2010
DOI: 10.1142/s0217751x10048950
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History of Supersymmetric Extensions of the Standard Model

Abstract: We recall the many obstacles which seemed, long ago, to prevent supersymmetry from possibly being a fundamental symmetry of Nature. We also present their solutions, leading to the construction of the supersymmetric extensions of the Standard Model. Finally we discuss briefly the early experimental searches for Supersymmetry.

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Cited by 15 publications
(20 citation statements)
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“…Model (MSSM). See [4,5] and references therein. It is usual in the MSSM framework to introduce R-parity in order to forbid baryon and lepton number violating interactions avoiding proton decay and processes like µ → eγ.…”
Section: One Of the Most Popular Extensions Of The Sm Is The Minimal mentioning
confidence: 99%
“…Model (MSSM). See [4,5] and references therein. It is usual in the MSSM framework to introduce R-parity in order to forbid baryon and lepton number violating interactions avoiding proton decay and processes like µ → eγ.…”
Section: One Of the Most Popular Extensions Of The Sm Is The Minimal mentioning
confidence: 99%
“…It all started more than 30 years ago from theoretical works pursued independently by Golfand and Likhtman [12], Volkov and Akulov [13], and Wess and Zumino [14]. For historical developments of the idea of supersymmetry and subsequent model building and phenomenology, we recommend the text books [15] and reviews [16,17]. We briefly outline the concept below.…”
Section: Supersymmetrymentioning
confidence: 99%
“…Putting numbers, m h < 160 GeV, for a choice of the cutoff close to the typical GUT scale Λ = 10 16 GeV. Now let us include the full structure of fermions and gauge bosons in RG equations.…”
Section: Trivialitymentioning
confidence: 99%
“…These quantities are specified by the underlying particle physics theory and need to be determined experimentally. Good WIMP candidates arise in Supersymmetry [2,3]: from the neutralino in the Minimal Supersymmetric Standard Model (MSSM) [4,5] to the lightest particle in models with extra dimensions [6,7], or models with R-parity violation where an unstable grav-itino is the dark matter candidate. A feature of gravitino dark matter is that it would leave no signal in directdetection experiments since the cross-section for the interaction between a gravitino and baryonic matter is suppressed by the Planck mass to the fourth power [8,9].…”
Section: Introductionmentioning
confidence: 99%