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arxiv: 1907.00648 · v1 · pith:POF37RSWnew · submitted 2019-07-01 · ✦ hep-ph

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

Pith reviewed 2026-05-25 12:04 UTC · model grok-4.3

classification ✦ hep-ph
keywords NMSSMHiggs bosonsignal strengthsdeviationscorrelationsparameter scanningsinglet mixing
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The pith

Deviations from SM signal strengths are expected for the 125 GeV Higgs in the NMSSM due to mixing and extra decays.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper claims that the 125 GeV Higgs boson in the Next-to-Minimal Supersymmetric Standard Model will not match Standard Model predictions exactly. Mixing with an extra singlet-like Higgs and possible new decays to light neutralinos or pseudo-scalars produce shifts in observed signal strengths. These shifts show characteristic correlations or anti-correlations between bosonic and fermionic final states. An efficient scanning method maps the regions of parameter space where these patterns appear. A sympathetic reader would care because the patterns give concrete, testable signatures that could distinguish the NMSSM from the pure Standard Model at the LHC.

Core claim

In the NMSSM deviations from the SM signal strengths of the 125 GeV Higgs boson are expected because of the mixing with the additional singlet-like Higgs boson and/or additional decays into pairs of light particles, like neutralinos, pseudo-scalar Higgs bosons or singlet Higgs bosons. The size of the possible deviations and their expected correlations or anti-correlations between bosonic and fermionic final states are analyzed using the efficient parameter scanning technique with complete coverage. The regions of parameter space with correlated or anti-correlated deviations of the signal strengths are identified.

What carries the argument

The efficient parameter scanning technique with complete coverage that maps regions of parameter space showing correlated or anti-correlated deviations in bosonic versus fermionic signal strengths.

If this is right

  • Signal strengths in bosonic channels such as diphoton and ZZ will deviate from SM values in a manner correlated or anti-correlated with fermionic channels such as bb and tau tau.
  • Additional invisible or exotic decays into light neutralinos or light Higgs states will reduce the visible signal strengths below SM expectations.
  • The size of the deviations is set by the mixing angle between the doublet-like and singlet-like Higgs states.
  • Parameter regions with large mixing produce the largest deviations while small-mixing regions remain closer to SM-like.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Current LHC Higgs coupling measurements already constrain the allowed size of these deviations and can be reinterpreted directly in the NMSSM.
  • Future precision measurements at the High-Luminosity LHC could detect the predicted correlation patterns even if individual channels remain consistent with the SM within present errors.
  • If no such correlated deviations appear, the NMSSM would require additional mechanisms, such as decoupling limits or new decay modes that cancel the mixing effects, to remain viable.

Load-bearing premise

The efficient parameter scanning technique with complete coverage can be used to identify regions of parameter space with correlated or anti-correlated deviations of the signal strengths.

What would settle it

A global fit to all bosonic and fermionic signal-strength measurements showing no deviation from Standard Model values in any region of NMSSM parameter space would falsify the claim that deviations are expected.

Figures

Figures reproduced from arXiv: 1907.00648 by Conny Beskidt (1), Germany), Karlsruhe, Karlsruhe Inst. for Technology KIT, Wim de Boer (1) ((1) Dept. of Phys..

Figure 1
Figure 1. Figure 1: FIG. 1. The sum of the mixing matrix elements squared for the SM-like Higgs boson as function of tan [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Sketch of the sampling technique to determine the allowed NMSSM parameter space. The sampling is done by [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. BRs of the 125 GeV Higgs boson into lighter particles as function of the mass of the lighter particle, which can be [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Fitted signal strengths [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. The figure demonstrates in the top left panel (a) the correlated deviation of all signal strengths from the SM expectation [PITH_FULL_IMAGE:figures/full_fig_p008_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. As Fig. 5, but for CASE II. In this case the change in signal strengths in panel (a) originates from the change [PITH_FULL_IMAGE:figures/full_fig_p009_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. As Fig. 5, but for CASE III. The variation of the signal strengths originates from a variation of all reduced couplings [PITH_FULL_IMAGE:figures/full_fig_p010_7.png] view at source ↗
Figure 6
Figure 6. Figure 6: In the third case the singlet-like and SM-like Higgs bosons are rather close in mass, which allows for a strong [PITH_FULL_IMAGE:figures/full_fig_p011_6.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Combined measurements of the products [PITH_FULL_IMAGE:figures/full_fig_p014_8.png] view at source ↗
read the original abstract

