Yannis K. Semertzidis Brookhaven National Laboratory Fundamental Interactions Trento/Italy, 21-25 June 2004 Theoretical and Experimental Considerations.

Slides:



Advertisements
Similar presentations
Spontaneous Parity Violation in Strong Interactions Dhevan Gangadharan (UCLA) On behalf of the STAR Collaboration WWND
Advertisements

B. Lee Roberts, SPIN2004 –Trieste -11 September p. 1/54 New Results on Muon (g-2) Past, Present and Future Experiments B. Lee Roberts Department.
B. Lee Roberts, NuFact WG4: 24 June p. 1/36 Muon (g-2) Past, Present and Future B. Lee Roberts Department of Physics Boston University
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Muon g-2 experimental results & theoretical developments
Measurement of the muon anomaly to high and even higher precision David Hertzog* University of Illinois at Urbana-Champaign * Representing the E821 Collaboration:
Basic Measurements: What do we want to measure? Prof. Robin D. Erbacher University of California, Davis References: R. Fernow, Introduction to Experimental.
B. Lee Roberts, BNL PAC 9 September p. 1/29 Muon (g-2) to 0.20 ppm P969 B. Lee Roberts Representing the new g-2 collaboration: Boston, BNL, BINP,
 B. Lee Roberts, Heidelberg – 11 June p. 154 The Magnetic and Electric Dipole Moments of the Muon Lee Roberts Department of Physics Boston University.
B. Lee Roberts, Oxford University, 19 October p. 1/55 The Muon: A Laboratory for Particle Physics Everything you always wanted to know about the.
B. Lee Roberts, PANIC05, Santa Fe, 27 October, p. 1/35 Muon (g-2) Status and Plans for the Future B. Lee Roberts Department of Physics Boston University.
B. Lee Roberts, HIFW04, Isola d’Elba, 6 June p. 1/39 Future Muon Dipole Moment Measurements at a high intensity muon source B. Lee Roberts Department.
A new method of measuring the muon g-2 Francis J.M. Farley Trinity College Dublin.
1 g-2 phase study from GEANT simulation Qinzeng Peng Advisor: James Miller Boston University Sep 28, 2004 Muon g-2 collaboration at BU: Lee Roberts, Rober.
B Production and Decay at DØ Brad Abbott University of Oklahoma BEACH 2004 June 28-July 3.
LHC’s Second Run Hyunseok Lee 1. 2 ■ Discovery of the Higgs particle.
Muon and electron g-2 A charged particle which has spin angular momentum s will have also a magnetic moment m. The ratio of the magnetic to angular moments.
Measurement of the Positive Muon Lifetime to 1 ppm David Webber Preliminary Examination March 31, 2005.
Measurements of R Value and Hadronic Form Factors at BES Haiming Hu Institute of High Energy Physics, CAS, Beijing Novosibirsk, Russian Feb. 27 – Mar.
Magnetic & Electric Dipole Moments. Yannis K. Semertzidis Brookhaven National Lab Axion Academic Training CERN, 1 December 2005 Muon g-2 experiment EDMs:
Conveneers: M. Grassi (INFN, Pisa), K. Ishida (RIKEN), Y. Semertzidis (BNL) Summary of WG4, Part Two. Yannis Semertzidis, BNL 1 August, 2004 Most muon.
Muon g-2 Experiment at Fermilab, Liang Li, SPCS 2013 June 5 th, Shanghai Particle Physics and Cosmology Symposium - SPCS2013 The (new) muon g-2.
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
Muon (g-2) Experiments Matthew Wright Luo Ouyang.
Trilinear Gauge Couplings at TESLA Photon Collider Ivanka Božović - Jelisavčić & Klaus Mönig DESY/Zeuthen.
G-2 accelerator and cryo needs Mary Convery Muon Campus Review 1/23/13.
Measurements of Transverse Spin Effects with the Forward Pion Detector of STAR Larisa Nogach Institute of High Energy Physics, Protvino for the STAR collaboration.
1 Electroweak Physics Lecture 5. 2 Contents Top quark mass measurements at Tevatron Electroweak Measurements at low energy: –Neutral Currents at low momentum.
June 17, 2004 / Collab Meeting Strategy to reduce uncertainty on a  to < 0.25 ppm David Hertzog University of Illinois at Urbana-Champaign n Present data.
Initial State Radiation and Inclusive Hadron Production at B A B AR Fabio Anulli University of Perugia, INFN – Laboratori Nazionali di Frascati On behalf.
Measurement of Vus. Recent NA48 results on semileptonic and rare Kaon decays Leandar Litov, CERN On behalf of the NA48 Collaboration.
Measuring the charged pion polarizability in the  →    −  reaction David Lawrence, JLab Rory Miskimen, UMass, Amherst Elton Smith, JLab.
K.K. Gan The Ohio State University New Results on  Lepton July 17, 2003.
Oct 6, 2008Amaresh Datta (UMass) 1 Double-Longitudinal Spin Asymmetry in Non-identified Charged Hadron Production at pp Collision at √s = 62.4 GeV at Amaresh.
