K K π +- Preliminary Results on γ γ
|
|
- Julian Kennedy
- 5 years ago
- Views:
Transcription
1 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ Two-Photon Production of Hadron K K π e + e + γ Global objective: provide data to undertand the phenomenon of confinement by tudying hadronic reonance below 1.7 GeV/c 2 that decay into K K π final tate. e - γ Repreenting CLEO Collaboration vp3@pitt.edu e - Motivation Experimental Tool Selection Criteria Sytematic Preliminary Reult Interpretation PANIC 02 1 October 3, 2002
2 Vladimir Savinov, Univerity of Pittburgh γ γ η(1440) Preliminary Reult on γ γ PANIC 02 2 October 3, 2002 K K π K K π Undertanding Hadron Ma Spectrum Quantatively would be Fundamental Verification of Low-Energy QCD Do we undertand thi pectrum theoretically? ak a theorit... Do we undertand thi pectrum experimentally? NO Check PDG review and try to make ene of all reported low-ma reonance! Thi tudy: hadron with mae below 1.7 GeV/c that decay to final tate K K π Experimental tool: production in two-photon colliion: Two-photon cro ection ~ Γ F (Q, Q ) γ γ Propertie of two-photon event: booted along beam axi, difficult to trigger on, tranvere momentum of the entire event peak at low value, no glueball produced 2
3 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ Experimental Statu of η(1440) Ma region between 1200 and 1500 MeV contain everal poorly-undertood hadron. Some of thee are, poibly, due to gluonic degree of freedom. η(1440) i one of thee hadron: wa oberved in hadron colliion and radiative decay of J/ϕ, not oberved in two-photon colliion until recently - glueball? Experiment diagree about the propertie of thi reonance... K K π PANIC 02 3 October 3, 2002
4 Vladimir Savinov, Univerity of Pittburgh L3 Collaboration / Phyic Letter B 501 (2001) 1 11 Recent new on η(1440) Preliminary Reult on γ γ K K π (BR ~ 1 for - meon) Γ γγ too mall for a meon - mixing with a glueball? An independent verification would be very ueful, alo, expecting larger ignal with CLEO PANIC 02 4 October 3, 2002
5 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ K K π Helium Reervoir Muon Chamber Superconducting Coil Barrel Shower Detector Drift Chamber SVX Detector Micro-Beta Quadrupole Vertex Detector End Cap Time of Flight Pole Tip Shower Detector Time of Flight Scintillator Magnet Yoke raf Meter PANIC 02 5 October 3, 2002
6 Vladimir Savinov, Univerity of Pittburgh Event Selection Criteria Preliminary Reult on γ γ K K π - Exactly four recontructed charged track in the entire detector (13% efficiency, 20% yt.) - Exactly 1 K candidate (vertex radially diplaced by two or more tandard deviation - Signal candidate propertie: - tranvere momentum below 100 MeV/c Thi election i baed (in part) on the hermeticity of CLEO detector, efficiency i hown for 1475 MeV - amount of energy detected in calorimeter in unmatched cluter below 100 MeV - at leat one large tranvere momentum track reaching barrel calorimeter - make ure event were recorded with reliable trigger and pa beam-ga rejection - 3 tandard deviation PID coniteny for charged K and non-k π uing TOF and dedx Efficiency of thi election for MC ample (independent data i alo ued): Signal MC (η(1440)): 0.84% (total ytematic i 30%) Thi i not unuual for low-ma untagged two-photon event PANIC 02 6 October 3, 2002
7 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ K K π Uing Data to Meaure Efficiencie and Etimate Sytematic Excluive two-photon K pair in data Event / 5 MeV/c 2 inv. ma K (GeV/c ) 2 inv. ma K (GeV/c ) 2 Invariant ma of K K candidate 2 (GeV/c ) PANIC 02 7 October 3, 2002
8 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ K K π Two-Photon K Pair Below 1.4 GeV/c 2 are utilized Tranvere momentum in calibration data (point) and ignal MC (line) P (GeV/c) 2 (GeV/c ) Invariant ma of K candidate in calibration data at low invariant ma PANIC 02 8 October 3, 2002
