Phenomenology of Vector Resonances from SEWSB at Future e+e- Colliders

Slides:



Advertisements
Similar presentations
CompHEP Automatic Computations from Lagrangians to Events Ivan Melo University of Zilina Fyzika za Štandardným modelom klope na dvere Svit,
Advertisements

Electroweak Symmetry Breaking from D-branes Joshua Erlich College of William & Mary Title U Oregon, May 22, 2007 w/ Chris Carone, Marc Sher, Jong Anly.
First measurement of EWK Z+2j production cross section and hadronic activity in rapidity gap in CMS A.Nikitenko (IC) for 7 TeV Analysis Team March, 2013.
1 17 th May 2007 C.P. Ward Sensitivity of ZZ->llnunu to Anomalous Couplings Pat Ward University of Cambridge.
Signatures of a new vector resonance from strongly interacting electroweak symmetry breaking M. Gintner, I. Melo, B. Trpišová University of Žilina Exotics.
1 A Feasibility Study for a Strange Sea Asymmetry Analysis at ATLAS: update II Laura Gilbert and Jeff Tseng 13/12/07.
Status Report on hbb Analysis Jyothsna Rani for the hbb group Andy, Avto, Marine, Tim, Boris All D0 Meeting 28 th January th January 2005.
WW Scattering studies for the Future Linear Collider Andres F. Osorio Postgraduate student High Energy Physics Group.
1 VV scattering in P-TDR (CHAPTER 13.2 Vol 2.2) A simple summary of what we intend to put in our chapter CPTweek / PRSsession 10/31/05 Sara Bolognesi (TORINO)
In the R-parity violating SUSY model at hadron colliders 张仁友 中国科学技术大学.
1 A Preliminary Model Independent Study of the Reaction pp  qqWW  qq ℓ qq at CMS  Gianluca CERMINARA (SUMMER STUDENT)  MUON group.
2004 Xmas MeetingSarah Allwood WW Scattering at ATLAS.
New Vector Resonance as an Alternative to Higgs Boson (Strong EWSB)
Olivier RavatLes Houches/June 3rd Higgs associated production at LHC : Thecase Olivier Ravat, Morgan Lethuillier IPN Lyon Les Houches 2003 : Physics.
   (Episodio II). Signal/Background Reaction:             0   e  e        0 e  e   0 X-section.
Jet Physics in ALICE Mercedes López Noriega - CERN for the ALICE Collaboration Hot Quarks 2006 Villasimius, Sardinia - Italy.
Prospects of Discovering a New Massless Neutral Gauge Boson at the ILC E. Boos 1, V. Bunichev 1 and H.J. Schreiber 2 1 Institute of Nuclear Physics, Moscow.
Electroweak Symmetry Breaking without Higgs Bosons in ATLAS Ryuichi Takashima Kyoto University of Education For the ATLAS Collaboration.
B  K   p  and photon spectrum at Belle Heyoung Yang Seoul National University for Belle Collaboration ICHEP2004.
Monte-Carlo event generation for CEPC 1 Xin Mo Institute of High Energy Physics Oct. 19, 2015 Monte-Carlo event generation for the CEPC.
Feasibility of Detecting Leptoquarks With the CDF Detector Althea Moorhead Mentor: Darin Acosta.
BESS Model Resonance in the pp W + W tt + X Channel at LHC M. Gintner, I. Melo, B. Trpišová University of Žilina Herlany, September 2006.
March 2005Sarah Allwood WW Scattering at ATLAS Sarah Allwood University of Manchester IOP HEPP conference 2005, Dublin.
BESS Model Resonance in the pp W + W tt + X Channel at LHC M. Gintner, I. Melo, B. Trpišová University of Žilina CERN, Nov 1, 2006.
Kinematics of Top Decays in the Dilepton and the Lepton + Jets channels: Probing the Top Mass University of Athens - Physics Department Section of Nuclear.
Vector boson scattering at CMS (LHC)
Dark Matter Mass Constrained by Relic Abundance, Direct Detections, and Colliders Ho-Chin Tsai CYCU 2013/03/22 Academia Sinica 3/22/13 Ho-Chin Tsai
Search for the 2nd KK states of the mUED model at the LHC Kang Young Lee Konkuk U. Seoul YongPyong Greenpia, Yong Pyong
1 UCSD Meeting Calibration of High Pt Hadronic W Haifeng Pi 10/16/2007 Outline Introduction High Pt Hadronic W in TTbar and Higgs events Reconstruction.
David Yaylali – UHawaii Dept of PhysicsSUSY 2011 – Fermilab Fermiophobic gauge bosons as an effective theory at the LHC.
Strong EWSB in Top Quark Production at ILC Ivan Melo M. Gintner, I. Melo, B. Trpišová (University of Žilina) Praha, Mar 30, 2006.
Dalitz Decays and Bremsstrahlung from in-Medium EM Spectral Functions Ralf Rapp Cyclotron Institute + Physics Department Texas A&M University College Station,
1 Dijet Resonances Kazım Z. Gümüş and Nural Akchurin Texas Tech University Selda Esen and Robert M. Harris Fermilab PRS JETMET Meeting July 6, 2005.
New Strong LHC Rogerio Rosenfeld Instituto de Física Teórica UNESP  
Chiral Extrapolations of light resonances
Higgs and Supersymmetry
Electroweak Physics Lecture 6
CompHEP Automatic Computations from Lagrangians to Events
Particle Physics Tour with CalcHEP
Generator Study of Tevatron collider
ppZZ4μ background process
Vector Boson Fusion at CMS
γ γ-> hadron Background Events at CLIC
Dart-yin A. Soh Institute of Physics, Academia Sinica
Loops and loopholes in LHC mono-jet searches
Phenomenology of Twin Higgs Model
NIKHEF / Universiteit van Amsterdam
National Taiwan University
Xinyu Miao Department of Physics Univ. of Arizona 03/30/07
4. Hidden Local Symmetry Effective (Field) Theory
Higgs Physics at a gg Collider
Phenomenology of Twin Higgs Model
Phenomenology of Twin Higgs Model
Double Gauge Boson Production at = 7, 8, and 13TeV
Xinyu Miao Department of Physics Univ. of Arizona 03/30/07
Strong Electroweak Symmetry Breaking from
Searches and EW physics at HERA
Charmless Quasi-two-Body Modes at BaBar
Phenomenology of Twin Higgs Model
The Operator Product Expansion Beyond Perturbation Theory in QCD
Status of NLOjet++ for dijet angular distributions
M. Ohlerich, A. Raspiareza, W. Lohmann DESY and MPI Munich
Monte-Carlo event generation for CEPC
Experimental and theoretical Group Torino + Moscow
Search for D0D0 Mixing at BESIII
c c c c c c c c c c a Charmed baryon spectroscopy at Belle
Missing Mass Reconstruction of Ds*(2317)± in pp →Ds±Ds(2317)±
Koji TSUMURA (Osaka Univ.)
Search for a New Vector Resonance in the pp WWtt+X Channel at LHC
Strong EWSB in Top Quark Production
Presentation transcript:

Phenomenology of Vector Resonances from SEWSB at Future e+e- Colliders 14th KSF, Smolenice Oct 13, 2004 Phenomenology of Vector Resonances from SEWSB at Future e+e- Colliders Ivan Melo D. Bruncko (IEP SAS Kosice) M. Gintner (University of Zilina) I. Melo (University of Zilina)

Outline Motivation for new vector (ρ) resonances Vector resonance models ρ signals in e+e- → ννtt

Chiral SB in QCD EWSB SU(2)L x SU(2)R → SU(2)V , vev ~ 90 MeV SU(2)L x SU(2)R → SU(2)V , vev ~ 246 GeV

WL WL → t t

Chiral effective Lagrangian A simple Lagrangian L = i gπ Mρ/v (π- ∂μ π+ - π+ ∂μ π- )ρ0μ + gV t γμ t ρ0μ + gA t γμ γ5 t ρ0μ (1) Chiral effective Lagrangian L = - v2 Tr [ Aμ Aμ] - a v2 /4 Tr[(ωμ + i g'' ρμ . τ/2 )2] + b1 IbL + b2 IbR + ... (2) gπ = Mρ /(2 v g''), gV ≈ g'' b2 /[4(1+b2)], Mρ ≈ √a v g''/2.

Unitarity constraints WL WL → WL WL , WL WL → t t, t t → t t gπ ≤ 1.75 (Mρ= 700 GeV) gV ≤ 1.7 (Mρ= 700 GeV) Low energy constraints g’’ ≥ 10 |b2| ≤ 0.08

Subset of fusion diagrams + approximations (Pythia) Full calculation of 66 diagrams at tree level (CompHEP)

Pythia vs CompHEP ρ (M = 700 GeV, Γ = 12.5 GeV, g’’ = 20, b2 = 0.08) Before cuts √s (GeV) 800 1000 1500 Pythia (fb) 0.35 0.95 3.27 CompHEP (fb) 0.66 1.16 3.33

Backgrounds (Pythia) e+e- → e+e- tt e+e- → tt γ σ(0.8 TeV) = 300.3 + 1.3 fb → 0.13 fb (0.20 fb) σ(1.0 TeV) = 204.9 + 2.4 fb → 0.035 fb (0.16 fb)

Conclusions ρ in e+e- → ννtt – sensitive probe of mt physics σ(1 TeV) = 0.16 (0.035) fb R values up to 8