Recognition: unknown
Double SM-like Higgs Production at future e^+ e^- colliders in the 3-Higgs Doublet Model under the S₃ symmetry
Pith reviewed 2026-05-08 02:51 UTC · model grok-4.3
The pith
In the S3-symmetric three-Higgs-doublet model, double SM-like Higgs production cross sections at future e+e- colliders can differ from the Standard Model by orders of magnitude.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors find that, in the S3-symmetric three-Higgs-doublet model without CP violation, after scanning the numerically allowed parameter space consistent with theoretical and experimental bounds, the double SM-like Higgs production rates in the hhZ and hhνν channels at future e+e- colliders can deviate from SM predictions by up to a few orders of magnitude, indicating that measurable signals of this beyond-Standard-Model scenario are possible.
What carries the argument
The S3-symmetric three-Higgs-doublet model, which reduces the number of free parameters in the Higgs potential via the discrete S3 symmetry and allows for a SM-like lightest Higgs while generating large contributions to double Higgs production from the additional scalars.
If this is right
- The e+e- → hhZ channel can show significantly enhanced cross sections, potentially observable with lower integrated luminosity.
- The e+e- → hhν_e ν̄_e channel similarly allows for large deviations from SM expectations.
- These deviations persist across the viable parameter space, making the processes sensitive probes of the model.
- Precision studies at future colliders could either discover or further constrain the S3-3H scenario.
Where Pith is reading between the lines
- Observing such deviations would suggest the presence of additional Higgs doublets arranged under S3 symmetry rather than other BSM frameworks.
- Non-observation would tighten bounds on the trilinear Higgs couplings in multi-doublet models.
- The analysis could be extended to include CP-violating phases or other collider energies to broaden the testable range.
- Connections to other observables like triple Higgs production might reveal correlated signatures.
Load-bearing premise
The lightest CP-even Higgs is assumed to be exactly SM-like, and the chosen scan points are taken to represent the full range of allowed deviations after constraints.
What would settle it
Precise measurement of the cross section for e+e- → hhZ at 500 GeV that agrees with the Standard Model within 10-20% accuracy would exclude the regions of the S3-3H parameter space that predict large enhancements.
Figures
read the original abstract
In this paper, we present the production of double SM-like Higgs $ (h) $ at the future electron positron colliders within the context of $ S_{3} $ model with three Higgs doublets (S3-3H) and no CP violation to describe beyond the Standard Model Higgs Physics. We focus first on the numerically allowed parameter space of the model, taking into account theoretical bounds from perturbative unitarity and vacuum stability, as well as by data at the Large Hadron Collider (LHC) and the Tevatron. The double Higgs production in the S3-3H model can deviate from the SM predictions up to a few orders of magnitude in both the $ e^+e^- \rightarrow hhZ $ and the $ e^+ e^- \rightarrow h h\nu_{e} \bar{\nu}_{e}$ channels. Thus, our findings indicate that the S3-3H model can lead to measurable deviations from the SM predictions of Higgs production at future $ e^+ e^- $ colliders. These results highlight the importance of studies at such colliders for searching physics beyond the Standard Model.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper investigates double production of the SM-like Higgs boson in the S3-symmetric three-Higgs-doublet model (S3-3H) at future electron-positron colliders. After scanning the parameter space subject to perturbative unitarity, vacuum stability, and LHC/Tevatron constraints with the lightest CP-even Higgs being SM-like, the authors find that the cross sections for e+e− → hhZ and e+e− → hhνeν̄e can deviate from Standard Model predictions by up to several orders of magnitude.
Significance. If the reported large deviations are representative of the allowed parameter space, this work would demonstrate that the S3-3H model offers testable predictions for enhanced double Higgs production at future colliders such as the ILC, providing a potential avenue to distinguish this BSM scenario from the SM.
major comments (1)
- [Numerical scan and results (Section 4)] The manuscript identifies specific points in the allowed parameter space where the cross-section ratios reach O(10–1000), but does not report the fraction of scanned points exhibiting such enhancements, nor any distribution or density measure of the cross-section ratios across the viable region. This omission leaves open whether the large deviations are generic or confined to isolated, finely tuned points, directly impacting the strength of the claim that the model 'can lead to measurable deviations'.
minor comments (2)
- [Abstract] The abstract states that deviations occur 'up to a few orders of magnitude' but gives no quantitative details on the scan implementation, number of points sampled, or how LHC/Tevatron bounds are imposed after the theoretical constraints; a brief clarification would strengthen the presentation.
- [Model description (Section 2)] Notation for the additional Higgs doublets (e.g., their vevs and mixing angles) is introduced but could be summarized in a single table early in the model section for easier reference when reading the production cross-section formulas.