9 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ Tight Selection Criteria and Two-Photon Background K K π Tranvere momentum v unmatched energy for bckg K * + K * - two-photon MC - thi effect i verified in data! DATA election affect the hape of ptran (GeV/c) P Signal MC P (GeV/c) ame hape before and after election E (GeV) Tranvere momentum for ignal candidate in data (below 2 GeV/c 2 ) and ignal η(1440) MC before and after unmatched energy election PANIC 02 9 October 3, 2002
10 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ Some Important Ditribution in Signal Data K K π kev/cm dedx 1/β TOF (W < 2.0 GeV/c 2) P(GeV/c) Thee ditribution are hown for data after applying all election criteria (for right plot we removed PID requirement). Plot prove that there are K K π event in data. PANIC October 3, 2002
11 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ Teting the Analyi on η Μeaurement c K K π Tight election Looened election We obtain central value of 6.7 kev in both tet, while we reported Γ γγ (η ) = 7.6 kev 0.8 kev (PRL 85, 3095 (2000)) - good (ame data ued). c PANIC October 3, 2002
12 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ K K π Invariant Ma Ditribution for Signal Candidate Can only do upper limit, no obervation. I thi urpriing? Not necearily: L3 integrated luminoity: 3% of CLEO but L3 γγ cro ection: 6 time larger We can do qrt(5) better with bckg 90% CL UL: approx. < 33 event Efficiency (with ytematic): Luminoity: 13.8 invere femtobarn Cro ection per 1 kev γγ width: 36 pb Setting 90% CL UL on the product: Γ (η(1440)) Β (η(1440) > ) γγ K K π < 14 ev (ytematic included, preliminary) (L3 report: ev for thi value) PANIC October 3, 2002
13 Vladimir Savinov, Univerity of Pittburgh Preliminary Reult on γ γ K K π Two More Fit for Other Ma and Width Hypothee PANIC October 3, 2002
14 Vladimir Savinov, Univerity of Pittburgh Concluion Preliminary Reult on γ γ K K π In our analyi we do not oberve any narrow reonance between 1.3 GeV and 1.7 GeV, alo, we do not confirm L3 obervation. For example, auming M = GeV, Γ = 50 MeV Γ (η(1440)) Β (η(1440) > ) γγ We et upper limit on the product of partial two-photon width and branching fraction (K branching fraction included) K K π < 14 ev (thi i 2.9 σ below L3 number of 49 ev 12 ev) Final reult of our analyi will include table of upper limit etimated uing variou value for the mytery reonance ma and width (analyi continue). PANIC October 3, 2002
Introduction The CLEO detector and Y(5S) data sample Analysis techniques: Exclusive approach Inclusive approach Summary
Introduction The CLEO detector and Y(5S) data ample Analyi technique: Excluive approach Incluive approach Summary Victor Pavlunin Purdue Univerity CLEO collaboration Preented at Firt Meeting of the APS
More informationMeasurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron
Meaurement of the Mae, Mixing, and Lifetime, of Hadron at the Tevatron Mike Strau The Univerity of Oklahoma for the CDF and DØ Collaboration 5 th Rencontre du Vietnam Hanoi, Vietnam Augut 5-11, 2004 Outline
More informationvided a long detailed ummary of what i known about the B meon branching fraction, and life time. Mot of the information they reported on the B meon br
An Update on CLEO' Study of B Meon Decay Bernard Gittelman Cornell Univerity - thaca New York, USA ntroduction The family of meon wa dicovered at Fermilab[1] in 1977. At that time, purely by coincidence
More information& & #!" # BABAR $ % Belle Conversano - 15 June 03
& & # ' (!" # BABAR $ % Belle QC@Work Converano - 15 June 3 Outline c )) & '# )', - "#'(" '&, " (/) ' %( (&, "."##(" Spectrocopy of c tate Potential model of [heavy-quark light-quark] meon have had o far
More informationD (s) Hadronic Decays From CLEO-c
D () Hadronic Decay From CLEOc e e D D D D γ γ π π Peter Onyii Cornell Univerity CLEO Collaboration Charm 26, June 57, 26 Peter Onyii CLEOc Charm Hadronic Decay Charm 26 1 / 37 Outline Scope of hadronic
More informationHeavy Flavour results from Tevatron
Heavy Flavour reult from Tevatron G.Boriov, Lancater Univerity, UK On behalf of CF and Ø collaboration Moriond-EW conference, la Thuile, 08 February 2012 Introduction For pat 10 year the Tevatron ha pioneered
More informationCLEO Results From Υ Decays
