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arxiv: 2605.20015 · v1 · pith:3RHWXH5Gnew · submitted 2026-05-19 · ✦ hep-ex

Search for soft unclustered energy patterns containing muons in the final state in pp collisions at sqrt{s} = 13 TeV with the ATLAS detector

Pith reviewed 2026-05-20 03:59 UTC · model grok-4.3

classification ✦ hep-ex
keywords soft unclustered energy patternsSUEPhidden sectorHidden Valleymuon final statemediatorexclusion limitsATLAS
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The pith

ATLAS observes no significant excess of soft unclustered energy patterns containing muons and sets exclusion limits on hidden-sector mediators.

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

The paper searches for soft unclustered energy patterns, known as SUEPs, which are high-multiplicity isotropic sprays of low-momentum particles that could arise in hidden sector theories beyond the Standard Model. It focuses on cases where these patterns include muons in the final state and uses 140 fb^{-1} of 13 TeV proton-proton collision data collected by the ATLAS detector. The search targets production of a scalar mediator through gluon-gluon fusion in Hidden Valley scenarios. No more events are seen than expected from known Standard Model processes. This allows the experiment to place upper limits on the rate of such mediator production and decay into SUEPs at various mediator masses.

Core claim

No significant excess over the Standard Model expectation is observed. Exclusion limits are set on the product of the mediator production cross section and the branching fraction for its decay into a SUEP, down to 0.05 fb for a mediator mass of m_S = 750 GeV, 0.4 fb for m_S = 400 GeV, and 70 fb for m_S = 125 GeV; the last value, when identifying the mediator with the Standard Model Higgs boson, translates to an upper limit on the branching fraction of around 0.2%.

What carries the argument

The SUEP signature in Hidden Valley models, consisting of high-multiplicity isotropic distributions of low-momentum particles including muons, used to probe possible decays of a scalar mediator produced via gluon-gluon fusion.

If this is right

  • Mediator cross section times branching fraction to SUEPs is excluded below 0.05 fb at 750 GeV mass.
  • The corresponding exclusion is 0.4 fb at 400 GeV and 70 fb at 125 GeV.
  • If the mediator is identified with the Higgs boson, its branching fraction to SUEPs is limited to roughly 0.2%.
  • These bounds constrain the parameter space of strongly-coupled hidden sector models that produce isotropic particle sprays.

Where Pith is reading between the lines

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

  • Extending the analysis to other final states such as electrons or photons could cover additional hidden sector decay modes.
  • Higher integrated luminosity at future LHC runs would allow tighter limits on lower-mass or lower-rate mediators.
  • The isotropic high-multiplicity signature may overlap with other beyond-Standard-Model phenomena such as dark showers or emerging jets.

Load-bearing premise

The signal is modeled using gluon-gluon fusion production of a scalar mediator in Hidden Valley scenarios with accurate simulation of SUEP decay products including muons, and that all relevant Standard Model backgrounds are correctly estimated without unaccounted contributions.

What would settle it

A statistically significant excess in the number or distribution of high-multiplicity isotropic muon events above the predicted Standard Model backgrounds would indicate the presence of SUEPs from a hidden sector mediator.

read the original abstract

Soft unclustered energy patterns (SUEPs) refer to high-multiplicity, isotropic distributions of low-momentum particles that could arise in strongly-coupled hidden sector theories. A search for SUEPs whose decay products contain muons in the final state is presented using 140 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV collected by the ATLAS detector at the Large Hadron Collider during 2015-2018. The analysis targets SUEP signatures via gluon-gluon fusion production of a scalar mediator in Hidden Valley scenarios. No significant excess over the Standard Model expectation is observed. Exclusion limits are set on the product of the mediator production cross section and the branching fraction for its decay into a SUEP, down to 0.05 fb for a mediator mass of $m_S$ = 750 GeV, 0.4 fb for $m_S$ = 400 GeV, and 70 fb for $m_S$ = 125 GeV; the last value, when identifying the mediator with the Standard Model Higgs boson, translates to an upper limit on the branching fraction of around 0.2%.

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

2 major / 2 minor

Summary. The manuscript presents a search for soft unclustered energy patterns (SUEPs) containing muons in the final state using 140 fb^{-1} of ATLAS pp collision data at √s = 13 TeV. The analysis targets gluon-gluon fusion production of a scalar mediator in Hidden Valley scenarios. No significant excess over the Standard Model expectation is observed. Exclusion limits are set on the product of the mediator production cross section and the branching fraction to SUEP, reaching 0.05 fb at m_S = 750 GeV, 0.4 fb at 400 GeV, and 70 fb at 125 GeV (corresponding to an upper limit of ~0.2% on the branching fraction if the mediator is identified with the SM Higgs boson).

