SUSY analysis with same-sign leptons in ATLAS Nicole Ruckstuhl, BND-school 2009.

Slides:



Advertisements
Similar presentations
R-parity conserving SUSY studies with jets and E T Miss Alexander Richards, UCL 1.
Advertisements

Searches for the Third Generation: SUSY with b-jets in ATLAS Searches for the Third Generation: SUSY with b-jets in ATLAS Monica D’Onofrio University of.
Dark Matter Masaki Asano (Tohoku U.) Collaborators: Keisuke Fujii (KEK) Katsumasa Ikematsu (KEK) Rei Sasaki (Tohoku U.) Taikan Suehara (ICEPP, U. of Tokyo)
Joe Sato (Saitama University ) Collaborators Satoru Kaneko,Takashi Shimomura, Masato Yamanaka,Oscar Vives Physical review D 78, (2008) arXiv:1002.????
Flavor and Dark Matter Zackaria Chacko University of Maryland, College Park.
Search for Supersymmetry with early LHC data David Stuart, UC, Santa Barbara. May 12, 2010.
Fourth Generation Leptons Linda Carpenter UC Irvine Dec 2010.
Little Higgs Model Dark Matter and Its Implications at the LHC Chuan-Ren Chen (NTNU) KIAS-NCTS Joint Workshop High-1 2/9 – 2/15 In collaboration.
Little Higgs Dark Matter and Its Implications at the LHC Chuan-Ren Chen (NTNU) XS 2014, 5/6/2014 In collaboration with H-C Tsai, M-C Lee, [hep-ph]
Relic Density at the LHC B. Dutta In Collaboration With: R. Arnowitt, A. Gurrola, T. Kamon, A. Krislock, D.Toback Phys.Lett.B639:46,2006, hep-ph/
Discovering Gluinos at Hadron Colliders SLAC Theory Group Jay Wacker December 5, 2008 In collaboration with: M. Lisanti, J. Alwall, M. Le.
1 Rutherford Appleton Laboratory The 13th Annual International Conference on Supersymmetry and Unification of the Fundamental Interactions Durham, 2005.
CDF D0 Supersymmetry at the Tevatron R. Demina University of Rochester.
Minimal Supersymmetric Standard Model (MSSM) SM: 28 bosonic d.o.f. & 90 (96) fermionic d.o.f. SUSY: # of fermions = # of bosonsN=1 SUSY: There are no particles.
Dark Matter at the LHC Bhaskar Dutta Texas A&M University
Susy05, Durham 21 st July1 Split SUSY at Colliders Peter Richardson Durham University Work done in collaboration with W. Kilian, T. Plehn and E. Schmidt,
1 the LHC Jet & MET Searches Adam Avakian PY898 - Special Topics in LHC Physics 3/23/2009.
Looking for SUSY Dark Matter with ATLAS The Story of a Lonely Lepton Nadia Davidson Supervisor: Elisabetta Barberio.
June 8, 2007DSU 2007, Minnesota Relic Density at the LHC B. Dutta In Collaboration With: R. Arnowitt, A. Gurrola, T. Kamon, A. Krislock, D. Toback Phys.
July 22 nd, 2005 A.Canepa, SUSY 2005, Durham 1 Search for chargino and neutralino in trilepton final states Anadi Canepa (Purdue University IN, USA) for.
Higgs and SUSY at the LHC Alan Barr on behalf of the ATLAS and CMS collaborations ICHEP-17 Aug 2004, Beijing ATLAS.
6/28/2015S. Stark1 Scan of the supersymmetric parameter space within mSUGRA Luisa Sabrina Stark Schneebeli, IPP ETH Zurich.
Data-based background predictions using forward events Victor Pavlunin and David Stuart University of California Santa Barbara July 10, 2008.
12 May 2004 Alan Barr UK ATLAS Physics SUSY Spin Measurements with ATLAS Alan Barr “What else could it possibly be?” “Don’t be so sure … ” hep-ph/
Tevatron Non-SUSY BSM: Searches for Physics Beyond the SM and MSSM David Stuart University of California, Santa Barbara DIS 2007, Munich April 2007.
What prospects for Supersymmetry at the Large Hadron Collider ? A brief introduction to the techniques with which ATLAS and CMS intend to constrain Supersymmetry.
Lepton Photon Symposium LP01 Searches for New Particles Gail G. Hanson Indiana University.
1Alan Barr PASCOS 09 PASCOS 2009 DESY 9 July 2009 …AT THE LHC DARK MATTER … Alan Barr University of Oxford On behalf of the ATLAS and CMS collaborations.
SUSY Dark Matter Collider – direct – indirect search bridge. Sabine Kraml Laboratoire de Physique Subatomique et de Cosmologie Grenoble, France ● 43. Rencontres.
What is mSUGRA? Physics in Progress, seminar talk, 11 th Feb 2010 Helmut Eberl.
Wednesday, Apr. 23, 2003PHYS 5326, Spring 2003 Jae Yu 1 PHYS 5326 – Lecture #24 Wednesday, Apr. 23, 2003 Dr. Jae Yu Issues with SM picture Introduction.
