B physics: new states, rare decays and branching ratios in CDF
|
|
- Karen Charla Cole
- 6 years ago
- Views:
Transcription
1 B physics: new states, rare decays and branching ratios in CDF Vyacheslav Krutelyov Texas A&M University For CDF Collaboration July 1, 2004 BEACH04 Chicago, IL
2 Outlines CDF Run2 Detector Triggers Searches B s(d) µ + µ D 0 µ + µ Measurements (successful searches) X(3872) B + J/ψ π + B s φφ and pentaquarks See talks by S.D Auria and D.Litvintsev BEACH04 2
3 Tevatron performance As you know the Tevatron is working very well this year Record initial luminosity = cm -2 s -1 ( cm -2 s -1 to CDF) Detector efficiency ~85-90% ~450pb -1 on tape pb -1 used for analysis so far BEACH04 3
4 η =1 η =0.6 2 ft steel 2 ft steel CDF Run2. CMP muon det (drift cham + scint) p T >2.5GeV η <0.6 CMU muon det (drift cham) p T >1.5GeV η <0.6 SVX II (5layer) silicon strip det σ svx+ip ~40µm η =1 η =0.6 COT tracker drift chamber δp T /p T2 ~0.1% δp T /p T 2 ~1.5%(L1/XFT) CMX muon det (drift cham + scint) p T >2GeV 0.6< η <1 s=1.96tev σ(inelastic)~60mb. L ~ cm -2 s -1 (~400pb -1 good recorded) Plan: ~ cm -2 s -1 (Run2a); ~ cm -2 s -1 (4-8/fb Run 2) 1.7MHz collision 20kHz L1 trigger 350Hz L2 60Hz L3/logging rate. ~80% L1 (~1/3 at L3) of the trigger (bandwidth) are B physics Run2 vs Run1 Better silicon coverage ( 2), muon detection, improved tracking. Better triggers: lower track p T, higher efficiency. BEACH04 4
5 Triggers used All are input to the various Level-3 triggers That use the offline quality information Dimuon trigger p T >1.5GeV, η <0.6 p T >2GeV, 0.6< η <1 p T, φ, muon ID used to cut on tracks Used for ψ,υ,β µµ(+x) Two Track Trigger p T >2GeV, η <1 p T, φ, d 0 info used to cut on 2 tracks Used for: B,D hadrons ; D µµ Semileptonic trigger p T, φ, d 0, muon ID used to cut on tracks Used for ψ,d,β µ(+x) no results presented in this talk primary vertex ~ 1 mm b, c decays secondary vertex impact parameter BEACH04 5
6 Triggers used Dimuon trigger p T >1.5GeV, η <0.6 p T >2GeV, 0.6< η <1 p T, φ, muon ID used to cut on tracks Used for ψ,υ,β µµ(+x) BEACH04 6
7 Entries χ / ndf / 28 amplitude ± center ± σ ± intercept (lin. bg) ± amplitude (exp. bg) 1.118e+15 ± 3.447e+15 decay const. (exp. bg) ± Triggers used Two Track Trigger p T >2GeV, η <1 p T, φ, d 0 info used to cut on 2 Used for: B,D hadrons ; D µµ primary vertex ~ 1 mm secondary vertex impact parameter b, c decays 2 Events / GeV/c CDF Run II Preliminary, 66±4 pb ± B φ K 13.4 ± 5.7 Events ± Data Fit φ Sideband 0 BEACH04 ± 2 B Candidate Mass [GeV/c ]
8 B(D) µµ: Theoretical motivations. Current limits. Flavor Changing Neutral Current. Loop contribution only in SM. Br SM (B s µ + µ - )=(3.4±0.5) 10-9 Br SM (B d µ + µ - )=(1.00±0.14) (hep-ph/ ) Br SM (D 0 µ + µ - )~3*10-13 (GIM suppressed) Only upper experimental limit exists: Br exp (B s µ + µ - )< % C.L. CDF Br exp (B d µ + µ - )< % C.L. Belle Br exp (D 0 µ + µ - )<4.1(4.2)* % C.L. BEATRICE(E771) Limits are far away from the SM value: can test for a possible new physics. MSSM: Br(B µ + µ - ) enhanced by tanβ>10 terms ~tan 6 β. Up to 100 over the SM prediction. R-parity violating models give tree level contributions. Not heavily constrained by other observables. Can be seen in Run2 (esp. B s µµ) Other models enhance less. E.g., universal extra dimensions. Up to +70% for B s µ + µ - b µ ν λ i23 λ i22 BEACH04 8 s msugra,so(10) RPV µ
9 D 0 µµ search Use D *± D 0 π ± tagged events Use D 0 π + π as a normalization mode. Blind from µid in 1.840<m µµ <1.882 GeV Cuts: d 0 (μ,π) >120μm, d xy (D 0 ) <150μm Δφ(μμ)>0.085 Background: combinatorial (from right sideband) expect 1.5±0.7 misidentification (punch-through/decay) expect N(D 0 π + π ) P(misID) 2 0.3±0.1 Br( D NCL( D µµ ) ε( D ππ) 0 µµ ) Br( D ππ) 0 0 N( D ππ) ε( D µµ ) BEACH04 9
10 D 0 µµ search 69pb -1 B(D 0 µµ)<2.4 90% C.L. B(D 0 µµ)<3.1 95% C.L. This result improves on the previous limits by ~ 2 ( from BEATRICE, and from E771 at 90% C.L.) BEACH04 10
11 Br(B s(d) μ+μ-) measurement. BR(B s µµ) 3% (CMU&CMP Run1) 2 α ε ( n σ, n Expect to detect at most few events that might only look like B s(d) μ+μ N total obs SM predicts 0 events really a search Don t look at the data signal region (blind search) Signal inside 5.169<M µµ <5.469 GeV/c 2 (±3σ window) demonstrate understanding of background events accurately estimate α (acceptance) and ε (efficiency) intelligently optimize cuts CL 25% Run1 Bs bg ) Ldt CL=90% upper limit on <n sig > for n obs and n bg 171pb-1 or 10 trillion collisions only Run1 σ Bs =0.9µbfor p T Βs >6 GeV/c, y <1 (use this as a baseline selection) Dimuon trigger and p T >6GeV baseline sample: 2940 events BEACH04 11
