Abstract

In the Next-to-Minimal Supersymmetric Standard Model (NMSSM), all singlet-dominated particles including one neutralino, one CP-odd Higgs boson and one CP-even Higgs boson can be simultaneously lighter than about 100 GeV. Consequently, dark matter (DM) in the NMSSM can annihilate into multiple final states to explain the galactic center gamma-ray excess (GCE). In this work we take into account the foreground and background uncertainties for the GCE and investigate these explanations. We carry out a sophisticated scan over the NMSSM parameter space by considering various experimental constraints such as the Higgs data, B-physics observables, DM relic density, LUX experiment and the dSphs constraints. Then for each surviving parameter point we perform a fit to the GCE spectrum by using the correlation matrix that incorporates both the statistical and systematic uncertainties of the measured excess. After examining the properties of the obtained GCE solutions, we conclude that the GCE can be well explained by the pure annihilations $$ {\tilde{\chi}}_1^0{\tilde{\chi}}_1^0\to b\overline{b} $$ and $$ {\tilde{\chi}}_1^0{\tilde{\chi}}_1^0\to {A}_1{H}_i $$ with A 1 being the lighter singlet- dominated CP-odd Higgs boson and H i denoting the singlet-dominated CP-even Higgs boson or SM-like Higgs boson, and it can also be explained by the mixed annihilation $$ {\tilde{\chi}}_1^0{\tilde{\chi}}_1^0 \to {W}^{+}{W}^{-} $$ , A 1 H 1. Among these annihilation channels, $$ {\tilde{\chi}}_1^0{\tilde{\chi}}_1^0\to {A}_1{H}_i $$ can provide the best interpretation with the corresponding p-value reaching 0.55. We also discuss to what extent the future DM direct detection experiments can explore the GCE solutions and conclude that the XENON-1T experiment is very promising in testing nearly all the solutions.

Highlights

  • We investigate the gamma-ray excess (GCE) solutions for the case that dark matter (DM) is singlino-dominated, and H1 acts as the SM-like Higgs boson

  • We took into account the recently reported foreground and background uncertainties for the GCE and investigated its explanation by DM annihilation in the framework of the Next-to-Minimal Supersymmetric Standard Model (NMSSM)

  • We carried out a sophisticated scan over the NMSSM parameter space by considering various experimental constraints such as the Higgs data, B−physics observables, DM relic density, LUX experiment and the dwarf spheroidal galaxies (dSphs) constraints

Read more

Summary

Theoretical setup for the GCE in the NMSSM

We start our analysis by recapitulating the basics of the NMSSM. As one of the most economical extensions of the MSSM, the NMSSM introduces one gauge singlet Higgs superfield in its matter content, and since one purpose of the extension is to solve the μ-problem of the MSSM, a Z3 symmetry is usually adopted in the construction of the superpotential to avoid the appearance of parameters with mass dimension. The properties of a singlino-dominated DM are quite different from those of a bino-dominated DM, which makes the DM physics in the NMSSM much richer than that in the MSSM [111] Another feature is that, in the presence of a singlino-dominated DM with mass below 100GeV, the singlet-dominated CP-even and CP-odd Higgs bosons can be simultaneously lighter than about 100GeV [111, 112], and the strengthes for the interactions among these particles are determined by the parameter κ which may be as large as 0.1.

Parameter scan strategy for GCE solution
GCE solutions with H2 being the SM-like Higgs boson
Solution I — the bb annihilation channel
Solution II — the H1A1 annihilation channel
GCE solutions with H1 being the SM-like Higgs boson
Solution V — the H2A1 annihilation channel
Explore the GCE solutions in future DM experiments
Summary
A Properties of the singlet-dominated particles
CP-odd Higgs mass matrix
CP-even Higgs mass matrix
Findings
Some properties of the singlet-dominated particles
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call