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Low-scale SUSY breaking and the (s)goldstino physics

For a 4D N=1 supersymmetric model with a low SUSY breaking scale (f) and general Kahler potential K(Phi^i,Phi_j^*) and superpotential W(Phi^i) we study, in an effective theory approach, the relation of the goldstino superfield to the (Ferrara-Zumino) superconformal symmetry breaking chiral superfiel...

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Detalles Bibliográficos
Autores principales: Antoniadis, I., Ghilencea, D.M.
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2013.01.015
http://cds.cern.ch/record/1491418
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author Antoniadis, I.
Ghilencea, D.M.
author_facet Antoniadis, I.
Ghilencea, D.M.
author_sort Antoniadis, I.
collection CERN
description For a 4D N=1 supersymmetric model with a low SUSY breaking scale (f) and general Kahler potential K(Phi^i,Phi_j^*) and superpotential W(Phi^i) we study, in an effective theory approach, the relation of the goldstino superfield to the (Ferrara-Zumino) superconformal symmetry breaking chiral superfield X. In the presence of more sources of supersymmetry breaking, we verify the conjecture that the goldstino superfield is the (infrared) limit of X for zero-momentum and Lambda->\infty. (Lambda is the effective cut-off scale). We then study the constraint X^2=0, which in the one-field case is known to decouple a massive sgoldstino and thus provide an effective superfield description of the Akulov-Volkov action for the goldstino. In the presence of additional fields that contribute to SUSY breaking we identify conditions for which X^2=0 remains valid, in the effective theory below a large but finite sgoldstino mass. The conditions ensure that the effective expansion (in 1/Lambda) of the initial Lagrangian is not in conflict with the decoupling limit of the sgoldstino (1/m_sgoldstino\sim Lambda/f, f<Lambda^2).
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spelling cern-14914182023-03-14T17:52:36Zdoi:10.1016/j.nuclphysb.2013.01.015http://cds.cern.ch/record/1491418engAntoniadis, I.Ghilencea, D.M.Low-scale SUSY breaking and the (s)goldstino physicsParticle Physics - TheoryFor a 4D N=1 supersymmetric model with a low SUSY breaking scale (f) and general Kahler potential K(Phi^i,Phi_j^*) and superpotential W(Phi^i) we study, in an effective theory approach, the relation of the goldstino superfield to the (Ferrara-Zumino) superconformal symmetry breaking chiral superfield X. In the presence of more sources of supersymmetry breaking, we verify the conjecture that the goldstino superfield is the (infrared) limit of X for zero-momentum and Lambda->\infty. (Lambda is the effective cut-off scale). We then study the constraint X^2=0, which in the one-field case is known to decouple a massive sgoldstino and thus provide an effective superfield description of the Akulov-Volkov action for the goldstino. In the presence of additional fields that contribute to SUSY breaking we identify conditions for which X^2=0 remains valid, in the effective theory below a large but finite sgoldstino mass. The conditions ensure that the effective expansion (in 1/Lambda) of the initial Lagrangian is not in conflict with the decoupling limit of the sgoldstino (1/m_sgoldstino\sim Lambda/f, f<Lambda^2).For a 4D N=1 supersymmetric model with a low SUSY breaking scale (f) and general Kahler potential K(@F^i,@F_j^@?) and superpotential W(@F^i) we study, in an effective theory approach, the relation of the goldstino superfield to the (Ferrara-Zumino) superconformal symmetry breaking chiral superfield X. In the presence of more sources of supersymmetry breaking, we verify the conjecture that the goldstino superfield is the (infrared) limit of X for zero-momentum and @L->~ (@L is the effective cut-off scale). We then study the constraint X^2=0, which in the one-field case is known to decouple a massive sgoldstino and thus provide an effective superfield description of the Akulov-Volkov action for the goldstino. In the presence of additional fields that contribute to SUSY breaking we identify conditions for which X^2=0 remains valid, in the effective theory below a large but finite sgoldstino mass. The conditions ensure that the effective expansion (in 1/@L) of the initial Lagrangian is not in conflict with the decoupling limit of the sgoldstino (1/m_s_g_o_l_d_s_t_i_n_o~@L/f, f<@L^2).For a 4D N=1 supersymmetric model with a low SUSY breaking scale ( f ) and general Kahler potential K(Φi,Φj†) and superpotential W(Φi) we study, in an effective theory approach, the relation of the goldstino superfield to the (Ferrara–Zumino) superconformal symmetry breaking chiral superfield X . In the presence of more sources of supersymmetry breaking, we verify the conjecture that the goldstino superfield is the (infrared) limit of X for zero-momentum and Λ→∞ ( Λ is the effective cut-off scale). We then study the constraint X2=0 , which in the one-field case is known to decouple a massive sgoldstino and thus provide an effective superfield description of the Akulov–Volkov action for the goldstino. In the presence of additional fields that contribute to SUSY breaking we identify conditions for which X2=0 remains valid, in the effective theory below a large but finite sgoldstino mass. The conditions ensure that the effective expansion (in 1/Λ ) of the initial Lagrangian is not in conflict with the decoupling limit of the sgoldstino ( 1/msgoldstino∼Λ/f , f<Λ2 ).For a 4D N=1 supersymmetric model with a low SUSY breaking scale (f) and general Kahler potential K(Phi^i,Phi_j^*) and superpotential W(Phi^i) we study, in an effective theory approach, the relation of the goldstino superfield to the (Ferrara-Zumino) superconformal symmetry breaking chiral superfield X. In the presence of more sources of supersymmetry breaking, we verify the conjecture that the goldstino superfield is the (infrared) limit of X for zero-momentum and Lambda->\infty. (Lambda is the effective cut-off scale). We then study the constraint X^2=0, which in the one-field case is known to decouple a massive sgoldstino and thus provide an effective superfield description of the Akulov-Volkov action for the goldstino. In the presence of additional fields that contribute to SUSY breaking we identify conditions for which X^2=0 remains valid, in the effective theory below a large but finite sgoldstino mass. The conditions ensure that the effective expansion (in 1/Lambda) of the initial Lagrangian is not in conflict with the decoupling limit of the sgoldstino (1/m_sgoldstino\sim Lambda/f, f<Lambda^2).arXiv:1210.8336CERN-PH-TH-2012-231CERN-PH-TH-2012-231oai:cds.cern.ch:14914182012-11-01
spellingShingle Particle Physics - Theory
Antoniadis, I.
Ghilencea, D.M.
Low-scale SUSY breaking and the (s)goldstino physics
title Low-scale SUSY breaking and the (s)goldstino physics
title_full Low-scale SUSY breaking and the (s)goldstino physics
title_fullStr Low-scale SUSY breaking and the (s)goldstino physics
title_full_unstemmed Low-scale SUSY breaking and the (s)goldstino physics
title_short Low-scale SUSY breaking and the (s)goldstino physics
title_sort low-scale susy breaking and the (s)goldstino physics
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/j.nuclphysb.2013.01.015
http://cds.cern.ch/record/1491418
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