In the Next-to Minimal Supersymmetric Standard Model (NMSSM) deviations from the SM signal strengths of the 125 GeV Higgs boson are expected, because of the mixing with the additional singlet-like Higgs boson and/or additional decays into pairs of light particles, like neutralinos, pseudo-scalar Higgs bosons or singlet Higgs bosons. In this paper the size of the possible deviations and their expected correlations or anti-correlations between \textit{bosonic} and \textit{fermionic} final states are analyzed using the efficient parameter scanning technique with complete coverage presented in a companion paper. The regions of parameter space with correlated or anti-correlated deviations of the signal strengths are identified.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The paper claims that deviations from SM-like signal strengths for the 125 GeV Higgs are expected in the NMSSM due to mixing with a singlet-like Higgs and/or additional decays to light particles (neutralinos, pseudoscalars, singlets). It analyzes the magnitude of these deviations and their correlations or anti-correlations between bosonic and fermionic final states by applying an efficient parameter-scanning technique asserted to have complete coverage (from a companion paper), and identifies the corresponding regions of NMSSM parameter space.

Significance. If the scan completeness holds, the work would usefully map expected patterns of correlated deviations, providing concrete targets for LHC analyses that could help discriminate NMSSM from the SM or other BSM scenarios. The emphasis on bosonic vs. fermionic correlations is a concrete, testable output.

major comments (1)
  1. [Abstract and §1] Abstract and §1: The central claim that specific regions with correlated/anti-correlated bosonic/fermionic signal-strength deviations can be identified rests on the assertion that the companion paper's scanning technique achieves 'complete coverage'. No independent check of that coverage, of the measure used to define 'complete', or of possible biases against regions with light singlets/neutralinos is supplied here. If the scan systematically under-samples those regions, the reported correlations are not guaranteed to be representative.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and for highlighting the importance of the scanning method's completeness. The central issue raised concerns the reliance on the companion paper for validation of complete coverage and the absence of an independent check or discussion of possible biases in this work. We respond to this point below and indicate where revisions can be made.

read point-by-point responses
  1. Referee: [Abstract and §1] Abstract and §1: The central claim that specific regions with correlated/anti-correlated bosonic/fermionic signal-strength deviations can be identified rests on the assertion that the companion paper's scanning technique achieves 'complete coverage'. No independent check of that coverage, of the measure used to define 'complete', or of possible biases against regions with light singlets/neutralinos is supplied here. If the scan systematically under-samples those regions, the reported correlations are not guaranteed to be representative.

    Authors: The scanning technique, including the precise definition of complete coverage, the measure employed, and explicit checks against under-sampling of regions containing light singlets or neutralinos, is developed and validated in the companion paper. The present manuscript applies that method to the specific question of 125 GeV Higgs signal-strength deviations and their bosonic/fermionic correlations. We acknowledge that an independent summary of these coverage properties is not repeated here. In a revised version we will add a concise paragraph in §2 that outlines the key features of the scan (including its handling of light-particle regions) while referring readers to the companion paper for the full technical validation. We maintain that the method does not systematically under-sample the relevant regions, but we agree that a brief reminder of this point will strengthen the presentation. revision: yes

Circularity Check

0 steps flagged

NMSSM signal strength analysis uses companion scan as tool without reducing claims to self-citation by construction

full rationale

The paper starts from the standard expectation in the NMSSM that the 125 GeV Higgs mixes with a singlet-like Higgs and can have additional decays, leading to deviations from SM signal strengths. It then uses an efficient scanning technique from a companion paper to explore parameter space and identify regions with correlated or anti-correlated deviations in bosonic and fermionic channels. This use of a self-cited method for scanning does not constitute circularity because the physical predictions derive from the NMSSM Lagrangian and mixing, not from redefining quantities in terms of the scan results. No self-definitional loops, fitted inputs presented as predictions, or uniqueness theorems imported from self-citations are present. The derivation chain remains self-contained against the NMSSM model assumptions.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The paper assumes the NMSSM framework with its additional singlet field and scans its parameters to find Higgs signal deviations; many free parameters typical of SUSY models are involved but not enumerated here.

free parameters (1)
  • NMSSM model parameters
    Multiple couplings, masses, and mixing angles in the NMSSM that are scanned over to find allowed regions.
axioms (1)
  • domain assumption NMSSM is a valid extension of the MSSM with an additional singlet superfield
    Assumed as the basis for the entire analysis.

