REVIEW 1 major objections 1 cited by
BSMArt 2: simpler and faster parameter space scans
T0 review · 1 major / 0 minor · reviewed 2026-06-28 · grok-4.3
Pith's one-line read An updated parameter scanning tool adds CMA-ES and other algorithms that make it easier to find diverse testable points in new physics models.
desk verdict BSMArt 2 adds a few standard scanners to an existing tool but gives no numbers to back the 'simpler and faster' claim. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The covariance matrix adaptation evolution strategy algorithm variants, used to optimize searches through the parameter space of new physics models.
What would settle it
Performing side-by-side tests on a benchmark new physics model, measuring the time to find a set number of distinct viable points and the variety of those points using both the new algorithms and conventional scanning techniques.
Extended reading notes
Core claim
The updated tool incorporates new algorithms including Affine Monte Carlo, Contour Finding, machine learning scanners, deep learning scanners, and covariance matrix adaptation evolution strategy methods. Two variants of the evolution strategy scans are used to identify diverse parameter points in models relevant to soft lepton excesses at the collider, showing that such points can be found readily.
Load-bearing premise
The newly added scanning algorithms deliver gains in speed, diversity of found points, or coverage compared to previous approaches.
Editorial extensions
If this is right
- The new methods allow efficient location of parameter points that could explain observed anomalies in collider data.
- Architectural changes make the tool easier to install and use with added examples.
- Multiple scanning options give users choices suited to different exploration tasks.
- Demonstrations with lepton excess models illustrate practical applications in high-energy physics.
Reading between the lines
- These scanning improvements might enable broader exploration of model spaces that were previously too computationally intensive.
- The techniques could apply to parameter searches in other areas of particle physics beyond collider anomalies.
- Combining the tool with automated model generation systems might accelerate the full cycle from model building to testing.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents BSMArt 2, an updated lightweight scanning tool for BSM parameter spaces that includes architectural improvements, simpler installation, expanded documentation, and new algorithms (Affine MC, Contour Finding, MLScanner, DLScanner, MLS, and CMA-ES). It showcases two CMA-ES variants applied to models relevant for soft lepton excesses at the LHC and claims that these make it easily possible to locate diverse and interesting parameter points for future testing.
Significance. A validated tool with demonstrably faster or more efficient scanning algorithms would aid exploration of new physics models by lowering barriers to finding viable parameter points. However, the central claims of simplicity and speed rest on unshown implementation details and lack any quantitative validation, which substantially reduces the assessed significance.
major comments (1)
- Abstract: the claims that the new algorithms make scans 'simpler and faster' and that 'it is easily possible to find diverse and interesting parameter points' are presented without any acceptance rates, wall-time measurements, parameter-space coverage metrics, diversity measures, or head-to-head comparisons against random sampling, MCMC, or the prior BSMArt version; these data are required to substantiate the central performance assertions.
Simulated Author's Rebuttal
We thank the referee for the constructive report. We address the major comment below.
read point-by-point responses
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Referee: Abstract: the claims that the new algorithms make scans 'simpler and faster' and that 'it is easily possible to find diverse and interesting parameter points' are presented without any acceptance rates, wall-time measurements, parameter-space coverage metrics, diversity measures, or head-to-head comparisons against random sampling, MCMC, or the prior BSMArt version; these data are required to substantiate the central performance assertions.
Authors: We agree that the abstract asserts performance improvements without the quantitative metrics requested. The manuscript describes the new algorithms and demonstrates their application to soft lepton excess models but does not contain acceptance rates, wall-time data, coverage metrics, or direct comparisons to random sampling, MCMC, or BSMArt 1. We will revise the abstract to remove unsubstantiated claims of simplicity and speed and add a dedicated subsection with benchmark results, including head-to-head comparisons where feasible. revision: yes
Circularity Check
No circularity: tool-description paper with no derivation chain
full rationale
The paper describes a software package (BSMArt 2) and new scanning algorithms (Affine MC, CMA-ES variants, etc.) for exploring BSM parameter spaces. It contains no equations, no fitted parameters, no predictions derived from first principles, and no load-bearing self-citations that close a logical loop. The central claim is an existence demonstration via the tool rather than a mathematical result that reduces to its own inputs. Absence of quantitative benchmarks is a separate evidentiary issue, not circularity.
