yannis k. semertzidis brookhaven national lab “muon g-2 collaboration” and
DESCRIPTION
Oklahoma University HEP Seminar, 25 March 2004. Muon g-2 and E lectric D ipole M oments in Storage Rings: Powerful Probes of Physics Beyond the SM. Yannis K. Semertzidis Brookhaven National Lab “Muon g-2 Collaboration” and “EDM in Storage Rings Collaboration”. ‡. - PowerPoint PPT PresentationTRANSCRIPT
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Muon g-2 and Electric Dipole Moments in Storage Rings: Powerful Probes of Physics Beyond the SM
Yannis K. SemertzidisBrookhaven National Lab
“Muon g-2 Collaboration” and
“EDM in Storage Rings Collaboration”
Oklahoma UniversityHEP Seminar, 25 March 2004
EdBdtsd
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†
†
‡
#
Muon g-2 Collaboration
†Spokesperson ‡Project Manager # Resident Spokesperson
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Prof. Vernon W. Hughes (1921 2003)
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g - 2 for the muon
Largest contribution : 800
12
a
Other standard model contributions :
QED hadronic weak
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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
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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
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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
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Evaluation of R
M. Davier et al., hep-ph/0208177.v3
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Evaluation of R
M. Davier et al., hep-ph/0208177.v3
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Difference between e+e- and
M. Davier et al., hep-ph/0208177.v3
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…Difference between e+e- and
M. Davier et al., Eur. Phys. J. C31, 503 (2003)
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• 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?
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• 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
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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 )
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Theory and Experiment vs. Year
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Experimental Principle
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Beamline:Polarized Muon Beam Production
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• The Muon Storage Ring: B ≈ 1.45T, Pμ≈3.09 GeV/c
• Inner Ring of Detectors
•High Proton Intensity from AGS
•Muon Injection
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Spin Precession in g-2 Ring(Top View)
Bmeaa
Momentumvector
Spin vector
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Spin Precession in g-2 Ring(Top View)
Bmeaa
Momentumvector
Spin vector
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4 Billion e+ with E>2GeV
aa
t
tAeNdtdN
cos1/ 0
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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
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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)(
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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.
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Vertical vs. Horizontal Tune
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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
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Magnetic Field measurement
The B field azimuthal variation at the center of the storage region. <B>1.45 T
The B field averagedover azimuth.
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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
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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
///
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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)
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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
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G.B. et al., hep-ex/0401008, PRL in Press
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Recent KLOE Results
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• 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
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• 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
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Beyond standard model, e.g. SUSY
tanGeV1001013sgn2
susy
10susy
ma
W. Marciano, J. Phys. G29 (2003) 225
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Current Status and Future Prospects
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SUSY Dark Matter
Following Ellis,Olive, Santoso,Spanos. Plot by K. Olive
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SUSY Dark Matter
Following Ellis,Olive, Santoso,Spanos. Plot by K. Olive
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SUSY Dark Matter
Following Ellis,Olive, Santoso,Spanos. Plot by K. Olive
Upper Limits onSUSY Mass Scalesare set by Muon g-2
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• 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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Electric Dipole Moments in Storage Rings
•EDMs: Why are they important?
•EDMs in Storage Rings
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Spin is the only vector…
0d
+
-
dd
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A Permanent EDM Violates both T & P Symmetries:
+
-
+
-
+
-T
P
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T-Violation CP-ViolationCPT
Andrei Sakharov 1967:
CP-Violation is one of three conditions to enable a universe containing initially equal amounts of matter and antimatter to evolve into a matter-dominated universe, which we see today….
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EDM Searches are Excellent Probes of Physics Beyond the SM:
One CP-Violating Phase (CKM), Needs loops with all quark families for a non-zero result (Third Order Effect).
SM:
42 CP-Violating Phases, Needs one loop for a non-zero result (First Order Effect).
SUSY:
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la Fortson
d
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EdBdtsd
Usual Experimental Method
Small Signal
Compare the Zeeman FrequenciesWhen E-field is Flipped:
dE421 +
-
TNEd
11
Carrier Signal
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Electric Dipole Moments in Storage Rings
e.g. 1T corresponds to 300 MV/m!
