Journal
JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 9, Pages -Publisher
SPRINGER
DOI: 10.1007/JHEP09(2017)084
Keywords
Hadron-Hadron scattering (experiments); Supersymmetry
Categories
Funding
- ARRS, Slovenia
- MSSR, Slovakia
- ANPCyT, Argentina
- BMWFW, Austria
- Fondation Partager le Savoir, France
- ARC, Australia
- ANAS, Azerbaijan
- DNRF, Denmark
- AvH Foundation, Germany
- FWF, Austria
- VSC CR, Czech Republic
- DFG, Germany
- CNPq, Brazil
- Herakleitos programme - EU-ESF
- SSTC, Belarus
- NSERC, Canada
- FAPESP, Brazil
- Thales programme - EU-ESF
- MIZS, Slovenia
- DST/NRF, South Africa
- MSMT CR, Czech Republic
- Investissements d'Avenir Labex and Idex, France
- MINECO, Spain
- MPO CR, Czech Republic
- Wallenberg Foundation, Sweden
- Region Auvergne, France
- YerPhI, Armenia
- SRC, Sweden
- ANR, France
- GSRT, Greece
- BRF, Norway
- CONICYT, Chile
- MPG, Germany
- SERI, Switzerland
- Minerva, Israel
- MOST, China
- Canton of Bern, Switzerland
- Generalitat Valenciana, Spain
- CAS, China
- SNSF, Switzerland
- CERCA Programme Generalitat de Catalunya, Spain
- COLCIENCIAS, Colombia
- MOST, Taiwan
- Leverhulme Trust, United Kingdom
- NSFC, China
- Canton of Geneva, Switzerland
- Royal Society, United Kingdom
- STFC, United Kingdom
- TAEK, Turkey
- DNSRC, Denmark
- IN2P3-CNRS, France
- NRC, Canada
- SRNSF, Georgia
- Greek NSRF
- CEA-DSM/IRFU, France
- Aristeia programme - EU-ESF
- CERN
- HGF, Germany
- GIF, Israel
- CFI, Canada
- BMBF, Germany
- BSF, Israel
- NSF, United States of America
- DOE, United States of America
- CNRST, Morocco
- JSPS, Japan
- Ontario Innovation Trust, Canada
- Canada Council, Canada
- BCKDF, Canada
- Hong Kong SAR, China
- RGC, China
- ISF, Israel
- Benoziyo Center, Israel
- I-CORE, Israel
- MEXT, Japan
- INFN, Italy
- NWO, Netherlands
- FQRNT, Canada
- MESTD, Serbia
- Compute Canada, Canada
- ERC, European Union
- EPLANET, European Union
- FP7, European Union
- ERDF, European Union
- Marie Sklodowska-Curie Actions, European Union
- Horizon, European Union
- MNiSW, Poland
- RCN, Norway
- FCT, Portugal
- NON, Poland
- MES of Russia, Russian Federation
- MNE/IFA, Romania
- JINR
- CRC, Canada
- NRC KI, Russian Federation
- CANARIE, Canada
- STFC [ST/N000331/1, ST/N000307/1, 1653101, ST/I005846/1, ST/L006162/1, ST/M006417/1, PP/E000452/1, ST/K003666/1, ST/H001158/2, ST/P002439/1, ST/K001361/1, ST/N000277/1, ST/N000234/1, ST/H001158/1, ST/N000447/1, ST/M001431/1, ST/L005662/1, ST/L001144/1] Funding Source: UKRI
- Division Of Physics
- Direct For Mathematical & Physical Scien [1624739] Funding Source: National Science Foundation
- Grants-in-Aid for Scientific Research [17K14268, 16H06489] Funding Source: KAKEN
- Science and Technology Facilities Council [ST/M001431/1, ST/H001158/1, ST/K001361/1, 1366825, ST/I005846/1, ST/N000234/1, ST/M006417/1, PP/E000452/1, ST/H001158/2, ST/N000277/1, ATLAS, ST/K003666/1, 1653101, GRIDPP, ST/L001144/1, ST/N000331/1, 1659192, ST/L005662/1] Funding Source: researchfish
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A search for strongly produced supersymmetric particles using signatures involving multiple energetic jets and either two isolated same-sign leptons (e or mu), or at least three isolated leptons, is presented. The analysis relies on the identification of b-jets and high missing transverse momentum to achieve good sensitivity. A data sample of proton-proton collisions at root s = 13 TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016, corresponding to a total integrated luminosity of 36.1 fb(-1), is used for the search. No significant excess over the Standard Model prediction is observed. The results are interpreted in several simplified supersymmetric models featuring R-parity conservation or R-parity violation, extending the exclusion limits from previous searches. In models considering gluino pair production, gluino masses are excluded up to 1.87 TeV at 95% confidence level. When bottom squarks are pair-produced and decay to a chargino and a top quark, models with bottom squark masses below 700 GeV and light neutralinos are excluded at 95% confidence level. In addition, model-independent limits are set on a possible contribution of new phenomena to the signal region yields.
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