are potentially within the reach of the LHC.

Highlights

  • Strongly coupled dynamics, associated with the compositeness of SM particles, can produce sizable deviations in their interactions at high energy and become the principal target of these SM precision tests [1,2,3,4,5,6,7,8,9,10]

  • It is crucial to understand how well can a framework of compositeness in the multi-TeV region fake the SM: how irrelevant can these new interactions be? From a low-energy perspective one would see no obstruction in arbitrarily soft interactions, but dispersion relations can be used to show that the basic requirement of unitarity of the microscopic (UV) theory, imposes certain positivity constraints that guarantee the existence of unsuppressed dimension-8 operators [12,13,14]

  • In this article we focus on fermions, and go beyond the traditional paradigm where fermion compositeness relies on chiral symmetry and the associated four-fermion dimension-6 operators

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Summary

Pseudo-Goldstini

We consider a strongly interacting supersymmetric sector It confines breaking SUSY spontaneously and leaving only massless Goldstini in the infrared (IR) spectrum, that we identify with (some of) the SM fermions; in addition to kinetic terms, Goldstini have selfinteractions that start at dimension-8. It may well be that a UV completion expressed as local Lagrangian is made of a series of higher-dimension operators that become important at energies of order the higher-spin states mass, yet resulting in a well-defined S-matrix at any finite energy This is somewhat analogous to what happens in Vasiliev’s theories in curved AdS space [25, 26], where the cutoff is given by the cosmological constant itself, i.e. the deepest IR observable, such that theory is never weakly coupled in the UV, where the curvature could in principle be neglected. This construction reproduces a form of MFV [36] that successfully surpasses flavor constraints even for a low SUSY-breaking scale

The effective Goldstini theory
The geometry of N Goldstini
Covariant derivatives and Maurer-Cartan form
Effective metric and invariant measure
The Goldstini effective action
Goldstini self-interactions
Model independent couplings to composite fields
Model dependent couplings to composite fields
Embedding quarks and leptons
Maximal R-symmetry
Embedding leptons
Embedding quarks and extra exotics
Explicit SUSY breaking
Collider phenomenology
Positivity constraints
Outlook — Dibosons
Phenomenology of the new colored states
Conclusions and outlook
A Dileptons at LEP
Full Text
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