Assumptions & free parameters
Cite this review
Pith. "Pith review of BSMArt 2: simpler and faster parameter space scans." pith.science (2026). https://pith.science/paper/JN74CYGZ
@misc{pith2026260605410,
author = {Pith},
title = {Pith review of: BSMArt 2: simpler and faster parameter space scans},
year = {2026},
howpublished = {\url{https://pith.science/paper/JN74CYGZ}},
note = {Machine review of arXiv:2606.05410}
}
read the original abstract
We present version 2 of BSMArt, a powerful yet lightweight scanning tool designed to simplify the exploration of parameter spaces of new physics models. Aside from architectural improvements, simpler installation and expanded documentation with examples, the new version includes additional tools and new machine learning and Monte Carlo scanning algorithms: Affine MC, Contour Finding, MLScanner, DLScanner, MLS, and CMA-ES. We showcase two variants of CMA-ES scans with physics applications relevant for soft lepton excesses at the LHC. We demonstrate that it is easily possible to find diverse and interesting parameter points for future testing.
Figures
Figures from the paper (5 more)
Forward citations
Cited by 1 Pith paper
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Dark matter in composite Higgs models with a scotogenic EFT
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Reference graph
Works this paper leans on
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[1]
"USER" when the observable is already a likelihood/ p-value
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[2]
This allows a soft cutoff, to safely handle extreme values
"SIGUSER" to apply a sigmoid function to a user-supplied value. This allows a soft cutoff, to safely handle extreme values
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"EXPUSER" when the supplied value is a log-likelihood so we would need to exponentiate it to obtain a likelihood
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MINUSEXPUSER
"MINUSEXPUSER" when the supplied value is a negative-log-likelihood so we would need to exponentiate the negative of it to obtain a likelihood. • "CFUNCTION" is a special function that gives zero within a specified range, and increases linearly outside of it. This is intended for use with the new CMAES ND scan described in the following sections. 17 In ad...
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[5]
PRIOR": <TYPE> in the variable definition, along with
Priors In general, algorithms such as MCMCs are designed to asymptote to sampling from the posterior distribution. Bayes’ theorem tells us that P (x|D) = P (D|x)π(x) P (D) ≡ P (D|x)π(x) Z , (1) where P (D|x) is the probability of observing data D given variables x, π(x) is the prior probability of variables x, P (D) ↔ Z is the probability of data D, which...
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Setup": {
Contour2D A simple algorithm for finding contours in two dimensions is implemented as a Contour2D scan. It works by first creating a very coarse grid, finding the contour, and then sampling points that lie close to this contour (but not too close to each other). It performs a specified number of iterations. The contour is specified by a function, or a thr...
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Networks
ContourGP An interesting algorithm was proposed in [44] to find contours using Gaussian Pro- cesses (GPs). Since GPs generalise very well from little data, they are excellent interpola- tors; but even better they give a prediction for the uncertainty of each point. Exploiting this, the ContourGP algorithm aims to choose not the points that lie closest to ...
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CMAES_ND
General exploratory scan We first perform a general exploratory scan consisting of 1000 independent runs of "CMAES_ND" working in parallel. A single run by itself often converges quickly to a valid region of the parameter space due to the exploitative and local nature of CMA-ES, albeit 48 covering a limited region of the parameter space. Therefore, a coll...
Show all 100 references
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[9]
Seeded HBOS ND scan From the seeds drawn from the exploratory general scan above, we initialise runs using "HBOS" novelty reward. We further demand the seeds used in this scan to have BR(˜χ0 2 → ˜χ0 1 + ℓ+ + ℓ−) > 0.07 (ℓ being e or µ) as this helps to explain the excesses eve...
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Optimiser
Seeded Optimiser ND scan The possibility for high branching ratios for the second lightest neutralino state de- caying to the LSP+leptons can be further explored. Here we illustrate the functionality of the "Optimiser" novelty detection option, by using it in a seeded scan foc...
2025
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Ranges for the observable constraints considered for the seeded BSMArt pMSSM CMAES-ND scan
Parameters Parameter Interval Parameter Interval M1 [−4, 4] TeV |M ˜L1|2 [0, 16] TeV2 M2 [−4, 4] TeV |M˜e1|2 [0, 16] TeV2 M3 [0, 10] TeV |M ˜L3|2 [0, 16] TeV2 µ [−4, 4] TeV |M˜e3|2 [0, 16] TeV2 At [−7, 7] TeV |M˜q1|2 [0, 16] TeV2 Ab [−7, 7] TeV |M˜u1|2 [0, 16] TeV2 Aτ [−7, 7] ...
