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Muon g-2: Powerful Probe of Physics Beyond the SM. Present Status and Future Prospects

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HEP Seminar SLAC, 27 April 2004. Muon g-2: Powerful Probe of Physics Beyond the SM. Present Status and Future Prospects. Yannis K. Semertzidis Brookhaven National Laboratory. ‡. Muon g-2 Collaboration. †. #. †. † Spokesperson ‡ Project Manager # Resident Spokesperson. - PowerPoint PPT Presentation
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Yannis K. Semertzidis Brookhaven National Laboratory HEP Seminar SLAC, 27 April 2004 B dt s d Muon g-2: Powerful Probe of Physics Beyond the SM. Present Status and Future Prospects
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Page 1: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Yannis K. SemertzidisBrookhaven National Laboratory

HEP SeminarSLAC, 27 April 2004

Bdtsd

Muon g-2: Powerful Probe of Physics Beyondthe SM. Present Status and Future Prospects

Page 2: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

#

Muon g-2 Collaboration

†Spokesperson ‡Project Manager # Resident Spokesperson

Page 3: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Prof. Vernon W. Hughes (1921 2003)

Page 4: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

g - 2 for the muon

Largest contribution : 800

12

a

Other standard model contributions :

QED hadronic weak

Page 5: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Theory of aµ

• aµ(theo) = aµ(QED)+aµ(had)+aµ(weak)

+ aµ(new physics)

• aµ(had) = aµ(had1) + aµ(had, HO) + aµ(had, LBL)

? -100.6 + 8.6 3.5 in units of 10-10

Page 6: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Cannot be calculated from pQCD alonebecause it involves low energy scales.

Hadronic contribution (had1)

However, by dispersion theory,this a(had1) can be related to

)(e)(

e

hadronseeR

measured in e+e- collisions.or τ decay.

24 2

2

)()(3

)1,(

m

sRsKsdsm

hada

Page 7: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Cannot be calculated from pQCD alonebecause it involves low energy scales.

Hadronic contribution (had1)

However, by dispersion theory,this a(had1) can be related to

)(e)(

e

hadronseeR

measured in e+e- collisionsor τ decay (assuming CVC).

24 2

2

)()(3

)1,(

m

sRsKsdsm

hada

Page 8: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Evaluation of R

M. Davier et al., hep-ph/0208177.v3

Page 9: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Evaluation of R

M. Davier et al., hep-ph/0208177.v3

Page 10: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Difference between e+e- and

M. Davier et al., hep-ph/0208177.v3

Page 11: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

…Difference between e+e- and

M. Davier et al., Eur. Phys. J. C31, 503 (2003)

Page 12: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

• aμ(had1,e+e-)=(696.3±7.)×10-10

• aμ(had1,τ) =(711.0±6.)×10-10

e+e- based τ basedCorrect Correct τ-data interpr. wrongCorrect WrongWrong* CorrectWrong* Wrong T. Blum, hep-lat/0212018*Other (e+e-) collaborations are looking into it see, e.g., the

KLOE Collaboration, hep-ex/0210013

• aμ(exp)- aμ(SM, e+e-)=33.7(11)×10-10

• aμ(exp) -aμ(SM, τ) = 9.4(11)×10-10

M. Davier, hep-ph/0312065

Why?

Page 13: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

• aμ(had1,e+e-)=(696.3±7.)×10-10

• aμ(had1,τ) =(711.0±6.)×10-10

e+e- based τ basedCorrect Correct τ-data interpr. Wrong**Correct WrongWrong* CorrectWrong* Wrong *Other (e+e-) collaborations are looking into it, e.g., the

KLOE Collaboration is about to announce their result.

• aμ(exp)- aμ(SM, e+e-)10

M. Davier, hep-ph/0312065

**e+e-0 +-, whereas τ-- -0, S.G., F.J., hep-ph/0310181

Page 14: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Theory of aµ

• aµ(theo) = aµ(QED)+aµ(had)+aµ(weak)

+ aµ(new physics)

• aµ(QED) = 11 658 470.6 (0.3) ×10-10

• aµ(had) = 694.9 (8.) ×10-10 (based on e+e-)

• aµ(had) = 709.6 (7.) ×10-10 (based on )

• aµ(weak) = 15.4 (0.3) ×10-10

• aµ(SM) = 11 659 181(8)×10-10 (based on e+e-)

• aµ(SM) = 11 659 196(7)×10-10 (based on )

Page 15: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Theory and Experiment vs. Year

Page 16: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Experimental Principle

Page 17: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Beamline:Polarized Muon Beam Production

Page 18: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

• The Muon Storage Ring: B ≈ 1.45T, Pμ≈3.09 GeV/c

• Inner Ring of Detectors

•High Proton Intensity from AGS

•Muon Injection

Page 19: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Spin Precession in g-2 Ring(Top View)

Bmeaa

Momentumvector

Spin vector

Page 20: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Spin Precession in g-2 Ring(Top View)

Bmeaa

Momentumvector

Spin vector

Page 21: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

4 Billion e+ with E>2GeV

aa

t

tAeNdtdN

cos1/ 0

Page 22: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

5-parameter Function Not Quite Adequate. Fourier Spectrum of the Residuals:

nff Ccbo 11

fg-2 ≈229 KHz fcbo≈466 KHz

Data of 2000,n = 0.137

Page 23: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Amplitudes of AN, AA, A , Consistent with Values from MC Simulations (10-2, 10-3, 10-3 respectively)

Modulation of N0, A, with fcbo:

tttAetNdtdN aa

t

cos1/ 0

a

tfeAt cbo

t

aacbo 2cos)(

Ncbo

t

N tfeANtN cbo 2cos1)( 00

Acbo

t

A tfeAAtA cbo 2cos1)(

Page 24: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

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.

