June_2004E. Gallas - SUSY 20041 Searches for Extra Dimensions and Heavy di-lepton Resonances at D0 Elizabeth Gallas Fermi National Accelerator Laboratory.

Slides:



Advertisements
Similar presentations
Dielectron Channel at CMS Cairo University November, Waled Emam Centre for Theoretical Physics at the British Univ. in Egypt.
Advertisements

Peter Schleper, Hamburg University SUSY07 Non-SUSY Searches at HERA 1 Non-SUSY Searches at HERA Peter Schleper Hamburg University SUSY07 July 27, 2007.
Search for Large Extra Dimensions at the Tevatron Bob Olivier, LPNHE Paris XXXVI ème Rencontre de Moriond Mars Search for Large Extra Dimensions.
Physics with Single, Multi- & Di-Photons at LEP HEP2003, Aachen, July HEP2003, Aachen, July Marat Gataullin (Caltech/L3) on behalf of LEP Collaborations.
1 Beate Heinemann, UC Berkeley and LBNL Università di Pisa, February 2010 Particle Physics from Tevatron to LHC: what we know and what we hope to discover.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Extra Dimensions Primer (see S. Hossenfelder) LED in many dimensions JLH, Lillie, Rizzo hep-ph/ SUSY05 DurhamJ. Hewett.
Electroweak Physics at the Tevatron Adam Lyon / Fermilab for the DØ and CDF collaborations 15 th Topical Conference on Hadron Collider Physics June 2004.
Michele Gallinaro, "QCD Results at CDF" - XXXVIII Rencontres de Moriond, March 22-29, QCD Results at CDF Inclusive Jet Cross Section Dijet Mass.
6/15/2004Michael Kirby, Duke University1 Tevatron W/Z/  Results Part II Attack of the DiBosons 15th Topical Conference on Hadron Collider Physics Michael.
Tevatron Non-SUSY BSM: Searches for Physics Beyond the SM and MSSM David Stuart University of California, Santa Barbara DIS 2007, Munich April 2007.
Search for Anomalous tWb Couplings at D0, L. Li (Shanghai Jiao Tong University) SUSY 2012, August 16, Liang Li Shanghai Jiao Tong University Search.
EPS 2003, July 19, 2003David Buchholz, Northwestern University Performance of the D0 Experiment in Run II Detector Commissioning and Performance Accelerator,
Kaluza-Klein gluon production at the LHC
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
Sreerup Raychaudhuri TIFR Extra Dimensions and Collider Physics Workshop on Synergy between High Energy and High Luminosity Frontiers Tata Institute of.
ICHEP-2002, AmsterdamG. Bernardi, LPNHE- Paris Search for Low Scale Gravity & Extra Dimensions at HERA, LEP, and the Tevatron Mini-review talk ICHEP-2002.
Search for Randall-Sundrum Gravitons with 1 fb -1 of Data Amitabha Das.
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,
Searches for the Standard Model Higgs at the Tevatron presented by Per Jonsson Imperial College London On behalf of the CDF and DØ Collaborations Moriond.
Large extra dimensions and CAST Biljana Lakić Rudjer Bošković Institute, Zagreb Joint ILIAS-CAST-CERN Axion Training, , CERN Joint ILIAS-CAST-CERN.
Ryan J. Hooper -- DPF, May 24-28, Searching For Large Extra Dimensions at D  Extra dimensionsExtra dimensions Overview of Run 1 resultsOverview.
1/32 Arnold Pompoš, Štrbské Pleso, Slovakia, April 14, 2004.
Search for Extra Dimensions at ATLAS Ambreesh Gupta University of Chicago PASCOS 2003 T.I.F.R, Mumbai, 3-8 January 2003.
Electroweak and Related Physics at CDF Tim Nelson Fermilab on behalf of the CDF Collaboration DIS 2003 St. Petersburg April 2003.
MARIA SPIROPULU MARCH Vanderbilt University Physics & Astronomy Colloquium Experimental Clues From Higher Dimensions.
1 EPS2003, Aachen Nikos Varelas ELECTROWEAK & HIGGS PHYSICS AT DØ Nikos Varelas University of Illinois at Chicago for the DØ Collaboration
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.
1 Search for new physics in dilepton and diphoton final states with CDF Xin Wu (University of Geneva, Switzerland) On behalf of the CDF collaboration.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Kaori Maeshima, FermilabLa Thuile, 4 th March Non SUSY Searches at the Tevatron Kaori Maeshima (Fermilab) For the D0 and CDF Collaborations.
