Alex Melnitchouk DPF conference - May 2002 1 Search for Fermiophobic Higgs in the h   Channel DPF 2002, Williamsburg Alex Melnitchouk (Brown University)

Slides:



Advertisements
Similar presentations
Search for Large Extra Dimensions at the Tevatron Bob Olivier, LPNHE Paris XXXVI ème Rencontre de Moriond Mars Search for Large Extra Dimensions.
Advertisements

Investigation on Higgs physics Group Ye Li Graduate Student UW - Madison.
Gregorio Bernardi / Paris 1 WH,ZH, WW and advanced techniques Higgs Sensitivity DØ Gregorio Bernardi.
Current limits (95% C.L.): LEP direct searches m H > GeV Global fit to precision EW data (excludes direct search results) m H < 157 GeV Latest Tevatron.
Search for Top Flavor Changing Neutral Current Decay t → qZ Ingyin Zaw DOE Review August 21, 2006.
Recent Results on the Possibility of Observing a Standard Model Higgs Boson Decaying to WW (*) Majid Hashemi University of Antwerp, Belgium.
Tau dilepton channel The data sample used in this analysis comprises high-p T inclusive lepton events that contain an electron with E T >20 GeV or a muon.
Fourth Generation Leptons Linda Carpenter UC Irvine Dec 2010.
Summary of Results and Projected Sensitivity The Lonesome Top Quark Aran Garcia-Bellido, University of Washington Single Top Quark Production By observing.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Top Turns Ten March 2 nd, Measurement of the Top Quark Mass The Low Bias Template Method using Lepton + jets events Kevin Black, Meenakshi Narain.
DPF Victor Pavlunin on behalf of the CLEO Collaboration DPF-2006 Results from four CLEO Y (5S) analyses:  Exclusive B s and B Reconstruction at.
Kevin Black Meenakshi Narain Boston University
The new Silicon detector at RunIIb Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96.
Higgs Searches at LEP2 E. Kneringer University of Innsbruck / Austria Collaboration LAKE LOUISE WINTER INSTITUTE Electroweak Physics February 1999.
1 Viktor Veszprémi (Purdue University, CDF Collaboration) SUSY 2005, Durham Search for the SM Higgs Boson at the CDF Experiment Search for the SM Higgs.
Top Quark Physics: An Overview Young Scientists’ Workshop, Ringberg castle, July 21 st 2006 Andrea Bangert.
DØ Higgs II Gordon Watts for the collaboration. 2 Gordon Watts (UW Seattle) WIN’ /07/2003 Outline Channels H  WW * H  H ++ H --  +  +  -
University of Science & Technology of China (USTC) University of Science & Technology of China (USTC) W/Z+  ATLAS On behalf of ATLAS Collaboration.
ATLAS UK Physics meeting
Heavy charged gauge boson, W’, search at Hadron Colliders YuChul Yang (Kyungpook National University) (PPP9, NCU, Taiwan, June 04, 2011) June04, 2011,
Charged Higgs Results from Tevatron Sudeshna Banerjee Tata Institute of Fundamental Research Mumbai, India For CDF and DØ Collaborations Fermilab, Chicago.
L. Bellagamba, Excited fermions and other searches at HERA 1 International Conference on High Energy Physics Amsterdam July 2002 Excited fermions.
Search for Randall-Sundrum Gravitons with 1 fb -1 of Data Amitabha Das.
Direct di-  Tevatron On behalf of the & Collaborations Liang HAN University of Science & Technology of China (USTC)
KIRTI RANJANDIS, Madison, Wisconsin, April 28, Top Quark Production Cross- Section at the Tevatron Collider On behalf of DØ & CDF Collaboration KIRTI.
Sensitivity Prospects for Light Charged Higgs at 7 TeV J.L. Lane, P.S. Miyagawa, U.K. Yang (Manchester) M. Klemetti, C.T. Potter (McGill) P. Mal (Arizona)
January 10, 2007 Aspen Photon Searches at the Tevatron.
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.
Higgs Searches at Tevatron Makoto Tomoto 戸本 誠 Fermilab/Nagoya University On behalf of the DØ & CDF Collaborations Tsukuba, April 21 st, 2006.
Lighting up the Higgs sector with photons at CDF Fermilab Joint Experimental-Theoretical Seminar Karen Bland for the CDF collaboration May 20,
Precision Cross section measurements at LHC (CMS) Some remarks from the Binn workshop André Holzner IPP ETH Zürich DIS 2004 Štrbské Pleso Štrbské Pleso.