Page 25: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Vertical vs. Horizontal Tune

Page 26: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Systematic/Statistical Uncertainties for the ωa Analysis.

Systematic Uncertainties

Size [ppm]

Coherent Betatron Oscillations (CBO)Pileup (Overlapping Signals) Gain ChangesLost MuonsOthersTotal Systematics

0.07 0.080.120.090.110.210.66

0.21 0.130.120.100.080.310.62

2001 2000

Statistical Uncertainty

Total Uncertainty: 0.7 0.7

Page 27: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Magnetic Field measurement

The B field azimuthal variation at the center of the storage region. <B>1.45 T

The B field averagedover azimuth.

Page 28: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Magnetic Field MeasurementSystematic Uncertainties for the ωp Analysis.

Source of ErrorsSize [ppm]

Absolute Calibration of Standard ProbeCalibration of Trolley ProbeTrolley Measurements of B-fieldInterpolation with Fixed ProbesUncertainty from Muon DistributionOthersTotal

0.050.150.10 0.10 0.030.100.24

0.050.090.05 0.07 0.030.100.17

2001 2000

Page 29: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Computation of aμ:

• Analyses of ωa and ωp are Separate and Independent (“Blind Analysis”). When Ready, only then, Offsets are Removed and aμ is Computed.

pap

paa

Bme

a

///

Page 30: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Computation of aμ:

R

R

Bm

eapap

paa

///

Data of 2001:aμ(exp)=11 659 214(8)(3)×10-10 (0.7 ppm)

(26) 3 208 707 0.003 / paR

(10) 39 345 3.183 / p W.L. et al., PRL 82, 711 (1999)

Page 31: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Average of aμ:

Exp. World Average:aμ(exp)=11 659 208(6)×10-10 (0.5 ppm)

aμ(exp)- aμ(SM) = 27 (10)×10-10, 2.7σ, based on e+e- data

aμ(exp)- aμ(SM) = 12 (9) ×10-10, 1.4σ, based on -data

CPT? 910)4.35.3( RRR

Page 32: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

G.B. et al., hep-ex/0401008, PRL in Press

Page 33: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Recent KLOE Results

Page 34: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

• aµ(had, LBL) = +8.6(3.5)10-10 Large N QCD+Chiral

• aµ(had, LBL) = +13.6(2.5)10-10 Melnikov + Vainshtein

• aµ(had, LBL) = +11.1(1.7)10-10 Dubnicka et al

• aµ(had, LBL) = +9.2(3.0)10-10 T+Ynd.

• aµ(had, LBL) = +11.0(2.0)10-10 W. Marciano, prelim.

• Use +12.0(3.5)10-10 WM

• aµ(QED) = 11 658 472.07(0.04)(0.1)10-10 Recent Kinoshita Update

Recent Developments in Theory

Page 35: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

• aµ(had,1) = 696.3(6.2)(3.6)×10-10 DEHZ

• aµ(had,1) = 696.2(5.7)(2.4)×10-10 HMNT

• aµ(had,1) = 694.8 (8.6) ×10-10 GJ

• aµ(had,1) = 692.4(5.9)(2.4)×10-10 HMNT inclusive

• aµ(had,1) = 693.5(5.0)(1.0)×10-10 TY

• Use = 694.4 (6.2)(3.6)×10-10 WM

• aµ(SM) = 11 659 184.1 (7.2)VP (3.5)LBL (0.3)EW,QED ×10-10

• aµ(Exp) = 11 659 208.0 (5.8)×10-10

aµ= aµ(Exp) - aµ(SM) = 23.9 (9.9)×10-10 or 2.4 deviation

Recent Developments in had1

Page 36: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Beyond standard model, e.g. SUSY

tanGeV1001013sgn2

susy

10susy

ma

W. Marciano, J. Phys. G29 (2003) 225

Page 37: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

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

Page 38: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Current Status and Future Prospects

Page 39: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

SUSY Dark Matter

Following Ellis,Olive, Santoso,Spanos. Plot by K. Olive

Page 40: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

SUSY Dark Matter

Following Ellis,Olive, Santoso,Spanos. Plot by K. Olive

Page 41: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

SUSY Dark Matter

Following Ellis,Olive, Santoso,Spanos. Plot by K. Olive

Upper Limits onSUSY Mass Scalesare set by Muon g-2

Page 42: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

Upgrade for Future Run: Goal 0.25 ppm

• Larger Acceptance Beamline.

• New Inflector with Open Ends.

• Larger Segmentation Detectors.

• Run for 25 Weeks w/ 2.6 times the Rate or for 16 Weeks at 4 times the Rate.

Page 43: Muon  g-2:  Powerful Probe of Physics Beyond the SM.  Present Status and Future Prospects

• 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


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