12 Signal & Background Need to select discriminating variables that leave most of the signal and remove most of the background. R < 1 (φ < 57 o ) P T µµ B s s µµ P T µ Φ y P µ T P vtx T x Most Promising Discriminating Variables Invariant mass M cτ : L xy Pt (B) 2D lifetime c Φ : φ(p TB ) φ(vtx) Isolation: P (B) P t (B) t + R <1 P t (trk) Largest expected background: gluon splitting g bb µµ BEACH04 12
13 Optimization Results Optimize on (M µµ, cτ, Φ, Iso) to get the best expected limit BR(B s µµ) (cτ, Φ,Iso) = (>200 mm, <0.10 rad, >0.65) and mass window ± 80 MeV around world avg Bs(d): GeV (5.279 GeV) = Bs(d): α ε total = (2.0 ± 0.2)% (α 6.6%, ε total 30%) Accepted bgd σ = (6 ± 2) fb Expected bacground <Bgd> in 171pb -1 = 1.1 ± 0.3 events n N( n n ) P( n n ) Poisson prob 2 α ε total bg σ Bs bg Ldt BEACH04 13
14 Observed limits BR(B s µ + µ ) < 5.8x10 7 (7.5x % C.L.) 90% C.L. 3 times better than Run I (previous world best) BR(B d µ + µ ) < 1.5x10 7 (1.9x % C.L.) 90% C.L. slightly better than (1.6x % C.L., just published) B-factory/Belle result BEACH04 14
15 for SUperSYmmetry C.L.) SO(10) R. Dermisek et al., hep-ph/ R-parity violating R. Arnowitt et al., PLB 538 (2002) 121, new plot by B.Dutta new CL Dark matter allowed region New limit excludes significant amounts of the previously allowed SUSY models parameters (more to go) BEACH04 15
16 Spectroscopy Exotic States X(3872) New narrow state observed first by Belle in decay modes J/ψπ + π Charmonium state not expected near mass peak. D* Dbar deuteron-like molecule? CDF confirms X in 220pb -1 Preference for M(ππ) > 500MeV 670±90 candidates, sign.~ 12σ Mass scale using ψ(2s) peak BEACH04 16
17 X(3872): Long-lived fraction CDF II CDF II II Long-lived fraction: F X(3872) =16.1 ± 4.9 ± 2.0 % cf F ψ(2s) = 28.3 ± 1.0 ± 0.7 % BEACH04 17
18 B J/ψ π + Cabibbo-suppressed decay B + J/ψπ + Br Expected to be 5% relative to Br(B + J/ψK + ) Br(B + J/ψπ + )/Br(B + J/ψK + )=4.2 ± 0.7% PDG02 Signal selection p T (B + )>6.5GeV, p T (K + )>2GeV, L xy >200µm BEACH04 18
19 Summary Great physics results are coming in from CDF Br(B s µµ)<5.8x10-7 at 90% C.L. Br(B d µµ)<1.5x10-7 at 90% C.L. Br(D µµ)<2.4x10-6 at 90% C.L. X(3872) confirmation accepted/published by PRL Long-lived fraction F X(3872) =16.1 ± 4.9 ± 2.0 %. BEACH04 19
20 BEACH04 20
Rare Decays at the Tevatron
Rare Decays at the Tevatron Sinéad M. Farrington University of Liverpool for the CDF and D0 Collaborations Beauty 05 21 st June 2005 Outline Overall motivations 0 B d,s µ + µ Motivation CDF and D0 methods
More informationFirst two sided limit on BR(B s μ + μ - ) Matthew Herndon, University of Wisconsin Madison SUSY M. Herndon, SUSY
First two sided limit on BR(B s μ + μ - ) Matthew Herndon, University of Wisconsin Madison SUSY 2011 M. Herndon, SUSY 2011 1 B s(d) μ + μ - Beyond the SM Indirect searches for new physics Look at processes
More informationFirst two sided limit on BR(B s µ + µ - ) Matthew Herndon, University of Wisconsin Madison SUSY M. Herndon, SUSY
First two sided limit on BR(B s µ + µ - ) Matthew Herndon, University of Wisconsin Madison SUSY 2011 M. Herndon, SUSY 2011 1 B s(d) µ + µ - Beyond the SM! Indirect searches for new physics! Look at processes
More informationRare B Meson Decays at Tevatron
Rare B Meson Decays at Tevatron Walter Hopkins CDF and DØ Collaborations Cornell University FPCP 2011 Walter Hopkins (CDF and DØ Collaborations, Cornell University)Rare B Meson Decays at Tevatron FPCP
More informationWalter Hopkins. February
B s µ + µ Walter Hopkins Cornell University February 25 2010 Walter Hopkins (Cornell University) Bs µ + µ February 25 2010 1 / 14 Motivation B s µ + µ can only occur through higher order diagrams in Standard
More informationB-physics with ATLAS and CMS
Physics at LHC-2008 Split-CROATIA, 29.9. 4.10.2008 B-physics with ATLAS and CMS Brigitte Epp, Astro- and Particle Physics, University of Innsbruck, Austria representing ATLAS / CMS collaborations B-physics
More informationObservation of the rare B 0 s µ + µ decay