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We also remove points excluded by LEP: m ˜χ± 1 < 91.9 GeV for ∆ m(˜χ± 1 , ˜χ0
Constraints Points with masses below 45 GeV are excluded by Z width. We also remove points excluded by LEP: m ˜χ± 1 < 91.9 GeV for ∆ m(˜χ± 1 , ˜χ0
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< 3 GeV and m ˜χ± 1 < 103 GeV for ∆m(˜χ± 1 , ˜χ0
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[14]
Codes": { 3
≥ 3 GeV. 57 Observable Allowed values Scan type mh [122, 128] GeV Both mχ0 2 [200, 400] GeV Seeded m ˜χ0 2 − m ˜χ0 1 [10, 30] GeV Seeded BR(˜χ0 2 → ˜χ0 1 + ℓ+ + ℓ−) > 0.07 Seeded Ωh2 [0.08, 1.14] Both DM DD p-value > 0.1 Both r-value < 1 Both TABLE VII. Ranges for the observab...
- [15]
-
[16]
Staub, SARAH 4 : A tool for (not only SUSY) model builders
F. Staub, SARAH 4 : A tool for (not only SUSY) model builders . Comput. Phys. Commun. 185 (2014) 1773–1790, arXiv:1309.7223 [hep-ph]
2014 arXiv
-
[17]
M. D. Goodsell, K. Nickel, and F. Staub, Two-Loop Higgs mass calculations in supersymmetric models beyond the MSSM with SARAH and SPheno . Eur. Phys. J. C 75 (2015) no. 1, 32, arXiv:1411.0675 [hep-ph]
2015 arXiv
-
[18]
M. D. Goodsell, S. Liebler, and F. Staub, Generic calculation of two-body partial decay widths at the full one-loop level . Eur. Phys. J. C 77 (2017) no. 11, 758, arXiv:1703.09237 [hep-ph]
2017 arXiv
-
[19]
Porod, SPheno, a program for calculating supersymmetric spectra, SUSY particle decays and SUSY particle production at e+ e- colliders
W. Porod, SPheno, a program for calculating supersymmetric spectra, SUSY particle decays and SUSY particle production at e+ e- colliders . Comput. Phys. Commun. 153 (2003) 275–315, arXiv:hep-ph/0301101
2003 arXiv
-
[20]
Porod and F
W. Porod and F. Staub, SPheno 3.1: Extensions including flavour, CP-phases and models beyond the MSSM . Comput. Phys. Commun. 183 (2012) 2458–2469, arXiv:1104.1573 [hep-ph]
2012 arXiv
-
[21]
Athron, J.-h
P. Athron, J.-h. Park, D. St¨ ockinger, and A. Voigt,FlexibleSUSY—A spectrum generator generator for supersymmetric models . Comput. Phys. Commun. 190 (2015) 139–172, arXiv:1406.2319 [hep-ph]
2015 arXiv
-
[22]
Athron, M
P. Athron, M. Bach, D. Harries, T. Kwasnitza, J.-h. Park, D. St¨ ockinger, A. Voigt, and J. Ziebell, FlexibleSUSY 2.0: Extensions to investigate the phenomenology of SUSY and non-SUSY models. Comput. Phys. Commun. 230 (2018) 145–217, arXiv:1710.03760 [hep-ph]
2018 arXiv
-
[23]
Athron, M
P. Athron, M. Bach, D. H. J. Jacob, W. Kotlarski, D. St¨ ockinger, and A. Voigt, Precise calculation of the W boson pole mass beyond the standard model with FlexibleSUSY . Phys. Rev. D 106 (2022) no. 9, 095023, arXiv:2204.05285 [hep-ph]
2022
-
[24]
Kotlarski and A
W. Kotlarski and A. Voigt, From Lagrangian to Higgs physics constraints for SUSY and non-SUSY models: interfacing FlexibleSUSY with HiggsTools and Lilith . 65 arXiv:2603.12119 [hep-ph]
-
[25]
B. C. Allanach, SOFTSUSY: a program for calculating supersymmetric spectra . Comput. Phys. Commun. 143 (2002) 305–331, arXiv:hep-ph/0104145
2002 arXiv
-
[26]
Aad et al., Searches for electroweak production of supersymmetric particles with compressed mass spectra in √s = 13 TeV pp collisions with the ATLAS detector
