B. Lee Roberts, Oxford University, 19 October 2004 - p. 1/55 The Muon: A Laboratory for Particle...
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Transcript of B. Lee Roberts, Oxford University, 19 October 2004 - p. 1/55 The Muon: A Laboratory for Particle...
B. Lee Roberts, Oxford University, 19 October 2004 - p. 1/55
The Muon: A Laboratory for Particle Physics
Everything you always wanted to know about the muon but were
afraid to ask.
B. Lee RobertsDepartment of Physics
Boston University
[email protected] http://physics.bu.edu/roberts.html
B. Lee Roberts, Oxford University, 19 October 2004 - p. 2/55
Outline
• Introduction to the muon
• Selected weak interaction parameters
• Muonium
• Lepton Flavor Violation
• Magnetic and electric dipole moments
• Summary and conclusions.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 3/55
The Muon (“Who ordered that?”)
• Lifetime ~2.2 s, practically forever
• 2nd generation lepton
• mme = 206.768 277(24)
• produced polarized
For decay in flight, “forward” and “backward” muons are highly polarized.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 4/55
The Muon – ctd.
• Decay is self analyzing
• It can be produced copiously in pion decay– PSI has 108 /s in a new beam
B. Lee Roberts, Oxford University, 19 October 2004 - p. 5/55
A precise measurement of + leads to a precise determination of GF
Predictive power in weak sector of SM:
Top quark mass prediction: mt = 177 20 GeV Input: GF (17 ppm), (4 ppb at q2=0), MZ (23 ppm),
2004 Update from D0 mt = 178 4.3 GeV
B. Lee Roberts, Oxford University, 19 October 2004 - p. 6/55
Lan @ PSI aims for a factor of 20 improvement
B. Lee Roberts, Oxford University, 19 October 2004 - p. 7/55
The Leptonic Currents
• Lepton current is (V – A)
There have been extensive studies at PSI by Gerber, Fetscher, et al. to look for other couplings in muon decay.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 8/55
Leptonic and hadronic currents• For nuclear capture there are induced
formfactors and the hadronic current contains 6 terms.– the induced pseudoscaler term is important
further enhanced in radiative muon capture
A new experiment at PSI MuCap hopes to resolve the present 3 discrepancy with PCAC
B. Lee Roberts, Oxford University, 19 October 2004 - p. 9/55
Muonium
Hydrogen (without the proton)
Zeeman splitting
p = 3.183 345 24(37) (120 ppb)
where p comes from proton NMR in the same B field
B. Lee Roberts, Oxford University, 19 October 2004 - p. 10/55
muonium and hydrogen hfs → proton structure
B. Lee Roberts, Oxford University, 19 October 2004 - p. 11/55
Lepton Flavor
• We have found empirically that lepton number is conserved in muon decay and in beta decay.– e.g.
• What about
or
B. Lee Roberts, Oxford University, 19 October 2004 - p. 12/55
General Statements
• We know that oscillate– neutral lepton flavor violation
• Expect charged lepton flavor violation at some level– enhanced if there is new dynamics at the TeV
scale• in particular if there is SUSY
• We expect CP in the lepton sector (EDMs as well as oscillations)– possible connection with cosmology
(leptogenesis)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 13/55
The Muon Trio:• Lepton Flavor Violation
• Muon MDM (g-2) chiral changing
• Muon EDM
B. Lee Roberts, Oxford University, 19 October 2004 - p. 14/55
Past and Future of LFV Limits
+e-→-e+
MEG → e – 10-13 BR sensitivity
• under construction at PSI, first data in 2006
MECO ++A→e++A– 10-17 BR
sensitivity• approved at
Brookhaven, not yet funded (Needs Congressional approval)
Bra
nchi
ng R
atio
Lim
it
B. Lee Roberts, Oxford University, 19 October 2004 - p. 15/55
Magnetic Dipole Moments
The field was started by Stern
B. Lee Roberts, Oxford University, 19 October 2004 - p. 16/55
Z. Phys. 7, 249 (1921)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 17/55
(in modern language)
673 (1924)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 18/55
Dirac + Pauli moment
B. Lee Roberts, Oxford University, 19 October 2004 - p. 19/55
Dirac Equation Predicts g=2
• radiative corrections change g
B. Lee Roberts, Oxford University, 19 October 2004 - p. 20/55
The CERN Muon (g-2) Experiments
The muon was shown to be a point particle obeying QED
The final CERN precision was 7.3 ppm
B. Lee Roberts, Oxford University, 19 October 2004 - p. 21/55
Standard Model Value for (g-2)
relative contribution of heavier things
B. Lee Roberts, Oxford University, 19 October 2004 - p. 22/55
Two Hadronic Issues:
• Lowest order hadronic contribution• Hadronic light-by-light
B. Lee Roberts, Oxford University, 19 October 2004 - p. 23/55
Lowest Order Hadronic from e+e- annihilation
B. Lee Roberts, Oxford University, 19 October 2004 - p. 24/55
a(had) from hadronic decay?
