Supersymmetric NJL-Type Model for a Real Superfield Composite

The Nambu–Jona-Lasinio (NJL) model is a classic theory for the strong dynamics of composite fields and symmetry breaking. Supersymmetric versions of the NJL-type models are certainly of interest too. Particularly, the case with a composite (Higgs) chiral superfield formed by two (quark) chiral superfields has received much attention. Here, we propose a prototype model with a four-chiral-superfield interaction, giving a real superfield composite. It has a spin-one composite vector field with properties being somewhat similar to a massive gauge boson of spontaneously broken gauge symmetry. As such, it is like the first supersymmetric analog to non-supersymmetric models with spin-one composites. The key formulation developed here is the picture of quantum effective action as a superfield functional with parameters like constant superfields, having explicit supersymmetric and Grassmann number dependent supersymmetry breaking parts. Following the standard non-perturbative analysis for NJL-type models, the gap equation analysis shows plausible signature of dynamical supersymmetry breaking which is worth more serious analysis. With an extra superfield model Lagrangian included, comparison between the models and their non-supersymmetric counterparts is discussed, illustrating the notion of supersymmetrization is nontrivial in the setting.

[1]  O. Kong,et al.  Dynamical symmetry breaking with four-superfield interactions , 2011, 1108.0214.

[2]  G. Jona-Lasinio,et al.  Dynamical Model of Elementary Particles Based on an Analogy with Superconductivity. II , 1961 .

[3]  W. Buchmüller,et al.  Chiral symmetry and supersymmetry in the Nambu-Jona-Lasinio model , 1982 .

[4]  Marciano Dynamical symmetry breaking and the top-quark mass. , 1990, Physical review. D, Particles and fields.

[5]  M. Carena,et al.  Dynamical symmetry breaking and the top quark mass in the minimal supersymmetric standard model , 1992 .

[6]  NJL breaking of supersymmetric GUTs , 1993, hep-ph/9303245.

[7]  N. Bogolyubov Reviews of Topical Problems: the Compensation Principle and the Self-Consistent Field Method , 1959 .

[8]  Robert D.C. Miller,et al.  A simple component field method for SUSY effective potential calculations , 1983 .

[9]  Dual realizations of dynamical symmetry breaking , 2006, hep-th/0608054.

[10]  M. Tanabashi,et al.  Is the t Quark Responsible for the Mass of W and Z Bosons , 1989 .

[11]  The vacuum structure in a supersymmetric gauged Nambu—Jona-Lasinio model , 1993, hep-ph/9304278.

[12]  M. Grisaru,et al.  Improved Methods for Supergraphs , 1979 .

[13]  Mahiko. Suzuki Approximate gauge symmetry of composite vector bosons , 2010, 1006.1319.

[14]  Marciano,et al.  Heavy top-quark mass predictions. , 1989, Physical review letters.

[15]  Hill,et al.  Minimal dynamical symmetry breaking of the standard model. , 1990, Physical review. D, Particles and fields.

[16]  U. Ellwanger,et al.  On the structure of composite goldstone supermultiplets , 1984 .

[17]  The top quark mass in a supersymmetric standard model with dynamical symmetry breaking , 1990 .

[18]  S. Weinberg Perturbative Calculations of Symmetry Breaking , 1973 .

[19]  M. Tanabashi,et al.  Dynamical electroweak symmetry breaking with large anomalous dimension and t quark condensate , 1989 .

[20]  G. Jona-Lasinio,et al.  DYNAMICAL MODEL OF ELEMENTARY PARTICLES BASED ON AN ANALOGY WITH SUPERCONDUCTIVITY. PART II , 1961 .