Buddtsd
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B
a edm
Ron McNabb’s Thesis 2003: C.L. 95% cme107.2 19
x
y
z
sβ
aω
edm
me
Ba Bu
c
2
Indirect Muon EDM limit from the g-2 Experiment
a
edm
tan
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Two Major Ideas:• Radial E-field to Cancel the g-2 Precession• Injecting CW and CCW
• Sensitivity: 10-24 e·cm statistical (1 yr, 0.75MW)• Sensitivity: 10-27 e·cm systematic error
• Muon EDM LOI: (http://www.bnl.gov/edm) to J-PARC.
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Parameter Values of Muon EDM Experiment
• Radial E-Field:• E=2MV/m• Dipole B-field: B ~ 0.25T , R ~ 10m
• Muon Momentum:
• F. Farley et al., hep-ex/0307006
2aBcE
5 MeV/c,500 P
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Muon EDM Letter of Intent to J-PARC/Japan, 2003
• †Spokesperson
• # Resident Spokesperson
†
†
#
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SUSY: EDM, MDM and Transition Moments are in Same Matrix
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Expected Muon EDM Value from a
)tan( 10 27
cme 10 2 10
SUSY22
CP
ad
CPiSUSYSUSY
DM
eDD
Dd
Dmea
FDDL
,
,2
and ,21 where
,2
12
121 5*5
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Predictions in Specific Models
The predicted value for the electron is 10 times lessthan the current experimental limit.
50 effect at 10-24 ecm Exp. Sensitivity!
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g-2 Values• Electron 0.00116 done
• Muon 0.00117 doing
• Proton 1.8 ------
• Deuteron -0.15 OK!
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Deuteron Coherence Time• E, B field stability
• Multipoles of E, B fields
• Vertical (Pitch) and Horizontal Oscillations
• Finite Momentum Acceptance ΔP/P
At this time we believe we can do p~10s
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Deuteron Statistical Error (200MeV):
TotcRpd fTNAPaE
a2
2
15.6
p : 10s. Polarization Lifetime (Coherence Time)A : 0.3. The left/right asymmetry observed by the polarimeterP : 0.55. The beam polarizationNc : 1011d/cycle. The total number of stored particles per cycleTTot: 107s. Total running time per yearf : 0.01 Useful event rate fractionER : 3.5MV/m. Radial electric field
cme105 28 d per year
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Deuteron EDM to 10-27 ecm Sensitivity Level is 100 times better than 199Hg
• T-odd Nuclear Forces: dd =210-22 ξ e·cm with the best limit for ξ<0.5 10-3 coming from the 199Hg EDM limit (Fortson, et al., PRL 2001), i.e. dd < 10-25 e·cm.
(Sushkov, Flambaum, Khriplovich Sov. Phys. JETP, 60, p. 873 (1984) and Khriplovich and Korkin, Nucl. Phys. A665, p. 365 (2000)).
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dd = dp + dn (I. Khriplovich)
It Improves the Current Proton EDM Limit by a Factor of ~10,000 and a Factor 60-100 on Neutron.
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Deuteron (D) EDM at 310-
27ecm
Relative strength of various EDM limits as a function of left handed down squark mass (O. Lebedev, K. Olive, M. Pospelov and A. Ritz, hep-ph/0402023)
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Possible Locations for a Deuteron EDM Experiment:
• Brookhaven National Laboratory
• Indiana University Cyclotron Facility
• KVI/The Netherlands
Proposal This Year…
$20-30M
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Effect of Vertical Component of E• Clock Wise and Counter-Clock Wise Injection:
Background: Same Sign Signal: Opposite Sign
• Protons β=0.15, γ=1.01, ω=115105 θE rad/s• Deuterons β=0.2, γ=1.02, ω= 13105 θE rad/s• Muons β=0.98, γ=5, ω= 2105 θE rad/s
• Other Diagnostics Include Injecting Forward vs Backward Polarized Beams as well as Radially Pol.
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We are Studying
• Target and Polarimetry (Deuteron case)
• E-field Directional/Amplitude Stability
• Beam and Spin Dynamics
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E-field Stability: Major Breakthrough Idea by Neil Shafer-Ray
E-field Stability of Order 10-8 to 10-9
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EDMs
Questions Physicists Ask:
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Electric Dipole Moment Searches:
• Exciting Physics, Forefront of SUSY/Beyond SM Search.
• Revolutionary New Way of Probing EDMs, Muon and Deuteron Cases-Very Exciting.
• Sensitive EDM Experiments could bring the Next Breakthrough in Elementary Particle Physics.
Summary