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Refined measurement of theB-hadron lifetime
Author(s) -
R. A. Ong,
J. A. Jaros,
G. S. Abrams,
D. Amidei,
A. Baden,
T. Barklow,
A. M. Boyarski,
J. Boyer,
P. R. Burchat,
D. L. Burke,
F. Butler,
J. Dorfan,
G. J. Feldman,
G. Gidal,
L. Gladney,
Michael S. Gold,
G. Goldhaber,
L. Golding,
J. S. Haggerty,
Gail Hanson,
K. Hayes,
D. Herrup,
R. J. Hollebeek,
W. R. Innes,
I. Juricic,
J. A. Kadyk,
D. Karlen,
S. R. Klein,
A. J. Lankford,
R. R. Larsen,
B. W. LeClaire,
M. E. Levi,
N. S. Lockyer,
V. Lüth,
M. E. Nelson,
A. Petersen,
B. Richter,
K. Riles,
P. C. Rowson,
T. Schaad,
H. Schellman,
W. B. Schmidke,
P. Sheldon,
G. H. Trilling,
D. Wood,
J. Yelton
Publication year - 1989
Publication title -
physical review letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 3.688
H-Index - 673
eISSN - 1079-7114
pISSN - 0031-9007
DOI - 10.1103/physrevlett.62.1236
Subject(s) - hadron , lepton , physics , particle physics , nuclear physics , quark , momentum (technical analysis) , electron , finance , economics
We report a new measurement of the average lifetime of hadrons containing bottom quarks. The B hadron decays are tagged by identifying leptons at high transverse momentum. From a fit to the lepton impact parameter distribution, the average B hadron lifetime is found to be (0.98 f 0.12 f 0.13) x lo-l2 sec. The lifetime of hadrons containing bottom quarks is a measure of the strength of the weak transitions between the bottom quark and the charm and up quarks. In terms of the 3 x 3 quark mixing matrix proposed by Kobayashi and Maskawaf the B hadron lifetime depends on the magnitude of the matrix elements Vub and &b. Studies of B semileptonic decay’ have shown that Iv&l is small compared to I&l, and therefore the B lifetime essentially measures II&l and limits lvUbl. The data used in this measurement were collected with the Mark II detector at the e+estorage ring PEP (EC, = 29 GeV). We have previously reported a B lifetime measurement3 based on a data sample of 80 pb-l. The present work: based on a data sample of 204 pb-l, includes the previous data and supersedes our earlier analysis. We use the same procedure of measuring the impact parameters of leptons produced in B decay. However, we have improved upon the previous result through direct measurement of the experimental resolution function, a more precise determination of the B production point, and a comprehensive analysis of inclusive lepton production. These improvements combined with the increased statistics make this measurement of the B lifetime the most precise from any experiment to date. The Mark II detector has been described in detail elsewhere.5 A high resolution drift chamber, known as the vertex chamber, is situated inside the main tracking chamber. The two drift chambers are immersed in a solenoidal magnetic field of 2.3 kG. Particle trajectories are measured with high precision in the (2, y) plane perpendicular to th e b earns, and the impact parameter is accurately determined in that plane. Electrons are identified over 64 % of the solid angle with a lead-liquid-argon calorimeter. Muons are identified over 44 % of the solid angle by-a system of hadron absorbers and proportional tubes.

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