Simulated Author's Rebuttal
We thank the referee for the constructive feedback and positive overall assessment of our manuscript. We address the major comment below and will incorporate the suggested improvements in the revised version.
read point-by-point responses
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Referee: [Numerical scan and results (Section 4)] The manuscript identifies specific points in the allowed parameter space where the cross-section ratios reach O(10–1000), but does not report the fraction of scanned points exhibiting such enhancements, nor any distribution or density measure of the cross-section ratios across the viable region. This omission leaves open whether the large deviations are generic or confined to isolated, finely tuned points, directly impacting the strength of the claim that the model 'can lead to measurable deviations'.
Authors: We agree that including quantitative information on the distribution of the cross-section ratios would strengthen the presentation and better contextualize the benchmark points. Our numerical scan was designed to delineate the viable parameter space after imposing all theoretical and experimental constraints, with the selected points chosen to demonstrate the maximum possible deviations within that space. To address the referee's concern, in the revised manuscript we will add a new figure (or subsection) in Section 4 displaying the histogram of the ratio σ_{S3-3H}/σ_{SM} for both the hhZ and hhνν channels over the full set of viable points, together with the fraction of points exhibiting enhancements above thresholds such as 10, 100, and 1000. This will clarify the prevalence of large deviations without altering the core claim that the model can produce measurable effects. revision: yes
Circularity Check
No significant circularity; standard external-constraint scan followed by forward prediction
full rationale
The paper first restricts the S3-3H parameter space using perturbative unitarity, vacuum stability, and external LHC/Tevatron data that force the lightest CP-even Higgs couplings to be SM-like. It then computes the e+e− → hhZ and hhνν cross sections from the surviving points. This workflow does not reduce any prediction to its inputs by construction: the double-Higgs rates depend on trilinear couplings that remain free after the single-Higgs constraints are applied. No self-definitional equations, no fitted quantities renamed as predictions, and no load-bearing self-citations appear in the derivation. The representativeness of the chosen scan points is a separate statistical-coverage question, not a circularity issue.
Axiom & Free-Parameter Ledger
free parameters (1)
- Higgs potential couplings and vacuum expectation values
axioms (3)
- domain assumption S3 symmetry governs the Higgs sector
- domain assumption No CP violation
- domain assumption Lightest CP-even Higgs is SM-like
invented entities (1)
-
Two additional Higgs doublets
no independent evidence
Reference graph
Works this paper leans on
-
[1]
[11, 40–42] and can be defined as 10 e+ e− Z h, H h h Z (a) e+ e− Z A2 h Z h (b) e+ e− Z Z h h (c) e+ e− Z h h Z (d) FIG
Double Higgs-Strahlung The differential cross section for the process (e+e− →hhZ) is taken from Refs. [11, 40–42] and can be defined as 10 e+ e− Z h, H h h Z (a) e+ e− Z A2 h Z h (b) e+ e− Z Z h h (c) e+ e− Z h h Z (d) FIG. 3. Feynman diagrams fore +e− →hhZproduction. dσ(e+e− →hhZ) dx1dx2 = G3 F m6 Z 384 √ 2π3s V 2 e +A 2 e A (1−r Z)2 ,(17) wherex 1,2 = 2...
-
[2]
Following Refs
Double Higgs from Vector Boson Fusion The double Higgs production processe +e− →hhν e¯νe is determined within the effective Wboson approximation. Following Refs. [11, 41, 42], the total cross section can be written 13 -10 -5 0 5 10 0.0 0.2 0.4 0.6 0.8 κhhh σ(e+e-->hhZ) ( fb) √s = 500 GeV -10 -5 0 5 10 9.4 9.6 9.8 10.0 10.2 κhhh σ(e+e-->hhZ) ( fb) √s = 100...
-
[3]
G. Aad et al. [ATLAS Collaboration], Phys. Lett. B716, 1 (2012) [arXiv:1207.7214 [hep-ex]]