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discussion (0)

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Reference graph

Works this paper leans on

43 extracted references · 43 canonical work pages · 36 internal anchors

  1. [1]

    Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC

    ATLAS Collaboration Collaboration, “Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC”, Phys.Lett. B716 (2012) 1–29, arXiv:1207.7214

  2. [2]

    Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC

    CMS Collaboration, “Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC”, Phys. Lett. B716 (2012) 30–61, arXiv:1207.7235

  3. [3]

    Vacuum Stability and Higgs Diphoton Decays in the MSSM

    M. Carena, S. Gori, I. Low et al., “Vacuum Stability and Higgs Diphoton Decays in the MSSM”, JHEP 02 (2013) 114, arXiv:1211.6136

  4. [4]

    A Higgs boson near 125 GeV with enhanced di-photon signal in the NMSSM

    U. Ellwanger, “A Higgs boson near 125 GeV with enhanced di-photon signal in the NMSSM”, JHEP 03 (2012) 044, arXiv:1112.3548

  5. [5]

    A Non Standard Model Higgs at the LHC as a Sign of Naturalness

    A. Arvanitaki and G. Villadoro, “A Non Standard Model Higgs at the LHC as a Sign of Naturalness”, JHEP 02 (2012) 144, arXiv:1112.4835

  6. [6]

    The constrained NMSSM and Higgs near 125 GeV

    J. F. Gunion, Y. Jiang, and S. Kraml, “The Constrained NMSSM and Higgs near 125 GeV”, Phys. Lett. B710 (2012) 454–459, arXiv:1201.0982

  7. [7]

    Enhancing $h \to \gamma \gamma$ with staus in SUSY models with extended gauge sector

    L. Basso and F. Staub, “Enhancing h→γγ with staus in SUSY models with extended gauge sector”, Phys. Rev. D87 (2013), no. 1, 015011, arXiv:1210.7946

  8. [8]

    Implications of LHC Higgs and SUSY searches for MSSM

    F. Mahmoudi, A. Arbey, M. Battaglia et al., “Implications of LHC Higgs and SUSY searches for MSSM”, PoS ICHEP2012 (2013) 124, arXiv:1211.2794

  9. [9]

    Radiative natural SUSY with a 125 GeV Higgs boson

    H. Baer, V. Barger, P. Huang et al., “Radiative natural SUSY with a 125 GeV Higgs boson”, Phys. Rev. Lett. 109 (2012) 161802, arXiv:1207.3343

  10. [10]

    The 125 GeV Higgs in the NMSSM in light of LHC results and astrophysics constraints

    D. A. Vasquez, G. Belanger, C. Boehm et al., “The 125 GeV Higgs in the NMSSM in light of LHC results and astrophysics constraints”, Phys.Rev. D86 (2012) 035023, arXiv:1203.3446

  11. [11]

    Fingerprinting Higgs Suspects at the LHC

    J. R. Espinosa, C. Grojean, M. M¨ uhlleitner et al., “Fingerprinting Higgs Suspects at the LHC”, JHEP 05 (2012) 097, arXiv:1202.3697

  12. [12]

    A 96 GeV Higgs boson in the general NMSSM

    K. Choi, S. H. Im, K. S. Jeong et al., “A 96 GeV Higgs boson in the general NMSSM”, arXiv:1906.03389

  13. [13]

    Review of Particle Physics

    Particle Data Group Collaboration, “Review of Particle Physics”, Phys. Rev. D98 (2018), no. 3, 030001

  14. [14]

    The Anatomy of Electro-Weak Symmetry Breaking. I: The Higgs boson in the Standard Model

    A. Djouadi, “The Anatomy of electro-weak symmetry breaking. I: The Higgs boson in the standard model”, Phys. Rept. 457 (2008) 1–216, arXiv:hep-ph/0503172