Klaus P. Jungmann, Kernfysisch Versneller Instituut, Groningen, NL Arbeitstreffen „Hadronen und Kerne“, Pommersfelden, 26 September 2001 Standard Model.
Shuangshi Fang (for the BESIII Collaboration ) Institute of High Energy Physics MesonNet meeting June 17-19,2013, Prague, CZE η and η’ physics at BESIII.
 B. Lee Roberts, KEK – 21 March p. 1/27 The Magnetic and Electric Dipole Moments of the Muon Lee Roberts for the muon g-2 collaboration Department.
Chunhui Chen, University of Pennsylvania 1 Heavy Flavor Production and Cross Sections at the Tevatron Heavy Flavor Production and Cross Sections at the.
Brian Plimley Physics 129 November Outline  What is the anomalous magnetic moment?  Why does it matter?  Measurements of a µ  : CERN.
1 Fukutaro Kajihara (CNS, University of Tokyo) for the PHENIX Collaboration Heavy Quark Measurement by Single Electrons in the PHENIX Experiment.
Muon g-2, Rare Decays P → l + l - and Transition Form Factors P →   Introduction Lepton anomalous magnetic moments (status) Rare  0 →e + e – Decay.
JPS 2003 in Sendai Measurement of spectral function in the decay 1. Motivation ~ Muon Anomalous Magnetic Moment ~ 2. Event selection 3. mass.
Huaizhang Deng Yale University Precise measurement of (g-2)  University of Pennsylvania.
Muon g-2 and Electric Dipole Moments in Storage Rings: Powerful Probes of Physics Beyond the SM Yannis K. Semertzidis Brookhaven National Lab “Muon g-2.
Study of e+e- annihilation at low energies Vladimir Druzhinin Budker Institute of Nuclear Physics (Novosibirsk, Russia) SND - BaBar Lepton-Photon, August,
Muon Anomalous Magnetic Moment --a harbinger of new physics Chang Liu Physics 564.
Priscilla Cushman University of Minnesota ICHEP Aug 16-22, 2004 Beijjing, China The g-2 Collaboration Boston University, Brookhaven National Laboratory,
Achim Denig Radiative DA F NE MENU 2004 Measurement of the Hadronic Cross Section via Radiative Return at DA  NE Achim Denig for the KLOE Collaboration.
A High Statistics Study of the Decay M. Fujikawa for the Belle Collaboration Outline 1.Introduction 2.Experiment Belle detector 3.Analysis Event selection.
Belle General meeting Measurement of spectral function in the decay 1. Motivation 2. Event selection 3. mass spectrum (unfolding) 4. Evaluation.
Measurement of the Muon Anomalous Magnetic Moment to 0.7 ppm Results from the Data of 2000 Yannis K. Semertzidis Brookhaven National Lab Muon g-2 Collaboration.
1) Status of the Muon g-2 Experiment 2) EDM Searches in Storage Rings Yannis K. Semertzidis Brookhaven National Lab Muon g-2 Collaboration and EDM Collaboration.
 Output of Project X  1 “blast” = 9mA*1ms = 5.6e13 (protons)/(1.4 s cycle)  = 4e13 p/s on average (!!)  = 50 kW average beam power  = 8e20/yr (2e7.
David Hertzog University of Illinois at Urbana-Champaign Our piece of the PhiPsi08 poster n Motivation n The theory situation n The basic experimental.
Part I: Muon g-2 theory update / motivation Part II: Possibilities for FNAL experiment at 0.1 ppm David Hertzog University of Illinois at Urbana-Champaign.
IV Euridice Collaboration Meeting Marseille, 8-11 February 2006 Hadronic Cross Section measurement at DA  NE with the KLOE detector Hadronic Cross Section.
Yannis K. Semertzidis Brookhaven National Laboratory HEP Seminar SLAC, 27 April 2004 Muon g-2: Powerful Probe of Physics Beyond the SM. Present Status.
An Tai QM2004, Oakland Jan.11-17, 2004 STAR 1 STAR measurements of open charm production in dAu collisions at √s NN =200 GeV An Tai For the STAR Collaboration.
Klaus P. Jungmann, Kernfysisch Versneller Instituut, Groningen, NL on behalf of the muon g-2 collaboration 3 rd Joint NIPNET ION-CATCHER HITRAP Collaboration.
1 Muon g-2 Experiment at BNL Presented by Masahiko Iwasaki (Tokyo Institute of Technology) Akira Yamamoto (KEK) for E821 g-2 Collaboration: Boston, BNL,
Yannis K. Semertzidis Brookhaven National Laboratory New opportunities at CERN CERN, 12 May 2009 Storage Ring EDM Experiments The storage ring method can.
– + + – Search for the μEDM using a compact storage ring A. Adelmann 1, K. Kirch 1, C.J.G. Onderwater 2, T. Schietinger 1, A. Streun 1 1 Paul Scherrer.
Marco Incagli - INFN Pisa CERN - 29 apr 2004
Vertical emittance measurement and modeling Correction methods
Does g-2 point to new physics?: Current Status and Future Plans
Charged Particle EDM (CPEDM)
A New Measurement of |Vus| from KTeV
electric dipole moments (EDM)
JLEIC Collaboration meeting Spring 2016 Ion Polarization with Figure-8
Measurement of Parity-Violation in the N→△ Transition During Qweak
Presentation transcript:

Yannis K. Semertzidis Brookhaven National Laboratory Fundamental Interactions Trento/Italy, June 2004 Theoretical and Experimental Considerations of Past and Future Muon g-2 Measurements

† † ‡ # Muon g-2 Collaboration † Spokesperson ‡ Project Manager # Resident Spokesperson

Prof. Vernon W. Hughes (1921  2003)

g - 2 for the muon Largest contribution : Other standard model contributions : QED hadronic weak

Theory of a µ a µ (theo) = a µ (QED)+a µ (had)+a µ (weak) + a µ (new physics) a µ (had) = a µ (had1) + a µ (had, HO) + a µ (had, LBL) ? -10   3.5 in units of

Cannot be calculated from pQCD alone because it involves low energy scales. Hadronic contribution (had1) However, by dispersion theory, this a  (had1) can be related to measured in e + e - collisions. or τ decay.

Cannot be calculated from pQCD alone because it involves low energy scales. Hadronic contribution (had1) However, by dispersion theory, this a  (had1) can be related to measured in e + e - collisions or τ decay (assuming CVC).

Evaluation of R M. Davier et al., hep-ph/ v3

Evaluation of R M. Davier et al., hep-ph/ v3

Difference between e + e - and  M. Davier et al., hep-ph/ v3

…Difference between e + e - and  M. Davier et al., Eur. Phys. J. C31, 503 (2003)

a μ (had1,e + e - )=(696.3±7.)× a μ (had1,τ) =(711.0±6.)× e + e - based τ based CorrectCorrect τ-data interpr. wrong Correct Wrong Wrong * Correct Wrong * Wrong T. Blum, hep-lat/ *Other (e + e - ) collaborations are looking into it see, e.g., the KLOE Collaboration, hep-ex/ a μ (exp)- a μ (SM, e + e - )=33.7(11)× a μ (exp) -a μ (SM, τ) = 9.4(11)× M. Davier, hep-ph/ Why?

a μ (had1,e + e - )=(696.3±7.)× a μ (had1,τ) =(711.0±6.)× e + e - based τ based CorrectCorrect τ-data interpr. Wrong** Correct Wrong Wrong * Correct Wrong * Wrong *Other (e + e - ) collaborations are looking into it, e.g., the KLOE Collaboration confirmed their result. a μ (exp)- a μ (SM, e + e - ) 10 M. Davier, hep-ph/ ** e + e -  0  +  -, whereas τ -  -   -  0 , S.G., F.J., hep-ph/ Issue not completely resolved yet…

Theory of a µ a µ (theo) = a µ (QED)+a µ (had)+a µ (weak) + a µ (new physics) a µ (QED) = (0.3) × a µ (had) = (8.) × (based on e + e - ) a µ (had) = (7.) × (based on  ) a µ (weak) = 15.4 (0.3) × a µ (SM) = (8)× (based on e + e - ) a µ (SM) = (7)× (based on  )

Theory and Experiment vs. Year

Experimental Principle: Polarize: Interact: Analyze: Parity Violating Decay Precess in a Uniform B-Field Parity Violating Decay

Beamline: Polarized Muon Beam Production

The Muon Storage Ring: B ≈ 1.45T, P μ ≈3.09 GeV/c Inner Ring of Detectors High Proton Intensity from AGS Muon Injection

Spin Precession in g-2 Ring (Top View)  Momentum vector Spin vector

Spin Precession in g-2 Ring (Top View)  Momentum vector Spin vector

4 Billion e + with E>2GeV

5-parameter Function Not Quite Adequate. Fourier Spectrum of the Residuals: f g-2 ≈229 KHz f cbo ≈466 KHz Data of 2000, n = 0.137

Amplitudes of A N, A A, A, Consistent with Values from MC Simulations (10 -2, 10 -3, respectively) Modulation of N 0, A, with f cbo :

2001 Run with Negative Muons In 2001 we have collected 3.7 Billion electrons with E>1.8GeV from a run with negative muons (μ - ). Run at n=0.122 and n=0.142.

