B. Lee Roberts, HIFW04, Isola d’Elba, 6 June 2004- p. 1/39 Future Muon Dipole Moment Measurements...
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Transcript of B. Lee Roberts, HIFW04, Isola d’Elba, 6 June 2004- p. 1/39 Future Muon Dipole Moment Measurements...
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B. Lee Roberts, HIFW04, Isola d’Elba, 6 June 2004 - p. 1/39
Future Muon Dipole Moment Measurements
at a high intensity muon source
B. Lee RobertsDepartment of Physics
Boston University
[email protected] http://physics.bu.edu/roberts.html
A Precision Path to the Frontier
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Outline• theory and motivation of dipole moments,
including the transition moment for μ→e conversion
• muon (g-2) present and future
• muon EDM
• summary and conclusions
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Magnetic moments, g-factors
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Electric and Magnetic Dipole Moments
Transformation properties:
An EDM implies both P and T are violated. An EDM at a measureable level would imply non-standard model CP. The baryon/antibaryon asymmetry in the universe, needs new sources of CP.
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Lagrangian for MDM and EDM
where α, β run from 0 to 3, and dμ is the electric dipole
moment. We could also use the dipole operator D
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Present EDM Limits
Particle Present EDM limit
(e-cm)
SM value
(e-cm)
n
future exp 10-24 to 10-25
*projected
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Unlike the EDM, there is a large SM value for the MDM
The Electron: to the level of the experimental error (4ppb),
Contribution of μ, (or anything heavier than the electron) is ≤4 ppb.
For the muon, the relative contribution of heavier particles
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Standard Model Value for (g-2)
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Two Hadronic Issues:• Lowest order hadronic contribution• Hadronic light-by-light
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Lowest Order Hadronic from e+e- annihilation
Can hadronic decay data be used? Eventually from the lattice?
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Hadronic light-by-light
• This contribution must be determined by calculation.
• While there have been issues with this contribution, things are settling down.
• a lattice calculation might improve things further, and give confidence in the models.
• the knowledge of this contribution limits knowledge of theory value.
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aμ is sensitive to all virtual particles which couple to the muon, e.g. SUSY
a toy model with equal susy masses gives:
If SUSY is discovered at LHC, then (g-2) will give a 20% determination of tan β
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SUSY connection between Dμ , μ → e
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Unlike the EDM, aμ is well measured.
the combined value is
Comparing with e+e- - data shows a discrepancy with the standard model of 2.4σ
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Where we came from:
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Today with e+e- based theory:
All E821 results were obtained with a “blind” analysis.
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Discrepancy with e+e- based theory
• What might this mean?• It all depends on your religion…
– if you believe in SUSY, then it is the predicted effect, and evidence for SUSY.
– if you are a non-believer then this discrepancy is interesting, or a fluctuation…
• Whatever you believe, muon (g-2) provides a wonderful test of the standard model.
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aμ implications for the muon EDM
This paper, published before our February 2001 announcement predicts a large muon EDM, and a corresponding SUSY contribution to aμ comparable to what we might be observing, with the e- EDM predicted to be 0.1 of the present limit.
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aμ implications for the muon EDM
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Basis of the experiments:
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Spin Precession Frequencies:
The EDM causes the spin to precess out of plane.
The motional E - field, β X B, is much stronger than laboratory electric fields.
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muon (g-2) storage ring
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Technique for muon (g-2)
use the magic γ = 29.3 and electrostatic focusing.
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Detectors and vacuum chamber
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E821 will improve muon EDM• however, the EDM signal is sitting on top
of a large background from g-2.
• we need to eliminate this background.
use a radial E field to turn off g-2 precession
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EDM – up/down Asymmetry• run off the magic γ and use a radial E-field
to turn off (g-2) precession
• Place detectors above and below the vacuum chamber and look for an up/down asymmetry which builds up with time
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The EDM ring• run with both μ+ and μ-.• there must be regions of combined E+B along
with separate focusing elements.• There needs to be a scheme to inject CW and
CCW.
E B p R
2 MV/m 0.25T 0.5 GeV/c 5 11μs 7 m
Possible Muon EDM Ring Parameters
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the lattice
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Detectors above and below
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up / down asymmetry
time (μs)
asym
met
ry
put in up-down/up+down
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NP2
• the figure of merit is Nμ times the polarization.
• we need
to reach the 10-24 e-cm level.
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Future Plans: (g-2)• we are preparing a proposal to BNL to
improve on our error from 0.5 ppm to ≤ 0.25 ppm.– proposal ready late July– defend in late September
This will require upgrades and ~28 weeks of beam time.• Longer term, if theory can support it, we
believe that at a high-intensity μ source we could reach 0.06 ppm.
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Future Plans: Muon EDM• The muon EDM experiment needs a high
intensity source, along with a polarized D beam to test systematic errors. A letter of intent was submitted to JPARC.
• A separate proposal to search for a Deuteron EDM is being prepared
(J. Miller, E. Stephenson and Y. Semertzidis
spokespersons).
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Deuteron EDM in a Storage Ring• Radial E-field to Control the g-2 Precession• Intense Polarized Deuteron Beams• Long Spin Coherence Time: 10s• Polarimeters: High Analyzing Power• Clockwise and Counter-Clockwise Injection
• Systematic Error: 10-27 ecm
• Statistical Error: 10-27 ecm
• Proposal This Summer to BNL, DOE/NSF
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Conclusions• The measured value of a differs from the SM
value by ~2.4 to 3 σ, and aμ will remain an important quantity. If SUSY is found, → tan β
• We propose to improve the precision of aμ .
• The muon EDM experiment can only be done at a high intensity muon source.
• We believe that a precision of 10-24 – 10-25 e-cm could be reached at a high intensity muon source.
• EDMs are an excellent opportunity to search for non-standard-model CP violation.