Observation of the rare B 0 s µ + µ decay The combined analysis of CMS and LHCb data Luke Pritchett April 22, 2016 Table of Contents Theory and Overview Detectors Event selection Analysis Flavor physics
More informationText. Decays of heavy flavour hadrons measured by CMS and ATLAS. M.Smizanska, Lancaster University
Text Decays of heavy flavour hadrons measured by CMS and ATLAS M. Outline Data collection and B-trigger strategies ID performance with increasing pileup Lifetimes B avg Bs, Bd Masses Λ b Bc Searches for
More informationSearches for BSM Physics in Rare B-Decays in ATLAS
Searches for BSM Physics in Rare B-Decays in ATLAS Iskander Ibragimov on behalf of the ATLAS Collaboration SUSY 14 The nd International Conference on Supersymmetry and Unification of Fundamental Interactions
More informationb hadron properties and decays (ATLAS)
b hadron properties and decays (ATLAS) Milind V. Purohit Univ. of South Carolina, USA for the ATLAS collaboration M. V. Purohit SM@LHC 2012 1 Outline Detector, Di muon trigger, Performance: Mass, vertex
More informationSearch for the very rare decays B s/d + - at LHCb
Search for the very rare decays B s/d + - at LHCb Justine Serrano Centre de Physique des Particules de Marseille On behalf of the LHCb collaboration EPS-HEP, July 22 th 2011, Grenoble Bs2MuMu @ LHCb Justine
More informationRare B decays in ATLAS and CMS
Rare B decays in ATLAS and CMS University Dec. 14 th 2006 Makoto Tomoto Nagoya University on behalf of CMS and ATLAS collaborations Makoto Tomoto (Nagoya University) Outline B physics in ATLAS and CMS
More informationThe X(3872) at the Tevatron
The X(387) at the Tevatron Ulrich Kerzel, University of Karlsruhe for the CDF and D0 collaborations BEAUTY 005 Physics at the Tevatron observe p p collisions at s =1.96 TeV 1 fb -1 luminosity delivered
More informationPoS(ICHEP2012)238. Search for B 0 s µ + µ and other exclusive B decays with the ATLAS detector. Paolo Iengo
Search for B s µ + µ and other exclusive B decays with the ATLAS detector. On behalf of the ATLAS Collaboration INFN Naples, Italy E-mail: paolo.iengo@cern.ch The ATLAS experiment, collecting data in pp
More informationStudies of rare B meson decays with the CMS detector
Studies of rare B meson decays with the detector J.Pazzini on behalf of the Collaboration Padova University & INFN - August - 3 J.Pazzini Studies of rare B meson decays with the detector (SUSY3) Introduction
More informationEarly physics with the LHCb detector
XXVIII PHYSICS IN COLLISION - Perugia, Italy, June, 25-28, 2008 Early physics with the LHCb detector Dirk Wiedner CERN for the LHCb collaboration 27 June 2008 Dirk Wiedner at PIC2008 Perugia 1 Outline
More informationLa ricerca dell Higgs Standard Model a CDF
La ricerca dell Higgs Standard Model a CDF Melisa Rossi INFN-TS Giornata di seminari INFN Trieste - 7 Luglio 2009 FNAL: Fermi National Accelerator Lab Tevatron currently provides the highest energy proton-antiproton
More informationRare heavy flavor decays at ATLAS & CMS
Rare heavy flavor decays at ATLAS & CMS A. Starodumov a a ETH, 8093 Zurich, Switzerland Two general purpose experiments, ATLAS and CMS, in addition to their main search/discovery program will perform a
More informationB the Tevatron
B Physics @ the Tevatron Stephanie Hansmann-Menzemer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg DESY, 9 th of November 7 xxx p.1/1 Tevatron p p collisions at s = 1.96 TeV observed by
More informationPoS(FPCP2009)013. Fabrizio Scuri I.N.F.N. - Sezione di Pisa - Italy
SLAC-PUB-15615 B µµ and B τν Decays I.N.F.N. - Sezione di Pisa - Italy E-mail: fabrizio.scuri@pi.infn.it on behalf of the BaBar, Belle, CDF and D0 Collaborations An overview of the most recent experimental
More informationThe LHCb Experiment: First Results and Prospects. Mitesh Patel (Imperial College London) The University of Birmingham, 4 th May 2011
The LHCb Experiment: First Results and Prospects Mitesh Patel (Imperial College London) The University of Birmingham, 4 th May 2011 Outline An extended Higgs sector? (B d µ + µ and B s µ + µ - ) New CP
More informationSpectroscopy and Decay results from CDF
Quarkonium Spectroscopy and Decay results from CDF KIT Quarkonium Workshop December 3, 2008 Outline Tevatron and CDF Bc Mass Lifetime bc X(3872) Mass splitting and mass X page 2 Tevatron p s = 1.96 TeV
More informationMeasurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron
Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron Mike Strauss The University of Oklahoma The Oklahoma Center for High Energy Physics for the CDF and DØ Collaborations Outline
More informationSUSY at Accelerators (other than the LHC)
SUSY at Accelerators (other than the LHC) Beate Heinemann, University of Liverpool Introduction Final LEP Results First Tevatron Run 2 Results Summary and Outlook IDM 2004, Edinburgh, September 2004 Why
More informationR. Mureşan. University of Oxford On behalf of LHCb Collaboration. Prepared for the CERN Theory Institute "Flavour as a Window to New Physics at LHC"
May 8 CERN Theory Institute Charm Physics at LHCb R. Mureşan University of Oxford On behalf of LHCb Collaboration Prepared for the CERN Theory Institute "Flavour as a Window to New Physics at LHC" R. Mureşan
More information(Towards) First Physics with LHCb
(Towards) First Physics with LHCb Beam induced splash in LHCb Physics at LHC 2008 Split, Croatia, 29 Sep - 4 Oct 2008 Introduction Detector overview and performance Extracting physics from (very) first
More informationBeauty(ful) and Charm(ing) physics with CDF II. Mario Campanelli DPNC Université de Genève
Beauty(ful) and Charm(ing) physics with CDF II Mario Campanelli DPNC Université de Genève Introduction: why? CDF is known in the physics community for having discovered the top quark, and running at the
More informationSearch for Resonant Slepton Production with the DØ-Experiment
Overview Search for Resonant Slepton Production with the DØ-Experiment Christian Autermann, III. Phys. Inst. A R-parity violating Supersymmetry Resonant Slepton Production and Neutralino Decay Data selection
More informationRare decays at LHCb Siim Tolk (NIKHEF, Amsterdam) on behalf of the LHCb Collaboration
Rare decays at LHCb Siim Tolk (NIKHEF, Amsterdam) on behalf of the LHCb Collaboration Bormio 2014 Rare decays at LHCb Siim Tolk (NIKHEF, Amsterdam) on behalf of the LHCb Collaboration Other talks from
More informationD 0 -D 0 mixing and CP violation at LHC
D -D mixing and CP violation at LHC Patrick Spradlin on behalf of the LHCb collaboration University of O Particle P 5 th International Workshop on the CKM Unitarity Triangle Rome, Italy 9-13 September
More informationReconstruction of. events in LHCb. Benjamin Carron
Reconstruction of B s J/ψ η, η c φ, J/ψ φ events in LHCb Benjamin Carron sanne Neuchâtel, March 3rd, 4 Swiss Physical Society 4 Physics Motivations Selection Procedure B s Channels analysis Selection Cuts
More informationEarly flavor physics at the LHC
Early flavor physics at the LHC Walter M. Bonivento sezione di Cagliari on behalf of the ATLAS, CMS and LHCb collaborations Thanks to: M.Smizanska (ATLAS), Urs Langenegger (CMS) and LHCb colleagues The
More informationCDF: Stato dell analisi
1 CDF: Stato dell analisi SOMMARIO Stato generale dell analisi a CDF Top/EWK physics highlights b/c physics INFN - Riunione della CSN 1 Roma 17 Maggio 2004 Giovanni Punzi SNS/INFN-Pisa 2 Data used for
More informationStatus and expectations for first physics with LHCb. M. Needham On behalf of the LHCb collaboration Symmetries and Spin July 20 th - 26 th Prague
Status and expectations for first physics with LHCb M. Needham On behalf of the LHCb collaboration Symmetries and Spin July 20 th - 26 th Prague Outline Introduction to LHCb Tour of the detector First
More informationB. Hoeneisen. Universidad San Francisco de Quito Representing the DØ Collaboration Flavor Physics and CP violation (2013)
Status report on the like-sign dimuon charge asymmetry in p p collisions and Measurement of the direct CP asymmetry in B J/ψK and B J/ψπ decays B. Hoeneisen Universidad San Francisco de Quito Representing
More informationCMS Conference Report
Available on CMS information server CMS CR 2001/004 CMS Conference Report April 13, 2001 Prospects of B-Physics with CMS a) Sunanda Banerjee 1) Abstract Prospects of studies of properties of b flavoured
More informationThe Collider Detector at Fermilab. Amitabh Lath Rutgers University July 25, 2002
The Collider Detector at Fermilab Amitabh Lath Rutgers University July 25, 2002 What is Fermilab? A user facility with the Tevatron: 4 mile ring with superconducting magnets. Collides protons with antiprotons.
