pith. sign in

arxiv: 0910.1785 · v5 · pith:YZ2Y4XD6new · submitted 2009-10-09 · ✦ hep-ph

The Next-to-Minimal Supersymmetric Standard Model

classification ✦ hep-ph
keywords nmssmmodelnext-to-minimalstandardsupersymmetricaspectsbaryogenesisbeta-functions
0
0 comments X
read the original abstract

We review the theoretical and phenomenological aspects of the Next-to-Minimal Supersymmetric Standard Model: the Higgs sector including radiative corrections and the 2-loop beta-functions for all parameters of the general NMSSM; the tadpole and domain wall problems, baryogenesis; NMSSM phenomenology at colliders, B physics and dark matter; specific scenarios as the constrained NMSSM, Gauge Mediated Supersymmetry Breaking, U(1)'-extensions, CP and R-parity violation.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 8 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. WIMP Dark Matter from a Natural Discrete Gauge Symmetry in the Standard Model

    hep-ph 2026-01 unverdicted novelty 6.0

    A Z4 × Z3 discrete gauge symmetry in the SM requires three new Majorana fermions whose lightest member is stable DM with mass from a singlet scalar VEV near the electroweak scale, enabling WIMP freeze-out via scalar-m...

  2. Search for Higgs boson decays into two neutral scalars with unequal masses in final states with b quarks and tau leptons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2026-05 unverdicted novelty 5.0

    No statistically significant excess is observed in the search for Higgs decays to two neutral scalars with unequal masses, setting 95% CL upper limits between 0.9 and 36.8 pb depending on mass and decay scenario.

  3. The neutral scalars of type-II 2HDM+S under the LHC

    hep-ph 2026-04 unverdicted novelty 5.0

    Exotic decays A/H to Z h_S or Z A_S exclude large regions of the type-II 2HDM+S parameter space for moderate tan beta values where conventional 2HDM channels are weak.

  4. Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\sqrt{s}$=13 and 13.6 TeV with the ATLAS detector

    hep-ex 2025-10 unverdicted novelty 5.0

    Search for resonant X -> S(bb) H(gamma gamma) production finds no significant excess and sets 95% CL limits on sigma*BR ranging from 9 fb to 0.06 fb over mass ranges 170-1000 GeV for X and 15-500 GeV for S.

  5. Deciphering compressed electroweakino excesses with MadAnalysis 5

    hep-ph 2025-07 conditional novelty 5.0

    MadAnalysis 5 v1.11 adds efficiency-table handling, reference-frame observables, and statistical tools, then applies them to two ATLAS Run-2 analyses of compressed electroweakino signatures inside the NMSSM.

  6. Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\sqrt{s}$=13 and 13.6 TeV with the ATLAS detector

    hep-ex 2025-10 accept novelty 4.0

    No significant excess observed in search for X → S(bb)H(γγ); 95% CL limits on σ×BR set from 9 fb to 0.06 fb over m_X 170-1000 GeV and m_S 15-500 GeV in 199 fb^{-1} of ATLAS data.

  7. Search for light pseudoscalar boson pairs produced from Higgs boson decays using the 4$\tau$ and 2$\mu$2$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV

    hep-ex 2025-08 accept novelty 4.0

    No excess observed in search for Higgs to a1 a1 decays; 95% CL upper limits on branching ratio range 0.007-0.079 for a1 masses 4-15 GeV, excluding >16% in Type III 2HD+S for tan beta >2.

  8. Is the observed 125 GeV Higgs boson expected to be SM-like in the NMSSM?

    hep-ph 2019-07 unverdicted novelty 4.0

    Analysis of the NMSSM shows that the 125 GeV Higgs is not expected to be exactly SM-like, with deviations in signal strengths that can be correlated or anti-correlated between bosonic and fermionic channels.