ATLAS Collaboration, G. Aad et al., Searches for electroweak production of supersymmetric particles with compressed mass spectra in √s = 13 TeV pp collisions with the ATLAS detector. Phys. Rev. D 101 (2020) no. 5, 052005, arXiv:1911.12606 [hep-ex]
2020
-
[27]
Aad et al., Search for chargino–neutralino pair production in final states with three leptons and missing transverse momentum in √s = 13 TeV pp collisions with the ATLAS detector
ATLAS Collaboration, G. Aad et al., Search for chargino–neutralino pair production in final states with three leptons and missing transverse momentum in √s = 13 TeV pp collisions with the ATLAS detector . Eur. Phys. J. C 81 (2021) no. 12, 1118, arXiv:2106.01676 [hep-ex]
2021
-
[28]
Tumasyan et al., Search for supersymmetry in final states with two or three soft leptons and missing transverse momentum in proton-proton collisions at √s = 13 TeV
CMS Collaboration, A. Tumasyan et al., Search for supersymmetry in final states with two or three soft leptons and missing transverse momentum in proton-proton collisions at √s = 13 TeV. JHEP 04 (2022) 091, arXiv:2111.06296 [hep-ex]
2022
-
[29]
Aad et al., Search for new phenomena in events with an energetic jet and missing transverse momentum in pp collisions at √s =13 TeV with the ATLAS detector
ATLAS Collaboration, G. Aad et al., Search for new phenomena in events with an energetic jet and missing transverse momentum in pp collisions at √s =13 TeV with the ATLAS detector. Phys. Rev. D 103 (2021) no. 11, 112006, arXiv:2102.10874 [hep-ex]
2021
-
[30]
Tumasyan et al., Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at √s = 13 TeV
CMS Collaboration, A. Tumasyan et al., Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at √s = 13 TeV. JHEP 11 (2021) 153, arXiv:2107.13021 [hep-ex]
2021
-
[31]
D. Agin, B. Fuks, M. D. Goodsell, and T. Murphy, Monojets reveal overlapping excesses for light compressed higgsinos . Phys. Lett. B 853 (2024) 138597, arXiv:2311.17149 [hep-ph]
2024
-
[32]
D. Agin, B. Fuks, M. D. Goodsell, and T. Murphy, Seeking a coherent explanation of LHC excesses for compressed spectra. Eur. Phys. J. C 84 (2024) no. 11, 1218, arXiv:2404.12423 [hep-ph]
2024
-
[33]
H. Baer, V. Barger, X. Tata, and K. Zhang, Winos from natural SUSY at the high luminosity LHC. Phys. Rev. D 109 (2024) no. 1, 015027, arXiv:2310.10829 [hep-ph] . 66
2024
-
[34]
Chakraborti, S
M. Chakraborti, S. Heinemeyer, and I. Saha, Consistent excesses in the search for ˜χ0 2 ˜χ± 1 : wino/bino vs. Higgsino dark matter . Eur. Phys. J. C 84 (2024) no. 8, 812, arXiv:2403.14759 [hep-ph]
2024
-
[35]
S. P. Martin, Implications of purity constraints on light Higgsinos . Phys. Rev. D 109 (2024) no. 9, 095045, arXiv:2403.19598 [hep-ph]
2024
-
[36]
Constantin, S
L. Constantin, S. Kraml, A. Lessa, T. Reymermier, and W. Waltenberger, On the coverage of electroweak-inos within the pMSSM with SModelS – a comparison with the ATLAS pMSSM study. arXiv:2512.14502 [hep-ph]
-
[37]
Ellwanger, C
U. Ellwanger, C. Hugonie, S. F. King, and S. Moretti, NMSSM explanation for excesses in the search for neutralinos and charginos and a 95 GeV Higgs boson . Eur. Phys. J. C 84 (2024) no. 8, 788, arXiv:2404.19338 [hep-ph]
2024
-
[38]
J. Y. Araz, B. Fuks, M. D. Goodsell, and T. Murphy, Deciphering compressed electroweakino excesses with MadAnalysis 5 . arXiv:2507.08927 [hep-ph]
