Back to Search Start Over

First Observation ofτ→3πηντandτ→f1πντDecays

Authors :
J. Masui
L. P. Perera
J. S. Miller
Y. S. Gao
S. Menary
S. J. Patton
D. W. Bliss
H. Yamamoto
Sheldon Stone
Paul Avery
Yang Li
T. S. Hill
R. Ehrlich
S. Schrenk
Richard L. Greene
E. H. Thorndike
D. L. Kreinick
C. Bebek
Yanwen Liu
J. G. Smith
R. Wang
D. Cinabro
G. Masek
Juliet Ritchie Patterson
D. L. Hartill
D. Z. Besson
D. He
S. D. Johnson
M. Yurko
D. Coppage
E. I. Shibata
G. Bonvicini
Sacha E Kopp
D. S. Crowcroft
Alain Bellerive
Yurii Maravin
John E. Bartelt
D. J. Lange
Y. J. Kwon
Alexander Undrus
S. B. Anderson
R. M. Hans
J. P. Alexander
K. Lingel
T. E. Browder
R. Ammar
W. T. Ford
R. D. Kass
R. Balest
M. S. Alam
R. Wanke
B. Gittelman
Marina Artuso
I. C. Lai
S. Chan
J. D. Richman
June Hyuk Lee
X. J. Zhou
H. Marsiske
A. H. Mahmood
M. Ogg
C. P. Ward
F. Li
A. D. Foland
F. R. Wappler
V. Savinov
C. P. Jessop
Horst Severini
J. Staeck
W. R. Ross
S. Glenn
R. A. Briere
M. A. Marsh
J. Zheng
K. K. Gan
T. Skwarnicki
D. H. Miller
L. K. Gibbons
A. Anastassov
S. B. Athar
P. Pomianowski
G. E. Gladding
S. Kotov
B. C. Barish
Z. Ling
J. Urheim
B. Valant-Spaight
R. Davis
I. P. J. Shipsey
Erik A. Johnson
S. Schuh
Ilya Kravchenko
P. C. Kim
M. Goldberg
G. C. Moneti
Vivek Sharma
John Yelton
K. M. Ecklund
H. Kagan
C. P. O'Grady
Jayashree Roy
P. Gaidarev
M.A. Palmer
C. D. Jones
G. J. Zhou
J. J. Thaler
N. Hancock
M. B. Spencer
N. Kwak
R. S. Galik
B. Nemati
G. H. A. Viehhauser
V.G. Shelkov
J. W. Hinson
T. Hart
C.Y. Prescott
R. J. Morrison
Mats A Selen
S. Roberts
B. E. Berger
D. Y.J. Kim
M. Lohner
I. Narsky
M. Bishai
J. J. O'Neill
D. M. Coffman
J. L. Rodriguez
H. A. Cho
A. J. Sadoff
A. J.R. Weinstein
T. Riehle
B. K. Heltsley
Frank Würthwein
S. J. Lee
Jianqiao Ye
G. D. Gollin
P. S. Drell
N. B. Mistry
R. J. Wilson
Vipul Jain
S. Prell
E. Gerndt
C. Qiao
T. E. Coan
Vitaliy Fadeyev
K. Honscheid
D. B. MacFarlane
N. Menon
C. R. Ng
C. Darling
A. Soffer
S. W. Gray
J. Mevissen
I. Karliner
Michael S. Witherell
T. K. Nelson
Ryszard Stroynowski
D. Fujino
A. M. Smith
J. E. Duboscq
K. W. Edwards
M.K. Sung
P. I. Hopman
H. N. Nelson
J. Kandaswamy
T. Bergfeld
S. J. Richichi
A. Wolf
Igor Volobouev
M. M. Zoeller
J. A. Ernst
P. Skubic
Alexander Ershov
S. E. Csorna
M. Gao
J. Gronberg
H. P. Paar
K. Kinoshita
Ilya Korolkov
G. W. Brandenburg
E. Nordberg
G. S. Ludwig
D. Peterson
K. W. McLean
R. Godang
T. Lee
M. Schmidtler
R. Mountain
M. Dickson
D. G. Cassel
R. Poling
B. I. Eisenstein
Philip Baringer
Xiangjun Xing
B. H. Behrens
R. Janicek
Harold S. Park
Alice Bean
Kenneth Bloom
G. Eigen
S.C. Timm
M. Chadha
James E. Fast
D. Ugolini
D. A. Roberts
Anders Ryd
M. Athanas
Sz Márka
Robert K. Kutschke
Karl Berkelman
A. Efimov
D. Riley
S. Blinov
M. L. Perl
Yuichi Kubota
D. M. Asner
P. M. Patel
Source :
Physical Review Letters. 79:2406-2410
Publication Year :
1997
Publisher :
American Physical Society (APS), 1997.

Abstract

We have observed new channels for $\ensuremath{\tau}$ decays with an $\ensuremath{\eta}$ in the final state. We study 3-prong tau decays, using the $\ensuremath{\eta}\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma}$ and $\ensuremath{\eta}\ensuremath{\rightarrow}3{\ensuremath{\pi}}^{0}$ decay modes and 1-prong decays with two ${\ensuremath{\pi}}^{0}$'s using the $\ensuremath{\eta}\ensuremath{\rightarrow}\ensuremath{\gamma}\ensuremath{\gamma}$ channel. The measured branching fractions are $B({\ensuremath{\tau}}^{\ensuremath{-}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{+}\ensuremath{\eta}{\ensuremath{\nu}}_{\ensuremath{\tau}})\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}({3.4}_{\ensuremath{-}0.5}^{+0.6}\ifmmode\pm\else\textpm\fi{}0.6)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$ and $B({\ensuremath{\tau}}^{\ensuremath{-}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{\ensuremath{-}}2{\ensuremath{\pi}}^{0}\ensuremath{\eta}{\ensuremath{\nu}}_{\ensuremath{\tau}})\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(1.4\ifmmode\pm\else\textpm\fi{}0.6\ifmmode\pm\else\textpm\fi{}0.3)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$. We observe clear evidence for ${f}_{1}\ensuremath{\rightarrow}\ensuremath{\eta}\ensuremath{\pi}\ensuremath{\pi}$ substructure and measure $B({\ensuremath{\tau}}^{\ensuremath{-}}\ensuremath{\rightarrow}{f}_{1}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\nu}}_{\ensuremath{\tau}})\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}({5.8}_{\ensuremath{-}1.3}^{+1.4}\ifmmode\pm\else\textpm\fi{}1.8)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$. We have also searched for ${\ensuremath{\eta}}^{\ensuremath{'}}(958)$ production and obtain 90% C.L. upper limits $B({\ensuremath{\tau}}^{\ensuremath{-}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\eta}}^{\ensuremath{'}}{\ensuremath{\nu}}_{\ensuremath{\tau}})l7.4\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}$ and $B({\ensuremath{\tau}}^{\ensuremath{-}}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}{\ensuremath{\eta}}^{\ensuremath{'}}{\ensuremath{\nu}}_{\ensuremath{\tau}})l8.0\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}5}$.

Details

ISSN :
10797114 and 00319007
Volume :
79
Database :
OpenAIRE
Journal :
Physical Review Letters
Accession number :
edsair.doi...........c7c556d3d07361bf5aa05c85f282f0b8