000593305 001__ 593305
000593305 005__ 20250724132157.0
000593305 0247_ $$2doi$$a10.1016/j.physletb.2023.137963
000593305 0247_ $$2INSPIRETeX$$aATLAS:2023tkt
000593305 0247_ $$2inspire$$ainspire:2626403
000593305 0247_ $$2ISSN$$a0031-9163
000593305 0247_ $$2ISSN$$a0370-2693
000593305 0247_ $$2ISSN$$a1873-2445
000593305 0247_ $$2arXiv$$aarXiv:2301.10731
000593305 0247_ $$2datacite_doi$$a10.3204/PUBDB-2023-05379
000593305 0247_ $$2altmetric$$aaltmetric:149753192
000593305 0247_ $$2WOS$$aWOS:001023908100001
000593305 0247_ $$2openalex$$aopenalex:W4377020023
000593305 037__ $$aPUBDB-2023-05379
000593305 041__ $$aEnglish
000593305 082__ $$a530
000593305 088__ $$2arXiv$$aarXiv:2301.10731
000593305 088__ $$2CERN$$aCERN-EP-2022-289
000593305 1001_ $$0P:(DE-HGF)0$$aATLAS Collaboration$$b0$$eCollaboration author
000593305 245__ $$aCombination of searches for invisible decays of the Higgs boson using 139 fb$^{−1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV collected with the ATLAS experiment
000593305 260__ $$aAmsterdam$$bNorth-Holland Publ.$$c2023
000593305 3367_ $$2DRIVER$$aarticle
000593305 3367_ $$2DataCite$$aOutput Types/Journal article
000593305 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1693474859_3213507
000593305 3367_ $$2BibTeX$$aARTICLE
000593305 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000593305 3367_ $$00$$2EndNote$$aJournal Article
000593305 500__ $$aPhys. Lett. B 842 (2023) 137963. All figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2021-05
000593305 520__ $$aMany extensions of the Standard Model predict the production of dark matter particles at the LHC. Sufficiently light dark matter particles may be produced in decays of the Higgs boson that would appear invisible to the detector. This Letter presents a statistical combination of searches for $H →$ invisible decays where multiple production modes of the Standard Model Higgs boson are considered. These searches are performed with the ATLAS detector using 139 fb$^{−1}$ of proton–proton collisions at a centre–of–mass energy of Image 1 at the LHC. In combination with the results at Image 2 and Image 3, an upper limit on the $H →$ invisible branching ratio of 0.107 (0.077) at the 95% confidence level is observed (expected). These results are also interpreted in the context of models where the 125 GeV Higgs boson acts as a portal to dark matter, and limits are set on the scattering cross-section of weakly interacting massive particles and nucleons.
000593305 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0
000593305 588__ $$aDataset connected to CrossRef, INSPIRE, Journals: bib-pubdb1.desy.de
000593305 650_7 $$2INSPIRE$$ap p: scattering
000593305 650_7 $$2INSPIRE$$ap p: colliding beams
000593305 650_7 $$2INSPIRE$$aHiggs particle: hadroproduction
000593305 650_7 $$2INSPIRE$$adark matter: pair production
000593305 650_7 $$2INSPIRE$$aHiggs particle: invisible decay
000593305 650_7 $$2INSPIRE$$aHiggs particle: decay modes
000593305 650_7 $$2INSPIRE$$aCERN LHC Coll
000593305 650_7 $$2INSPIRE$$aATLAS
000593305 650_7 $$2INSPIRE$$aHiggs particle: branching ratio
000593305 650_7 $$2INSPIRE$$abranching ratio: upper limit
000593305 650_7 $$2INSPIRE$$aWIMP nucleon: scattering
000593305 650_7 $$2INSPIRE$$aWIMP nucleon: cross section
000593305 650_7 $$2INSPIRE$$achannel cross section: upper limit
000593305 650_7 $$2INSPIRE$$amultiple production
000593305 650_7 $$2INSPIRE$$aWIMP: dark matter
000593305 650_7 $$2INSPIRE$$aWIMP: mass
000593305 650_7 $$2INSPIRE$$astatistical
000593305 650_7 $$2INSPIRE$$aexperimental results
000593305 650_7 $$2INSPIRE$$a7000 GeV-cms
000593305 650_7 $$2INSPIRE$$a8000 GeV-cms
000593305 650_7 $$2INSPIRE$$a13000 GeV-cms
000593305 693__ $$0EXP:(DE-H253)LHC-Exp-ATLAS-20150101$$1EXP:(DE-588)4398783-7$$5EXP:(DE-H253)LHC-Exp-ATLAS-20150101$$aLHC$$eLHC: ATLAS$$x0
000593305 773__ $$0PERI:(DE-600)1466612-1$$a10.1016/j.physletb.2023.137963$$gVol. 842, p. 137963 -$$p137963 $$tPhysics letters / B$$v842$$x0031-9163$$y2023
000593305 7870_ $$0PUBDB-2023-04754$$aATLAS Collaboration$$d2023$$iIsParent$$rarXiv:2301.10731 ; CERN-EP-2022-289$$tCombination of searches for invisible decays of the Higgs boson using 139 fb−1 of proton-proton collision data at s=13 TeV collected with the ATLAS experiment
000593305 8564_ $$uhttps://bib-pubdb1.desy.de/record/593305/files/1-s2.0-S0370269323002976-main.pdf$$yOpenAccess
000593305 8564_ $$uhttps://bib-pubdb1.desy.de/record/593305/files/1-s2.0-S0370269323002976-main.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000593305 909CO $$ooai:bib-pubdb1.desy.de:593305$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000593305 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-HGF)0$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000593305 9131_ $$0G:(DE-HGF)POF4-611$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vFundamental Particles and Forces$$x0
000593305 9141_ $$y2023
000593305 915__ $$0StatID:(DE-HGF)0160$$2StatID$$aDBCoverage$$bEssential Science Indicators$$d2022-11-09
000593305 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000593305 915__ $$0StatID:(DE-HGF)0501$$2StatID$$aDBCoverage$$bDOAJ Seal$$d2022-09-05T14:12:53Z
000593305 915__ $$0StatID:(DE-HGF)0500$$2StatID$$aDBCoverage$$bDOAJ$$d2022-09-05T14:12:53Z
000593305 915__ $$0StatID:(DE-HGF)0113$$2StatID$$aWoS$$bScience Citation Index Expanded$$d2022-11-09
000593305 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000593305 915__ $$0StatID:(DE-HGF)0571$$2StatID$$aDBCoverage$$bSCOAP3 sponsored Journal$$d2022-11-09
000593305 915__ $$0StatID:(DE-HGF)0570$$2StatID$$aSCOAP3
000593305 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz$$d2023-08-25$$wger
000593305 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bPHYS LETT B : 2022$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bDOAJ : Peer review$$d2022-09-05T14:12:53Z
000593305 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences$$d2023-08-25
000593305 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5$$d2023-08-25
000593305 9201_ $$0I:(DE-H253)ATLAS-20120731$$kATLAS$$lLHC/ATLAS Experiment$$x0
000593305 980__ $$ajournal
000593305 980__ $$aVDB
000593305 980__ $$aUNRESTRICTED
000593305 980__ $$aI:(DE-H253)ATLAS-20120731
000593305 9801_ $$aFullTexts