001     599325
005     20231204212022.0
024 7 _ |a ATLAS:2023scm
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024 7 _ |a inspire:2696558
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024 7 _ |a 10.3204/PUBDB-2023-07321
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037 _ _ |a PUBDB-2023-07321
041 _ _ |a English
088 _ _ |a ATLAS-CONF-2023-041
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100 1 _ |a ATLAS Collaboration
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245 _ _ |a Search for narrow low-mass resonances in the four-muon final state with the ATLAS detector at the LHC
260 _ _ |c 2023
300 _ _ |a 21
336 7 _ |a report
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336 7 _ |a REPORT
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336 7 _ |a Report
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336 7 _ |a Output Types/Report
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336 7 _ |a Report
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336 7 _ |a TECHREPORT
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500 _ _ |a Preliminary results. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2023-041. The authors list may be incomplete!
520 _ _ |a A search for new low-mass resonances in the four-muon final state in the four-muon invariant mass range from $10-50$~GeV is performed using $pp$ collision data recorded with the ATLAS detector at the Large Hadron Collider. The data correspond to an integrated luminosity of 20.3 fb$^{-1}$ at a centre-of-mass energy ($\sqrt{s}$) of 8T eV collected in 2012, and 51.5 fb$^{-1}$ and 58.5 fb$^{-1}$ collected at $\sqrt{s}=13$ TeV in 2015--2017 and 2018, respectively. An excess at 18 GeV in the invariant mass spectrum of the four-muon system of the selected $\Upsilon(1\mathrm{S})+\mu^+\mu^-\to\mu^+\mu^-\,\mu^+\mu^-$ final state is observed in the 8 TeV data. Although not blinded, typical selection criteria are used and variations studied to explore the stability of the excess, resulting in local significances of the excess of between be $3.6\,\sigma$ and $6.3\,\sigma$ corresponding to global significances of $1.9\,\sigma$ to $5.4\,\sigma$. A baseline choice of selection cuts defined for the analysis at 8~TeV was defined in the 8~TeV data to be further probed at Run 2. Subsequent analysis of 13 TeV data finds a smaller excess at the same four-muon invariant mass with a significance of $1.9\,\sigma$ in early 13~TeV data runs, while data collected with more restrictive trigger selections in the 2018 dataset finds no evidence of a signal. LHCb and CMS have observed no excess at this mass. Signal MC and di-$\Upsilon(1\mathrm{S})$ production studies in data are used to quantify performance across the three data-taking periods, finding reductions in expected sensitivity in the 13 TeV dataset compared to that at 8 TeV. The lack of observation of a signal in the 13 TeV is assessed to be in tension with the structure observed at an invariant mass of 18 GeV in the 8 TeV dataset, up to a maximum of $2.7\sigma$. We subsequently set and report limits on the total production cross section times branching fraction to a four-muon final state for a new state at a mass of 18 GeV for a variety of models.
536 _ _ |a 611 - Fundamental Particles and Forces (POF4-611)
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588 _ _ |a Dataset connected to INSPIRE
650 _ 7 |a four-muon
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650 _ 7 |a resonance
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650 _ 7 |a Upsilon+mumu
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650 _ 7 |a BPHYS
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693 _ _ |a LHC
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856 4 _ |y OpenAccess
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856 4 _ |y OpenAccess
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910 1 _ |a Deutsches Elektronen-Synchrotron
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913 1 _ |a DE-HGF
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914 1 _ |y 2023
915 _ _ |a OpenAccess
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915 _ _ |a Creative Commons Attribution CC BY 4.0
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920 1 _ |0 I:(DE-H253)ATLAS-20120731
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