More informationHQL Virginia Tech. Bob Hirosky for the D0 Collaboration. Bob Hirosky, UNIVERSITY of VIRGINIA. 26May, 2016
Bs CP-odd lifetime in Bs J/ψf0 and Afb for baryons at D0 2016 Virginia Tech Bob Hirosky for the D0 Collaboration 1 Tevatron Data D0 continues a rich physics program analyzing ~10fb-1 of recorded data from
More informationLHCb Physics and prospects. Stefano Perazzini On behalf of LHCb Collabora4on MENU nd June 2010
LHCb Physics and 2010-11 prospects Stefano Perazzini On behalf of LHCb Collabora4on MENU2010 2 nd June 2010 Physics: OUTLINE Flavor physics and CPV in the quark sector Search for New Physics The LHCb Experiment
More informationJet reconstruction in LHCb searching for Higgs-like particles
Jet reconstruction in LHCb searching for Higgs-like particles Alessandro Camboni (on behalf of LHCb Collaboration) DISCRETE'08 Valencia Dec 12th, 2008 Motivation Jet reconstruction is important for searches
More informationFirst two-sided limit of the B s µ + µ decay rate
Cornell University Floyd R. Newman Laboratory for Elementary-Particle Physics First two-sided limit of the B s µ + µ decay rate Wine and Cheese Seminar Fermilab, 7/15/2011 Julia Thom-Levy, Cornell University
More informationRecent results from rare decays
Recent results from rare decays Jeroen van Tilburg (Physikalisches Institut Heidelberg) Don t worry about the number of slides: Only half of them is new Advanced topics in Particle Physics: LHC physics,
More informationRecent Results from BaBar
Recent Results from BaBar BEACH 2008 Conference Columbia, South Carolina David Norvil Brown University of Louisville Recent Results From BaBar Physics Reach B-physics CP Violation & Mixing, CKM matrix
More informationBeauty physics with B s and Λ b
Beauty physics with B s and Λ b Rolf Oldeman INFN Roma 1 "La Sapienza" Selected topics Masses Lifetimes B s lifetime difference Charmless B s and Λ b decays B s oscillations Rare decays covered today by
More informationSearch for B (s,d) μμ in LHCb
Search for B (s,d) μμ in LHCb Diego artinez Santos (CERN) (on behalf of the LHCb Collaboration) CERN-PH-EP-011-09, submitted to PLB http://arxiv.org/abs/1103.465 1 Outline Observables: Branching Ratios
More informationLHCb Discovery potential for New Physics
Beam induced splash in LHCb Imperial College London LHCb Discovery potential for New Physics Introduction Physics with LHCb Flavour physics can provide unique input on the type of New Physics If we express
More informationMeasurement of the Dipion Mass Spectrum in the Decay X(3872) J/ψ π + π at the CDF II Experiment
Measurement of the Dipion Mass Spectrum in the Decay X(387) J/ψ π + π at the CDF II Experiment A. Rakitin June 7, 5 Thesis Defense MIT, Cambridge, Massachusetts http://www-cdf.fnal.gov/ rakitin/defense.pdf
More informationBenjamin Carron Mai 3rd, 2004
Physics Motivations Reconstruction of B s J/ψ η Benjamin Carron Mai 3rd, 4 B s J/ψ (µ + µ ) η (γγ) and B s J/ψ (e + e ) η (γγ) Selection Cuts Resolutions BR of the η B/S Ratios Annual Signal Yields and
More informationFlavour Physics at hadron machines
Flavour Physics at hadron machines KIAS Phenomenology Workshop Seoul, Korea, 17-19 November 2011 T. Nakada EPFL-LPHE Lausanne, Switzerland B physics, started with hadron machine First discovery of b-quark
More informationThe HL-LHC physics program
2013/12/16 Workshop on Future High Energy Circular Collider 1 The HL-LHC physics program Takanori Kono (KEK/Ochanomizu University) for the ATLAS & CMS Collaborations Workshop on Future High Energy Circular
More informationStatus and physics at LHCb
Vienna Seminar, Particle physics and the LHC, 26.11.11 Status and physics at LHCb, Jeroen van Tilburg 1/42 Status and physics at LHCb Vienna Central European Seminar Particle Physics and the LHC Jeroen