-
[39]
Bagnaschi, M
E. Bagnaschi, M. Chakraborti, S. Heinemeyer, and I. Saha, Consistent Excesses in the LHC Electroweak SUSY Searches: GUT-based Singlino/Higgsino Interpretation in the NMSSM. arXiv:2512.16783 [hep-ph]
-
[40]
D. Agin, B. Fuks, M. D. Goodsell, and T. Murphy, A joint explanation for the soft lepton and monojet LHC excesses in the wino-bino model . Eur. Phys. J. C 85 (2025) no. 10, 1145, arXiv:2506.21676 [hep-ph]
2025 arXiv
-
[41]
M. D. Goodsell and A. Joury, BSMArt: Simple and fast parameter space scans . Comput. Phys. Commun. 297 (2024) 109057, arXiv:2301.01154 [hep-ph]
2024
-
[42]
A. E. Faraggi and M. D. Goodsell, MW in string derived Z ′ models. Eur. Phys. J. C 84 (2024) no. 6, 589, arXiv:2312.13411 [hep-ph]
2024
-
[43]
GAMBIT Collaboration, G. D. Martinez, J. McKay, B. Farmer, P. Scott, E. Roebber, A. Putze, and J. Conrad, Comparison of statistical sampling methods with ScannerBit, the GAMBIT scanning module . Eur. Phys. J. C 77 (2017) no. 11, 761, arXiv:1705.07959 [hep-ph]
2017
-
[44]
Feroz and M
F. Feroz and M. P. Hobson, Multimodal nested sampling: an efficient and robust alternative to MCMC methods for astronomical data analysis . Mon. Not. Roy. Astron. 67 Soc. 384 (2008) 449, arXiv:0704.3704 [astro-ph]
2008 arXiv
-
[45]
Feroz, M
F. Feroz, M. P. Hobson, and M. Bridges, MultiNest: an efficient and robust Bayesian inference tool for cosmology and particle physics . Mon. Not. Roy. Astron. Soc. 398 (2009) 1601–1614, arXiv:0809.3437 [astro-ph]
2009 arXiv
-
[46]
Feroz, M
F. Feroz, M. P. Hobson, E. Cameron, and A. N. Pettitt, Importance Nested Sampling and the MultiNest Algorithm . Open J. Astrophys. 2 (2019) no. 1, 10, arXiv:1306.2144 [astro-ph.IM]
2019 arXiv
-
[47]
Staub, xBIT: an easy to use scanning tool with machine learning abilities
F. Staub, xBIT: an easy to use scanning tool with machine learning abilities . arXiv preprint arXiv:1906.03277 (2019) , arXiv:1906.03277 [hep-ph] . https://arxiv.org/abs/1906.03277
1906 arXiv
-
[48]
Shang and Y
L. Shang and Y. Zhang, EasyScan HEP: A tool for connecting programs to scan the parameter space of physics models . Comput. Phys. Commun. 296 (2024) 109027, arXiv:2304.03636 [hep-ph]
2024
-
[49]
Hammad, M
A. Hammad, M. Park, R. Ramos, and P. Saha, Exploration of parameter spaces assisted by machine learning . Comput. Phys. Commun. 293 (2023) 108902, arXiv:2207.09959 [hep-ph]
2023
-
[50]
Hammad and R
A. Hammad and R. Ramos, DLScanner: A parameter space scanner package assisted by deep learning methods. Comput. Phys. Commun. 314 (2025) 109659, arXiv:2412.19675 [hep-ph]
2025
-
[51]
M. A. Diaz, S. Dasmahapatra, and S. Moretti, hep-aid: A Python Library for Sample Efficient Parameter Scans in Beyond the Standard Model Phenomenology . arXiv:2412.17675 [hep-ph]
-
[52]
E. Guo, P. Jackson, J. M. Yang, and P. Zhu, Jarvis-HEP: A lightweight Python framework for workflow composition and parameter scans in high-energy physics . arXiv:2604.25557 [hep-ph]
-
[53]
R. Boto, T. N. Dao, F. Egle, K. Elyaouti, M. Gabelmann, M. M¨ uhlleitner, and J. Plotnikov, NMSSMScanner: Efficient Scans in the NMSSM Parameter Space Proof of Concept. arXiv:2604.25009 [hep-ph] . 68
-
[54]