06/30/05 Mathieu Agelou – LowX’05 1 Sensitivity to PDFs at the Tevatron. Mathieu Agelou CEA – Saclay Low x workshop, Sinaia, Romania.
Low scale gravity black holes at LHC Enikő Regős ( CERN )
7/20/07Jiyeon Han (University of Rochester)1 d  /dy Distribution of Drell-Yan Dielectron Pairs at CDF in Run II Jiyeon Han (University of Rochester) For.
Search for Extra-Dimensions at D0 Tevatron and D0 status Extra Dimensions Large ED Tev-1 ED Randall Sundrum Model M. Jaffré LAL Orsay for the D0 Collaboration.
Search for Extra Dimensions in diphotons at CMS Duong Nguyen Brown University USLOU Meeting Fermilab, Oct , 2010.
Susan Burke DØ/University of Arizona DPF 2006 Measurement of the top pair production cross section at DØ using dilepton and lepton + track events Susan.
1 Arnold Pompoš, SUSY03, Tucson, Arizona, June 5-10, 2003.
Don LincolnExperimental QCD and W/Z+Jet Results 1 Recent Dijet Measurements at DØ Don Lincoln Fermi National Accelerator Laboratory for the DØ Collaboration.
Randall- Sundrum Gravitons and Black Holes at the LHC Kevin Black Harvard University For the ATLAS and CMS Collaborations.
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.
1 Experimental Particle Physics PHYS6011 Fergus Wilson, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2) 3.Collider Experiments.
New Phenomena Searches at CDF Aron Soha (University of California at Davis) For the CDF Collaboration February 19, 2006 Lake Louise Winter Institute.
Beate Heinemann University of Liverpool For the CDF collaboration EPS 2003, Aachen, Physics Beyond the Standard Model with Photonic Final.
Search for a Standard Model Higgs Boson in the Diphoton Final State at the CDF Detector Karen Bland [ ] Department of Physics,
1 Exotics Searches in Photon and Lepton Final States with the ATLAS Detector Tetiana Berger-Hryn’ova (LAPP, Annecy le Vieux) on behalf of the ATLAS collaboration.
ICHEP ’04, Beijing, August 20, 2004Eric Kajfasz, CPPM/D01 Search for Extra-Dimensions at pp and ep Colliders Eric Kajfasz, CPPM/D0
Elba -- June 7, 2006 Collaboration Meeting 1 CDF Melisa Rossi -- Udine University On behalf of the Multilepton Group CDF Collaboration Meeting.
Collider Signals of Extra Dimension Scenarios
Searches for Resonances in dilepton final states Searches for Resonances in dilepton final states PANIC th -14 th November 2008, Eilat, ISRAEL A.
RANDALL-SUNDRUM GRAVITON IDENTIFICATION IN DILEPTON AND DIPHOTON EVENTS WITH ATLAS V.A. Bednyakov JINR, LNP with A.A. Pankov, A.V. Tsytrinov ICTP Affiliated.
DIS 2003, May 22-27, St PetersburgAndrew Mehta Electroweak Physics and Searches1 Electroweak Physics + Searches Andrew Mehta DIS 2003, St. Petersburg,
Search for large extra dimensions at the Tevatron V. Krutelyov (UCSB) for CDF and D0 Collaborations DIS-2008 Conference, London April 7-11, 2008 Large.
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]
QWG Sept 20-22, Jundong Huang Indiana University 1 DØ Quarkonium Production at DØ Jundong Huang Indiana University Quarkonium Workshop FermiLab September.
Search for Standard Model Higgs in ZH  l + l  bb channel at DØ Shaohua Fu Fermilab For the DØ Collaboration DPF 2006, Oct. 29 – Nov. 3 Honolulu, Hawaii.
Search for Anomalous Production of Multi-lepton Events at CDF Alon Attal Outline  Motivation  R p V SUSY  CDF & lepton detection  Analysis  Results.
DØ Searches Yuri Gershtein On behalf of the DØ collaboration.
Venkat Kaushik, Jae Yu University of Texas at Arlington
Deep Inelastic Scattering 2006
Not-SUSY-Nor-Higgs Exotic Searches at TeVatron Run II
Louisiana Tech University
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
Search for Narrow Resonance Decaying to Muon Pairs in 2.3 fb-1
Gregorio Bernardi, LPNHE - Paris G. Bernardi, LPNHE- Paris
SUSY particles searches with R-parity violation at DØ, Tevatron
Collider Signals of Large Extra Dimension
Susan Burke, University of Arizona
Presentation transcript:

June_2004E. Gallas - SUSY Searches for Extra Dimensions and Heavy di-lepton Resonances at D0 Elizabeth Gallas Fermi National Accelerator Laboratory Computing Division 12th International Conference on Supersymmetry and Unification of Fundamental Interactions June 17-23, 2004 Epochal Tsukuba, Tsukuba, Japan.

June_2004E. Gallas - SUSY Outline 3-Space / Time: –Fermilab Tevatron with Experiment DØ / mid Run 2 What can Extra Dimensions (ED) do for you ? Phenomenology (of interest for pp colliders) –2 particular ED models Large Extra Dimensions –ADD (Arkani-Hamed, Dimopoulos, Dvali) TeV -1 ‘longitudinal’ Extra Dimensions –DDG (Dienes, Dudas, Gherghetta) –DØ: A window into ‘Extra Dimensions’ (ED) DØ: Lepton/Photon Final state searches for : –Large Extra Dimensions (ED) –TeV-1 ‘longitudinal’ Extra Dimensions –Z’ boson Summary and Conclusions –

June_2004E. Gallas - SUSY Chicago  Tevatron Main Injector & Recycler DØ CDF  p source TEVATRON Run 2 Upgrade New Main Injector : 150 GeV –Store protons, shoot to target for anti-proton production New recycler : –Magnet storage ring for anti- proton Higher energy: –1.96 TeV vs 1.8 TeV –Higher cross sections (30 % for the SUSY) Higher antiproton intensity: –6x6  36x36 bunches (3.5 μs  396 ns) –Higher luminosity Run 1 : 2x10 31 cm -2 s -1 Run 2 : 2x10 32 cm -2 s -1

June_2004E. Gallas - SUSY SMT DØ Run 2a Upgrade Solenoid (2T) 4-layer Silicon Vertex and 16-layer Fiber Trackers Muon forward chamber ( |  |<2 ), shielding New preshower, upgrade Calorimeter electronics Upgrade to Trigger and DAQ system

June_2004E. Gallas - SUSY What can Extra Dimensions do for you ? …proposals dating at least back to 1920’s… Recent renaissance in the theory proposes: –unite all known forces (including gravity) known particles, electroweak and strong interactions –confined to a ‘brane’ - a hypersurface in the “bulk” of 4+n Dim gravity appears weak – diluted in extra dimensions. –There is no “desert” –Offers alternative to the “hierarchy problem” only one important scale in nature -- may be accessible at Tevatron and LHC energies –Lends practical aspects to string theory… it’s not just a beautiful idea… we can test it !

June_2004E. Gallas - SUSY Large Extra Dimensions (LED) in the ADD Model ADD (Arkani-Hamed, Dimopoulos, Dvali) model assumes: –n Extra Dimensions of size R –SM particles and interactions are confined to 4D-world (brane) –Gravity propagates in 4+n Dimensional space Gravity appears weak – diluted in extra dimensions –In this formulation: where M Pl (apparent 4D Planck Scale): Ms (fundamental Planck Scale) is brought to the TeV range Constraints (cosmology, tabletop expts): –Extra dimensions ‘compactified’ (R C < 1 mm) –require n>1 (g forces at large distances) Collider experiments – only probe for ED for n  3 !

