The return of the King: No-Scale F-SU(5)

We revisit the viable parameter space in No-Scale F-SU(5), examining the Grand Unified Theory within the context of the prevailing gluino mass limits established by the LHC. The satisfaction of both the No-Scale boundary condition and the experimentally measured Standard Model (SM) like Higgs boson...

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Main Authors: Tianjun Li, James A. Maxin, Dimitri V. Nanopoulos
Format: Article
Language:English
Published: Elsevier 2017-01-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269316306852
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spelling doaj-35c719f69ecb4eac9e95d191132b499a2020-11-24T23:28:50ZengElsevierPhysics Letters B0370-26931873-24452017-01-01764C16717310.1016/j.physletb.2016.11.022The return of the King: No-Scale F-SU(5)Tianjun Li0James A. Maxin1Dimitri V. Nanopoulos2Key Laboratory of Theoretical Physics and Kavli Institute for Theoretical Physics China (KITPC), Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, PR ChinaDepartment of Physics and Engineering Physics, The University of Tulsa, Tulsa, OK 74104, USAGeorge P. and Cynthia W. Mitchell Institute for Fundamental Physics and Astronomy, Texas A&M University, College Station, TX 77843, USAWe revisit the viable parameter space in No-Scale F-SU(5), examining the Grand Unified Theory within the context of the prevailing gluino mass limits established by the LHC. The satisfaction of both the No-Scale boundary condition and the experimentally measured Standard Model (SM) like Higgs boson mass requires a lower limit on the gluino mass in the model space of about 1.9 TeV, which maybe not coincidentally is the current LHC supersymmetry search bound. This offers a plausible explanation as to why a supersymmetry signal has thus far not been observed at the LHC. On the contrary, since the vector-like flippon particles are relatively heavy due to the strict condition that the supersymmetry breaking soft term Bμ must vanish at the unification scale, we also cannot address the recently vanished 750 GeV diphoton resonance at the 13 TeV LHC. Therefore, No-Scale F-SU(5) returns as a King after the spurious 750 GeV diphoton excess was gone with the wind.http://www.sciencedirect.com/science/article/pii/S0370269316306852
collection DOAJ
language English
format Article
sources DOAJ
author Tianjun Li
James A. Maxin
Dimitri V. Nanopoulos
spellingShingle Tianjun Li
James A. Maxin
Dimitri V. Nanopoulos
The return of the King: No-Scale F-SU(5)
Physics Letters B
author_facet Tianjun Li
James A. Maxin
Dimitri V. Nanopoulos
author_sort Tianjun Li
title The return of the King: No-Scale F-SU(5)
title_short The return of the King: No-Scale F-SU(5)
title_full The return of the King: No-Scale F-SU(5)
title_fullStr The return of the King: No-Scale F-SU(5)
title_full_unstemmed The return of the King: No-Scale F-SU(5)
title_sort return of the king: no-scale f-su(5)
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2017-01-01
description We revisit the viable parameter space in No-Scale F-SU(5), examining the Grand Unified Theory within the context of the prevailing gluino mass limits established by the LHC. The satisfaction of both the No-Scale boundary condition and the experimentally measured Standard Model (SM) like Higgs boson mass requires a lower limit on the gluino mass in the model space of about 1.9 TeV, which maybe not coincidentally is the current LHC supersymmetry search bound. This offers a plausible explanation as to why a supersymmetry signal has thus far not been observed at the LHC. On the contrary, since the vector-like flippon particles are relatively heavy due to the strict condition that the supersymmetry breaking soft term Bμ must vanish at the unification scale, we also cannot address the recently vanished 750 GeV diphoton resonance at the 13 TeV LHC. Therefore, No-Scale F-SU(5) returns as a King after the spurious 750 GeV diphoton excess was gone with the wind.
url http://www.sciencedirect.com/science/article/pii/S0370269316306852
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