CLEO Results From Υ Decays V. Credé 1 2 1 Cornell University, Ithaca, NY 2 now at Florida State University Tallahassee, FL Hadron 05 Outline 1 Introduction The Υ System CLEO III Detector CLEO III Υ Data
More informationZ ττ Observation Status
Obervation Statu Standard Model Plenary Meeting, CERN Ryan Reece Univerity of Pennylvania Novemeber 12, 21 On behalf of the ubgroup Ryan Reece Penn ryan.reece@cern.ch Obervation Statu 1 / 32 Outline l
More informationOBSERVATION OF THE DALITZ DECAY OF THE FIRST EXCITED STATE OF THE CHARMED-STRANGE MESON
OBSERVATION OF THE DALITZ DECAY OF THE FIRST EXCITED STATE OF THE CHARMED-STRANGE MESON A Diertation Preented to the Faculty of the Graduate School of Cornell Univerity in Partial Fulfillment of the Requirement
More informationProduction asymmetries of b and c hadrons at LHCb
Journal of Phyic: Conference Serie PAPER OPEN ACCESS Production aymmetrie of b and c hadron at o cite thi article: F Ferrari and Collaboration 26 J. Phy.: Conf. Ser. 77 25 Related content - Hadron Beam
More informationStudy of e + e annihilation to a proton-antiproton pair. Vladimir Druzhinin BINP, Novosibirsk
Study of e + e annihilation to a proton-antiproton pair Vladimir Druzhinin BINP, Novoibirk e + e - pp cro ection b E p M E G m G C 4, ) ( ) ( 3 ) ( 4 ) ( C i the Coulomb factor. The cro ection i nonzero
More informationHadronic D Decays and the D Meson Decay Constant with CLEO c
Hadronic D Decays and the D Meson Decay Constant with CLEO c representing the CLEO Collaboration presented at the 3nd International Conference on High Energy Physics, Beijing, China, Aug. 16, 004 This
More informationSetting the Charm Decay Scale
Setting the Charm Decay Scale e e D D D D γ γ π π Peter Onyii Cornell Univerity CLEO Collaboration Texa A&M, 21 Apr 26 Peter Onyii Charm Hadronic BF Texa A&M, 21 Apr 26 1 / 38 Outline Intro to CLEOc Open
More informationAbsolute D Hadronic Branching Fractions at CLEO-c
Absolute D Hadronic Branching Fractions at CLEO-c Xin Shi Cornell University CLEO Collaboration Lake Louise Winter Institute 24 February 2011 Xin Shi (Cornell University) Absolute D Hadronic BFs at CLEO-c
More informationarxiv: v1 [hep-ex] 1 Oct 2013
arxiv:131.89v1 [hepex] 1 Oct 13 Charge Aymmetrie in Semileptonic B Decay Lancater Univerity Email: i.ertram@lancater.ac.uk I preent meaurement made y the D collaoration of the timeintegrated flavorpecific
More informationSearch for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum in Run2
Search for quark and luino with the ATLAS detector in final tate with jet and miin tranvere momentum in Run Naoya Univerity E-mail: yuta@hepl.phy.naoya-u.ac.jp Depite the abence of experimental evidence,
More informationStudies of Rare Beauty and Charm Decays with the CMS Experiment
Studie of Rare eauty and Charm Decay with the CMS Experiment Joe Lazo-Flore (UNL) for the CMS Collaboration SUSY eijing, China Augut 3, Outline The CMS detector Tracking and Muon recontruction -Phyic trigger
More informationKai Yi! University of Iowa. on behalf of the CMS Collaboration
Kai Yi! Univerity of Iowa on behalf of the CMS Collaboration Outline Motivation! The CMS detector and Jet Recontruction! Monojet + MET! Dijet Reonance! Multijet Reonance! Multijet Tranvere Momentum Sum
More informationCP Violation Studies in the Bs System at DØ
CP Violation Studie in the B Sytem at DØ B B? Rick Van Kooten Indiana Univerity Repreenting the DØ Collaboration 35th International Conference on High Energy Phyic Pari, France 4 July 1 CP Violation in
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 informationB physics results from the Tevatron mixing and CP violation
phyic reult from the Tevatron mixing and CP violation for the CDF and DØD collaboration Moriond EW 2009 La Thuile, Italy 1 Introduction Mixing meaurement M (DØ & CDF) Semileptonic aymmetry A l Mixing interference
More informationPoS(EPS-HEP2015)543. Measurements of CP violation in B mixing through B J/ψ X decays at LHCb. Greig A. Cowan
