Search for The charge asymmetry in top anti-top resonance Smail BELAAOUJARajaa CHERKAOUI ELMOURSLI Marcel VOS UniversityMohmed V Faculty of sciences Nuclear.

Slides:



Advertisements
Similar presentations
4/29/2004CERN TeV4LHC Meeting Using Charge Asymmetries to measure LHC single top Quark production Matthew T. Bowen University of Washington CERN TeV4LHC.
Advertisements

Quark Compositeness Search with γ +Jet Final State at the LHC Satyaki Bhattacharya, Sushil S. Chauhan, Brajesh Choudhary, Debajyoti Choudhury Department.
Regina Demina, University of Rochester 02/08/2012 Forward-backward asymmetry in top-antitop production in proton-antiproton collisions.
Search for Large Extra Dimensions at the Tevatron Bob Olivier, LPNHE Paris XXXVI ème Rencontre de Moriond Mars Search for Large Extra Dimensions.
26th Rencontres de Blois, Particle Physics and Cosmology, 2014 BSM Higgs Searches at the LHC C. H. Shepherd-Themistocleous PPD, Rutherford Appleton Laboratory.
Jörgen Sjölin Stockholm University LHC experimental sensitivity to CP violating gtt couplings November, 2002 Page 1 Why CP in gtt? Standard model contribution.
Chiral freedom and the scale of weak interactions.
Top Physics at the Tevatron Mike Arov (Louisiana Tech University) for D0 and CDF Collaborations 1.
1/25  s with XD & Kaluza-Klein excitation of gluon at ATLAS Exotic signals at Hadron Colliders 04,Durham Exotic signals at Hadron Colliders 04 Marc Escalier,
Tevatron Non-SUSY BSM: Searches for Physics Beyond the SM and MSSM David Stuart University of California, Santa Barbara DIS 2007, Munich April 2007.
Kaluza-Klein gluon production at the LHC
Gauge Boson-Pair Production in pp Collision at 14 TeV Using ATLAS at the LHC Erez Reinherz-Aronis.
1 A Preliminary Model Independent Study of the Reaction pp  qqWW  qq ℓ qq at CMS  Gianluca CERMINARA (SUMMER STUDENT)  MUON group.
Heavy resonances in the top quark sector: from hadron colliders to the ILC Germán Rodrigo Beijing, March 2010.
DZero experiment in Теватрон последние три года работал на проектной светимости, и за 1 месяц работы набирал интегральную светимость больше чем.
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
Study of the to Dilepton Channel with the Total Transverse Energy Kinematic Variable Athens, April 17 th 2003 Victoria Giakoumopoulou University of Athens,
Discovery Potential of ATLAS for Extended Gauge Symmetries Daisuke Naito (Okayama University, Japan) for the ATLAS Collaboration Nov. 1st, 2006
J/  production in p+p collisions at PHENIX and gluon distribution QWG meeting at FNAL September Hiroki Sato (Kyoto University) for the PHENIX collaboration.
Top quark properties in ATLAS Ruth Laura Sandbach X-SILAFAE-2014, Medellin, Colombia 27/11/2014 X-SILAFAE
PHENO 2008 April 29th Tom Schwarz University of California Davis Measurement of the Forward-Backward Asymmetry In Top Production with 1.9 fb -1.
Liu Minghui Nanjing MC study of W polarization and ttbar spin correlation Liu Minghui, Zhu Chengguang April 27, 2008.
Search for a Z′ boson in the dimuon channel in p-p collisions at √s = 7TeV with CMS experiment at the Large Hadron Collider Search for a Z′ boson in the.
Feasibility of Detecting Leptoquarks With the CDF Detector Althea Moorhead Mentor: Darin Acosta.
CIPANP, June 2012 David Toback, Texas A&M University – CDF Collaboration Top Quark Properties with the Full Run II Dataset 1 October 2011 David Toback,
Moriond EW 2013BSM Higgs Searches at the Tevatron 1 Beyond the SM scalar boson searches in TeVatron Elemér Nagy CPPM on behalf of the CDF and D0 Collaborations.
Alternatives: Beyond SUSY Searches in CMS Dimitri Bourilkov University of Florida For the CMS Collaboration SUSY06, June 2006, Irvine, CA, USA.
