Study of τ decays to four-hadron final states with kaons
(144)
Arms, K
a
Gan, K K
a
Severini, H
b
Asner, D M
c
Dytman, S A
c
Love, W
c
Mehrabyan, S
c
Mueller, J A
c
Savinov, V
c
Li, Z
d
Lopez, A
d
Mendez, H
d
Ramirez, J
d
Huang, G S
e
Miller, D H
e
Pavlunin, V
e
Sanghi, B
e
Shibata, E I
e
Shipsey, I P J
e
Adams, G S
f
Chasse, M
f
Cravey, M
f
Cummings, J P
f
Danko, I
f
Napolitano, J
f
Muramatsu, H
g
Park, C S
g
Park, W
g
Thayer, J B
g
Thorndike, E H
g
Coan, T E
h
Gao, Y S
h
Liu, F
h
Stroynowski, R
h
Artuso, M
i
Boulahouache, C
i
Blusk, S
i
Butt, J
i
Dambasuren, E
i
Dorjkhaidav, O
i
Li, J
i
Menaa, N
i
Mountain, R
i
Nandakumar, R
i
Redjimi, R
i
Sia, R
i
Skwarnicki, T
i
Stone, S
i
Wang, J C
i
Zhang, K
i
Csorna, S E
j
Bonvicini, G
k
Cinabro, D
k
Dubrovin, M
k
Bornheim, A
l
Pappas, S P
l
Weinstein, A J
l
Briere, R A
m
Chen, G P
m
Ferguson, T
m
Tatishvili, G
m
Vogel, H
m
Watkins, M E
m
Rosner, J L
n
Adam, N E
o
Alexander, J P
o
Berkelman, K
o
Cassel, D G
o
Crede, V
o
Duboscq, J E
o
Ecklund, K M
o
Ehrlich, R
o
Fields, L
o
Galik, R S
o
Gibbons, L
o
Gittelman, B
o
Gray, R
o
Gray, S W
o
Hartill, D L
o
Heltsley, B K
o
Hertz, D
o
Hsu, L
o
Jones, C D
o
Kandaswamy, J
o
Kreinick, D L
o
Kuznetsov, V E
o
Mahlke Kruger H
o
Meyer, T O
o
Onyisi, P U E
o
Patterson, J R
o
Peterson, D
o
Pivarski, J
o
Riley, D
o
Ryd, A
o
Sadoff, A J
o
Schwarthoff, H
o
Shepherd, M R
o
Stroiney, S
o
Sun, W M
o
Thayer, J G
o
Urner, D
o
Wilksen, T
o
Weinberger, M
o
Athar, S B
p
Avery, P
p
Breva Newell, L
p
Patel, R
p
Potlia, V
p
Stoeck, H
p
Yelton, J
p
Rubin, P
q
Cawlfield, C
r
Eisenstein, B I
r
Gollin, G D
r
Karliner, I
r
Kim, D
r
Lowrey, N
r
Naik, P
r
Sedlack, C
r
Selen, M
r
Williams, J
r
Wiss, J
r
Edwards, K W
s,t
Besson, D
u
Pedlar, T K
v
Cronin Hennessy, D
w
Gao, K Y
w
Gong, D T
w
Kubota, Y
w
Klein, T
w
Lang, B W
w
Li, S Z
w
Poling, R
w
Scott, A W
x
Smith, A
w
Stepaniak, C J
w
Urheim, J
w,z
Dobbs, S
x
Metreveli, Z
x
Seth, K K
y
Tomaradze, A
x
Zweber, P
x
Ernst, J
y
Mahmood, A H
y
more..
|
-
1
-
-
18144386605
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.94.011803
-
E. Gamiz, Phys. Rev. Lett. 94, 011803 (2005). PRLTAO 0031-9007 10.1103/PhysRevLett.94.011803
-
(2005)
Phys. Rev. Lett.
, vol.94
, pp. 011803
-
-
Gamiz, E.1
-
2
-
-
18044394643
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.60.112002
-
S.J. Richichi (CLEO Collaboration), Phys. Rev. D 60, 112002 (1999). PRVDAQ 0556-2821 10.1103/PhysRevD.60.112002
-
(1999)
Phys. Rev. D
, vol.60
, pp. 112002
-
-
Richichi, S.J.1
-
3
-
-
85040630175
-
-
EPCFFB 1434-6044 10.1007/s100520050062
-
R. Barate (ALEPH Collaboration), Eur. Phys. J. C 1, 65 (1998). EPCFFB 1434-6044 10.1007/s100520050062
-
(1998)
Eur. Phys. J. C
, vol.1
, pp. 65
-
-
Barate, R.1
-
4
-
-
0001419102
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.55.1436
-
Bing An Li, Phys. Rev. D 55, 1436 (1997); PRVDAQ 0556-2821 10.1103/PhysRevD.55.1436
-
(1997)
Phys. Rev. D
, vol.55
, pp. 1436
-
-
An Li, B.1
-
5
-
-
84856132266
-
-
The ratio B(τ-→K-ωντ)/B(τ-→K- ρ0ντ) should be 1 instead of 1/3 in the paper, according to private communication with the author.
-
The ratio B(τ-→K-ωντ)/B(τ-→K- ρ0ντ) should be 1 instead of 1/3 in the paper, according to private communication with the author.
