G-2: Past and Future G. Bunce for the g-2 Collaboration Spin2006, Kyoto.

Slides:



Advertisements
Similar presentations
K. Kirch Search for the EDM at low ? Motivation Frozen spin technique High and low A compact storage ring experiment?
Advertisements

October 14, 2009 Tsutomu Mibe ( 三部 勉) KEK 1.
Hertzog / Experiment DOE Intensity Frontier Review The g-2 Experimental Essentials David Hertzog University of Illinois  University of Washington Beam.
(g – 2)  B. Lee Roberts e + e - collisions  to  : Novosibirsk 1 March p. 1/30 Muon (g-2) to 0.2 ppm B. Lee Roberts Department of Physics Boston.
Potential for measurement of the tensor electric and magnetic polarizabilities of the deuteron and other nuclei in experiments with polarized beams Alexander.
B. Lee Roberts, P5: 27 March p. 1/25 Muon (g-2) to 0.25 ppm B. Lee Roberts on behalf of the New Muon (g-2) Collaboration: E969.
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, Hampton University, 23 March p. 1/31 The Muon’s Magnetic Moment What’s all the fuss about anyway? B. Lee Roberts Department of Physics.
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
Muon g-2 experimental results & theoretical developments
Fermilab Accelerator Complex in the Near Term: Muon Physics Program Eric Prebys Accelerator Physics Center FNAL.
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.
WG4:  physics B. Lee Roberts, on behalf of the Intense Muon Physics Working Group - p. 1/48 WG4 Summary and Future Plans The muon trio and more B. Lee.
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 A 1 ppm measurement of the positive muon lifetime Qinzeng Peng Advisor: Robert Carey Boston University October 28, 2010 MuLan collaboration at BU: Robert.
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.
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.
Yannis K. Semertzidis, CERN flavour, 15 May p. 1/26 The next muon g-2 experiment to 0.25 ppm Yannis K. Semertzidis Brookhaven National Laboratory.
A Precision Measurement of the Positive Muon Lifetime Using a Pulsed Muon Beam and the  Lan Detector R.M. Carey, P. Cushman, P.T. Debevec, W. Earle, F.E.
Yannis K. Semertzidis, BNL DOE review: 19 April p. 1/25 Muon g-2 (E969) to 0.25 ppm Yannis K. Semertzidis Brookhaven National Laboratory We made.
(g – 2)  B. Lee Roberts, Dipole Moments In Storage Rings AGS/RHIC Workshop,7 June p. 1/36 Muon (g-2): Past, Present and Future B. Lee Roberts On.
1 Polarimeter for dEDM experiment G. Venanzoni Laboratori Nazionali di Frascati for the dEDM collaboration Workshop on Flavour in the era of LHC – Cern.
Muon (g-2) Experiments Matthew Wright Luo Ouyang.
Energy calibration at LHC J. Wenninger. Motivation In general there is not much interest for accurate knowledge of the momentum in hadron machines. 
B. Lee Roberts, P5: 27 March p. 1/25 Muon (g-2) to 0.25 ppm B. Lee Roberts on behalf of the New Muon (g-2) Collaboration: E969.
David M. Webber University of Illinois at Urbana-Champaign For the MuLan Collaboration A new determination of the positive muon lifetime to part per million.
Possibilities of measurement of tensor polarizabilities of the deuteron and other nuclei in experiments with polarized beams Alexander J. Silenko Research.
G-2 accelerator and cryo needs Mary Convery Muon Campus Review 1/23/13.
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.
Dipole Moments in Storage Rings Yannis K. Semertzidis Brookhaven National Laboratory Dipole Moments in Storage Rings BNL, 7 June 2006 Organizers: Gerco.
 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.
David M. Webber For the MuLan Collaboration University of Wisconsin-Madison Formerly University of Illinois at Urbana-Champaign August 12, 2011 A part-per-million.
Yannis K. Semertzidis Brookhaven National Laboratory Fundamental Interactions Trento/Italy, June 2004 Theoretical and Experimental Considerations.
Brian Plimley Physics 129 November Outline  What is the anomalous magnetic moment?  Why does it matter?  Measurements of a µ  : CERN.
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.
Muon Anomalous Magnetic Moment --a harbinger of new physics Chang Liu Physics 564.
More beam (muons) from the AGS AGS RHIC Users Group Meeting EDM Workshop Brookhaven National Laboratory 7 June 2006 Phil Pile.
Priscilla Cushman University of Minnesota ICHEP Aug 16-22, 2004 Beijjing, China The g-2 Collaboration Boston University, Brookhaven National Laboratory,
Yannis K. Semertzidis, RHIC/AGS Users meeting, 9 June 2006 Muon g-2 experiment (E969) to 0.25 ppm and deuteron EDM (dEDM) to e∙cm Yannis K. Semertzidis.
(g – 2)  James Miller CERN Workshop October p. 1/27 Muon (g-2) to 0.25 ppm James Miller (For the new Muon (g-2) Collaboration, E969) Department.
First results from CMD-3 detector at VEPP-2000 collider Budker Institute of Nuclear Physics, SB RAS, Novosibirsk, Russia September 2011 E.Solodov (for.
The Muon g-2 Experiment – Investigating how the spin of a muon is affected as it moves through a magnetic field Astrid Rodrigues.
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.
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.
Classical picture: rotation of the something Introduction to Spin Physics mass charge One of three intrinsic characteristics of elementary particle 2015October.
B. Lee Roberts, PHIPSI 2009, Beijing – 14 October p. 1/30 Status of the (g - 2)  Fermilab Project Lee Roberts Department of Physics Boston University.
Yannis K. Semertzidis Brookhaven National Laboratory HEP Seminar SLAC, 27 April 2004 Muon g-2: Powerful Probe of Physics Beyond the SM. Present Status.
E989 Muon (g-2) EMG Lee Roberts for the E989 Collaboration B. Lee Roberts - EMG- 13 February
Electric Dipole Moment of the Deuteron Experiment: EDM Violates T-Symmetry: Connected to CP-Violation and the Matter-Antimatter Asymmetry of the Universe.
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.
G4beamline Spin Tracking Tom Roberts, Muons, Inc. In G4beamline 2.12, the tracking of muon and electron spins is introduced: – decay of pions into polarized.
Kevin Lynch MuLan Collaboration Boston University CIPANP 2006 A new precision determination of the muon lifetime Berkeley, Boston, Illinois, ITU, James.
– + + – 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.
Geant4 in the FNAL g-2 Experiment Kevin Lynch Boston University August 2009 g-2 Collaboration Meeting.
Towards a measurement of the muon electric dipole moment with a compact storage ring Klaus Kirch Nufact08, Valencia, 2008.
Update on the EDMs in Storage Rings
The Anomalous Magnetic Dipole Moment of the Muon
nuSTORM at Fermilab D Adey
High precision measurement of the beam energy at VEPP-4M collider by Yury Tikhonov KEDR&VEPP-4M collaboration Budker INP, Novosibirsk Outlook Introduction.
Presentation transcript:

g-2: Past and Future G. Bunce for the g-2 Collaboration Spin2006, Kyoto

Phys. Rev. D73, (2006) Final report of the E821 muon anomalous magnetic moment measurement at BNL G.W. Bennett, B. Bousquet, H.N. Brown, G. Bunce, R.M.Carey, P. Cushman, G.T. Danby, P.T. Debevec, M. Deile, H. Deng, W. Deninger, S.K. Dhawan, V.P. Druzhinin, L. Duong, E. Efstathiadis, F.J.M. Farley, G.V. Fedotovich, S. Giron, F.E. Gray, D. Grigoriev, M. Grosse-Perdekamp, A. Grossman, M.F. Hare, D.W. Hertzog, X. Huang, V.W. Hughes, M. Iwasaki, K. Jungmann, D. Kawall, M. Kawamura, B.I Khazin, J. Kindem, F. Krienen, I. Kronkvist, A. Lam, R. Larsen, Y.Y. Lee, I. Logoshenko, R. McNabb, W. Meng, J. Mi, J.P. Miller, Y. Mizumachi, W.M. Morse, D. Nikas, C.J.G. Onderwater, Y. Orlov, C.S. Ozben, J.M. Paley, Q. Peng, C.C. Polly, J. Pretz, R. Prigl, G. zu Putlitz, T. Qian, S.I. Redin, O. Rind, B.L.Roberts, N. Ryskulov, S. Seykh, Y.K. Semertzidis, P. Shagin, Yu. M. Shatunov, E.P. Sichtermann, E. Solodov, M. Sossong, A. Steinmetz, L.R. Sulak, C. Timmermans, A. Trofimov, D. Urner, P. von Walter, D. Warburton, D. Winn, A. Yamamoto, and D. Zimmermann