More informationMeasuring CP violation in. B s φφ with LHCb. Jim Libby (University of Oxford) for the LHCb collaboration. 14/12/2006 CKM 2006 Nagoya 1
Measuring CP violation in B s φφ with LHCb Jim Libby (University of Oxford) for the LHCb collaboration 4//6 CKM 6 Nagoya Outline Motivation for the study B s φφ Brief introduction to LHCb Expected signal
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. Rare B decays at CMS
Available on CMS information server CMS CR -2017/115 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 17 April 2017 (v4, 10 May 2017) Rare
More informationSUSY-related Lepton and Hadron Flavor Results from Belle Yutaro Sato
SUSY-related Lepton and Hadron Flavor Results from Belle Yutaro Sato For the Belle Collaboration (Nagoya Univ., KMI) 27 th Aug. 2015, SUSY2015 @ Lake Tahoe, USA New physics search at Belle 2 New particles
More informationSearch for long-lived particles at CMS
Search for long-lived particles at CMS Jie Chen Florida State University for the CMS Collaboration 03/19/12 Jie Chen @ SEARCH12 1 Outline Brief introduction to long-lived particle Neutral long-lived particles
More informationFlavor Physics beyond the SM. FCNC Processes in the SM
Flavor Physics beyond the SM 48 FCNC Processes in the SM A SM ( B ΔF = ΔF = 1 W q W b b u, c, t q b u, c, t q 0 q B ) ~ ( V V 0 q ) tb tq g m 16π m t W A SM ( b q) = V V tb tq g 16π m m t W FCNC in SM
More informationHeavy Flavour Physics at the LHC. Lessons from the first phase of the LHC DESY 27 September 2012
Heavy Flavour Physics at the LHC University of Warwick and CERN Lessons from the first phase of the LHC DESY 27 September 2012 1 Outline Heavy flavour production at the LHC The LHCb experiment Selected
More informationSUSY at Accelerators (other than the LHC)
SUSY at Accelerators (other than the LHC) Beate Heinemann, University of Liverpool Introduction Final LEP Results First Tevatron Run 2 Results Summary and Outlook IDM 2004, Edinburgh, September 2004 Why
More informationATLAS studies of spectroscopy and B-decays
ATLAS studies of spectroscopy and B-decays Zdeněk Doležal on behalf of the ATLAS Collaboration Charles University in Prague 53rd International Winter Meeting on Nuclear Physics 26-30 January 2015 Outline
More informationSeaches fo log-lived paticles with displaced signatues at the LHC. Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations
Seaches fo log-lived paticles with displaced signatues at the LHC Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations Outline A review of the most recent results from ATLAS &
More informationCP Violation Studies at DØ
CP Violation Studies at DØ Bd Bs Bd Bs Rick Van Kooten Indiana University For the DØ Collaboration LHCP 13 Barcelona, Spain 13 18 May 13? CP Violation Three kinds: In mixing: Mass eigenstates in mesonic
More informationD Hadronic Branching Fractions and DD Cross Section at ψ (3770) from CLEO c
D Hadronic Branching Fractions and DD Cross Section at ψ (3770) from CLEO c V. Credé 1 2 1 Cornell University, Ithaca, NY 2 now at Florida State University Tallahassee, FL Hadron 05 Outline 1 CESR-c CLEO-c
More informationLFV in Tau Decays: Results and Prospects at the LHC. Tau th International Workshop on Tau Lepton Physics Beijing September 22th, 2016
LFV in Tau Decays: Results and Prospects at the LHC Kristof De Bruyn On behalf of the ATLAS, CMS & LHCb Collaborations Tau 216 14th International Workshop on Tau Lepton Physics Beijing September 22th,
More informationExotic hidden-flavour at ATLAS: Search for X b à π + π - ϒ(1S)
Exotic hidden-flavour at ALAS: Search for X b à π + π - ϒ(1S) Cameron Cuthbert for the ALAS collaboration November 1 th 214 1 S Outline 1. Spectroscopy at ALAS he building blocks: ψ and ϒ ψ(2s) reconstruction
More informationRadiative penguins at hadron machines. Kevin Stenson! University of Colorado!
