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Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb^-1 of sqrt(s) = 7 TeV proton-proton collisions

High Energy Physics - Experiment · Submitted 8 Jun 2012

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim No evidence is found for physics beyond the Standard Model.

how it is stated · asserted 1.00 read the record →

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arXiv ID1206.1760 (version 2)
Pith IDFS3OMF7T, Pith's permanent record of this paper and its review
CitationATLAS Collaboration. "Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb^-1 of sqrt(s) = 7 TeV proton-proton collisions." arXiv:1206.1760 (2012). https://pith.science/paper/FS3OMF7T
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,448 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.32 · human participants 0.01 · controlled comparison 0.08 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.88 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

Results are presented of a search for new particles decaying to large numbers of jets in association with missing transverse momentum, using 4.7 fb^-1 of pp collision data at sqrt(s) = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2011. The event selection requires missing transverse momentum, no isolated electrons or muons, and from >=6 to >=9 jets. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of a MSUGRA/CMSSM supersymmetric model, where, for large universal scalar mass m_0, gluino masses smaller than 840 GeV are excluded at the 95% confidence level, extending previously published limits. Within a simplified model containing only a gluino octet and a neutralino, gluino masses smaller than 870 GeV are similarly excluded for neutralino masses below 100 GeV.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Results are presented of a search for new particles decaying to large numbers of jets in association with missing transverse momentum, using 4.7 fb^-1 of pp collision data at sqrt(s) = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2011. contribution 0.92 0.95 0.04 asserted 0.98
s1 The event selection requires missing transverse momentum, no isolated electrons or muons, and from >=6 to >=9 jets. method 1.00 0.89 0.02 asserted 0.99
s2 No evidence is found for physics beyond the Standard Model. result 1.00 0.96 0.92 asserted 1.00
s3 The results are interpreted in the context of a MSUGRA/CMSSM supersymmetric model, where, for large universal scalar mass m_0, gluino masses smaller than 840 GeV are excluded at the 95% confidence level, extending previously published limits. interpretation 0.97 0.89 0.19 asserted 1.00
s4 Within a simplified model containing only a gluino octet and a neutralino, gluino masses smaller than 870 GeV are similarly excluded for neutralino masses below 100 GeV. interpretation 0.68 0.88 0.07 asserted 1.00

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from observation or experiment 0.60.

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not examined
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  • references and citing sentences
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  • C citations
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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

Results are presented of a search for new particles decaying to large numbers of jets in association with missing transverse momentum, using 4.7 fb^-1 of pp collision data at sqrt(s) = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2011. The event selection requires missing transverse momentum, no isolated electrons or muons, and from >=6 to >=9 jets. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of a MSUGRA/CMSSM supersymmetric model, where, for large universal scalar mass m_0, gluino masses smaller than 840 GeV are excluded at the 95% confidence level, extending previously published limits. Within a simplified model containing only a gluino octet and a neutralino, gluino masses smaller than 870 GeV are similarly excluded for neutralino masses below 100 GeV.

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References
How the literature uses it

40 arXiv papers cite this in 64 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 46 sentences without a confident label

Builds on it 1 paper
Uses its method or tool 1 paper
  • In order to apply this analysis, we estimate the efficiency times acceptance in our model in the different signal regions by simulating our signal ($X̃_1^0+ X̃_1^0- j j$ production via the processes defining $σ_1$, followed by $X̃_1^0+ →Z ν̅_e$ with $BR = 1$), and then applying the cuts in [ref] .

    "L=R" -- $U(1)_R$ Lepton Number at the LHC · Topology (1) : $X̃_1^0+ →Z ν̅_e$ · 0.87

Uses its data or values 10 papers
  • To study constraints on such SUSY models, we reinterpret the results of the ATLAS large jet multiplicity plus missing energy search [ref] and the CMS same-sign dilepton with jets plus missing energy search [ref] .

    Can R-parity violation hide vanilla supersymmetry at the LHC? · R-parity violating SUSY signal · 0.80

  • In this case, however, the efficiency times acceptance turns out to be smaller.[From simulation via MG5 $+$ Pythia $+$ Delphes of $X̃^+-_1 X̃^-+_1 j j$ via the processes in the definition of $σ_1$ (see Subsection [ref]).] The strongest constraint arises again from signal region D (tight) in [ref] , and gives an upper bound on our model cross section of about 60 fb.

    "L=R" -- $U(1)_R$ Lepton Number at the LHC · Topology (4) : $X̃_1^+- →W^+ ν_e$ · 0.95

  • The exclusion limits on squark and gluino masses, when they are comparable, are approximately $1.5$ TeV at $95%$ CL with $20$ fb$^-1$ of integrated luminosity [ref] .

    Natural Supersymmetry, Muon $g-2$, and the Last Crevices for the Top Squark · LHC bounds: · 0.87

Cites it as support 1 paper
Cites it as background 3 papers

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