S. S. AbdusSalam et al., Simple and statistically sound recommendations for analysing physical theories. Rept. Prog. Phys. 85 (2022) no. 5, 052201, arXiv:2012.09874 [hep-ph]
2022
-
[55]
M. D. Goodsell and A. Joury, Active learning BSM parameter spaces. Eur. Phys. J. C 83 (2023) no. 4, 268, arXiv:2204.13950 [hep-ph]
2023
-
[56]
M. D. Goodsell and R. Moutafis, How heavy can dark matter be? Constraining colourful unitarity with SARAH . Eur. Phys. J. C 81 (2021) no. 9, 808, arXiv:2012.09022 [hep-ph]
2021
-
[57]
Goodman and J
J. Goodman and J. Weare, Ensemble samplers with affine invariance . Commun. Appl. Math. Comput. Sc. 5 (2010) no. 1, 65–80
2010
-
[58]
Heinrich, G
L. Heinrich, G. Louppe, and K. Cranmer, diana-hep/excursion: Initial Zenodo Release , Nov., 2018. https://doi.org/10.5281/zenodo.1634428
2018 doi
-
[59]
F. A. de Souza, M. Crispim Rom˜ ao, N. F. Castro, M. Nikjoo, and W. Porod, Exploring parameter spaces with artificial intelligence and machine learning black-box optimization algorithms. Phys. Rev. D 107 (2023) no. 3, 035004, arXiv:2206.09223 [hep-ph]
2023
-
[60]
J. C. Rom˜ ao and M. Crispim Rom˜ ao,Combining evolutionary strategies and novelty detection to go beyond the alignment limit of the Z3 3HDM . Phys. Rev. D 109 (2024) no. 9, 095040, arXiv:2402.07661 [hep-ph]
2024
-
[61]
F. A. de Souza, N. F. Castro, M. Crispim Rom˜ ao, and W. Porod, Exploring scotogenic parameter spaces and mapping uncharted dark matter phenomenology with multi-objective search algorithms. JHEP 10 (2025) 116, arXiv:2505.08862 [hep-ph]
2025
-
[62]
F. A. de Souza, R. Boto, M. Crispim Rom˜ ao, P. N. Figueiredo, J. C. Rom˜ ao, and J. P. Silva, Unearthing large pseudoscalar Yukawa couplings with machine learning . JHEP 07 (2025) 268, arXiv:2505.10625 [hep-ph]
2025
-
[63]
F. A. de Souza, R. Boto, M. Crispim Rom˜ ao, P. N. de Figueiredo, and J. C. Rom˜ ao, Machine Learning insights on the Z3 3HDM with Dark Matter . arXiv:2603.00254 [hep-ph]
-
[64]
H. Bahl, T. Biek¨ otter, S. Heinemeyer, C. Li, S. Paasch, G. Weiglein, and J. Wittbrodt, HiggsTools: BSM scalar phenomenology with new versions of HiggsBounds and 69 HiggsSignals. Comput. Phys. Commun. 291 (2023) 108803, arXiv:2210.09332 [hep-ph]
2023
-
[65]
Belanger, F
G. Belanger, F. Boudjema, P. Brun, A. Pukhov, S. Rosier-Lees, P. Salati, and A. Semenov, Indirect search for dark matter with micrOMEGAs2.4 . Comput. Phys. Commun. 182 (2011) 842–856, arXiv:1004.1092 [hep-ph]
2011 arXiv
-
[66]
Alguero, G
G. Alguero, G. Belanger, F. Boudjema, S. Chakraborti, A. Goudelis, S. Kraml, A. Mjallal, and A. Pukhov, micrOMEGAs 6.0: N-component dark matter . Comput. Phys. Commun. 299 (2024) 109133, arXiv:2312.14894 [hep-ph]
2024
-
[67]
J. E. Camargo-Molina, B. O’Leary, W. Porod, and F. Staub, Vevacious: A Tool For Finding The Global Minima Of One-Loop Effective Potentials With Many Scalars . Eur. Phys. J. C 73 (2013) no. 10, 2588, arXiv:1307.1477 [hep-ph]
2013 arXiv
-
[68]
D. M. Straub, flavio: a Python package for flavour and precision phenomenology in the Standard Model and beyond . arXiv:1810.08132 [hep-ph]
-
[69]
Alwall, R
J. Alwall, R. Frederix, S. Frixione, V. Hirschi, F. Maltoni, O. Mattelaer, H. S. Shao, T. Stelzer, P. Torrielli, and M. Zaro, The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations. JHEP 07...
