Study of B meson decays to three-body charmless hadronic final states
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Garmash, A
b,i
Abe, K
i,ar
Abe, T
i
Adachi, I
i
Aihara, H
at
Akatsu, M
w
Asano, Y
ay
Aushev, T
m
Bakich, A M
ao
Ban, Y
ah
Bedny, I
b
Behera, P K
az
Bizjak, I
n
Bondar, A
b
Bozek, A
ab
Bracko M
n,u
Browder, T E
h
Casey, B C K
h
Chang, P
aa
Chao, Y
aa
Chen, K
aa
Cheon, B G
an
Chistov, R
m
Choi, S
g
Choi, Y
an
Chuvikov, A
ai
Danilov, M
m
Dash, M
ba
Dong, L Y
k
Drutskoy, A
m
Eidelman, S
b
Eiges, V
m
Fukunaga, C
av
Gabyshev, N
i
Gershon, T
i
Golob, B
n,t
Gordon, A
v
Guo, R
y
Haba, J
i
Hagner, C
ba
Hara, T
af
Hastings, N C
i
Hayashii, H
x
Hazumi, M
i
Higuchi, I
as
Hinz, L
s
Hokuue, T
w
Hoshi, Y
ar
Hou, W
aa
Huang, H
aa
Igarashi, Y
i
Iijima, T
w
Inami, K
w
Itoh, R
i
Iwasaki, H
i
Iwasaki, M
at
Iwasaki, Y
i
Jang, H K
am
Kang, J H
bc
Kang, J S
p
Katayama, N
i
Kawai, H
c
Kawasaki, T
ad
Kichimi, H
i
Kim, D W
an
Kim, H J
bc
Kim, Hyunwoo
p
Kim, S K
am
Kinoshita, K
e
Korpar, S
n,u
Krizan P
n,t
Krokovny, P
b
Kuzmin, A
b
Kwon, Y
bc
Leder, G
l
Lee, S H
am
Li, J
al
Lin, S
aa
MacNaughton, J
l
Majumder, G
ap
Mandl, F
l
Matsumoto, H
ad
Matyja, A
ab
Mitaroff, W
l
Miyata, H
ad
Moloney, G R
v
Mori, T
au
Nagasaka, Y
j
Nakadaira, T
at
Nakano, E
ae
Nakao, M
i
Nam, J W
an
Natkaniec, Z
ab
Nishida, S
i
Nitoh, O
aw
Ohshima, T
w
Okabe, T
w
Okuno, S
o
Olsen, S L
h
Ostrowicz, W
ab
Ozaki, H
i
Palka, H
ab
Park, C W
p
Park, H
r
Park, K S
an
Parslow, N
ao
Piilonen, L E
ba
Rozanska, M
ab
Sagawa, H
i
Saitoh, S
i
Sakai, Y
i
Sarangi, T R
az
Satapathy, M
az
Satpathy, A
e,i
Schneider, O
s
Schumann J
aa
Schwanda, C
i,l
Schwartz, A J
e
Semenov, S
m
Senyo, K
w
Seuster, R
h
Sevior, M E
v
Shibuya, H
aq
Shwartz, B
b
Sidorov, V
b
Singh, J B
ag
Soni, N
ag
Stanic S
ay
Staric M
n
Sugi, A
w
Sumisawa, K
i
Sumiyoshi, T
av
Suzuki, S
bb
Suzuki, S Y
i
Swain, S K
h
Takasaki, F
i
Tamai, K
i
Tamura, N
ad
Tanaka, J
at
Tanaka, M
i
Teramoto, Y
ae
Tomura, T
at
Trabelsi, K
h
Tsuboyama, T
i
Tsukamoto, T
i
Uehara, S
i
Unno, Y
c
Uno, S
i
Varner, G
h
Varvell, K E
ao
Wang, C H
z
Wang, M
aa
Watanabe, Y
au
Won, E
p
Yabsley, B D
ba
Yamada, Y
i
Yamaguchi, A
as
Yamamoto, H
as
Yamashita, Y
ac
Yamauchi, M
i
Yanai, H
ad
Yuan, Y
k
Yusa, Y
as
Zhang, J
ay
Zhang, Z P
al
Zhilich, V
b
Zontar D
n,t
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For (Formula presented) rejection, we use the muon mass hypothesis to calculate the invariant mass of the two tracks.
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For the (Formula presented) and (Formula presented) modes, we treat the fit result as a Gaussian measurement and quote 90% C.L. upper limits using the procedure of G.J. Feldman and R.D. Cousins, Phys. Rev. D 57, 3873 (1998). For (Formula presented) we quote only the upper edge of the Feldman-Cousins interval: this corresponds to an upper limit of confidence level greater than 90%. For the (Formula presented) mode, where we observe a (Formula presented) signal, we quote (Formula presented) where (Formula presented) and (Formula presented) are the central value and the error returned by the fit.
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