• Assume: CVC, no 2nd-class currents, isospin breaking corrections.
• n.b. decay has no isoscalar piece, while e+e- does• Many inconsistencies in comparison of e+e- and
decay:
- Using CVC to predict branching ratios gives 0.7 to 3.6 discrepancies with reality.
- F from decay has different shape from e+e-.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 25/55
• Comparison with CMD-2 in the Energy Range 0.37 <s<0.93 GeV2
(375.6 0.8stat 4.9syst+theo) 10-10
(378.6 2.7stat 2.3syst+theo) 10-10
KLOECMD2
1.3% Error0.9% Error
a= (388.7 0.8stat 3.5syst
3.5theo) 10-10
2 contribution to ahadr
• KLOE has evaluated the Dispersions Integral for the 2-Pion-Channel in the Energy Range 0.35 <s<0.95 GeV2
• At large values of s (>m) KLOE is consistent with CMD and therefore
They confirm the deviation from -data!.
Pion Formfactor
CMD-2KLOE
0.4 0.5 0.6 0.7 0.8 0.9
s [GeV2]
45
40
35
30
25
20
15
10
5
45
0
KLOE Data on R(s)
Courtesy of G. Venanzone
B. Lee Roberts, Oxford University, 19 October 2004 - p. 26/55
A. Höcker at ICHEP04
B. Lee Roberts, Oxford University, 19 October 2004 - p. 27/55
ahad [e+e–
] = (693.4 ± 5.3 ± 3.5) 10 –10
a SM
[e+e–
] = (11 659 182.8 ± 6.3had ± 3.5LBL ± 0.3QED+EW) 10 –10
Weak contribution aweak = + (15.4 ± 0.3) 10
–10
Hadronic contribution from higher order : ahad [( /)3] = – (10.0 ± 0.6) 10
–10
Hadronic contribution from LBL scattering: ahad [LBL] = + (12.0 ± 3.5) 10
–10
a exp – a
SM =(25.2 ± 9.2) 10
–
10
2.7 ”standard deviations“
Observed Difference with Experiment:
BNL E821 (2004):a
exp =(11 659 208.0 5.8) 10 10
not yet published
not yet published
preliminary
SM Theory from ICHEP04 (A. Höcker)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 28/55
Hadronic light-by-light
• This contribution must be determined by calculation.
• the knowledge of this contribution limits knowledge of theory value.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 29/55
aμ is sensitive to a wide range of new physics
• muon substructure
• anomalous couplings• SUSY (with large tanβ )
• many other things (extra dimensions, etc.)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 30/55
SUSY connection between a , Dμ , μ → e
B. Lee Roberts, Oxford University, 19 October 2004 - p. 31/55
Courtesy K.Olivebased on Ellis, Olive, Santoso, Spanos
In CMSSM, a can be combined with b → s, cosmological relic density h2, and LEP Higgs searches to constrain mass
Allowedband a(exp) – a(e+e- theory)
Excluded by direct searches
Excluded for neutral dark matter
Preferred
same discrepancy no discrepancy
With expected improvements in ahad + E969 the error on the difference
B. Lee Roberts, Oxford University, 19 October 2004 - p. 32/55
Spin Precession Frequencies: in B field
The EDM causes the spin to precess out of plane.
