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Measurement of the kaon content of three-prong tau decays

Authors :
M. K. Sullivan
H. Yamamoto
S. J. Yellin
D. E. Pellett
Y. X. Wang
J. Lys
G. S. Greenbaum
R. L. Holtzapple
G. Zapalac
E. M. Wang
H. H. Bingham
George P Yost
S. C. Loken
S. Khacheryan
R. R. Ross
D. O. Caldwell
G. R. Lynch
A. Lu
D. R. Nygren
R. J. Madaras
G. Godfrey
W.A. Wenzel
Gilbert Shapiro
A. M. Eisner
M. L. Stevenson
K. T. Knöpfle
E. S. Miller
R. C. Berg
Werner Hofmann
J. M. Hauptman
R. R. Kofler
Philippe Eberhard
D. J. Lambert
H. P. Paar
Y. T. Oyang
Orin I. Dahl
M. T. Ronan
K. H. Fairfield
H. Marsiske
C. D. Buchanan
W. Vernon
N. A. Nicol
A. P.T. Palounek
R. Belcinski
M. G. Strauss
S. B. Chun
E.E. Bloom
A. R. Clark
D.A. Bauer
J. J. Eastman
G. E. Masek
R. W. Stephens
Source :
Bauer, D.A.; Belcinski, R.; Berg, R.C.; Bingham, H.H.; Bloom, E.E.; Buchanan, C.D.; et al.(1993). Measurement of the Kaon Content of Three-Prong Tau Decays. Physical Review D, 50(1). Lawrence Berkeley National Laboratory: Lawrence Berkeley National Laboratory. Retrieved from: http://www.escholarship.org/uc/item/9vw4v3hw
Publication Year :
1994

Abstract

We present branching fraction measurements of three-prong decays of the [tau][sup [minus]] lepton based on data from the TPC/Two-Gamma detector at SLAC PEP. The decays are classified according to the identities of the charged tracks to give simultaneous measurements of [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]] [ital K][sup [minus]][pi][sup +][pi][sup [minus]]]=0.58[sub [minus]0.13][sup +0.15]% and [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]] [ital K][sup [minus]][ital K][sup +][pi][sup [minus]]]=0.15[sub [minus]0.07][sup +0.09]%, and upper limits of [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]][pi][sup [minus]][ital K][sup +][pi][sup [minus]]][lt]0.25%, [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]] [ital K][sup [minus]][pi][sup +][ital K][sup [minus]]][lt]0.09%, and [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]] [ital K][sup [minus]][ital K][sup +][ital K][sup [minus]]][lt]0.21%, where additional neutrals may be present in each case. The branching fractions are normalized to the world average three-prong topological branching fraction and there is an estimated 20% systematic error in addition to the listed statistical errors. We find the mass distributions in the [ital K][sup [minus]][pi][sup +][pi][sup [minus]] decay are consistent with [ital K][sub 1] dominance, and obtain branching fractions of [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]] [ital K][sub 1][sup [minus]](1270)]=0.41[sub [minus]0.35][sup +0.41]% and [ital B][[tau][sup [minus]][r arrow][nu][sub [tau]] [ital K][sub 1][sup [minus]](1400)]=0.76[sub [minus]0.33][sup +0.40]%.

Details

ISSN :
05562821
Volume :
50
Issue :
1
Database :
OpenAIRE
Journal :
Physical review. D, Particles and fields
Accession number :
edsair.doi.dedup.....2a71be91a3afa34463a34d3179f1a71b