Peter Kammel

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Peter Kammel First Results from the New First Results from the New Muon Lifetime Experiments Muon Lifetime Experiments at PSI at PSI G F g P L 1A MuCap “MuSun” project MuLan

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First Results from the New Muon Lifetime Experiments at PSI. G F. g P. Peter Kammel. MuLan. MuCap. L 1A. “MuSun” project. MuCap. g P. MuCap Physics Case. EW current key probe Understanding hadrons from QCD Symmetries of Standard Model Muon Capture Formfactors. - PowerPoint PPT Presentation

Transcript of Peter Kammel

Page 1: Peter Kammel

Peter Kammel

First Results from the New Muon First Results from the New Muon Lifetime Experiments at PSILifetime Experiments at PSI

GFgP

L1A

MuCap

“MuSun”project

MuLan

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EW current key probe Understanding hadrons from QCD Symmetries of Standard Model

Muon Capture

Formfactors

MuCap Physics CaseMuCap Physics Case

MuCap

- + p + n rateS at q2= -0.88 m2- + p + n rateS at q2= -0.88 m

2

Lorentz, T invariance+ second class currentssuppressed by isospin symm.

apart from gP = 8.3 ± 50% apart from gP = 8.3 ± 50%

All form factors precisely known fromSM symmetries and data

gg

PP

The Black Sheep of Form Factors T. Hemmert

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gP determined by chiral symmetry of QCD:

gP= (8.74 0.23) – (0.48 0.02) = 8.26 0.23

PCAC pole term Adler, Dothan, Wolfenstein

ChPT leading order one loop two-loop <1% N. Kaiser Phys. Rev. C67 (2003) 027002

• gP basic and experimentally least known EW nucleon form factor

• solid QCD prediction via HBChPT (2-3% level)

• basic test of QCD symmetries

• gP basic and experimentally least known EW nucleon form factor

• solid QCD prediction via HBChPT (2-3% level)

• basic test of QCD symmetries

Recent reviews:T. Gorringe, H. Fearing, Rev. Mod. Physics 76 (2004) 31V. Bernard et al., Nucl. Part. Phys. 28 (2002), R1

Pseudoscalar Form Factor gPseudoscalar Form Factor gPPMuCa

p

n

p

-

gNN

F

W

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InterpretationInterpretation of Experiments ?of Experiments ?

T = 12 s-1

pμ↑↓

singlet (F=0)

S= 710 s-1

n+

triplet(F=1)

μ

pμ↑↑

ppμ

para (J=0)ortho (J=1)

λop

ortho=506 s-1 para=200 s-1

ppμ ppμ ppμ

• Interpretation requires knowledge of pp population

• Strong dependence on hydrogen density

ppP

ppO

p

100% LH2

p

ppP

ppO

1 % LH2

time (s)

λ pp

MuCap

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Lifetime method

1010 →e decays

measure to 10ppm,

S = 1/ - 1/to 1%

Unambiguous interpretation at 1% LH2 density Clean stop definition in active target (TPC) to avoid wall stops

Ultra-pure gas system and purity monitoring at 10 ppb level

Isotopically pure “protium”

MuCap Experimental StrategyMuCap Experimental Strategy

fulfill all requirements simultaneouslyunique MuCap capabilities

MuCap

log

(co

un

ts)

te-t

μ+

μ –

S reduces lifetime by 10-3

→ e

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3D tracking w/o material in fiducial volume

Muons stop in active TPC targetMuons stop in active TPC target

p-

Observed muon stopping distribution

E

e-

10 bar ultra-pure hydrogen, 1.16% LH2

2.0 kV/cm drift field ~5.4 kV on 3.5 mm anode half gapbakeable glass/ceramic materials

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Time SpectraTime Spectra

-e impact parameter cut

huge background suppression

diffusion (deuterium) monitoring

blinded master clock frequency

variety of consistency checks

6 m

m In

sid

e T

PC

MuCap

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ResultsResults

SMuCap = 725.0 13.7stat 10.7sys s-1S

MuCap = 725.0 13.7stat 10.7sys s-1

Average of HBChPT calculations of S:

(MuCap 2007)gP = 7.3 ± 1.1gP = 7.3 ± 1.1

Apply new rad. correction (2.8%):

arXiv:0704.2072v1 [nucl-ex]

arXiv:0704.3968v1 [hep-ph]Czarnecki, Marciano,Sirlin

further sub percent theory required

MuCap

accepted PRL

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• MuCap result nearly model independent First precise and unambiguous result

• Consistent with chiral prediction Does not confirm radiative muon capture (RMC) discrepancy

• Final result (’06 and ’07 data) will reduce error twofold

• MuCap result nearly model independent First precise and unambiguous result

• Consistent with chiral prediction Does not confirm radiative muon capture (RMC) discrepancy

• Final result (’06 and ’07 data) will reduce error twofold

ggP P Landscape after MuCap 06Landscape after MuCap 06

Before MuCap experiments inconclusive and mutually inconsistent

MuCap

MuCap

- + p + n +

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MuLan Scientific CaseMuLan Scientific Case

Fundamental electroweak parameters

GF

Implicit to all EW precision physics

Uniquely related to muon decay

PrecisionGF relation no longer theory limited

9 ppm 0.0007 ppm 23 ppm

GF MZ

QED

MuLan2004

MuLanGoal

theory 17 ppm 18 ppm 90 ppb 30 ppm 9 ppm 18 ppm <0.3 ppm

0.5 ppm 1 ppm <0.3 ppm

17 ppm 18 ppm 90 ppb 30 ppm 9 ppm 18 ppm <0.3 ppm

0.5 ppm 1 ppm <0.3 ppm

van Ritbergen and Stuart:

2-loop QED corrections

MuLan

exp

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PSI DC proton beam590 MeV, 1.7 mA

Kicker On

Fill Period

Measurement Period

time

Num

ber

(log

scal

e)

-12.5 kV

12.5 kV

Real data

MuLan ExperimentMuLan Experiment“Early-to-late” changes

• Instrumental shiftsGain or threshold

Time response

• Effective acceptanceResidual polarization or precession

Pileup

• Missing events

Systematics

MuLan

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MuLan = 2.197 013(21)(11) s (11ppm)

(World) = 2.197 019(21) s (9.6 ppm)

GF = 1.166 371(6) x 10-5 GeV-2 (5 ppm)

MuLan = 2.197 013(21)(11) s (11ppm)

(World) = 2.197 019(21) s (9.6 ppm)

GF = 1.166 371(6) x 10-5 GeV-2 (5 ppm)

arXiv:0704.1981v1 [hep-ex]

MuLan

6/5/07 accepted PRL

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“Calibrating the Sun” via Muon Capture on the Deuteron + d + d n + n + n + n +

Goal

total d capture rate to 1% precision

Motivation• first precise measurement of basic EW reaction in 2N system, benchmark measurement with 10x higher precision

• impact on fundamental astrophysics reactions (SNO, pp)

• comparison of modern high precision calculations (EFT/SNPA)

• high precision feasible by Cap technique and careful optimization

model-independent connection via EFT & Lmodel-independent connection via EFT & L1A1A

MEC

EFTL1A

proposal end 2007

“MuSun”

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Synergy and OutlookSynergy and Outlook

log

(co

un

ts)

timeμ+

μ –

20 ppm 10 ppm 1 ppm?? 30 ppm 10 ppm

2006 2008projected

•MuLan

•MuCap

•MuSun needs both, gP and precision lifetimes