Meaurement of CP violation in B mixing through B J/ψ X decay at Univerity of Edinburgh E-mail: g.cowan@ed.ac.uk B meon provide an ideal laboratory for meaurement of CP violation and earche for CP violation
More informationCLEO c. Anders Ryd Cornell University June 7, e e cc D D. D K,D K e
CLEOc Cornell University June 7, 25 e e cc D D D K,D K e K K e 1 Outline CLEOc experiment and the physics program Some early results D> Absolute hadronic branching fractions Semileptonic decays 2 Testing
More informationNew Physics search with LHCb. A.Hicheur (EPF Lausanne) Moriond QCD 2008
New Phyic earch with LHC A.Hicheur (EPF Lauanne) Moriond QCD 2008 Outline General framework decriing weak decay here to dig for NP? Studie covered in thi talk B ocillation Meaurement of ocillation parameter
More informationLHCb Physics, Performance, Prospects
7th Patra Workhop Mykono, June 26-July 1, 211 LHCb Phyic, Performance, Propect Olaf Steinkamp on behalf of the LHCb collaboration Phyik-Intitut der Univerität Zürich Winterthurertrae 19 CH-857 Zürich olaf@phyik.uzh.ch
More informationSearch for heavy neutrinos in kaon decays
Search for heavy neutrinos in kaon decays L. Littenberg (work mainly done by A.T.Shaikhiev INR RAS) HQL-2016 Outline Motivation Previous heavy neutrino searches Experiment BNL-E949 Selection criteria Efficiency
More informationSEARCHES FOR SUPERSYMMETRY IN EVENTS CONTAINING A Z BOSON, JETS AND MISSING TRANSVERSE MOMENTUM
SEARCHES FOR SUPERSYMMETRY IN EVENTS CONTAINING A Z BOSON, JETS AND MISSING TRANSVERSE MOMENTUM NExT Workhop 9 April 05 Emma Kuwertz on behalf of the Collaboration Univerity of Victoria Overview Preenting
More informationLight-Meson Spectroscopy at Jefferson Lab
Light-Meson Spectroscopy at Jefferson Lab Volker Credé Florida State University, Tallahassee, Florida PANDA Collaboration Meeting Uppsala, Sweden 06/10/2015 Outline Introduction 1 Introduction 2 Detector
More informationTop quark pair production measurements using the ATLAS detector at the LHC
op quark pair production meaurement uing the ALAS detector at the LHC Ki Lie on behalf of the ALAS Collaboration Univerity of Illinoi at Urbana-Champaign Phenomenology 25 May 5th, 25 K. Lie (Univ. of Illinoi)
More informationAnalysis of the forbidden decay 0 +e + +e with WASA-at-COSY
Analysis of the forbidden decay 0 +e + +e with WASA-at-COSY Florian Bergmann 23.03.2011 1 Reminder: C-parity C-operator: turns particle into antiparticle E.g.: C e = C e C: phase factor Majorana particle:
More informationRecent CMS results on heavy quarks and hadrons. Alice Bean Univ. of Kansas for the CMS Collaboration
Recent CMS results on heavy quarks and hadrons Alice Bean Univ. of Kansas for the CMS Collaboration July 25, 2013 Outline CMS at the Large Hadron Collider Cross section measurements Search for state decaying
More informationMeasurement of B s Oscillations and CP Violation Results from DØ
Meaurement of B Ocillation and CP Violation Reult from DØ John Ellion Univerity of California, Riveride for the DØ Collaboration PANIC 008, Eilat, Irael 1 The DØ Detector Tracker: Excellent coverage η
More informationMeasurement of the e + e - π 0 γ cross section at SND
Measurement of the e + e - π 0 γ cross section at SND L.Kardapoltsev (for SND collaboration) Budker Institute of Nuclear Physics, Novosibirsk state university PhiPsi 2017, Mainz, Germany June 2017 Outline
More informationSearch for Gluonic Excitations with GlueX at Jefferson Lab
Search for Gluonic Excitations with GlueX at Jefferson Lab Volker Credé Florida State University Tallahassee, FL The Structure and Dynamics of Hadrons Hirschegg, 01/19/2007 Outline 1 2 3 4 Outline 1 2
More informationLight flavor hadron production as a function of the chargedparticle multiplicity at the LHC
IL NUOVO CIMENO C (7) 7 DOI.9/ncc/i7778 Colloquia: IFAE 6 Light flavor hadron production a a function of the argedparticle multiplicity at the LHC N. Jacazio( )( ) on behalf of the ALICE Collaboration
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 informationStrangeonia. Of the 22 expected resonances, only 7 are well identified. Strangeonia. η-η' h1 (1386) (1020) f2' (1525) f1 (1426) (1680)
