Decays of Supersymmetric Particles: the program SUSY-HIT (SUspect-SdecaY-Hdecay-InTerface)
By Abdelhak Djouadi, Michael Spira, M. Muhlleitner. 2006
501 citations recorded by the source corpus.
We present the program package SUSY-HIT for the computation of supersymmetric particle decays within the framework of the Minimal Supersymmetric extension of the Standard Model. The code is based on two existing programs HDECAY and SDECAY for the calculation of the decay widths and branching ratios of, respectively, the MSSM Higgs bosons and the SUSY particles, and calls a program for the calculation of the SUSY particle spectrum such as SuSpect. Including all important higher order effects, the package allows the consistent calculation of the MSSM particle spectrum and decays with the presently highest level of precision.
Subfields: Artificial Intelligence, Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/ac411099b3cc6ef1eff4ae07632577c3920f7254
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In Artificial Intelligence
- Atlas Collaboration
- Christophe Grojean
- M. Muhlleitner
- A. Weiler
- J. Ruderman
- Abdelhak Djouadi
- M. Raidal
- G. Arcadi
In Astronomy and Astrophysics
- Atlas Collaboration
- M. Raidal
- G. Arcadi
- Abdelhak Djouadi
- Alexander Pukhov
- A. Weiler
- G. B'elanger
- M. Muhlleitner
In Nuclear and High Energy Physics
- Atlas Collaboration
- M. Raidal
- G. Arcadi
- Abdelhak Djouadi
- M. Muhlleitner
- Alexander Pukhov
- Christophe Grojean
- G. B'elanger
Citations in the corpus
- Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at √s = 13 TeV with the ATLAS detector (2017, unknown): “5b [59], which accounts for finite b-quark and τlepton masses.”
- micrOMEGAs_3: A program for calculating dark matter observables (2013, methodology): “The following packages have been attached to micrOMEGAs using the SLHAplus interface: SOFTSUSY [110], SPHENO [111], ISAJET [112], SuperIso [103], SUSY-HIT [113], HDECAY [93], SusyBSG [114].”
- Natural SUSY endures (2011, methodology): “We calculate the SUSY spectrum and the decay tables for SUSY particles with the program SUSY-HIT [131].”
- The measurement of the Higgs self-coupling at the LHC: theoretical status (2012, unknown): “As the Higgs boson of a mass around 125GeV dominantly decays into b-quark pairs with a branching ratio of ≈ 60% and other decay modes such as H → γγ and H → WW ∗ → 2l2ν are rare [89, 90], and as the production cross sections are already low, we will focus on the three possibly promising detection ch”
- Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector (2017, methodology): “In the case of the hMSSM scenario, Higgs masses and branching fractions are computed using HDecay [85, 86].”
- Dark Matter through the Higgs portal (2019, methodology): “For this purpose, we have used the program HDECAY [204–206] which calculates the partial widths and the branching ratios of all Higgs decays (in the SM but also in some of its extensions like the 2HDM and the MSSM as will be seen later in this review) including all relevant higher order effects.”
- Fully covering the MSSM Higgs sector at the LHC (2015, methodology): “At high tan β values, say tan β >∼ 10, the decay pattern of the heavier neutral H/A bosons is extremely simple [10, 82, 83] as a result of the strong enhancement of the couplings”
- Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb−1 of pp collisions at s=13$$ \sqrt{s}=13 $$ TeV with the ATLAS detector (2018, methodology): “In the case of the hMSSM scenario, Higgs masses and branching fractions are computed using HDecay [85, 86].”
- Effective Lagrangian for a light Higgs-like scalar (2013, methodology): “In the ideal case in which one is able to kill completely the SM tree-level contribution by means of appropriate kinematic cuts, 13Here and in the following our approximated formulas have been obtained by using eHDECAY [9] with mh = 125 GeV.”