Radiative penguins at hadron machines Kevin Stenson! University of Colorado! Introduction γ + b q u,c,t W s q b q u,c,t W + s q b q ν W W + u,c,t s q!! Radiative penguins involve b to s,d transitions with
More informationCDF recent results Paolo Mastrandrea (INFN Roma) on behalf of the CDF Collaboration
CDF recent results Paolo Mastrandrea (INFN Roma) on behalf of the CDF Collaboration Società Italiana di Fisica - XCVII Congresso Nazionale - L'Aquila, 26-30 Settembre, 2011 SIF 2011, L'Aquila 26-30 September
More informationLatest time-dependent CP-violation results from BaBar
Latest time-dependent CP-violation results from BaBar Owen Long, UC Santa Barbara TM All results are preliminary XXXVIIth Rencontres de Moriond QCD and Hadronic Interactions March 17, 2002 The CKM matrix
More informationFuture and Prospects for Heavy Flavour Physics at LHC
15 October 2010 Future and Prospects for Heavy Flavour Physics at LHC Pascal Perret LPC Clermont On behalf of the ATLAS, CMS & LHCb Collaboration The present: Content LHC & Detector performances highlight
More informationB Hadron lifetimes using a displaced track trigger
B Hadron lifetimes using a displaced track trigger Why B Lifetimes are interesting Overview one analysis Results and prospects Sneha Malde University of Oxford 1 B Hadrons B Mesons B Baryons Name B + B
More informationStudy of Multimuon Events at CDF
Study of Multimuon Events at CDF Kevin Pitts University of Illinois Outline History: b production and decay puzzles from the 1990s Recent results Inclusive B cross sections bb cross section New study of
More informationSearch for the rare decays B 0 s à μ+ μ and B 0 à μ + μ. 1- Nov Hiroshi Nakano
Search for the rare decays B 0 s à μ+ μ and B 0 à μ + μ 1- Nov- 2011 Hiroshi Nakano Contents 1. Introduc@on 2. The LHCb detector 3. Analysis strategy 4. Event selec@on 5. Evalua@on of the normaliza@on
More informationA-Exam: The Rare B s µ + µ decay and tanβ
A-Exam: The Rare B s µ + µ decay and tanβ Walter Hopkins Physics Department, Cornell University. The rare B decay of B s µ + µ is a promising decay channel to find beyond the Standard Model (BSM) physics
More informationSome Thoughts on What Else to Trigger with the FTK
Some Thoughts on What Else to Trigger with the FTK Beate Heinemann, University of Liverpool Sbottom Stop Bs->mumu Other rare B decays Summary ATLAS FTK Meeting, 04/21/2005 Disclaimer: these are just a
More informationPhysics at the Tevatron. Lecture III
Physics at the Tevatron Lecture III Beate Heinemann University of California, Berkeley Lawrence Berkeley National Laboratory CERN Academic Training Lectures, November 2007 1 Outline Lecture I: The Tevatron,
More informationEvidence for D 0 - D 0 mixing. Marko Starič. J. Stefan Institute, Ljubljana, Slovenia. March XLII Rencontres de Moriond, La Thuile, Italy
Evidence for D - D mixing - D mixing (page 1) Introduction Mixing observed in K, Bd and B s (26), not yet in D system D mixing in the SM governed by box diagrams Effective GIM suppression mixing in D system
More informationBrief Report from the Tevatron. 1 Introduction. Manfred Paulini Lawrence Berkeley National Laboratory Berkeley, California 94720
Brief Report from the Lawrence Berkeley National Laboratory Berkeley, California 9472 1 Introduction It might appear surprising to include a report from the Fermilab, a proton-antiproton collider, in a
More informationBABAR results on Lepton Flavour Violating (LFV) searches for τ lepton + pseudoscalar mesons & Combination of BABAR and BELLE LFV limits
BABAR results on Lepton Flavour Violating (LFV) searches for τ lepton + pseudoscalar mesons & Combination of BABAR and BELLE LFV limits Swagato Banerjee 9 th International Workshop on Tau Lepton Physics
More informationLHCb results and prospects
LHCb results and prospects M. Witek (IFJ PAN Cracow, Poland) On behalf of the LHCb Collaboration Miami 2011 Conference Fort Lauderdale, Florida 800 physicists 15 countries 54 institutes CERN LHC Large
More informationResults from B-Physics (LHCb, BELLE)
Prospects for Charged Higgs Uppsala, Sweden, 16-18 September 2014. Results from B-Physics (LHCb, BELLE) Valery Pugatch Kiev Institute for Nuclear Research, NASU On behalf of the LHCb Collaboration 1 OUTLINE
More informationElectroweak Physics at the Tevatron
Electroweak Physics at the Tevatron Adam Lyon / Fermilab for the DØ and CDF collaborations 15 th Topical Conference on Hadron Collider Physics June 2004 Outline Importance Methodology Single Boson Measurements
More informationMatthew Charles, University of Iowa
Charm Decays in Matthew Charles, University of Iowa Representing the Collaboration The 3nd International Conference on High Energy Physics Beijing August 16, 4 Introduction Search for D l + l [11-964]
More informationBelle results on Lepton Flavor Violation in tau decays. K. Inami (Nagoya Univ.) for Belle collaboration
Belle results on Lepton Flavor Violation in tau decays K. Inami (Nagoya Univ.) for Belle collaboration 2 Belle B factory at KEK KEKB: e + (3.5 GeV) e (8GeV) σ(ττ)~0.9nb, σ(bb)~1.1nb A B factory is also