Significance. If the background modeling and efficiency corrections hold, the result constrains Hidden Valley models with muon-containing SUEP decays across a range of mediator masses. The limits are derived from standard ATLAS null-result procedures on a large dataset and provide new coverage for an exotic high-multiplicity isotropic signature. The translation of the lowest-mass limit into a Higgs branching-fraction bound is a useful cross-check against existing invisible-decay constraints.

major comments (2)
  1. [Section 5.2] Section 5.2 (Background estimation): The signal region is defined by high particle multiplicity, low p_T, isotropy, and the presence of muons. The paper relies on Monte Carlo simulation for the dominant QCD multi-jet, V+jets, and heavy-flavor backgrounds. A quantitative assessment of possible mismodeling of muon production correlations with the soft unclustered topology (e.g., from hadronization or pile-up) is needed, as any residual bias would directly shift the observed limits (0.05 fb, 0.4 fb, 70 fb).
  2. [Section 6.1] Section 6.1 (Limit extraction): The reported limits assume that all relevant SM backgrounds are correctly estimated without unaccounted contributions in the muon-enriched isotropic region. The manuscript should include a dedicated study of the impact of varying the background normalization or shape within the uncertainties on the final exclusion contours.
minor comments (2)
  1. [Figure 3] Figure 3: The caption should explicitly state the integrated luminosity and the exact definition of the SUEP selection variables used in the plot.
  2. [Table 1] Table 1: The efficiency values for the muon identification and isolation requirements should be listed separately from the overall acceptance.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments on the background estimation and limit extraction sections. We address each point below and have incorporated additional material in the revised version to strengthen the presentation of these aspects.

read point-by-point responses
  1. Referee: [Section 5.2] Section 5.2 (Background estimation): The signal region is defined by high particle multiplicity, low p_T, isotropy, and the presence of muons. The paper relies on Monte Carlo simulation for the dominant QCD multi-jet, V+jets, and heavy-flavor backgrounds. A quantitative assessment of possible mismodeling of muon production correlations with the soft unclustered topology (e.g., from hadronization or pile-up) is needed, as any residual bias would directly shift the observed limits (0.05 fb, 0.4 fb, 70 fb).

    Authors: We agree that a quantitative assessment of potential mismodeling of muon production correlations with the soft unclustered topology is important to include. The current manuscript validates the Monte Carlo predictions in several control regions that share key features with the signal region, including muon-enriched samples and regions with varying multiplicity. To directly address the referee's concern, the revised manuscript will add an explicit study in Section 5.2 in which we vary hadronization and pile-up modeling parameters relevant to muon production and evaluate the resulting shifts in background yields within the signal region. The impact of these variations on the extracted limits will also be quantified. revision: yes

  2. Referee: [Section 6.1] Section 6.1 (Limit extraction): The reported limits assume that all relevant SM backgrounds are correctly estimated without unaccounted contributions in the muon-enriched isotropic region. The manuscript should include a dedicated study of the impact of varying the background normalization or shape within the uncertainties on the final exclusion contours.

    Authors: The limit extraction employs a profile likelihood fit in which background normalization and shape uncertainties are incorporated as nuisance parameters and profiled together with the signal strength. To provide the dedicated study requested, the revised Section 6.1 will include explicit variations of the background normalizations and shapes within their assigned uncertainties, with the resulting changes to the exclusion contours shown in additional figures or tables. This will illustrate the robustness of the reported limits (0.05 fb at 750 GeV, 0.4 fb at 400 GeV, and 70 fb at 125 GeV) against such variations. revision: yes

Circularity Check

0 steps flagged

No circularity: experimental search sets data-driven limits without self-referential reductions

full rationale

The paper is a standard ATLAS experimental search for an exotic signature in 140 fb^{-1} of 13 TeV data. Signal is modeled via gluon-gluon fusion in Hidden Valley scenarios with full detector simulation; backgrounds are estimated from Monte Carlo or control regions. The central result (no excess, exclusion limits on mediator cross-section times branching fraction) follows directly from comparing observed yields in the signal region to predicted SM expectations. No equation in the analysis defines a quantity in terms of itself, renames a fit as a prediction, or relies on a self-citation chain for a uniqueness theorem. The derivation is self-contained against external benchmarks (detector calibration, SM cross-sections, and validated MC generators) and does not reduce to its own inputs by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 1 invented entities

The search relies on standard assumptions about detector performance and background modeling plus a postulated signal model for the hidden sector.

axioms (2)
  • domain assumption Standard Model processes and detector response are accurately modeled by Monte Carlo simulations for background estimation.
    Used to predict expected event yields in the absence of new physics.
  • domain assumption Muon identification and reconstruction efficiencies are well known from control samples.
    Critical for signal acceptance and background rejection in the muon final state.
invented entities (1)
  • Scalar mediator in Hidden Valley scenario no independent evidence
    purpose: Produced via gluon-gluon fusion and decaying to SUEP
    New particle postulated to generate the target signature in hidden sector theories.

pith-pipeline@v0.9.0 · 5750 in / 1301 out tokens · 35629 ms · 2026-05-20T03:59:55.771112+00:00 · methodology

discussion (0)

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