June_2004E. Gallas - SUSY LED Tevatron Search Modes Direct Searches (graviton escapes the brane) –look for JET recoiling against missing ET (next talk) Indirect Searches (this talk) –virtual graviton - contributions to l + l -,  production

June_2004E. Gallas - SUSY Virtual Graviton Exchange The predicted cross section is described by: where  g = F/M S 4 == ( in TeV -4 ) describes strength of gravity in the presence of LED and F is a dimensionless parameter ~ 1 which depends on the formalism (for the effective Lagrangian): GRW: F = 1 HLZ: F = log(M s 2 /M 2 ), n =2 F = 2/(n-2), n > 2 Hewett F = 2 / , =±1 Experimentally, the process is defined by the –invariant mass of the di-boson or di-leptons (M) –cosine of the scattering angle,  * (|cos  *|). SM term interference term direct gravity term

June_2004E. Gallas - SUSY Search for ED in ee/  channel Dataset 200 pb -1 Use di-EM objects –both ee and  Selections Two EM with Et > 25 GeV with tight quality cuts Fiducial requirements: central EM objects: |eta| < 1.1 central/forward objects: 1.5 < |eta| < 2.4 LED signal MC for  g =0.6 fakes Bkg

June_2004E. Gallas - SUSY Highest mass Drell-Yan event Invariant mass 475 GeV/c 2, cos θ* = 0.01

June_2004E. Gallas - SUSY di-EM Mass,Cos θ* distributions

June_2004E. Gallas - SUSY Uncertainties: Uncertainties in  G for di-EM sample

June_2004E. Gallas - SUSY LED:  LED in  at DØ - M S > 880 GeV (95% CL) Run 2 Preliminary Luminosity = 100 pb -1 Select events with  2 muons P T > 15 GeV M  > 50 GeV

June_2004E. Gallas - SUSY Summary: Limits on LED M S for various formalisms F No evidence for signatures in excess of high-mass dielectron, diphoton or dimuon events over SM expectation, from coupling to Kaluza-Klein gravitons Fit (di-EM Mass,Cos θ*) distribution –Single parameter for ED effects: η G = F/M 4 S Translate η G limits to 95% CL lower limits on Planck scale M S, in TeV, using different formalisms for F DiEM limits - combine Run I & Run 2 – best limits on LED to date Di  limits for Run 2 with more statistics -- in preparation

June_2004E. Gallas - SUSY Dedicated ee Search for ‘longitudinal’ Extra Dimensions Another ED model (TeV -1 “longitudinal” EDs): –proposed by Dienes, Dudas, and Gherghetta (DDG) –Fermions confined to 4D –but SM gauge bosons propagate in TeV -1 ED of size: R = 1/M C –Predicts Kaluza-Klein states of gauge bosons (  KK, W KK, Z KK, g KK ) produced directly (with sufficient energy) produced indirectly (virtual exchange of KK modes) Lepton pair production cross section depends on –  C =  2 / 3 M C 2, where M C = ‘compactification’ scale of TeV -1 ED This analysis: –look for virtual exchanges of KK excitations of the Z and 

June_2004E. Gallas - SUSY Jet mis-ID signal  C =5TeV -2 SM + fakes Dedicated ee Search for TeV-1 Dimensions (DDG) Predicts strong negative interference effects unlike LED discussed before Use di-EM dataset (200 pb -1 ) –adding track match –fiducial requirements – same as for LED analysis Find upper limit on  C < 2.63 TeV and thereby (lower limit): M c > 1.12 TeV (95% CL) First search of this type

June_2004E. Gallas - SUSY Z Limits from ee: SM, E 6 Various models propose new neutral gauge bosons –SM couplings –variety of E 6 GUT inspired Dataset 200 pb -1 – same as in ED analysis Limits on Z ’ mass in GeV/c 2 : SM couplings Run I Run II E 6 couplings Z I Zχ Zψ Zη

June_2004E. Gallas - SUSY Z’:  No evidence: Set limits M(Z’) > 610 GeV Run 2 Preliminary This is a previous result under revision with increased statistics: We used the same dimuon sample as used for LED  search to look for heavy Z-like resonances

June_2004E. Gallas - SUSY Summary No signal for new physics observed so far –but some interesting events ! New Limits from DØ: Extra Dimensions and Z’ * limits under revision with increased statistics improved limits on additional gauge bosons ! most sensitive collider search for ED’s to date! –higher efficiency in widest acceptance –di-EM channels using 200 pb -1 integrated luminosity (now 300 pb -1 on tape) –first collider search for TeV -1 ‘longitudinal’ Extra Dimensions TopicPrelim. Run 2 LED : ee and  M S >1.43 TeV (Run 1&2) LED :  M S > 880 GeV * TeV -1 ‘longitudinal’ ED: ee M c > 1.12 TeV Z’ :  M(Z’) > 610 GeV * Z’ : eeM(Z’) > 780 GeV