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dc.date.accessioned2020-05-19T19:47:02Z
dc.date.available2020-05-19T19:47:02Z
dc.date.created2020-01-13T08:55:17Z
dc.date.issued2019
dc.identifier.citationAad, Georges Abbott, Brad Abbott, Dale C. Abdinov, Ovsat Bahram oglu Abed Abud, Adam Abeling, Kira Abhayasinghe, Deshan Kavishka Abidi, Syed Haider AbouZeid, Hass Abraham, Nadine L. Bjørke, Kristian Bugge, Magnar Kopangen Cameron, David Gordon Catmore, James Richard Feigl, Simon Garonne, Vincent Gramstad, Eirik Hellesund, Simen Morisbak, Vanja Oppen, Henrik Ould-Saada, Farid Pedersen, Maiken Read, Alexander Lincoln Rye, Eli Bæverfjord Røhne, Ole Myren Sandaker, Heidi Vadla, Knut Oddvar Høie Buanes, Trygve Djuvsland, Julia Isabell Eigen, Gerald Fomin, Nikolai Lee, Graham Richard Lipniacka, Anna Martin dit Latour, Bertrand Mæland, Steffen Stugu, Bjarne Træet, Are Sivertsen Abramowicz, Halina Abreu, Henso Abulaiti, Yiming Acharya, Bobby S. Achkar, Baida Adachi, Shunsuke Adam, Lennart Adam-Bourdarios, Claire Adamczyk, Leszek Adamek, Lukas Adelman, Jareed Adersberger, Michael Adigüzel, Aytül ATLAS, Collaboration . Search for bottom-squark pair production with the ATLAS detector in final states containing Higgs bosons, b-jets and missing transverse momentum. Journal of High Energy Physics (JHEP). 2019, 2019:60(12), 1-50
dc.identifier.urihttp://hdl.handle.net/10852/75986
dc.description.abstractThe result of a search for the pair production of the lightest supersymmetric partner of the bottom quark (˜b1) using 139 fb−1 of proton-proton data collected at √ s = 13 TeV by the ATLAS detector is reported. In the supersymmetric scenarios considered both of the bottom-squarks decay into a b-quark and the second-lightest neutralino, ˜b1 → b + ˜χ 0 2 . Each ˜χ 0 2 is assumed to subsequently decay with 100% branching ratio into a Higgs boson (h) like the one in the Standard Model and the lightest neutralino: ˜χ 0 2 → h + ˜χ 0 1 . The ˜χ 0 1 is assumed to be the lightest supersymmetric particle (LSP) and is stable. Two signal mass configurations are targeted: the first has a constant LSP mass of 60 GeV; and the second has a constant mass difference between the ˜χ 0 2 and ˜χ 0 1 of 130 GeV. The final states considered contain no charged leptons, three or more b-jets, and large missing transverse momentum. No significant excess of events over the Standard Model background expectation is observed in any of the signal regions considered. Limits at the 95% confidence level are placed in the supersymmetric models considered, and bottom-squarks with mass up to 1.5 TeV are excluded.en_US
dc.languageEN
dc.rightsAttribution 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.titleSearch for bottom-squark pair production with the ATLAS detector in final states containing Higgs bosons, b-jets and missing transverse momentumen_US
dc.typeJournal articleen_US
dc.creator.authorAad, Georges
dc.creator.authorAbbott, Brad
dc.creator.authorAbbott, Dale C.
dc.creator.authorAbdinov, Ovsat Bahram oglu
dc.creator.authorAbed Abud, Adam
dc.creator.authorAbeling, Kira
dc.creator.authorAbhayasinghe, Deshan Kavishka
dc.creator.authorAbidi, Syed Haider
dc.creator.authorAbouZeid, Hass
dc.creator.authorAbraham, Nadine L.
dc.creator.authorBjørke, Kristian
dc.creator.authorBugge, Magnar Kopangen
dc.creator.authorCameron, David Gordon
dc.creator.authorCatmore, James Richard
dc.creator.authorFeigl, Simon
dc.creator.authorGaronne, Vincent
dc.creator.authorGramstad, Eirik
dc.creator.authorHellesund, Simen
dc.creator.authorMorisbak, Vanja
dc.creator.authorOppen, Henrik
dc.creator.authorOuld-Saada, Farid
dc.creator.authorPedersen, Maiken
dc.creator.authorRead, Alexander Lincoln
dc.creator.authorRye, Eli Bæverfjord
dc.creator.authorRøhne, Ole Myren
dc.creator.authorSandaker, Heidi
dc.creator.authorVadla, Knut Oddvar Høie
dc.creator.authorBuanes, Trygve
dc.creator.authorDjuvsland, Julia Isabell
dc.creator.authorEigen, Gerald
dc.creator.authorFomin, Nikolai
dc.creator.authorLee, Graham Richard
dc.creator.authorLipniacka, Anna
dc.creator.authorMartin dit Latour, Bertrand
dc.creator.authorMæland, Steffen
dc.creator.authorStugu, Bjarne
dc.creator.authorTræet, Are Sivertsen
dc.creator.authorAbramowicz, Halina
dc.creator.authorAbreu, Henso
dc.creator.authorAbulaiti, Yiming
dc.creator.authorAcharya, Bobby S.
dc.creator.authorAchkar, Baida
dc.creator.authorAdachi, Shunsuke
dc.creator.authorAdam, Lennart
dc.creator.authorAdam-Bourdarios, Claire
dc.creator.authorAdamczyk, Leszek
dc.creator.authorAdamek, Lukas
dc.creator.authorAdelman, Jareed
dc.creator.authorAdersberger, Michael
dc.creator.authorAdigüzel, Aytül
dc.creator.authorATLAS, Collaboration
cristin.unitcode185,15,4,60
cristin.unitnameHøyenergifysikk
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2
dc.identifier.cristin1771014
dc.identifier.bibliographiccitationinfo:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Journal of High Energy Physics (JHEP)&rft.volume=2019:60&rft.spage=1&rft.date=2019
dc.identifier.jtitleJournal of High Energy Physics (JHEP)
dc.identifier.volume2019
dc.identifier.issue12
dc.identifier.doihttps://doi.org/10.1007/JHEP12(2019)060
dc.identifier.urnURN:NBN:no-79061
dc.subject.nviVDP::Kjerne- og elementærpartikkelfysikk: 431
dc.type.documentTidsskriftartikkelen_US
dc.type.peerreviewedPeer reviewed
dc.source.issn1126-6708
dc.identifier.fulltextFulltext https://www.duo.uio.no/bitstream/handle/10852/75986/1/Aad2019_Article_SearchForBottom-squarkPairProd.pdf
dc.type.versionPublishedVersion
cristin.articleid60
dc.relation.projectNFR/255182


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