C o l u m n 3 Mukesh Saini Florida State University, Tallahassee, FL, 2010 1 Strangeonia Strangeonia s s Of the 22 expected resonances, only 7 are well identified η-η' (1020) h1 (1386) f1 (1426) f2' (1525)
More informationB B. Mass (GeV/c 2 ) σ (e + e - Hadrons)(nb)
NEW RESULTS ON CLEO'S HEAVY QUARKS BOTTOM AND CHARM Scott Menary Univerity of California, Santa Barbara menary@charm.phyic.ucb.edu Repreenting the CLEO Collaboration ABSTRACT While the top quark i conned
More informationBeauty 2013, Bologna. Measurements of CP violation and mixing in Bs. 0 decays at LHCb. on behalf of the LHCb collaboration
LPHE Beauty 13, Bologna Meaurement of CP violation and mixing in B decay at Frédéric Dupertui on behalf of the collaboration Laboratoire de Phyique de Haute Energie (LPHE) Ecole Polytechnique Fédérale
More informationMeasurements of the W Boson Mass and Trilinear Gauge Boson Couplings at the Tevatron
Measurements of the Boson Mass and Trilinear Gauge Boson Couplings at the Tevatron John Ellison University of California, Riverside, USA Selection of and Z events Measurement of the mass Tests of the gauge
More informationMukesh Saini. Florida State University, Tallahassee, FL. February 26, FSU Nuclear Physics Seminar. February 26
C o l u m n 3 Mukesh Saini Florida State University, Tallahassee, FL, 2010 1 OUTLINE Introduction Meson Spectroscopy Strangeonia Experiment CEBAF & CLAS HyCLAS & g12 Calibrations Analysis Summary 2 QCD
More informationCLEO-c: Progress and Future
CLEO-c: Progress and Future David G. Cassel Cornell University Outline Motivations CLEO-c and CESR-c Preliminary CLEO-c Results CLEO-c Gluonic Program Summary and Outlook SURA Washington February 10, 2005
More informationMuon commissioning and Exclusive B production at CMS with the first LHC data
Muon commissioning and Exclusive B production at CMS with the first LHC data Silvia Taroni INFN Milano Bicocca On the behalf of the CMS collaboration Outline Introduction CMS detector Muon detection in
More informationExperimental Search for the Decay
Experimental Search for the Decay νν K. Mizouchi (Kyoto University) (1) Physics Motivation (2) Detector (3) Selection Criteria (4) Branching Ratio (5) γγ Background Subtraction (6) Conclusions νν : Physics
More informationCurrent status and results of the experiments at VEPP-2000
Current status and results of the experiments at VEPP-2000 Boris Shwartz, BINP, Novosibirsk, Introduction VEPP-2000 status Detectors Preliminary results 17.06.2013 MesonNet meeting, Prague, Czech Republic
More informationphysics program (searching new physics hidden in beauty and charm) S. T Jampens LAPP (CNRS/IN2P3 and Université de Savoie)
phyic program (earching new phyic hidden in beauty and charm) b b b S. T Jampen LAPP (CNRS/IN2P3 and Univerité de Savoie) On behalf of the LHCb collaboration Outline LHCb experiment LHCb environment at
More informationStudy of Baryon Form factor and Collins effect at BESIII
Study of Baryon Form factor and Collins effect at BESIII Wenbiao Yan On behalf of BESIII Collaboration INT Program INT-17-3 Hadron imaging at Jefferson Lab and at a future EIC 1 Bird s View of BEPCII &
More informationCDF Run II Status and prospects
CF Run II Statu and propect C. Pagliarone INFN-Pia, V. Livornee 191, 561 Pia, Italy e-mail: pagliarone@fnal.gov (On the behalf of the CF Collaboration) Abtract Run II at the evatron Collider tarted at
More informationRecent results at the -meson region from the CMD-3 detector at the VEPP-2000 collider
Recent results at the -meson region from the CMD-3 detector at the VEPP-2000 collider Vyacheslav Ivanov *1, Evgeny Solodov 1, Evgeny Kozyrev 1, and Georgiy Razuvaev 1 1 Budker Institute of Nuclear Physics,
More informationMINITAB Stat Lab 3
MINITAB Stat 20080 Lab 3. Statitical Inference In the previou lab we explained how to make prediction from a imple linear regreion model and alo examined the relationhip between the repone and predictor
More informationQuark-Gluon Plasma in Proton-Proton Scattering at the LHC?
