neutron decay
play

Neutron Decay Status and the future of the beta asymmetry - PowerPoint PPT Presentation

Neutron Decay Status and the future of the beta asymmetry measurement Takeyasu Ito Los Alamos National Laboratory The 4th International Workshop on the CKM Unitarity Triangle December 12-16, 2006 Nagoya University Nagoya, Japan Outline


  1. Neutron β Decay Status and the future of the beta asymmetry measurement Takeyasu Ito Los Alamos National Laboratory The 4th International Workshop on the CKM Unitarity Triangle December 12-16, 2006 Nagoya University Nagoya, Japan

  2. Outline • Introduction • Principle of the A measurement • Current status • Ongoing and future experiments – Perkeo III – UCNA – abBA • Summary

  3. Neutron β decay and V ud 2 G V 2 = V ud V ) 2 (1 + � R G F Neutron lifetime 2 2 1 R Kf ( G 3 G ) � ( τ = 885.7±0.8 s PDG2006) � = + V A Angular correlation in polarized neutron decay (Jackson et al ‘57) � � � � p p p p � d d 1 a e � A e B � � � � = � � + + � � + � � 0 n � � E E E E � � � � e e � � � � G 2 2 2 ( ) ( ) 1 Re Re � � � + � � � � A � � a , A 2 , B 2 = = � = G 2 2 2 1 3 1 3 1 3 + � + � + � V δλ / δ a ~ 3.3; a = –0.103 ± 0.004 (PDG2006) δλ / δ A ~ 2.6; A = –0.1173 ± 0.0013 (PDG2006) δλ / δ B ~ 13.4; B = –0.981 ± 0.004 (PDG2006)

  4. V ud Experimental Status |V ud | * |G A /G V | * δ A/A =0.6%

  5. Contribution to the V ud uncertainty 0 + → 0 + neutron 2984.48 s 4908.7 s 2 = 2 = V ud V ud � n (1 + 3 � 2 )(1 + � R ) ft (1 + RC )(1 + � R ) δ V ud (10 -4 ) δ V ud (10 -4 ) Contribution Contribution τ n ( δτ n = 0.8 s) 1.1 4 δ R λ ( δ A/A = 0.6%) 1.5 12 δ C 1.9 2 Δ R Δ R total 2.7 total 13 Marciano and Sirlin, PRL 96 , 032002 (2006)

  6. Principle of the A- coefficient Measurement Detector 1 Detector 2 B field e θ n Polarized neutron Decay electron dW =[1+ β PA cos θ ] d Γ ( E ) N ( E ) N ( E ) � A ( E ) 1 2 P A � cos = � � exp N ( E ) N ( E ) + 1 2 (End point energy = 782 keV)

  7. Potential Sources of Systematics • Neutron polarization determination • Background • Detector-related effects – Electron backscattering – Edge effect (fiducial volume selection) – Detector response, calibration

  8. Summary of previous systematics Experiment A Systematic Corrections (Beta-Asymmetry) P Background -0.1146 ± 0.0019 PERKEO 1986 2.6% 3% -0.1116 ± 0.0014 PNPI 1991 27% small ILL-TPC 1995 -0.1160 ± 0.0015 1.9% 3% -0.1189 ± 0.0012 PERKEO II 1997 1.5% 1.6% (15% environment) -0.1189 ± 0.0007 PERKEO II 2002 1.1% 0.5% (15% environment) Next generation experiment should address all these potential systematic errors.

  9. Perkeo II Experiment Electron energy spectrum •Dead layer: 20 keV •Threshold: 60 keV •S/N in ROI = 7

  10. Ongoing/Future Experiments Experiment Location Status Remarks Perkeo II ILL Analysis Data taking completed in 2004 Perkeo III ILL Construction Measures A aSPECT FRM-II Data taking/ Measures a Analysis aCorn NIST Construction Measures a UCNA LANL Construction/ Uses UCN to measure A to δ A/A = 0.2% Commissioning abBA ORNL-SNS Proposal/ Simultaneous measurement of a, b, B, A to δ A/A = 0.1% Detector (stat), δ a/a = 0.1% (stat) development Nab ORNL-SNS Proposal Uses unpolarized neutrons to measure a, b PANDA ORNL-SNS Proposal Measures C (= A + B )

  11. Perkeo III Experiment •Higher decay rate •Lower background •Smaller edge effect

  12. UCNA Experiment — General Approach Novel features: UCN from pulsed spallation source MWPC + plastic scintillator as β detector Goal: 0.2% measurement of A ( δ A/A = 0.2%) Neutron Polarization • – UCN (can produce >99% polarization with 7T magnetic field) – Diamond-like carbon coated neutron guide (low depolarization) Background • – Pulsed UCN source – MWPC+Plastic scintillator Electron backscattering • – MWPC+Plastic scintillator Fiducial volume selection • – MWPC Detector Characterization • – Off-line calibration system – Larger light collection

  13. Interlude — What are UCN? • Very slow neutrons (v < 8m/s) • Totally reflected by some materials • Hence, they can be totally confined within a bottle for periods in excess of 100 seconds. • Typically: velocity < 8m/s g kinetic energy < 3x10 -7 eV 3m wavelength > 500Å or temperature < 4 mK • cf: Gravity: 10 -7 eV/ meter. Magnetic field ( µ B): 10 -7 eV/ 1.7 T.

  14. UCNA Experiment — Apparatus Field Expansion Region Neutron Absorber

  15. UCNA Apparatus in LANSCE Area B

  16. UCNA Experiment — Status and timeline • Status – UCN source: commissioning – Beta detector: completed – Polarizer/spin flipper: commissioning – Neutron guides: construction • Plan – 2007: Commissioning, 1% measurement – 2008–: Physics run for 0.2% measurement • Future plans – Measurements of other correlation coefficients – Use of silicon detector

  17. Beta decay spectrum from UCN S/N in 200-400 keV = 13

  18. abBA — General approach • Simultaneous measurement of a, b, B, A • Coincidence detection of decay electrons and protons • Use of segmented Si detector as β detector • Use of pulsed cold neutron beam from spallation source • Use of 3 He neutron polarizer • Use of superconducting magnet providing 4 π coverage Goal: 0.1 % measurement of A

  19. ORNL-SNS-FNPB SNS: •Spallation neutron source driven by 1.4 GeV, 1mA proton linac •Construction completed in 2006 FNPB: •Beam line for fundamental neutron physics •Consists of cold line and UCN line •Start operation in 2007

  20. abBA — Experimental Layout at FNPB

  21. abBA — β spectrometer

  22. abBA — Status and Plans • Status – Proposal approved by FNPB PRAC – 3 He polarizer exists – Detector technology proven – Preliminary spectrometer design • Plans – 2007: Spectrometer design – 2008: Construction – 2009–: Commissioning & Physics run

  23. Summary • No new published A measurement results since 2002 • Several experiments aiming at δ A/A~10 -3 with different approaches on the way

Recommend


More recommend