Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/114869
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dc.contributor.authorAaboud, M.-
dc.contributor.authorAad, G.-
dc.contributor.authorAbbott, B.-
dc.contributor.authorAbdinov, O.-
dc.contributor.authorAbeloos, B.-
dc.contributor.authorAbidi, S.-
dc.contributor.authorAbouZeid, O.-
dc.contributor.authorAbraham, N.-
dc.contributor.authorAbramowicz, H.-
dc.contributor.authorAbreu, H.-
dc.contributor.authorAbreu, R.-
dc.contributor.authorAbulaiti, Y.-
dc.contributor.authorAcharya, B.-
dc.contributor.authorAdachi, S.-
dc.contributor.authorAdamczyk, L.-
dc.contributor.authorAdelman, J.-
dc.contributor.authorAdersberger, M.-
dc.contributor.authorAdye, T.-
dc.contributor.authorAffolder, A.-
dc.contributor.authorAfik, Y.-
dc.contributor.authoret al.-
dc.date.issued2018-
dc.identifier.citationEuropean Physical Journal C: Particles and Fields, 2018; 78(2):154-1-154-33-
dc.identifier.issn1434-6044-
dc.identifier.issn1434-6052-
dc.identifier.urihttp://hdl.handle.net/2440/114869-
dc.description.abstractA search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ˜χ + 1 ˜χ − 1 pair production and of ˜χ ± 1 ˜χ 0 2 and ˜χ + 1 ˜χ − 1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the ˜ τL state is set to be halfway between the masses of the ˜χ ± 1 and the ˜χ 0 1 .Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ˜χ + 1 ˜χ − 1 for a massless ˜χ 0 1 . Common ˜χ ± 1 and ˜χ 0 2 masses up to 760 GeV are excluded in the case of production of ˜χ ± 1 ˜χ 0 2 and ˜χ + 1 ˜χ − 1 assuming a massless ˜χ 0 1 . Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the ˜χ ± 1 and the ˜χ 0 1 are also studied by varying the ˜ τL mass between the masses of the ˜χ ± 1 and the ˜χ 0 1 .-
dc.description.statementofresponsibilityM. Aaboud, G. Aad … Damir Duvnjak … Paul D. Jackson … Andreas Petridis … Martin White … et al.-
dc.language.isoen-
dc.publisherSpringer-
dc.rights© CERN for the benefit of the ATLAS collaboration 2018. This article is an open access publication. This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecomm ons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. Funded by SCOAP3.-
dc.source.urihttp://dx.doi.org/10.1140/epjc/s10052-018-5583-9-
dc.subjectATLAS Collaboration-
dc.titleSearch for the direct production of charginos and neutralinos in final states with tau leptons in √s=13TeV pp collisions with the ATLAS detector-
dc.title.alternativeSearch for the direct production of charginos and neutralinos in final states with tau leptons in root s=13TeV pp collisions with the ATLAS detector-
dc.typeJournal article-
dc.identifier.doi10.1140/epjc/s10052-018-5583-9-
pubs.publication-statusPublished-
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