Quark-Gluon Plama in Proton-Proton Scattering at the LHC? K. Werner (a), Iu. Karpenko (b), T. Pierog (c) (a) SUBATECH, Univerity of Nante INP/CNRS EMN, Nante, France (b) Bogolyubov Intitute for Theoretical
More informationhadronic decays at BESIII Abstract hadronic decays using a double tag technique. Among measurement for twelve Λ c
hadronic decays at BESIII Qingnian XU 1 University of Chinese Academy of Sciences (UCAS) 19B Yuquan Lu, Shijingshan District, Beijing, China E-mail:xuqingnian10@mails.ucas.ac.cn. Abstract Based on 567
More informationThe BES-III experiment
The BES-III experiment Igor Denysenko for the BES-III collaboration JINR Dubna on leave from BITP, Kiev Hadron Structure and QCD July 4-8, 2012, Gatchina, Russia BEPCII/BESIII at IHEP(Beijing) 2004: start
More informationp and transverse momentum p BF
Strangene roduction at high Q with the H detector Julia E. Ruiz abaco Centro de Invetigacione y Etio Avanzado del Intituto Politécnico Nacional Antigua carretera a Progreo Km. 6 97, Mérida, Yucatán, México
More informationarxiv:hep-ex/ v1 10 Nov 2000
Recent Results from BES arxiv:hep-ex/1132v1 1 Nov 2 Xiaoyan Shen Representing the BES Collaboration Institute of High Energy Physics, Academy of Sciences, Beijing 139, P.R. China Abstract We report partial
More informationLepton Universality in ϒ(nS) Decays at CLEO
Hajime Muramatsu, University of Rochester BNM2008@ATAMI JAPAN JAN/2008 1 Lepton Universality in ϒ(nS) Decays at CLEO Hajime Muramatsu University of Rochester For the CLEO Collaboration Hajime Muramatsu,
More informationHadron Spectroscopy Lecture 1 Introduction and Motivation
Hadron Spectroscopy Lecture 1 Introduction and Motivation National Nuclear Physics Summer School at MIT Matthew Shepherd Indiana University Outline 1. Overview and Motivation 1.1.Uniue features of QCD
More informationLecture 7: Testing Distributions
CSE 5: Sublinear (and Streaming) Algorithm Spring 014 Lecture 7: Teting Ditribution April 1, 014 Lecturer: Paul Beame Scribe: Paul Beame 1 Teting Uniformity of Ditribution We return today to property teting
More informationSearches for Exotics in Upsilon Decays in BABAR
Searches for Exotics in Upsilon Decays in BABAR Yury Kolomensky UC Berkeley/LBNL For the BABAR Collaboration 14th Lomonosov Conference on Elementary Particle Physics August 24, 2009, Moscow Light Higgs
More informationVol. 5 (2012) Acta Physica Polonica B Proceedings Supplement No 4 PANDA AT FAIR. Tord Johansson. representing the PANDA Collaboration
Vol. 5 (2012) Acta Physica Polonica B Proceedings Supplement No 4 PANDA AT FAIR Tord Johansson representing the PANDA Collaboration Departmet of Physics and Astronomy, Uppsala University Box 516, 75120
More informationVincent Poireau CNRS-IN2P3, LAPP Annecy, Université de Savoie, France On behalf of the BaBar collaboration
CNRS-IN2P3, LAPP Annecy, Université de Savoie, France On behalf of the BaBar collaboration Moriond QCD, 24 March 2014 1 OUTLINE 9 GeV e - 3.1 GeV e + Recorded 531 fb -1 in total (4S): 433 fb -1 (3S): 30
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 informationZ a>2 s 1n = X L - m. X L = m + Z a>2 s 1n X L = The decision rule for this one-tail test is
M09_BERE8380_12_OM_C09.QD 2/21/11 3:44 PM Page 1 9.6 The Power of a Tet 9.6 The Power of a Tet 1 Section 9.1 defined Type I and Type II error and their aociated rik. Recall that a repreent the probability
More informationAlice TPC particle identification
Alice TPC particle identification on the way to Anti-Nuclei and exotic states INTERNATIONAL SCHOOL OF NUCLEAR PHYSICS 34th Course Probing the Extremes of Matter with Heavy Ions Erice-Sicily: 16-24 September
More informationStudy on the Two-Photon Transition from ψ(2s) to J/ψ at BESIII
Study on the Two-Photon Transition from ψ(2s) to J/ψ at BESIII 吕晓睿 Xiao-Rui Lu (E-mail: xiaorui@gucas.ac.cn) Graduate University of Chinese Academy of Sciences (GUCAS) List of Contents: Introduction (on
More informationChapter 12 Simple Linear Regression
Chapter 1 Simple Linear Regreion Introduction Exam Score v. Hour Studied Scenario Regreion Analyi ued to quantify the relation between (or more) variable o you can predict the value of one variable baed
More informationMeasurement of the η mass by the NA48 Experiment
Measurement of the η mass by the NA48 Experiment Rainer Wanke Institut für Physik, Universität Mainz Crystal Ball Meeting Mainz, March 20, 2004 Rainer Wanke, Crystal Ball Meeting, Mainz, March 20, 2004