The motional E - field, β X B, is much stronger than laboratory electric fields.
spin difference frequency = s - c
0
B. Lee Roberts, Oxford University, 19 October 2004 - p. 33/55
Inflector
Kicker Modules
Storagering
Central orbitInjection orbit
Pions
Target
Protons
π
(from AGS) p=3.1GeV/c
Experimental Technique
π
μνS
Spin
Momentum
B
• Muon polarization• Muon storage ring• injection & kicking• focus by Electric Quadrupoles• 24 electron calorimeters
R=711.2cm
d=9cm
(1.45T)
Electric Quadrupoles
polarized
B. Lee Roberts, Oxford University, 19 October 2004 - p. 34/55
muon (g-2) storage ring
B. Lee Roberts, Oxford University, 19 October 2004 - p. 35/55
The Storage Ring Magnet
r = 7112 mm
B0 = 1.45 T
cyc = 149 ns
(g-2) = 4.37 s
= 64.4 s
p = 3.094 GeV/c
B Field Measurement
2001
B. Lee Roberts, Oxford University, 19 October 2004 - p. 37/55
B. Lee Roberts, Oxford University, 19 October 2004 - p. 38/55
Detectors and vacuum chamber
Detector acceptance depends on radial position of the when it decays.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 39/55
B. Lee Roberts, Oxford University, 19 October 2004 - p. 40/55
Fourier Transform: residuals to 5-parameter fit
beam motion across a
scintillating fiber – ~15 turn period
B. Lee Roberts, Oxford University, 19 October 2004 - p. 41/55
Where we came from:
B. Lee Roberts, Oxford University, 19 October 2004 - p. 42/55
Today with e+e- based theory:All E821 results were obtained with a “blind” analysis.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 43/55
Life Beyond E821?
• With a 2.7 discrepancy, you’ve got to go further.
• A new upgraded experiment was approved by the BNL PAC in September
E969• Goal: total error = 0.2 ppm
– lower systematic errors– more beam
B. Lee Roberts, Oxford University, 19 October 2004 - p. 44/55
E969: Systematic Error Goal
• Field improvements will involve better trolley calibrations, better tracking of the field with time, temperature stability of room, improvements in the hardware
• Precession improvements will involve new scraping scheme, lower thresholds, more complete digitization periods, better energy calibration
Systematic uncertainty (ppm) 1998 1999 2000 2001 E969
Goal
Magnetic field – p 0.5 0.4 0.24 0.17 0.1
Anomalous precession – a 0.8 0.3 0.3 0.21 0.1
B. Lee Roberts, Oxford University, 19 October 2004 - p. 45/55
Improved transmission into the ring
InflectorInflector aperture
Storage ring aperture
E821 Closed End E821 Prototype Open End
B. Lee Roberts, Oxford University, 19 October 2004 - p. 46/55
E969: backward decay beam
Pions @ 5.32 GeV/c
Decay muons @ 3.094 GeV/c
No hadron-induced prompt flash
Approximately the same muon flux is realized
x 1 more
muons
Expect for both sides
Pedestal vs. Time
Near side Far side
E821
E821: Pions @ 3.115 GeV/c
momentum
collimator
B. Lee Roberts, Oxford University, 19 October 2004 - p. 47/55
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.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 48/55
Present EDM Limits
Particle Present EDM limit
(e-cm)
SM value
(e-cm)
n
future exp 10-24 to 10-25
*projected
B. Lee Roberts, Oxford University, 19 October 2004 - p. 49/55
μ EDM may be enhancedabove mμ/me × e EDM
Magnitude increases withmagnitude of ν Yukawa couplings
and tan β
μ EDM greatly enhanced when heavy neutrinos non-degenerate
Model Calculations of EDM
B. Lee Roberts, Oxford University, 19 October 2004 - p. 50/55
aμ implications for the muon EDM
B. Lee Roberts, Oxford University, 19 October 2004 - p. 51/55
Recall
The EDM causes the spin to precess out of plane.
EDM Systematic errors are huge in E821 because of (g-2) precession!
B. Lee Roberts, Oxford University, 19 October 2004 - p. 52/55
Muon EDM
• use radial E field to “turn off” g-2 precession so the spin follows the momentum.
• look for an up-down asymmetry which builds up with time
B. Lee Roberts, Oxford University, 19 October 2004 - p. 53/55
Beam Needs: NP2
• the figure of merit is Nμ times the polarization.