  15. [15]

    The Anatomy of Electro-Weak Symmetry Breaking. II: The Higgs bosons in the Minimal Supersymmetric Model

    A. Djouadi, “The Anatomy of electro-weak symmetry breaking. II. The Higgs bosons in the minimal supersymmetric model”, Phys. Rept. 459 (2008) 1–241, arXiv:hep-ph/0503173

  16. [16]

    A Supersymmetry Primer

    S. P. Martin, “A Supersymmetry primer”, Perspectives on supersymmetry II, Ed. G. Kane (1997) arXiv:hep-ph/9709356

  17. [17]

    On the Alignment Limit of the NMSSM Higgs Sector

    M. Carena, H. E. Haber, I. Low et al., “Alignment limit of the NMSSM Higgs sector”, Phys. Rev. D93 (2016), no. 3, 035013, arXiv:1510.09137

  18. [18]

    The Next-to-Minimal Supersymmetric Standard Model

    U. Ellwanger, C. Hugonie, and A. M. Teixeira, “The Next-to-Minimal Supersymmetric Standard Model”, Phys.Rept. 496 (2010) 1–77, arXiv:0910.1785

  19. [19]

    The mu Problem and the Strong CP Problem

    J. E. Kim and H. P. Nilles, “The mu Problem and the Strong CP Problem”, Phys. Lett. 138B (1984) 150–154

  20. [20]

    The Higgs Sector of the Next-to-Minimal Supersymmetric Standard Model

    D. Miller, R. Nevzorov, and P. Zerwas, “The Higgs sector of the next-to-minimal supersymmetric standard model”, Nucl.Phys. B681 (2004) 3–30, arXiv:hep-ph/0304049

  21. [21]

    A Natural SUSY Higgs Near 125 GeV

    L. J. Hall, D. Pinner, and J. T. Ruderman, “A Natural SUSY Higgs Near 126 GeV”, JHEP 04 (2012) 131, arXiv:1112.2703

  22. [22]

    NMSSM Higgs Benchmarks Near 125 GeV

    S. King, M. M¨ uhlleitner, and R. Nevzorov, “NMSSM Higgs Benchmarks Near 125 GeV”, Nucl.Phys. B860 (2012) 207–244, arXiv:1201.2671

  23. [23]

    On Naturalness of the MSSM and NMSSM

    Z. Kang, J. Li, and T. Li, “On Naturalness of the MSSM and NMSSM”, JHEP 1211 (2012) 024, arXiv:1201.5305. 12

  24. [24]

    A SM-like Higgs near 125 GeV in low energy SUSY: a comparative study for MSSM and NMSSM

    J.-J. Cao, Z.-X. Heng, J. M. Yang et al., “A SM-like Higgs near 125 GeV in low energy SUSY: a comparative study for MSSM and NMSSM”, JHEP 1203 (2012) 086, arXiv:1202.5821

  25. [25]

    Higgs bosons near 125 GeV in the NMSSM with constraints at the GUT scale

    U. Ellwanger and C. Hugonie, “Higgs bosons near 125 GeV in the NMSSM with constraints at the GUT scale”, Adv.High Energy Phys. 2012 (2012) 625389, arXiv:1203.5048

  26. [26]

    A comparison of the Higgs sectors of the CMSSM and NMSSM for a 126 GeV Higgs boson

    C. Beskidt, W. de Boer, and D. Kazakov, “A comparison of the Higgs sectors of the CMSSM and NMSSM for a 126 GeV Higgs boson”, Phys.Lett. B726 (2013) 758–766, arXiv:1308.1333

  27. [27]

    Dark Matter in a Constrained NMSSM

    C. Hugonie, G. Belanger, and A. Pukhov, “Dark matter in the constrained NMSSM”, JCAP 0711 (2007) 009, arXiv:0707.0628

  28. [28]

    Light NMSSM Neutralino Dark Matter in the Wake of CDMS II and a 126 GeV Higgs

    J. Kozaczuk and S. Profumo, “Light NMSSM neutralino dark matter in the wake of CDMS II and a 126 GeV Higgs boson”, Phys. Rev. D89 (2014), no. 9, 095012, arXiv:1308.5705

  29. [29]