-
-
-
-
6
-
-
0026910982
-
-
NIMAER 0168-9002 10.1016/0168-9002(92)90770-5
-
Y. Kubota (CLEO Collaboration), Nucl. Instrum. Methods Phys. Res., Sect. A NIMAER 0168-9002 320, 66 (1992); 10.1016/0168-9002(92)90770-5
-
(1992)
Nucl. Instrum. Methods Phys. Res., Sect. A
, vol.320
, pp. 66
-
-
Kubota, Y.1
-
9
-
-
17044443243
-
-
NIMAER 0168-9002 10.1016/S0168-9002(02)02162-9
-
M. Artuso (CLEO Collaboration), Nucl. Instrum. Methods Phys. Res., Sect. A NIMAER 0168-9002 502, 91 (2003). 10.1016/S0168-9002(02)02162-9
-
(2003)
Nucl. Instrum. Methods Phys. Res., Sect. A
, vol.502
, pp. 91
-
-
Artuso, M.1
-
10
-
-
35949036344
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.39.1587
-
E. Farhi, Phys. Rev. Lett. 39, 1587 (1977). PRLTAO 0031-9007 10.1103/PhysRevLett.39.1587
-
(1977)
Phys. Rev. Lett.
, vol.39
, pp. 1587
-
-
Farhi, E.1
-
11
-
-
0043289601
-
-
CPHCBZ 0010-4655 10.1016/0010-4655(85)90123-7
-
S. Jadach and Z. Was, Comput. Phys. Commun. 36, 191 (1985); CPHCBZ 0010-4655 10.1016/0010-4655(85)90123-7
-
(1985)
Comput. Phys. Commun.
, vol.36
, pp. 191
-
-
Jadach, S.1
Was, Z.2
-
12
-
-
0026154388
-
-
CPHCBZ 0010-4655 10.1016/0010-4655(91)90037-L
-
S. Jadach Z. Was Comput. Phys. Commun. 64, 267 (1991); CPHCBZ 0010-4655 10.1016/0010-4655(91)90037-L
-
(1991)
Comput. Phys. Commun.
, vol.64
, pp. 267
-
-
Jadach, S.1
Was, Z.2
-
13
-
-
0026155753
-
-
CPHCBZ 0010-4655 10.1016/0010-4655(91)90038-M
-
S. Jadach, J.H. Kuhn, and Z. Was, Comput. Phys. Commun. 64, 275 (1991). CPHCBZ 0010-4655 10.1016/0010-4655(91)90038-M
-
(1991)
Comput. Phys. Commun.
, vol.64
, pp. 275
-
-
Jadach, S.1
Kuhn, J.H.2
Was, Z.3
-
14
-
-
27744562272
-
-
CERN-DD/EE/84-1
-
R. Brun, CERN, Report No. CERN-DD/EE/84-1, 1987 (unpublished).
-
(1987)
-
-
Brun, R.1
-
15
-
-
0001340366
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.57.3873
-
G.J. Feldman and R.D. Cousins, Phys. Rev. D 57, 3873 (1998). PRVDAQ 0556-2821 10.1103/PhysRevD.57.3873
-
(1998)
Phys. Rev. D
, vol.57
, pp. 3873
-
-
Feldman, G.J.1
Cousins, R.D.2
-
16
-
-
4243358999
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.76.4119
-
CLEO Collaboration, J.E. Bartelt, Phys. Rev. Lett. 76, 4119 (1996). PRLTAO 0031-9007 10.1103/PhysRevLett.76.4119
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 4119
-
-
Bartelt, J.E.1
-
17
-
-
0001124064
-
-
ZPCFD2 0170-9739 10.1007/s002880050387
-
D. Buskulic (ALEPH Collaboration), Z. Phys. C ZPCFD2 0170-9739 74, 263 (1997). 10.1007/s002880050387
-
(1997)
Z. Phys. C
, vol.74
, pp. 263
-
-
Buskulic, D.1
-
18
-
-
34447297049
-
-
PYLBAJ 0370-2693 10.1016/j.physletb.2004.06.001
-
S. Eidelman (Particle Data Group), Phys. Lett. B 592, 1 (2004). PYLBAJ 0370-2693 10.1016/j.physletb.2004.06.001
-
(2004)
Phys. Lett. B
, vol.592
, pp. 1
-
-
Eidelman, S.1
-
19
-
-
84856132265
-
-
The ratio B(τ-→K-ωντ)/B(τ-→K-π+π- π0ντ,ex.K0)=(0.554±0.056±0.063) is a bit higher than, but consistent with, the ratio B(τ-→h-ωντ)/B(τ- →h-h+h-π0ντ,ex.K0)=(0.446±0.015), suggesting a similar hadronization pattern in τ-→K-π+π-π0ντ and τ-→π-π+π-π0ντ decays.
-
The ratio B(τ-→K-ωντ)/B(τ-→K-π+π- π0ντ,ex.K0)=(0.554±0.056±0.063) is a bit higher than, but consistent with, the ratio B(τ-→h-ωντ)/B(τ- →h-h+h-π0ντ,ex.K0)=(0.446±0.015), suggesting a similar hadronization pattern in τ-→K-π+π-π0ντ and τ-→π-π+π-π0ντ decays.
-
-
-
|