Searches for Physics Beyond the Standard Model (Exotica) in pp collisions at 7 TeV at the CMS Experiment Sergei Shmatov Joint Institute for Nuclear Research,
Probing the new physics heavy bosons at LHC In collaboration with Shou-Shan Bao, Xue Gong, Shi-Yuan Li, Zong-Guo Si and Yu-Feng Zhou Hong-Lei Li
Higgs boson pair production in new physics models at hadron, lepton, and photon colliders October Daisuke Harada (KEK) in collaboration.
Charged Higgs boson at the LHC 이강영 ( 건국대학교 연세대학교
Status Of Tevatron Collider Experiments and its Physics 성균관 대학교 물리학과 유인태 유인태 Workshop on Physics at Hadron Colliders KIAS 2005 년 6 월 24 일.
RECENT RESULTS FROM THE TEVATRON AND LHC Suyong Choi Korea University.
October 2011 David Toback, Texas A&M University Research Topics Seminar1 David Toback Texas A&M University For the CDF Collaboration CIPANP, June 2012.
2008/02/22 特定領域「フレーバーの物理の新展開」研究会 CDF での Top Flavor の物理 戸村 友宣 ( 筑波大学 )
03/31/2006S. M. Lietti - UED Search at SPRACE 1 Universal Extra Dimensions Search at SPRACE S. M. Lietti DOSAR Workshop at U.T. Arlington.
Kinematics of Top Decays in the Dilepton and the Lepton + Jets channels: Probing the Top Mass University of Athens - Physics Department Section of Nuclear.
29 August, 2007 Ashfaq Ahmad, Search for Charged Higgs at the LHC 1 Search for Charged Higgs at the LHC Ashfaq Ahmad (Stony Brook)
Charge asymmetry: a theory appraisal Germán Rodrigo Brugge, May 31 - June 4, 2010.
ATLAS: Moroccan participation Rajaa Cherkaoui El Moursli Mohammed V Agdal University Faculty of Sciences 1Valencia November 2010.
Searching for in High Mass Dilepton Spectrum at CDF, Fermilab ADD model Drell-Yan production of a graviton of varying string scale M S = M Pl(4+n) [4]
Choong Sun Kim (C.S. Kim) Department of Physics, Yonsei University, Korea.
Eric COGNERAS LPC Clermont-Ferrand Prospects for Top pair resonance searches in ATLAS Workshop on Top Physics october 2007, Grenoble.
A Search for Higgs Decaying to WW (*) at DØ presented by Amber Jenkins Imperial College London on behalf of the D  Collaboration Meeting of the Division.
Fourth Generation Leptons Linda Carpenter April 2011.
1 Top cross section and SM properties at CDF Alison Lister Université de Genève For the CDF collaboration.
A T : novel variable to study low transverse momentum vector boson production at hadron colliders. Rosa María Durán Delgado The University of Manchester.
New Strong LHC Rogerio Rosenfeld Instituto de Física Teórica UNESP  
The Top Quark at CDF Production & Decay Properties
Nady Bakhet PhD Student – Cairo University PhD Thesis Title
Electroweak Physics Lecture 6
M. V. Chizhov DESY/Sofia University, Bulgaria
Search for Dark Matter in Jets plus MET final state for Non-therma Dark Matter model Using Data From Proton-Proton Collisions at √s = 13TeV Sonaina Undleeb.
Journées de Prospective
THE SIMULATION OF POLARIZED BARYONS
Dart-yin A. Soh Institute of Physics, Academia Sinica
The two-Higgs-doublet model implementation in MadGraph v4
Not-SUSY-Nor-Higgs Exotic Searches at TeVatron Run II
CMS Physics Analysis in China
Prospect for Top Properties Measurement in Atlas
Jessica Leonard Oct. 23, 2006 Physics 835
Searches at LHC for Physics Beyond the Standard Model
Status of NLOjet++ for dijet angular distributions
CMS Physics Analysis in China
Greg Heath University of Bristol
Monte-Carlo event generation for CEPC
Double Heavy Hadrons at LHC Sino-French Workshop Dec , 2006
Experimental and theoretical Group Torino + Moscow
C.M.S.:.
Search for a New Vector Resonance in the pp WWtt+X Channel at LHC
Presentation transcript:

Search for The charge asymmetry in top anti-top resonance Smail BELAAOUJARajaa CHERKAOUI ELMOURSLI Marcel VOS UniversityMohmed V Faculty of sciences Nuclear laboratory Workshop, rabat october 2010

contents The charge asymmetry at HC Top quark asymmetry at Tevatron Top quark asymmetry at LHC The top quark charge asymmetry Beyond the SM MadGraph Generator Charge asymmetry study for resonance spin1 color singlet Charge asymmetry study for resonance spin1 color octet Conclusion and perspective

The charge asymmetry at HC QCD prediction: – At tree level, tt~pair production at HC is charge symmetric. – But at Ο(α s 3 ) order tt~ pair production is a charge asymmetic

Graphs originated by that contribute to the QCD charge asymmetry in quark-antiquark production

Is The asymmetry a CP violation? The asymmetry appears in a restriction of phase space The charge asymmetric defined as: N t ( cosθ ): number of top quark produced in an angle θ N tbar ( cosθ ): number of anti-top quark produced in an angleθ CP invariance the asymmetry is equivalent to Forward-backwards asymmetry

Top quark asymmetry at Tevatron ( ) Lepton+jet channel energy With luminosity of 3.2 fb -1 The total charge asymmety generated at the tevatron by QCD at NLO :

Top quark asymmetry at LHC ( ) The production cross section of top quarks is, dominated by gluon-gluon fusion gluon-gluon fusion represents the 84% of the top quark at 10TeV and 90% at 14TeV The charge aymmetry generated from the qqbar and qg is small in the most of kinimatics phase space

The top quark charge asymmetry Beyond the SM: topBSM The topBSM is implemented to study BSM effects in the ttbar invariant mass spectrum This model includes some number of resonances states which there are production of an intermediate particle X that decaying into ttbar:

This model includes the following possible resonances in the ttbar spectrum: o spin-0, color singlet =higgs-like particule couples only to quarks o spin-0, color octet = is a scalar, colored particle that couples only to top quarks o spin-1, color singlet = similar to the SM Z boson o spin-1, color octet = similar to a heavy gluon o spin-2, ADD model = graviton particle of the large extra dimensions model o spin-2, RS model The top quark charge asymmetry Beyond the SM: topBSM

Charge asymmetry study for resonances spin1 color singlet and spin1 color octet that produce the top anti-top quarks Tool used : MadGraph generator

MadGraph generator The MadGraph generator allows to: Generates the process Make the Faymann diagrams Calculate the amplitude of helicity

MadGraph characteristics Both for SM as well as BSM Easy to implement new models Can generate multiple process in the same run Decay chains specifications Call for the pythia package (hadronization) and PGS (detector sim) for a full simulation Web server interface from which the simulation itself can be done on-line or off-line Can create root files at each stape

MadGraph structure

Charge asymmetry study for resonance spin1 color singlet In this resonance state, the particule X(spin1 color singlet) is a similar to the SM Z boson The process generated: With elimination of o1 resonance and coupling to the gluons √ś=7TeV

Top quark Anti-top quark For the asymetry is more importante Top anti-top Asymmetry

A= Top distribution with cut on η: anti-top distribution with cut on η:

Leptons Asymmetry mu- mu+

A= distribution with cut on η:

Cut on the invariant mass with Resonance S1 mtt > 500 GeVmtt > 700 GeVmtt > 1000 GeV

In this resonance state the particule X(spin1 color octet) is a similar to a heavy gluon, it has the same couplings as the gluon The process generated: We have exclued the s1 resonance, the photons, the gluons and the Z boson √ś=7TeV Charge asymmetry study for resonance spin1 color octet

Top anti-top Asymetry Top quark Anti-top quark

A= anti-top distribution with cut on η: Top distribution with cut on η:

A=-0, distribution with cut on η:

Resonance O1 mtt > 500 GeVmtt > 700 GeVmtt > 1000 GeV Cut on the invariant mass with

Conclusion and perspective The value of the asymmetry deponds on the cut on the invaraint mass The results are significante Futur work: generate samples of heavy color octet resonances decaying to ttbar with arbitrary vector and axial-vector couplings to quark(fully leptonic channel):

Reference Paola ferrario Tesis docttoral,July G. L.Strycheckr et al. [CDF Cllaboration],Conf. Note 9724 (march2009). O. Antunano, J. H. Kuhn and G. Rodrigo, Phys. Rev. D (2008). G. Rodrigo, PoS RADCOR (2008). [arXiv: [hep-ph]].

thank you for your attention