More informationFlavour Physics at LHC
Flavour Physics at LHC ICFP2009, Hanoi, September 2009 Tatsuya Nakada LPHE/EPFL Introduction (I) There exist solid observations for physics beyond the Standard Model T. Nakada ICFP2009 Hanoi September
More informationTop and Electroweak Physics at. the Tevatron
Top and Electroweak Physics at 1 the Tevatron Graham W. Wilson University of Kansas for the CDF and DØ Collaborations April APS 2008, St. Louis, MO. April 12 th 2008 Introduction Top Physics Overview Cross-section
More informationRecent Results on New Phenomena and Higgs Searches at DZERO
Recent Results on New Phenomena and Higgs Searches at DZERO Neeti Parashar Louisiana Tech University Ruston, Louisiana U.S.A. 1 Outline Motivation for DØ Run II Detector at Fermilab The Fermilab Tevatron
More informationarxiv: v1 [hep-ex] 2 Dec 2010
Status and Prospects for Heavy Flavour Physics at LHC arxiv:101.0511v1 [hep-ex] Dec 010 Clermont Université - CNRS/INP3 - Laboratoire de Physique Corpusculaire - BP 8006 - F 63177 Aubière Cedex - France
More informationStudy of Bs J/ψη and Bs J/ψη' decays at LHCb
21st International Conference on Supersymmetry and Unification of Fundamental Interactions ICTP Trieste, Italy, 26 31 August 2013 Study of Bs J/ψη and Bs J/ψη' decays at LHCb D. Savrina (ITEP&SINP MSU)
More informationclfv & BNV LHCb Gerco Onderwater on behalf of the LHCb collaboration
clfv & BNV Searches @ LHCb Gerco Onderwater on behalf of the LHCb collaboration Flavour2017, Qui Nhơn, Việt Nam, 13-19 August 2017 2 34 Outline LHCb Experiment LFV with muons : τ LFV with electrons : D0
More informationStudies of charmonium production in e + e - annihilation and B decays at BaBar
Studies of charmonium production in e + e - annihilation and B decays at BaBar I. Garzia, INFN Sezione di Ferrara On behalf of the BaBar Collaboration XVI International Conference on Hadron Spectroscopy
More informationProduction and Decays of Heavy Flavours in ATLAS
Production and Decays of Heavy Flavours in ATLAS Vincenzo Canale Università di Napoli Federico II and INFN Alessandro Cerri University of Sussex Xth Rencontres du Vietnam - Flavour Physics Conference ICISE,
More informationRESULTS FROM B-FACTORIES
XL International Meeting on Fundamental Physics Benasque, May 12 RESULTS FROM B-FACTORIES (IFIC Valencia) τ - τ + τ - τ + B factories KEKB s=10.58 GeV e + e- Υ(4s) Υ(4s) B B z ~ c βγ τ B ~ 200µm BaBar
More informationAnalysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments
Analysis of a Multi-Muon Signal at Collider and Fixed-Target Experiments In Collaboration with Manuel Drees August 23rd, 2010 SUSY10 1 Introduction 2 Ghost Events 3 Simulation 4 Outlook and Summary Introduction
More informationThe Compact Muon Solenoid Experiment. CMS Note. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. CMS prospects for heavy flavour physics
Available on CMS information server CMS NOTE -2011/008 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 10 November 2011 (v2, 14 November 2011) CMS
More informationSearches for Leptonic Decays of the B-meson at BaBar
Searches for Leptonic Decays of the B-meson at BaBar Stephen Jacob Sekula (MIT) on behalf of the BaBar collaboration Presented at Frontiers in Contemporary Physics III Vanderbilt University May 22-28,
More informationLatest results on b- physics from the ATLAS and CMS experiments. E. Pasqualucci (INFN Roma) On behalf of the ATLAS and CMS Collaborations
Latest results on b- physics from the ATLAS and CMS experiments E. Pasqualucci (INFN Roma) On behalf of the ATLAS and CMS Collaborations Latest ATLAS and CMS results Rare and semi- rare B 0 (s) decays
More informationMeasurement of the. Maren Ugland. Bergen group meeting
Measurement of the B µµ BF s Maren Ugland Bergen group meeting - 25.11.2009 Introduction Neutral B-meson decays to two leptons are very sensitive to new physics. Since B s 0 l + l - involves a flavor changing
More informationarxiv: v1 [hep-ex] 20 Jan 2013
Heavy-Flavor Results from CMS arxiv:.69v [hep-ex] Jan University of Colorado on ehalf of the CMS Collaoration E-mail: keith.ulmer@colorado.edu Heavy-flavor physics offers the opportunity to make indirect
More informationBelle Hot Topics. Nagoya University Koji Ikado (for the Belle Collaboration) Flavor Physics and CP Violation Conference (FPCP2006) Apr.
Belle Hot Topics Nagoya University Koji Ikado (for the Belle Collaboration) Flavor Physics and CP Violation Conference (FPCP2006) Apr. 9, 2006 Outline Search for the Purely Leptonic Decay Β τν Results
More informationAnalysis of a Λ 0 b decay mode
Analysis of a Λ 0 b decay mode María Magdalena Falla Solórzano Advisor Dr. Héctor Méndez Puerto Rico University HEP Group Master of Science in Physics Presentation May 2, 2013 1 Outline 1. OBJECTIVES 2.
More informationWeak Decays, CKM, Anders Ryd Cornell University
Weak Decays, CKM, CP Violation Anders Ryd Cornell University Presented at the International Conference on Weak Interactions and Neutrinos Delphi, Greece, June 6-11, 2005 Page: 1 Flavor Physics The study
More information