2014 arXiv
-
[70]
Sj¨ ostrand, S
T. Sj¨ ostrand, S. Ask, J. R. Christiansen, R. Corke, N. Desai, P. Ilten, S. Mrenna, S. Prestel, C. O. Rasmussen, and P. Z. Skands, An introduction to PYTHIA 8.2 . Comput. Phys. Commun. 191 (2015) 159–177, arXiv:1410.3012 [hep-ph]
2015 arXiv
-
[71]
Bierlich et al., A comprehensive guide to the physics and usage of PYTHIA 8.3
C. Bierlich et al., A comprehensive guide to the physics and usage of PYTHIA 8.3 . SciPost Phys. Codeb. 2022 (2022) 8, arXiv:2203.11601 [hep-ph]
2022 arXiv
-
[72]
M. D. Goodsell, HackAnalysis 2: A powerful and hackable recasting tool . arXiv:2406.10042 [hep-ph]
-
[73]
Kraml, S
S. Kraml, S. Kulkarni, U. Laa, A. Lessa, W. Magerl, D. Proschofsky-Spindler, and W. Waltenberger, SModelS: a tool for interpreting simplified-model results from the LHC and its application to supersymmetry . Eur. Phys. J. C 74 (2014) 2868, arXiv:1312.4175 [hep-ph]. 70
2014 arXiv
-
[74]
Ambrogi et al., SModelS v1.2: long-lived particles, combination of signal regions, and other novelties
F. Ambrogi et al., SModelS v1.2: long-lived particles, combination of signal regions, and other novelties. Comput. Phys. Commun. 251 (2020) 106848, arXiv:1811.10624 [hep-ph]
2020
-
[75]
Alguero, S
G. Alguero, S. Kraml, and W. Waltenberger, A SModelS interface for pyhf likelihoods . Comput. Phys. Commun. 264 (2021) 107909, arXiv:2009.01809 [hep-ph]
2021
-
[76]
Alguero, J
G. Alguero, J. Heisig, C. K. Khosa, S. Kraml, S. Kulkarni, A. Lessa, H. Reyes-Gonz´ alez, W. Waltenberger, and A. Wongel, Constraining new physics with SModelS version 2 . JHEP 08 (2022) 068, arXiv:2112.00769 [hep-ph]
2022
-
[77]
M. M. Altakach, S. Kraml, A. Lessa, S. Narasimha, T. Pascal, C. Ramos, Y. Villamizar, and W. Waltenberger, SModelS v3: going beyond Z2 topologies. JHEP 11 (2024) 074, arXiv:2409.12942 [hep-ph]
2024
-
[78]
H. Bahl, J. Braathen, M. Gabelmann, and G. Weiglein, anyH3: precise predictions for the trilinear Higgs coupling in the Standard Model and beyond . Eur. Phys. J. C 83 (2023) no. 12, 1156, arXiv:2305.03015 [hep-ph] . [Erratum: Eur.Phys.J.C 84, 498 (2024)]
2023
-
[79]
Precise predictions for trilinear Higgs couplings and Higgs pair production in extended scalar sectors with anyH3 and anyHH,
H. Bahl, J. Braathen, M. Gabelmann, K. Radchenko, and G. Weiglein, “Precise predictions for trilinear Higgs couplings and Higgs pair production in extended scalar sectors with anyH3 and anyHH,” in International Workshop on Future Linear Colliders . 3, 2026. arXiv:2603.28296 [hep-ph]
2026
-
[80]
DESY-26-010
anyH3 and anyHH: precise predictions for trilinear Higgs couplings and double Higgs production in extended scalar sectors . DESY-26-010
-
[81]
Kahlhoefer, A
F. Kahlhoefer, A. M¨ uck, S. Schulte, and P. Tunney,Interference effects in dilepton resonance searches for Z ′ bosons and dark matter mediators . JHEP 03 (2020) 104, arXiv:1912.06374 [hep-ph]
2020
-
[82]
Alvarez, M
E. Alvarez, M. Est´ evez, and R. M. Sand´ a Seoane,Z′-explorer: A simple tool to probe Z ′ models against LHC data . Comput. Phys. Commun. 269 (2021) 108144, arXiv:2005.05194 [hep-ph]
2021
-
[83]
V. M. Lozano, R. M. S. Seoane, and J. Zurita, Z′-explorer 2.0: Reconnoitering the dark matter landscape. Comput. Phys. Commun. 288 (2023) 108729, arXiv:2109.13194 [hep-ph]. 71
2023
-
[84]
B. Fuks, M. Klasen, D. R. Lamprea, and M. Rothering, Precision predictions for electroweak superpartner production at hadron colliders with Resummino . Eur. Phys. J. C 73 (2013) 2480, arXiv:1304.0790 [hep-ph]
2013 arXiv
-
[85]
Conte, B
E. Conte, B. Fuks, and G. Serret, MadAnalysis 5, A User-Friendly Framework for Collider Phenomenology. Comput. Phys. Commun. 184 (2013) 222–256, arXiv:1206.1599 [hep-ph]
2013 arXiv
-
[86]
Conte, B
E. Conte, B. Dumont, B. Fuks, and C. Wymant, Designing and recasting LHC analyses with MadAnalysis 5 . Eur. Phys. J. C 74 (2014) no. 10, 3103, arXiv:1405.3982 [hep-ph]
2014 arXiv
-
[87]
Conte and B
E. Conte and B. Fuks, Confronting new physics theories to LHC data with MADANALYSIS 5. Int. J. Mod. Phys. A 33 (2018) no. 28, 1830027, arXiv:1808.00480 [hep-ph]
2018 arXiv
-
[88]
Pedregosa, G
F. Pedregosa, G. Varoquaux, A. Gramfort, V. Michel, B. Thirion, O. Grisel, M. Blondel, P. Prettenhofer, R. Weiss, V. Dubourg, J. Vanderplas, A. Passos, D. Cournapeau, M. Brucher, M. Perrot, and E. Duchesnay, Scikit-learn: Machine Learning in Python . Journal of Machine Learnin...