Vertical vs. Horizontal Tune

Systematic/Statistical Uncertainties for the ω a Analysis. Systematic Uncertainties Size [ppm] Coherent Betatron Oscillations (CBO) Pileup (Overlapping Signals) Gain Changes Lost Muons Others Total Systematics Statistical Uncertainty Total Uncertainty:

Magnetic Field measurement The B field azimuthal variation at the center of the storage region.  1.45 T The B field averaged over azimuth.

Magnetic Field Measurement Systematic Uncertainties for the ω p Analysis. Source of Errors Size [ppm] Absolute Calibration of Standard Probe Calibration of Trolley Probe Trolley Measurements of B-field Interpolation with Fixed Probes Uncertainty from Muon Distribution Others Total

Computation of a μ : Analyses of ω a and ω p are Separate and Independent (“Blind Analysis”). When Ready, only then, Offsets are Removed and a μ is Computed.

Computation of a μ : Data of 2001: a μ (exp)= (8)(3)× (0.7 ppm) W.L. et al., PRL 82, 711 (1999)

Average of a μ : Exp. World Average: a μ (exp)= (6)× (0.5 ppm) a μ (exp)- a μ (SM) = 27 (10)×10 -10, 2.7σ, based on e + e - data a μ (exp)- a μ (SM) = 12 (9) ×10 -10, 1.4σ, based on  -data CPT?

G.B. et al., hep-ex/ , PRL in Press

Recent KLOE Results

a µ (had, LBL) = +8.6(3.5)  Large N QCD+Chiral a µ (had, LBL) = +13.6(2.5)  Melnikov + Vainshtein a µ (had, LBL) = +11.1(1.7)  Dubnicka et al a µ (had, LBL) = +9.2(3.0)  T+Ynd. a µ (had, LBL) = +11.0(2.0)  W. Marciano, prelim. Use +12.0(3.5)  WM a µ (QED) = (0.04)(0.1)  Recent Kinoshita Update Recent Developments in Theory

a µ (had,1) = 696.3(6.2)(3.6)× DEHZ a µ (had,1) = 696.2(5.7)(2.4)× HMNT a µ (had,1) = (8.6) × GJ a µ (had,1) = 692.4(5.9)(2.4)× HMNT inclusive a µ (had,1) = 693.5(5.0)(1.0)× TY Use = (6.2)(3.6)× WM a µ (SM) = (7.2) VP (3.5) LBL (0.3) EW,QED × a µ (Exp) = (5.8)×  a µ = a µ (Exp) - a µ (SM) = 23.9 (9.9)× or 2.4  deviation Recent Developments in had1

Beyond standard model, e.g. SUSY W. Marciano, J. Phys. G29 (2003) 225

Current Status and Future Prospects

SUSY Dark Matter Following Ellis, Olive, Santoso, Spanos. Plot by K. Olive

SUSY Dark Matter Following Ellis, Olive, Santoso, Spanos. Plot by K. Olive

SUSY Dark Matter Following Ellis, Olive, Santoso, Spanos. Plot by K. Olive Upper Limits on SUSY Mass Scales are set by Muon g-2

Planning a New Run ~2006. Goal ~0.2ppm Use Backward Muons (i.e. P 5.3GeV/c, P 3.1GeV/c). Provides great  -Rejection. Increase Beamline acceptance (  4) Open up the two Inflector ends (  1.7) Studying two methods of data taking: a) Charge Integration, b) Record Individual pulses

Improvements… Backward Muons: no Light Flash at Injection; Improves Gate-on Times and Gain Effects. RF-Scraping to Reduce Muon Losses and the CBO Amplitude. Charge Integration: Immune to Pileup and Gain Changes. New method, needs study…

Experimental measurement of the anomalous magnetic moment of negative muons to 0.7 ppm. Combined with the positive muon result: 0.5ppm More data from the theory front are/will be analyzed: Novosibirsk, KLOE, BaBar, Belle. The g-2 collaboration is working towards reducing the experimental error by a factor of ~2. Prospects and Summary

SUSY: EDM, MDM and Transition Moments are in Same Matrix