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Goldstino and sgoldstino in microscopic models and the constrained superfields formalism

We examine the exact relation between the superconformal symmetry breaking chiral superfield (X) and the goldstino superfield in microscopic models of an arbitrary Kahler potential (K) and in the presence of matter fields. We investigate the decoupling of the massive sgoldstino and scalar matter fie...

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Detalles Bibliográficos
Autores principales: Antoniadis, I., Dudas, E., Ghilencea, D.M.
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2011.12.005
http://cds.cern.ch/record/1394020
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author Antoniadis, I.
Dudas, E.
Ghilencea, D.M.
author_facet Antoniadis, I.
Dudas, E.
Ghilencea, D.M.
author_sort Antoniadis, I.
collection CERN
description We examine the exact relation between the superconformal symmetry breaking chiral superfield (X) and the goldstino superfield in microscopic models of an arbitrary Kahler potential (K) and in the presence of matter fields. We investigate the decoupling of the massive sgoldstino and scalar matter fields and the offshell/onshell-SUSY expressions of their superfields in terms of the fermions composites. For general K of two superfields, we study the properties of the superfield X after integrating out these scalar fields, to show that in the infrared it satisfies (offshell) the condition $X^3=0$ and $X^2\not=0$. We then compare our results to those of the well-known method of constrained superfields discussed in the literature, based on the conjecture $X^2=0$. Our results can be used in applications, to couple offshell the (s)goldstino fields to realistic models such as the MSSM.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-13940202023-03-14T19:04:07Zdoi:10.1016/j.nuclphysb.2011.12.005http://cds.cern.ch/record/1394020engAntoniadis, I.Dudas, E.Ghilencea, D.M.Goldstino and sgoldstino in microscopic models and the constrained superfields formalismParticle Physics - TheoryWe examine the exact relation between the superconformal symmetry breaking chiral superfield (X) and the goldstino superfield in microscopic models of an arbitrary Kahler potential (K) and in the presence of matter fields. We investigate the decoupling of the massive sgoldstino and scalar matter fields and the offshell/onshell-SUSY expressions of their superfields in terms of the fermions composites. For general K of two superfields, we study the properties of the superfield X after integrating out these scalar fields, to show that in the infrared it satisfies (offshell) the condition $X^3=0$ and $X^2\not=0$. We then compare our results to those of the well-known method of constrained superfields discussed in the literature, based on the conjecture $X^2=0$. Our results can be used in applications, to couple offshell the (s)goldstino fields to realistic models such as the MSSM.We examine the exact relation between the superconformal symmetry breaking chiral superfield ( X ) and the goldstino superfield in microscopic models of an arbitrary Kahler potential ( K ) and in the presence of matter fields. We investigate the decoupling of the massive sgoldstino and scalar matter fields and the offshell/onshell-SUSY expressions of their superfields in terms of the fermions composites. For general K of two superfields, we study the properties of the superfield X after integrating out these scalar fields, to show that in the infrared it satisfies (offshell) the condition X 3 = 0 and X 2 ≠ 0 . We then compare our results to those of the well-known method of constrained superfields discussed in the literature, based on the conjecture X 2 = 0 . Our results can be used in applications, to couple offshell the (s)goldstino fields to realistic models such as the MSSM.We examine the exact relation between the superconformal symmetry breaking chiral superfield (X) and the goldstino superfield in microscopic models of an arbitrary Kahler potential (K) and in the presence of matter fields. We investigate the decoupling of the massive sgoldstino and scalar matter fields and the offshell/onshell-SUSY expressions of their superfields in terms of the fermions composites. For general K of two superfields, we study the properties of the superfield X after integrating out these scalar fields, to show that in the infrared it satisfies (offshell) the condition $X^3=0$ and $X^2\not=0$. We then compare our results to those of the well-known method of constrained superfields discussed in the literature, based on the conjecture $X^2=0$. Our results can be used in applications, to couple offshell the (s)goldstino fields to realistic models such as the MSSM.arXiv:1110.5939CERN-PH-TH-2011-219CPHT-RR067.1011CERN-PH-TH-2011-219CPHT-RR067-1011oai:cds.cern.ch:13940202011-10-28
spellingShingle Particle Physics - Theory
Antoniadis, I.
Dudas, E.
Ghilencea, D.M.
Goldstino and sgoldstino in microscopic models and the constrained superfields formalism
title Goldstino and sgoldstino in microscopic models and the constrained superfields formalism
title_full Goldstino and sgoldstino in microscopic models and the constrained superfields formalism
title_fullStr Goldstino and sgoldstino in microscopic models and the constrained superfields formalism
title_full_unstemmed Goldstino and sgoldstino in microscopic models and the constrained superfields formalism
title_short Goldstino and sgoldstino in microscopic models and the constrained superfields formalism
title_sort goldstino and sgoldstino in microscopic models and the constrained superfields formalism
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/j.nuclphysb.2011.12.005
http://cds.cern.ch/record/1394020
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