work page internal anchor Pith review arXiv 2012
-
[4]
Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC
S. Chatrchyan et al. [CMS Collaboration], Phys. Lett. B716, 30 (2012) [arXiv:1207.7235 [hep-ex]]. 19
work page Pith review arXiv 2012
-
[5]
M. G´ omez-Bock, M. Mondrag´ on and A. P´ erez-Mart´ ınez, Eur. Phys. J. C81(2021) 942 [arXiv:2102.02800 [hep-ph]]
- [6]
- [7]
-
[8]
E. Barradas-Guevara, O. F´ elix-Beltr´ an and E. Rodr´ ıguez-J´ auregui, Phys. Rev. D90, (2014) 095001 [arXiv:1402.2244 [hep-ph]]
-
[9]
E. Barradas-Guevara, O. F´ elix-Beltr´ an and E. Rodr´ ıguez-J´ auregui, [arXiv:1507.05180 [hep- ph]]
-
[10]
D. Emmanuel-Costa, O. M. Ogreid, P. Osland and M. N. Rebelo, JHEP02, (2016), 154 [arXiv:1601.04654 [hep-ph]]
- [11]
-
[12]
A. Kunˇ cinas, P. Osland, O. M. Ogreid, M.N. Rebelo, Phys. Rev. D101, (2020) 075052 [arXiv:2001.01994 [hep-ph]]
- [13]
- [14]
- [15]
-
[16]
D. Domenech, M. J. Herrero, R. A. Morales and M. Ramos, Phys. Rev. D106, (2022) 115027 [arXiv:2208.05452 [hep-ph]]
- [17]
- [18]
- [19]
-
[20]
D. Lopez-Val and J. Sola, Phys. Rev. D81, 033003 (2010) [arXiv:0908.2898 [hep-ph]]
-
[21]
E. Asakawa, D. Harada, S. Kanemura, Y. Okada and K. Tsumura, Phys. Rev. D82, 115002 (2010) [arXiv:1009.4670 [hep-ph]]
- [22]
- [23]
- [24]
- [25]
- [26]
-
[27]
S. Antusch, E. Cazzato and O. Fischer, JHEP1604, 189 (2016) [arXiv:1512.06035 [hep-ph]]
-
[28]
S. Kanemura, K. Kaneta, N. Machida, S. Odori and T. Shindou, Phys. Rev. D94, 015028 (2016) [arXiv:1603.05588 [hep-ph]]
- [29]
-
[30]
S. De Curtis, S. Moretti, K. Yagyu and E. Yildirim, Phys. Rev. D95, 095026 (2017) [arXiv:1702.07260 [hep-ph]]
- [31]
- [32]
- [33]
-
[34]
D. Barducci, S. De Curtis, S. Moretti and G. M. Pruna, JHEP02, (2014) 005 [arXiv:1311.3305 [hep-ph]]
-
[35]
A. Vasquez, C. Degrande, A. Tonero and R. Rosenfeld, JHEP05(2019), 020 [arXiv:1901.05979 [hep-ph]]
-
[36]
S. Luki´ c et al., Eur. Phys. J. C77(2017) 475 [arXiv:1610.00628 [hep-ex]]
-
[37]
HiggsBounds: Confronting Arbitrary Higgs Sectors with Exclusion Bounds from LEP and the Tevatron
P. Bechtle, O. Brein, S. Heinemeyer, G. Weiglein and K. E. Williams, Comput. Phys. Commun. 181, (2010) 138-167 [arXiv:0811.4169 [hep-ph]]
work page Pith review arXiv 2010
-
[38]
P. Bechtle, O. Brein, S. Heinemeyer, G. Weiglein and K. E. Williams, Comput. Phys. Commun. 182, (2011) 2605-2631 [arXiv:1102.1898 [hep-ph]]
work page Pith review arXiv 2011
-
[39]
P. Bechtle, O. Brein, S. Heinemeyer, O. St˚ al, T. Stefaniak, G. Weiglein and K. E. Williams, Eur. Phys. J. C74, (2014) 2693 [arXiv:1311.0055 [hep-ph]]
work page Pith review arXiv 2014
-
[40]
P. Bechtle, O. Brein, S. Heinemeyer, O. Stal, T. Stefaniak, G. Weiglein and K. Williams, PoS CHARGED2012(2012) 024 [arXiv:1301.2345 [hep-ph]]
-
[41]
P. Bechtle, S. Heinemeyer, O. St˚ al, T. Stefaniak and G. Weiglein, Eur. Phys. J. C74, (2014) 2711 [arXiv:1305.1933 [hep-ph]]
-
[42]
A. Djouadi, H. E. Haber and P. M. Zerwas, Phys. Lett. B375, (1996) 203-212 [arXiv:hep- ph/9602234 [hep-ph]]
-
[43]
P. Osland and P. N. Pandita, Phys. Rev. D59, (1999) 055013 [arXiv:hep-ph/9806351 [hep- 21 ph]]
-
[44]
A. Djouadi, W. Kilian, M. Muhlleitner and P. M. Zerwas, Eur. Phys. J. C10, (1999) 27-43 [arXiv:hep-ph/9903229 [hep-ph]]
-
[45]
Brau et al
J. Brau et al. ILC-REPORT-2007-001, AAI-PUB-2007-002, BNL-79150-2007, CERN-2007- 006, CHEP-A07-001, CLNS-07-1991, COCKCROFT-07-04, DESY-07-046, FERMILAB-TM- 2382, JAI-2007-001, JINR-E9-2007-039, JLAB-R-2007-01, KEK-REPORT-2007-2, LBNL- 62867, LNF-07-9-NT, SLAC-R-857
2007
-
[46]
J. Brau et al. [ILC Collaboration], arXiv:0712.1950 [physics.acc-ph]
-
[47]
Physics and Detectors at CLIC: CLIC Conceptual Design Report
L. Linssen, A. Miyamoto, M. Stanitzki, and H. Weerts, CERN-2012-003 , ANL-HEP-TR- 12-01 , DESY-12-008 , KEK-Report-2011-7, [physics.ins-det/1202.5940]
work page Pith review arXiv 2012
-
[48]
E. Accomando et al. (CLIC PhysicsWorking Group), CERN-2004-005, [hep-ph/0412251]
discussion (0)
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