Magnetic moments, g-factors

We measure the difference frequency between the spin and momentum precession With an electric quadrupole field for vertical focusing 0

Inflector Kicker Modules Storage ring Central orbit Injection orbit Pions Target Protons (from AGS)p=3.1GeV/c Experimental Technique Muon polarization Muon storage ring injection & kicking focus by Electric Quadrupoles 24 electron calorimeters R=711.2cm d=9cm (1.45T) Electric Quadrupoles (from Q. Peng)

muon (g-2) storage ring Muon lifetime t  = 64.4  s (g-2) period t a = 4.37  s Cyclotron period t C = 149 ns

We count high-energy electrons as a function of time.

Storage Ring Cross Section Field in ppm

E821 achieved 0.5 ppm and the e + e - based theory is also at the 0.6 ppm level. Both can be improved. All E821 results were obtained with a “blind” analysis.

Bill Marciano presentation to P5 Committee

A (g-2)  Experiment to ± 0.25 ppm Precision –BNL E969 Collaboration R.M. Carey, I. Logashenko, K.R. Lynch J.P. Miller B.L. Roberts- Boston University; G. Bunce W. Meng, W. Morse, P. Pile, Y.K. Semertzidis -Brookhaven; D. Grigoriev B.I. Khazin S.I. Redin Yuri M. Shatunov, E. Solodov – Budker Institute; F.E. Gray B. Lauss E.P. Sichtermann – UC Berkeley and LBL; Y. Orlov – Cornell University; J. Crnkovic,P. Debevec D.W. Hertzog, P. Kammel S. Knaack, R. McNabb – University of Illinois UC; K.L. Giovanetti – James Madison University; K.P. Jungmann C.J.G. Onderwater – KVI Groningen; T.P. Gorringe, W. Korsch – U. Kentucky, P. Cushman – Minnesota; Y. Arimoto, Y. Kuno, A. Sato, K. Yamada – Osaka University; S. Dhawan, F.J.M. Farley – Yale University

E821 achieved 0.54 ppm and is statistics dominated. All E821 results were obtained with a “blind” analysis. world average

E969 New Baseline – 0.25 ppm total error Systematic error goals: –for  a : 0.1 ppm –for  p : 0.1 ppm Statistical error goal: –for  a : 0.2 ppm Total Error Goal: –a  : 0.25 ppm Beam with 4x quadrupoles: factor 2-3 Injection magnet opened: factor 2 in stored muons Field measurement improvements Segmented calorimeters for pileup

Open the superconducting injector magnet. Length = 1.7 m; Central field = 1.45T Open end prototype, built and tested → X2 Increase in Beam

New segmented detectors of tungsten / scintillating- fiber ribbons to deal with pile-up prototype under construction bases will be gated. new custom electronics and DAQ

Systematic uncertainty (ppm) E969 Goal Magnetic field –  p Anomalous precession –  a Statistical uncertainty (ppm) Total Uncertainty (ppm) Summary of goals

Summary Historically (g-2) has placed a major hurdle in the path of new theories beyond the standard model. The (g-2) result must fit with other evidence into a consistent picture of new physics. We hope that this measurement will be pursued to even greater precision in the future, either at BNL or at the Japan Hadron Facility. I would like to thank Lee Roberts and Bill Marciano for the use of many slides.