    The semi-constrained NMSSM satisfying bounds from the LHC, LUX and Planck

    U. Ellwanger and C. Hugonie, “The semi-constrained NMSSM satisfying bounds from the LHC, LUX and Planck”, JHEP 08 (2014) 046, arXiv:1405.6647

  30. [30]

    The impact of a 126 GeV Higgs on the neutralino mass

    C. Beskidt, W. de Boer, and D. I. Kazakov, “The impact of a 126 GeV Higgs on the neutralino mass”, Phys. Lett. B738 (2014) 505–511, arXiv:1402.4650

  31. [31]

    Natural NMSSM after LHC Run I and the Higgsino dominated dark matter scenario

    J. Cao, Y. He, L. Shang et al., “Natural NMSSM after LHC Run I and the Higgsino dominated dark matter scenario”, JHEP 08 (2016) 037, arXiv:1606.04416

  32. [32]

    Searching for Singlino-Higgsino Dark Matter in the NMSSM

    Q.-F. Xiang, X.-J. Bi, P.-F. Yin et al., “Searching for Singlino-Higgsino Dark Matter in the NMSSM”, Phys. Rev. D94 (2016), no. 5, 055031, arXiv:1606.02149

  33. [33]

    Perspectives of direct Detection of supersymmetric Dark Matter in the NMSSM

    C. Beskidt, W. de Boer, D. I. Kazakov et al., “Perspectives of direct Detection of supersymmetric Dark Matter in the NMSSM”, Phys. Lett. B771 (2017) 611–618, arXiv:1703.01255

  34. [34]

    The higgsino-singlino sector of the NMSSM: Combined constraints from dark matter and the LHC

    U. Ellwanger and C. Hugonie, “The higgsino?singlino sector of the NMSSM: combined constraints from dark matter and the LHC”, Eur. Phys. J. C78 (2018), no. 9, 735, arXiv:1806.09478

  35. [35]

    An effective scanning method of the NMSSM parameter space

    C. Beskidt and W. de Boer, “An effective scanning method of the NMSSM parameter space”, arXiv:1905.07963

  36. [36]

    The constrained next-to-minimal supersymmetric standard model

    A. Djouadi, U. Ellwanger, and A. M. Teixeira, “The Constrained next-to-minimal supersymmetric standard model”, Phys. Rev. Lett. 101 (2008) 101802, arXiv:0803.0253

  37. [37]

    The Constrained NMSSM with a 126 GeV Higgs boson: A global analysis

    K. Kowalska, S. Munir, L. Roszkowski et al., “The Constrained NMSSM with a 125 GeV Higgs boson – A global analysis”, arXiv:1211.1693

  38. [38]

    NMSDECAY: A Fortran Code for Supersymmetric Particle Decays in the Next-to-Minimal Supersymmetric Standard Model

    D. Das, U. Ellwanger, and A. M. Teixeira, “NMSDECAY: A Fortran Code for Supersymmetric Particle Decays in the Next-to-Minimal Supersymmetric Standard Model”, Comput.Phys.Commun. 183 (2012) 774–779, arXiv:1106.5633

  39. [39]

    Minuit: A System for Function Minimization and Analysis of the Parameter Errors and Correlations

    F. James and M. Roos, “Minuit: A System for Function Minimization and Analysis of the Parameter Errors and Correlations”, Comput.Phys.Commun. 10 (1975) 343–367

  40. [40]

    Option MODSEL 8 2 in NMSSMTools

  41. [41]

    On the radiative corrections to the neutral Higgs boson masses in the NMSSM

    G. Degrassi and P. Slavich, “On the radiative corrections to the neutral Higgs boson masses in the NMSSM”, Nucl.Phys. B825 (2010) 119–150, arXiv:0907.4682

  42. [42]

    The electroweak sector of the NMSSM at the one-loop level

    F. Staub, W. Porod, and B. Herrmann, “The Electroweak sector of the NMSSM at the one-loop level”, JHEP 1010 (2010) 040, arXiv:1007.4049. 13 Appendix A: Higgs and neutralino mixing matrix in the NMSSM The neutral components from the two Higgs doublets and singlet mix to form three physical CP-even scalar ( S) bosons and two physical CP-odd pseudo-scalar (P...

  43. [43]

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