2011
-
[89]
Paszke, S
A. Paszke, S. Gross, F. Massa, A. Lerer, J. Bradbury, G. Chanan, T. Killeen, Z. Lin, N. Gimelshein, L. Antiga, et al., Pytorch: An imperative style, high-performance deep learning library. Advances in neural information processing systems 32 (2019)
2019
-
[90]
N. V. Chawla, K. W. Bowyer, L. O. Hall, and W. P. Kegelmeyer, SMOTE: Synthetic Minority Over-sampling Technique. Journal of Artificial Intelligence Research 16 (2002) 321–357
2002
-
[91]
J. Ren, L. Wu, J. M. Yang, and J. Zhao, Exploring supersymmetry with machine learning . Nucl. Phys. B 943 (2019) 114613, arXiv:1708.06615 [hep-ph]
2019 arXiv
-
[92]
Basiouris, M
V. Basiouris, M. Crispim Rom˜ ao, S. F. King, and G. K. Leontaris, Modular family symmetry in fluxed GUTs . Phys. Rev. D 111 (2025) no. 1, 015012, arXiv:2407.06618 [hep-ph]
2025
-
[93]
R. Boto, T. P. Rebelo, J. C. Rom˜ ao, and J. P. Silva, Machine Learning in the 2HDM2S model for Dark Matter . arXiv:2509.01677 [hep-ph] . 72
-
[94]
R. Boto, J. A. C. Matos, J. C. Rom˜ ao, and J. P. Silva, Surveying the complex three Higgs doublet model with Machine Learning . JHEP 03 (2026) 182, arXiv:2510.02445 [hep-ph]
2026
-
[95]
R. Boto, K. Elyaouti, D. Fontes, M. Gon¸ calves, M. M¨ uhlleitner, J. C. Rom˜ ao, R. Santos, and J. P. Silva, Reassessing CP Violation in the C2HDM with Machine Learning . arXiv:2601.15227 [hep-ph]
-
[96]
Adapting arbitrary normal mutation distributions in evolution strategies: The covariance matrix adaptation,
N. Hansen and A. Ostermeier, “Adapting arbitrary normal mutation distributions in evolution strategies: The covariance matrix adaptation,” pp. 312 – 317. 06, 1996
1996
-
[97]
Nomura, M
M. Nomura, M. Shibata, and R. Hamano, cmaes: A Simple yet Practical Python Library for CMA-ES, 2026. arXiv:2402.01373 [cs.NE] , https://arxiv.org/abs/2402.01373
2026
-
[98]
Akimoto, Y
Y. Akimoto, Y. Nagata, I. Ono, and S. Kobayashi, Theoretical foundation for CMA-ES from information geometry perspective. Algorithmica 64 (2012) no. 4, 698–716
2012
-
[99]
rep., CERN, Geneva, 2024
CMS Collaboration, Phenomenological MSSM interpretation of CMS searches in pp collisions at 13 TeV tech. rep., CERN, Geneva, 2024. https://cds.cern.ch/record/2906621
2024
-
[100]
Aad et al., ATLAS Run 2 searches for electroweak production of supersymmetric particles interpreted within the pMSSM
ATLAS Collaboration, G. Aad et al., ATLAS Run 2 searches for electroweak production of supersymmetric particles interpreted within the pMSSM . JHEP 05 (2024) 106, arXiv:2402.01392 [hep-ex]
2024
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