1 EPS2003, Aachen Nikos Varelas ELECTROWEAK & HIGGS PHYSICS AT DØ Nikos Varelas University of Illinois at Chicago for the DØ Collaboration
Search for the Higgs boson in H  ZZ (*) decay modes on ATLAS German D Carrillo Montoya, Lashkar Kashif University of Wisconsin-Madison On behalf of 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.
1 TOP MASS MEASUREMENT WITH ATLAS A.-I. Etienvre, for the ATLAS Collaboration.
Lake Louise (February 2002) Ivo van Vulpen 1 Z boson pair production Ivo van Vulpen Outline: LEP and its operation between ZZ production & final.
R. Dean Schamberger Recent Results from the D Ø Experiment DIS 2009, Madrid April 2009.
Flavour independent neutral Higgs boson searches at LEP Ivo van Vulpen NIKHEF On behalf of the LEP collaborations EPS conference 2005.
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.
ATLAS Higgs Search Strategy and Sources of Systematic Uncertainty Jae Yu For the ATLAS Collaboration 23 June, 2010.
April 7, 2008 DIS UCL1 Tevatron results Heidi Schellman for the D0 and CDF Collaborations.
Search for the Standard Model Higgs in  and  lepton final states P. Grannis, ICHEP 2012 for the DØ Collaboration Tevatron, pp √s = 1.96 TeV -
Jessica Levêque Rencontres de Moriond QCD 2006 Page 1 Measurement of Top Quark Properties at the TeVatron Jessica Levêque University of Arizona on behalf.
La Thuile, March, 15 th, 2003 f Makoto Tomoto ( FNAL ) Prospects for Higgs Searches at DØ Makoto Tomoto Fermi National Accelerator Laboratory (For the.
Beate Heinemann University of Liverpool For the CDF collaboration EPS 2003, Aachen, Physics Beyond the Standard Model with Photonic Final.
RHIC-PV, April 27, 2007 M. Rijssenbeek 1 The Measurement of W ’s at the CERN and FNAL hadron colliders W ’s at RHIC ! W ’s at CERN – UA2 W ’s at FNAL -
Search for a Standard Model Higgs Boson in the Diphoton Final State at the CDF Detector Karen Bland [ ] Department of Physics,
EPS Manchester Daniela Bortoletto Associated Production for the Standard Model Higgs at CDF D. Bortoletto Purdue University Outline: Higgs at the.
Aug _5071 Top stop by charm channel analysis using D0 runI data OUTLINE physics process of top to stop Monte Carlo simulation for signal data.
Elba -- June 7, 2006 Collaboration Meeting 1 CDF Melisa Rossi -- Udine University On behalf of the Multilepton Group CDF Collaboration Meeting.
LEP Search for Single Top production and new fermions Mario Antonelli LNF-INFN Frascati ICHEP 2002 Amsterdam on behalf of the 4- LEP experiments.
Viktor Veszpremi Purdue University, CDF Collaboration Tev4LHC Workshop, Oct , Fermilab ZH->vvbb results from CDF.
DPF Conf., Oct. 29, 2006, HawaiiViktor Veszpremi, Purdue U.1 Search for the SM Higgs Boson in the Missing E T + b-jets Final State at CDF V. Veszpremi.
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.
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.
Eric COGNERAS LPC Clermont-Ferrand Prospects for Top pair resonance searches in ATLAS Workshop on Top Physics october 2007, Grenoble.
Search for Anomalous Production of Multi-lepton Events at CDF Alon Attal Outline  Motivation  R p V SUSY  CDF & lepton detection  Analysis  Results.
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.
Low Mass Standard Model Higgs Boson Searches at the Tevatron Andrew Mehta Physics at LHC, Split, Croatia, September 29th 2008 On behalf of the CDF and.
Fourth Generation Leptons Linda Carpenter April 2011.
1 Donatella Lucchesi July 22, 2010 Standard Model High Mass Higgs Searches at CDF Donatella Lucchesi For the CDF Collaboration University and INFN of Padova.
Higgs Searches at the Tevatron (Run I)
Search for SM Higgs in WW* channel at CDF
Venkat Kaushik, Jae Yu University of Texas at Arlington
g g s High Mass Higgs at the Tevatron
Investigation on Diboson Production
VBF H(->bb)+photon
Jessica Leonard Oct. 23, 2006 Physics 835
SUSY SEARCHES WITH ATLAS
Presentation transcript:

Alex Melnitchouk DPF conference - May Search for Fermiophobic Higgs in the h   Channel DPF 2002, Williamsburg Alex Melnitchouk (Brown University) on behalf of D0 Collaboration

Alex Melnitchouk DPF conference - May Fermiophobic Higgs. Theoretical Outlook Many of SM extensions predict enhanced rate for Higgs decay into photon pairs due to suppressed couplings to - light quarks, - heavy quarks (TopColor) - up-type fermions (MSSM+smth) - all fermions Enhanced  rate is also predicted by some models that employ Extra Dimensions as well as other Exotic models.

Alex Melnitchouk DPF conference - May Fermiophobic Higgs. Experimental Outlook From Experimental Point of View it is convenient to consider  decays of the Higgs in two extreme cases: 1. all fermion couplings are zero (Fermiophobic Higgs) 2. Top Quark coupling is allowed (Topcolor Higgs)

Alex Melnitchouk DPF conference - May Enhancement of h   decays h   Branching Ratio Higgs Mass Standard Model Fermiofobic Higgs some other non SM predictions in general we should be prepared for any Br(h   ) due to new physics - quote S.Mrenna, J.Wells (hep-ph/ )

Alex Melnitchouk DPF conference - May Why Look for Fermiophobic Higgs at Fermilab ? Tevatron performance offers search possibilities beyond current mass limits within next few years In comparison with LEP there is additional possibility of Higgs production via gluon fusion  also TopColor Higgs can be looked for D0 is working on WW and  channels Both analyses rely mostly on the calorimeter (most understood of all D0 sub-detectors) Comparative Advantages : WW is predicted to have higher Branching ratio  is a clean signature, has smaller backgrounds

Alex Melnitchouk DPF conference - May Cross-Sections of Signal Production. Final States  Major final states are : -   -   or more jets t Higgs Mass Cross-Section, pb -1 W (Z) g g t h q q h q q h Production Processes: gluon fusion, W/Z associated, W/Z fusion

Alex Melnitchouk DPF conference - May Background Cross Sections jj jj  total QCD M  d  /d M  pb -1 /GeV Major Backgrounds are QCD processes that in the final state contain : - two real photons - one real photon and a hadronic jet that fakes a photon - two hadronic jets faking photons

Alex Melnitchouk DPF conference - May Previous Results RunI (0.1 fb -1 ) D0 :  2 jets analysis found 4 events (expected background = 6.0 +/-2.1 ) set mass limit of 78.5 GeV at 95% C.L. CDF :  2 jets;  e, , MissingEt analysis found 6 events (expected background = 6.2 +/-2.1 ) set mass limit of 82 GeV at 95% C.L. LEP limit : GeV at 95% CL

Alex Melnitchouk DPF conference - May Tevatron RunII Sensitivities (gluon fusion not included) G.Landsberg and K.Matchev(hep-ex/ ) estimated Tevatron RunII limits on h  Branching Ratio as a function of Higgs Mass with 95%CL Higgs Mass Br(h   RunI (0.1 fb -1 ) RunIIa (2.0 fb -1 ) RunIIb (30 fb -1 ) Fermiophobic h Preliminary LEP exclusion contour, A Andre Sopczak(hep-ph/ )

Alex Melnitchouk DPF conference - May Tevatron RunII Sensitivities (gluon fusion included) Higgs Mass h   Branching Ratio RunI (0.1 fb -1 ) RunIIa (2.0 fb -1 ) RunIIb (30 fb -1 ) MSSM+smth h

Alex Melnitchouk DPF conference - May Something about Photon ID specifics? Not sure what to put for this

Alex Melnitchouk DPF conference - May Selection of  Candidate Events Trigger: diEM or Single EM high Pt triggers Kinematic cuts: Pt >20GeV Acceptance cuts: Central Calorimeter (CC) (|  |<1.1) or EndCap Calorimeter (EC) (1.5<|  |<2.4), away (  0.015) from  -cracks in CC Photon ID: -0.05<Isolation<0.1, 0.95<Emfraction<1.05, shower shape consistent with EM shape (8x8 Hmatrix  2 <75), total Pt (within |  |<0.1) of tracks <1.46 GeV

Alex Melnitchouk DPF conference - May Monte Carlo Estimate of h  X Efficiencies W/Z associated W/Z fusiongluon fusion M= / / / / / / / / / / / / / / / / /- 0.7 Included : ID (without  2 cut ), Acceptance NOT included : Kinematic cuts

Alex Melnitchouk DPF conference - May Signal and Background Monte Carlo Distributions = (E(  1) - E(  2)) / (E(  1) + E(  2)) (Some or all of these (if any) as they are or remade for double-checking their validity)

Alex Melnitchouk DPF conference - May di-EM Invariant Mass from 11/01-04/02 D0 data estimated background contribution from direct  tight and loose cuts (calorimeter info only) Isolated  Candidate Events + tracking info Aslo need to calculate other QCD backgrounds, (and Z?)

Alex Melnitchouk DPF conference - May Other plots ? In case there are any suggestions

Alex Melnitchouk DPF conference - May Event Display of  Candidate (or  jet) ? Do you think it is worth to pick a most “ h->gamma gamma looking ” event out of the mass distribution two slides ago and show various event displays of it?

Alex Melnitchouk DPF conference - May Conclusions …