• we need
to reach the 10-24 e-cm level. • Since SUSY calculations range from 10-22 to
10-32 e cm, more muons is better.
= 5*10-7
(Up-
Dow
n)/(
Up+
Dow
n)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 54/55
Summary and Outlook
• The muon has provided us with much knowledge on how nature works.
• New experiments on the horizion continue this tradition.
• Muon (g-2), with a precision of 0.5 ppm, has a 2.7 discrepancy with the standard model.
• This new physics, if confirmed, would show up in an EDM as well.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 55/55
Outlook• Scenario 1
– LHC finds SUSY– (g-2), LFV help provide information on
important aspects of this new reality; for (g-2) → tan
• Scenario 2– LHC finds the Standard Model Higgs at a
reasonable mass, nothing else, (g-2) discrepancy and m might be the only indication of new physics
– virtual physics, e.g. (g-2), EDM, →e conversion would be even more important.
Stay tuned !
Thank you
B. Lee Roberts, Oxford University, 19 October 2004 - p. 56/55
Extra slides
B. Lee Roberts, Oxford University, 19 October 2004 - p. 57/55
Better agreement between exclusive and inclusive (2) data than in 1997-1998 analyses
Agreement between Data (BES) and pQCD (within correlated systematic errors)
use QCD
use data
use QCD
Evaluating the Dispersion Integral
from A. Höcker ICHEP04
B. Lee Roberts, Oxford University, 19 October 2004 - p. 58/55
Tests of CVC (A. Höcker – ICHEP04)
B. Lee Roberts, Oxford University, 19 October 2004 - p. 59/55
Shape of F from e+e- and hadronic decay
zoom
Comparison between t data and e+e- data from CDM2 (Novosibirsk)
New precision data from KLOE confirms
CMD2
B. Lee Roberts, Oxford University, 19 October 2004 - p. 60/55
The MECO ApparatusStraw Tracker
Crystal Calorimeter
Muon Stopping Target
Muon Beam Stop
Superconducting Production Solenoid
(5.0 T – 2.5 T)
Superconducting Detector Solenoid
(2.0 T – 1.0 T)
Superconducting Transport Solenoid
(2.5 T – 2.1 T)
Collimators
10-17 BR single event sensitivity
p beam
approved but not funded
B. Lee Roberts, Oxford University, 19 October 2004 - p. 61/55
MEG @ PSI (10-13 BR sensitivity)
MEG will start running in 2006
B. Lee Roberts, Oxford University, 19 October 2004 - p. 62/55
Experimental Experimental boundbound
Largely favouredLargely favoured and confirmed by and confirmed by KamlandKamland
Additional contributionAdditional contribution toto slepton mixingslepton mixing fromfrom VV2121, matrix element , matrix element responsible responsible forfor solar neutrino deficit solar neutrino deficit. (. (J. Hisano & N. Nomura, Phys. Rev. J. Hisano & N. Nomura, Phys. Rev. D59D59 (1999) (1999) 116005)116005)..
All All solar solar experimentsexperiments combinedcombined
tan(tan() = ) = 3030
tan(tan() = 0) = 0
MEG MEG goalgoal
AfterAfterKamlandKamland
Connection with oscillations
B. Lee Roberts, Oxford University, 19 October 2004 - p. 63/55
E821 ωp systematic errors (ppm)
E969
(i)(I)
(II)
(III)
(iv)
*higher multipoles, trolley voltage and temperature response, kicker eddy currents, and time-
varying stray fields.
B. Lee Roberts, Oxford University, 19 October 2004 - p. 64/55
Systematic errors on ωa (ppm)
σsystematic 1999 2000 2001 E969
Pile-up 0.13 0.13 0.08 0.07
AGS Background 0.10 0.10 *
Lost Muons 0.10 0.10 0.09 0.04
Timing Shifts 0.10 0.02 0.02
E-Field, Pitch 0.08 0.03 * 0.05
Fitting/Binning 0.07 0.06 *
CBO 0.05 0.21 0.07 0.04
Beam Debunching 0.04 0.04 *
Gain Change 0.02 0.13 0.13 0.03
total 0.3 0.31 0.21 0.11Σ* = 0.11