1992
DOI: 10.1103/physrevd.45.3272
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Sparticle spectroscopy

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Cited by 144 publications
(501 citation statements)
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“…This has been studied within supersymmetric GUT frameworks such as SO (10) and PatiSalam SU(4) × SU(2) R × SU(2) L [166,158,167,168,169]. For example, within the Pati-Salam model the D term corrections must be included because they leave an imprint in the scalar masses of the charges carried by the broken GUT generator (these charges determine the coefficients of the g 2 terms above).…”
Section: The Ubiquitous Tan βmentioning
confidence: 99%
See 1 more Smart Citation
“…This has been studied within supersymmetric GUT frameworks such as SO (10) and PatiSalam SU(4) × SU(2) R × SU(2) L [166,158,167,168,169]. For example, within the Pati-Salam model the D term corrections must be included because they leave an imprint in the scalar masses of the charges carried by the broken GUT generator (these charges determine the coefficients of the g 2 terms above).…”
Section: The Ubiquitous Tan βmentioning
confidence: 99%
“…For example, within the Pati-Salam model the D term corrections must be included because they leave an imprint in the scalar masses of the charges carried by the broken GUT generator (these charges determine the coefficients of the g 2 terms above). Therefore the analysis of the sparticle spectra [169] might reveal the nature of the GUT symmetry breaking pattern. In addition, they split the soft Higgs masses by 22) where g X is the gauge coupling constant defined at GUT scale.…”
Section: The Ubiquitous Tan βmentioning
confidence: 99%
“…Since we are otherwise ignorant of the size of D 2 we will take it to be a free parameter in our subsequent analysis, although we will take it to be relatively small. For SO (10), including the D-term contributions to the sfermion and Higgs masses, we obtain the well-known GUT scale inputs for the sfermion and Higgs soft SUSY breaking masses [22,23,26,27,62]:…”
Section: So(10) Breaking and Scalar Massesmentioning
confidence: 99%
“…Additional D-term contributions to the soft mass matrices arise from the reduction of rank of the gauge group, associated with a broken U(1) generator proportional to 2I R + 3(B − L)/2 where I R is the 3rd component of weak isospin pertaining to the SU(2) R subgroup of SO (10) and (B − L) is the difference between baryon and lepton number [22,23,26,27,62]. The sfermion and Higgs soft masses squared each receive a contribution proportional to a quantity D 2 , which can be positive or negative, that parametrizes the D-term contribution from the breaking of the GUT group.…”
Section: Introductionmentioning
confidence: 99%
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