By Mengqing Wu XXXV Physics in Collision September 15-19, 2015 University of Warwick Dark matter searches with the ATLAS detector.
1 Supersymmetry Yasuhiro Okada (KEK) January 14, 2005, at KEK.
Inclusive analysis of supersymmetry in EGRET-point with one-lepton events: pp → 1ℓ + 4j + E Tmiss + Х V.A. Bednyakov, S.N. Karpov, E.V. Khramov and A.F.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
ATLAS Dan Tovey 1 Measurement of the LSP Mass Dan Tovey University of Sheffield On Behalf of the ATLAS Collaboration.
Latest Physics Results from ALEPH Paolo Azzurri CERN - July 15, 2003.
December 3rd, 2009 Search for Gluinos and Squarks in events with missing transverse momentum DIS 2013: XXI. International workshop on Deep-Inelastic Scattering.
22 December 2006Masters Defense Texas A&M University1 Adam Aurisano In Collaboration with Richard Arnowitt, Bhaskar Dutta, Teruki Kamon, Nikolay Kolev*,
SUSY08 Seoul 17 June 081 Daniel Teyssier RWTH Aachen University Searches for non-standard SUSY signatures in CMS on behalf of the CMS collaboration.
Feasibility of Detecting Leptoquarks With the CDF Detector Althea Moorhead Mentor: Darin Acosta.
SUSY Studies with ATLAS Experiment 2006 Texas Section of the APS Joint Fall Meeting October 5-7, 2006 Arlington, Texas Nurcan Ozturk University of Texas.
Latest New Phenomena Results from Alexey Popov (IHEP, Protvino) For the DO Collaboration ITEP, Moscow
The Search For Supersymmetry Liam Malone and Matthew French.
Dave Toback Texas A&M University HCP 2004 June 17 th Run II Searches for Supersymmetry Dave Toback Texas A&M University June 17 th 2004 HCP2004.
SEARCH FOR AN INVISIBLE HIGGS IN tth EVENTS T.L.Cheng, G.Kilvington, R.Goncalo Motivation The search for the Higgs boson is a window on physics beyond.
Gennaro Corcella 1, Simonetta Gentile 2 1. Laboratori Nazionali di Frascati, INFN 2. Università di Roma, La Sapienza, INFN Z’production at LHC in an extended.
Elba -- June 7, 2006 Collaboration Meeting 1 CDF Melisa Rossi -- Udine University On behalf of the Multilepton Group CDF Collaboration Meeting.
1 Arnold Pompoš, SUSY03, Tucson, Arizona, June 5-10, 2003.
WIN 05, Delphi, Greece, June 2005Filip Moortgat, CERN WIN 05 Inclusive signatures: discovery, fast but not unambiguous Exclusive final states & long term.
Signatures of lepton-jet production at the LHC Eva Halkiadakis (Rutgers University) with Adam Falkowski, Yuri Gershtein (Rutgers University) Josh Ruderman.
M. Frank, K. H., S.K. Rai (arXiv: ) Phys.Rev.D77:015006, 2008 D. Demir, M. Frank, K. H., S.K. Rai, I.Turan ( arXiv: ) Phys.Rev.D78:035013,
SPS5 SUSY STUDIES AT ATLAS Iris Borjanovic Institute of Physics, Belgrade.
DIS2003 A.Tilquin Searches for Physics Beyond the Standard Model at LEP What is the Standard Model Why to go beyond and how Supersymmetry Higgs sector.
880.P20 Winter 2006 Richard Kass 1 Detector Systems momentumenergy A typical detector beam looks something like: BaBar, CDF, STAR, ATLAS, GLAST…… particle.
Elba -- June 7, 2006 Collaboration Meeting 1 CDF Melisa Rossi -- Udine University On behalf of the Multilepton Group CDF Collaboration Meeting.
Research and Study of SUSY 藏京京 1. Summary of Supersymmetry Supersymmetry (SUSY) is a symmetry that relates elementary particles of one spin to another.
Interpreting a CMS lljjP T Excess With the Golden Cascade of the MSSM October 1st, 2014 Journal Club Ben Allanach, Are R. Raklev, and Anders Kvellestad.
Search for Anomalous Production of Multi-lepton Events at CDF Alon Attal Outline  Motivation  R p V SUSY  CDF & lepton detection  Analysis  Results.
Jieun Kim ( CMS Collaboration ) APCTP 2012 LHC Physics Workshop at Korea (Aug. 7-9, 2012) 1.
Fourth Generation Leptons Linda Carpenter April 2011.
SESAPS November 11, B. Scurlock, University of Florida1 Bobby Scurlock Darin Acosta Paolo Bartalini Richard Cavanaugh Alexey Drozdetskiy Guenakh.
1-lepton + Multijets Analysis bRPV interpretation
ATLAS: Missing Transverse Energy in the Search for Supersymmetry
mSUGRA SUSY Searches at the LHC
Searches at LHC for Physics Beyond the Standard Model
SUSY SEARCHES WITH ATLAS
Supersymmetry Searches with the ATLAS Experiment at the LHC
Presentation transcript:

SUSY analysis with same-sign leptons in ATLAS Nicole Ruckstuhl, BND-school 2009

(Minimal) SuperSymmetry 2 Supersymmetry predicts a partner for each SM particle. Interactions involving SUSY particles are the same as SM interactions! SUSY partners have the same charges (EM/color). The couplings have the same strength. Neutral and charged bosiono’s mix into neutralino’s and chargino’s

SUSY Breaking and R-Parity 3 New interactions. Direct mass terms : SUSY particles are heavier than SM partner. The couplings for SM-like interactions involving SUSY particle are unchanged. SUSY particles are always produced in pairs. SUSY particles always decay to another SUSY particle + SM particles The lightest SUSY particle (LSP) is stable. SUSY events will always consist of 2 decay chains.

SUSY signals 4 SUSY signals at the LHC depend on phase space point. Some features are common to “most” points. If χ 0 1 is the LSP, 2 massive particle remain undetected: High Missing E T Sqarks and gluino’s are often the initial particles. They decay to the LSP through sfermions and bosino’s. Long decay chains with many leptons and jets Decay chains more of less independent. Two same-sign leptons possible

SUSY signals 5 High Missing E T At least 2 high energetic jets Exactly 2 same-sign high energy leptons

Backgrounds 6 What SM background can have: high missing E T, at least 2 high energy jets, exactly 2 same sign leptons (no tau’s) SampleSS-leptonsMissing E T jetsX-section (pb) ttnoyes W+jetsnoyes 4.8 · 10 4 tnoyes 43.2 W+bbnoyes 17.9 Z+jetsno yes4.3 · 10 3 Wtnoyes 14.4 WWnoyesno15.5 ZZyesno 1.4 And QCD

Same-Sign Lepton Analysis 7 Possible event Selection: Missing E T > 80 GeV At least two high energy jets (P T > 80 GeV) Exactly two ss-leptons (P T >20 GeV) SampleEvents after selection (200 pb -1 ) SM1.3 ± 0.2 SU12.4 ± 0.4 SU32.7 ± 0.7 SU440.2 ± 4.4 SU61.1 ± 0.2 How to determine the background? Efficiencies are “easy” Fake rates are more complicated

Background estimation method 8 M T =Missing E T + P T leptons + P T jets A SR is the signal region. The background is A SR can be estimated by: A’ SR = (A SB / B SB )B SR

Results 9 DataSignal+BGEsimated BG No SUSY1.3 ± ± 1.1 SU13.7 ± ± 1.2 SU34.0 ± ± 1.1 SU441.5 ± ± 3.2 SU62.4 ± ± 1.2 How sure is this method. Some systematic studies already done, (jet energy scale, jet energy resolution, different generator.) More needs doing: Effect of fake rate. Use some information about correlation.