Search for the direct production of charginos and neutralinos in final states with tau leptons in √s = 13 TeV pp collisions with the ATLAS detector
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Published version
Author(s)
Type
Journal Article
Abstract
A 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 13 TeV. No significant
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 τ˜L 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 τ˜L mass between the masses of the χ˜
±
1 and
the χ˜
0
1 .
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 13 TeV. No significant
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 τ˜L 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 τ˜L mass between the masses of the χ˜
±
1 and
the χ˜
0
1 .
Date Issued
2018-02-22
Date Acceptance
2018-01-24
Citation
European Physical Journal C: Particles and Fields, 2018, 78 (2)
ISSN
1434-6044
Publisher
Springer Verlag (Germany)
Journal / Book Title
European Physical Journal C: Particles and Fields
Volume
78
Issue
2
Copyright Statement
© CERN for the benefit of the ATLAS collaboration 2018. This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.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.
Identifier
http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000426403300001&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=1ba7043ffcc86c417c072aa74d649202
Subjects
Science & Technology
Physical Sciences
Physics, Particles & Fields
Physics
DYNAMICAL SUPERSYMMETRY BREAKING
HADRON COLLIDERS
PARTON DISTRIBUTIONS
MEASURING MASSES
ENERGY
PARTICLE
EXTENSION
LHC
MODEL
DECAY
Publication Status
Published
Article Number
ARTN 154