More informationarxiv:hep-ex/ v1 4 Jun 2001
T4 Production at Intermediate Energie and Lund Area Law Haiming Hu, An Tai arxiv:hep-ex/00607v 4 Jun 00 Abtract The Lund area law wa developed into a onte Carlo program LUARLW. The important ingredient
More informationNew Limits on Heavy Neutrino from NA62
CERN E-mail: michal.koval@cern.ch The NA6 experiment at CERN collected large samples of charged kaon decays in flight with a minimum bias trigger configuration in 7 and in 15 using a completely new detector
More informationIdentification of Central Production in the π + π π + π Channel at COMPASS
Identification of Central Production in the π + π π + π Channel at COMPASS ASI-Spin-Praha-009 Johannes Bernhard for the COMPASS collaboration Institut für Kernphysik Mainz July 8 th Outline 1 Introduction
More informationStudy of Transitions and Decays of Bottomonia at Belle
1 Study of Transitions and Decays of Bottomonia at Belle Saurabh Sandilya University of Cincinnati (On behalf of the Belle Collaboration) Outline Introduction (Bottomonia, KEKB & Belle detector) Transitions
More informationThreshold photoproduction of J/y with the GlueX experiment. Lubomir Pentchev Jefferson Lab for the GlueX collaboration
Threshold photoproduction of J/y with the GlueX experiment Lubomir Pentchev Jefferson Lab for the GlueX collaboration 7 th Workshop of the APS Topical Group on Hadron Physics, Washington, DC February 1-3
More informationStatus / Hadron Spectroscopy at COMPASS
Status / Hadron Spectroscopy at COMPASS Johannes Bernhard 1 Institut für Kernphysik Mainz January 22 nd 2010 1 johannes.bernhard@cern.ch Outline 1 Introduction 2 Recoil Proton Detector 3 Trigger 4 Analysis
More informationBolt stress inspection by Electromagnetic Acoustic Transducer(EMAT) and PZT
Bolt tre inpection by Electromagnetic Acoutic Tranducer(EMAT) and PZT Y.P. Shen 1, G.B. Ma 2,3, C. Ma 2, X.X. Zhu 1 and J.H. Zhao 1 More info about thi article: http://www.ndt.net/?id=22223 Abtract 1 Phaerie
More informationPrecision measurement of kaon radiative decays in NA48/2
Precision measurement of kaon radiative decays in NA48/2 INFN Sezione di Perugia E-mail: monica.pepe@pg.infn.it Kaon decays are an excellent laboratory to test low energy strong interaction perturbative
More informationTransverse momentum spectra of identified charged hadrons with the ALICE detector in Pb-Pb collisions at the LHC
Transverse momentum spectra of identified charged hadrons with the ALICE detector in Pb-Pb collisions at the LHC for the ALICE Collaboration Museo Storico della Fisica e Centro Studi e Ricerche Enrico
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 informationEmittance limitations due to collective effects for the TOTEM beams
LHC Project ote 45 June 0, 004 Elia.Metral@cern.ch Andre.Verdier@cern.ch Emittance limitation due to collective effect for the TOTEM beam E. Métral and A. Verdier, AB-ABP, CER Keyword: TOTEM, collective
More informationThe Jefferson Lab 12 GeV Program
The Jefferson Lab 12 GeV Program The Jefferson Lab facilities have undergone a substantial upgrade, both of accelerator, CEBAF, and of the experimental installations. We will discuss the progress to completion
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 informationLight Meson Decays at BESIII
Light Meson Decays at BESIII Liqing QIN (for the Collaboration ) Shandong University XVI International Conference on Hadron Spectroscopy Sep. 13-18, 2015, Newport News, VA OUTLINE n Introduction n Recent
More information* ) B s( * ) B s( - 2 -
- 1 - ϒ Λ B s( * ) B s( * ) ϒ B s( * ) Λ B s( * ) - 2 - ϒ(5S) Study at CLEO CLEO studies B s in both inclusive and exclusive modes. Data was taken with the CLEO III detector. Data set ϒ(5S) ϒ(4S) Continuum
More informationCharmed Baryon spectroscopy at Belle 1. Y. Kato KMI topics. Mainly based on the paper recently accepted by PRD ( arxiv: )
Charmed Baryon spectroscopy at Belle 1 Y. Kato KMI topics Mainly based on the paper recently accepted by PRD ( arxiv:1312.1026) Introduction 2 The mass of matter is almost made of nucleons. But they are
More informationInternational Workshop on Heavy Quarkonium Oct. 2007, DESY Hamburg. Prospects for Panda. Charmonium Spectroscopy
International Workshop on Heavy Quarkonium 17 20 Oct. 2007, DESY Hamburg Prospects for Panda Charmonium Spectroscopy M. Pelizäus (Ruhr Universität Bochum) for the Panda Collaboration 1 FAIR accelerator
More informationQCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration
QCD at CDF Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration Jet Inclusive Cross-Section Underlying event studies Jet Shapes Specific processes _ W+Jets, γ + γ, γ + b/c, b-jet / bb jet Diffraction
More informationMuon reconstruction performance in ATLAS at Run-2
2 Muon reconstruction performance in ATLAS at Run-2 Hannah Herde on behalf of the ATLAS Collaboration Brandeis University (US) E-mail: hannah.herde@cern.ch ATL-PHYS-PROC-205-2 5 October 205 The ATLAS muon
More informationFirst Run-2 results from ALICE
First Run-2 results from ALICE Goethe University Frankfurt & GSI on behalf of the ALICE Collaboration XLV International Symposium on Multiparticle Dynamics Wildbad Kreuth, 4-9 Oct 2015 1 Outline Introduction
More informationSearch for the η e + e - decay at the SND detector
Search for the η e + e - decay at the SND detector Berdyugin A.V. SND VEPP-2000 SND detector at VEPP-2000 NIM A449 (2000) 125-139 1 beam pipe, 2 tracking system, 3 aerogel Cherenkov counter, 4 NaI(Tl)
More informationarxiv: v1 [hep-ex] 2 Nov 2010
Early b-physics at CMS Andrea Rizzi EH Zurich, Switzerland arxiv:.64v [hep-ex] Nov he CMS experiment at the Large Hadron Collider collected in the first months of operation a luminosity of about /nb. he
More informationNon-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC
WDS'12 Proceedings of Contributed Papers, Part III, 142 146, 212. ISBN 978-8-7378-226-9 MATFYZPRESS Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC I. Chalupková, Z.
More informationTesting the m-e universality with ±
Testing the m-e universality with ± ± K l n decays Venelin Kozhuharov University of Sofia St. Kl. Ohridski / JINR Dubna Neutrino Oscilation Workshop 2006 on behalf of the NA48/2 collaboration Cambridge,
More informationStatus and Performance of the ATLAS Experiment
Status and Performance of the ATLAS Experiment P. Iengo To cite this version: P. Iengo. Status and Performance of the ATLAS Experiment. 15th International QCD Conference (QCD 10), Jun 2010, Montpellier,
More informationATLAS: Status and First Results
ATLAS: Status and First Results, University of Sheffield, on behalf of the ATLAS Collaboration 1 Overview of the ATLAS detector Status of the experiment Performance and physics results in the first six
More informationMassachusetts Institute of Technology Dynamics and Control II
I E Maachuett Intitute of Technology Department of Mechanical Engineering 2.004 Dynamic and Control II Laboratory Seion 5: Elimination of Steady-State Error Uing Integral Control Action 1 Laboratory Objective:
More informationWolfgang Gradl. on behalf of the BABAR collaboration. Tau 2016, Beijing 23 rd September 2016
ISR K u K u π (π ) Wolfgang Gradl on behalf of the collaboration Tau 216, Beijing 23 rd September 216 Motivation γ µ QED is precision physics u l 1 2 (u 2) l testbed for QED experimentally: electron ok
More informationWhy the f 0 (980) is mostly s s
Why the f 0 (980) i motly Eef van Beveren Departamento de Fíica, Univeridade de Coimbra P-3000 Coimbra, Portugal eef@teor.fi.uc.pt George Rupp Centro de Fíica da Interacçõe Fundamentai Intituto Superior
More informationSearch for Lepton Flavour Violation (LFV) in Three-Body Tau Decays at BaBar
SLACPUB1147 August 005 1 Search for Lepton Flavour Violation (LFV) in ThreeBody Tau Decays at BaBar M. Hodgkinson (on behalf of the BaBar collaboration) a a High Energy Physics Group, University of Manchester,
More informationPerformance of muon and tau identification at ATLAS
ATL-PHYS-PROC-22-3 22/2/22 Performance of muon and tau identification at ATLAS On behalf of the ATLAS Collaboration University of Oregon E-mail: mansoora.shamim@cern.ch Charged leptons play an important
More informationPHY492: Nuclear & Particle Physics. Lecture 23. HW Particle Detectors
PHY49: Nuclear & Particle Phyic Lecture 3 HW Particle Detector Homework 13.1 x min = mω λ 1 x min = mω λ ; x 3 = mω min λ V ( x min + x, y) = 1 mω x min + x ( ) + y + λ 4 3 ; 4 xmin = m ω 4 λ x min + x
More informationMeasurements of the dilepton continuum in ALICE. Christoph Baumann Resonance Workshop, Austin
Measurements of the dilepton continuum in ALICE Christoph Baumann 07.03.2012 Resonance Workshop, Austin ALICE Central Detectors: Inner Tracking System Time Projection Chamber Time-of-Flight Transition
More information