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dc.date.accessioned2015-11-10T13:07:39Z
dc.date.available2015-11-10T13:07:39Z
dc.date.created2015-09-21T14:31:33Z
dc.date.issued2015
dc.identifier.citationAad, Georges Abbott, Brad Abdallah, Jalal Abdel Khalek, Samah Abdinov, Ovsat Bahram oglu Aben, Rosemarie Abi, Babak Abolins, Maris AbouZeid, Hass Abramowicz, Halina Buanes, Trygve Dale, Ørjan Eigen, Gerald Kastanas, Alex Liebig, Wolfgang Lipniacka, Anna Martin dit Latour, Bertrand Rosendahl, Peter Lundgaard Sandaker, Heidi Sjursen, Therese B. Smestad, Lillian Stugu, Bjarne Ugland, Maren Bugge, Lars Cameron, David Gordon Catmore, James Richard Czyczula, Zofia Franconi, Laura Gjelsten, Børge Kile Gramstad, Eirik Morisbak, Vanja Ould-Saada, Farid Pajchel, Katarina Pedersen, Maiken Read, Alexander Lincoln Røhne, Ole Myren Stapnes, Steinar Strandlie, Are Abreu, Henso Abreu, Rômulo F. Abulaiti, Yiming Acharya, Bobby S. Adamczyk, Leszek Adams, David Adelman, Jareed Adomeit, Stefanie Adye, Tim Agatonovic-Jovin, Tatjana Aguilar Saavedra, Juan Antonio Agustoni, Marco ATLAS, Collaboration . Searches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at √s = 8 Tev. Journal of High Energy Physics (JHEP). 2015, 2015(1)
dc.identifier.urihttp://hdl.handle.net/10852/47671
dc.description.abstractSearches for heavy long-lived charged particles are performed using a data sample of 19.1 fb−1 from proton-proton collisions at a centre-of-mass energy of √s = 8 Tev collected by the ATLAS detector at the Large Hadron Collider. No excess is observed above the estimated background and limits are placed on the mass of long-lived particles in various supersymmetric models. Long-lived tau sleptons in models with gauge-mediated symmetry breaking are excluded up to masses between 440 and 385 GeV for tan β between 10 and 50, with a 290 GeV limit in the case where only direct tau slepton production is considered. In the context of simplified LeptoSUSY models, where sleptons are stable and have a mass of 300 GeV, squark and gluino masses are excluded up to a mass of 1500 and 1360 GeV, respectively. Directly produced charginos, in simplified models where they are nearly degenerate to the lightest neutralino, are excluded up to a mass of 620 GeV. R-hadrons, composites containing a gluino, bottom squark or top squark, are excluded up to a mass of 1270, 845 and 900 GeV, respectively, using the full detector; and up to a mass of 1260, 835 and 870 GeV using an approach disregarding information from the muon spectrometer.en_US
dc.languageEN
dc.language.isoenen_US
dc.publisherInstitute of Physics Publishing (IOPP)
dc.rightsAttribution 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.titleSearches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at √s = 8 Teven_US
dc.typeJournal articleen_US
dc.creator.authorAad, Georges
dc.creator.authorAbbott, Brad
dc.creator.authorAbdallah, Jalal
dc.creator.authorAbdel Khalek, Samah
dc.creator.authorAbdinov, Ovsat Bahram oglu
dc.creator.authorAben, Rosemarie
dc.creator.authorAbi, Babak
dc.creator.authorAbolins, Maris
dc.creator.authorAbouZeid, Hass
dc.creator.authorAbramowicz, Halina
dc.creator.authorBuanes, Trygve
dc.creator.authorDale, Ørjan
dc.creator.authorEigen, Gerald
dc.creator.authorKastanas, Alex
dc.creator.authorLiebig, Wolfgang
dc.creator.authorLipniacka, Anna
dc.creator.authorMartin dit Latour, Bertrand
dc.creator.authorRosendahl, Peter Lundgaard
dc.creator.authorSandaker, Heidi
dc.creator.authorSjursen, Therese B.
dc.creator.authorSmestad, Lillian
dc.creator.authorStugu, Bjarne
dc.creator.authorUgland, Maren
dc.creator.authorBugge, Lars
dc.creator.authorCameron, David Gordon
dc.creator.authorCatmore, James Richard
dc.creator.authorCzyczula, Zofia
dc.creator.authorFranconi, Laura
dc.creator.authorGjelsten, Børge Kile
dc.creator.authorGramstad, Eirik
dc.creator.authorMorisbak, Vanja
dc.creator.authorOuld-Saada, Farid
dc.creator.authorPajchel, Katarina
dc.creator.authorPedersen, Maiken
dc.creator.authorRead, Alexander Lincoln
dc.creator.authorRøhne, Ole Myren
dc.creator.authorStapnes, Steinar
dc.creator.authorStrandlie, Are
dc.creator.authorAbreu, Henso
dc.creator.authorAbreu, Rômulo F.
dc.creator.authorAbulaiti, Yiming
dc.creator.authorAcharya, Bobby S.
dc.creator.authorAdamczyk, Leszek
dc.creator.authorAdams, David
dc.creator.authorAdelman, Jareed
dc.creator.authorAdomeit, Stefanie
dc.creator.authorAdye, Tim
dc.creator.authorAgatonovic-Jovin, Tatjana
dc.creator.authorAguilar Saavedra, Juan Antonio
dc.creator.authorAgustoni, Marco
dc.creator.authorATLAS, Collaboration
cristin.unitcode185,15,4,60
cristin.unitnameHøyenergifysikk
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2
dc.identifier.cristin1266122
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=2015&rft.spage=&rft.date=2015
dc.identifier.jtitleJournal of High Energy Physics (JHEP)
dc.identifier.volume2015
dc.identifier.doihttp://dx.doi.org/10.1007/JHEP01(2015)068
dc.identifier.urnURN:NBN:no-51717
dc.subject.nviVDP::Kjerne- og elementærpartikkelfysikk: 431
dc.type.documentTidsskriftartikkelen_US
dc.type.peerreviewedPeer reviewed
dc.source.issn1029-8479
dc.identifier.fulltextFulltext https://www.duo.uio.no/bitstream/handle/10852/47671/2/10.1007%2FJHEP01%282015%29068.pdf
dc.type.versionPublishedVersion
cristin.articleid68


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