CORE
🇺🇦
make metadata, not war
Services
Research
Services overview
Explore all CORE services
Access to raw data
API
Dataset
FastSync
Content discovery
Recommender
Discovery
OAI identifiers
OAI Resolver
Managing content
Dashboard
Bespoke contracts
Consultancy services
Support us
Support us
Membership
Sponsorship
Community governance
Advisory Board
Board of supporters
Research network
About
About us
Our mission
Team
Blog
FAQs
Contact us
Measurement of the branching fractions for Cabibbo-suppressed decays
D
+
→
K
+
K
−
π
+
π
0
D^{+}\to K^{+} K^{-}\pi^{+}\pi^{0}
D
+
→
K
+
K
−
π
+
π
0
and
D
(
s
)
+
→
K
+
π
−
π
+
π
0
D_{(s)}^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}
D
(
s
)
+
→
K
+
π
−
π
+
π
0
at Belle
Authors
Hiroaki Aihara
Said Ahmed Al Said
+197 more
David Asner
Hulya Atmacan
Vladimir Aulchenko
Tagir Aushev
Rachid Ayad
Varghese Babu
Seema Bahinipati
Konstantin Belous
Jake Bennett
Martin Bessner
Vishal Bhardwaj
Tadeas Bilka
Alexandr Bobrov
Denis Bodrov
Giovanni Bonvicini
Jyotirmoi Borah
Andrzej Bozek
Marko Bracko
Paolo Branchini
Thomas Browder
Antonio Budano
Marcello Campajola
Daniel Cervenkov
Paoti Chang
Augustine Chen
Byunggu Cheon
Haneol Cho
Kihyeon Cho
Sungjin Cho
Sookyung Choi
Youngil Choi
Seema Choudhury
David Cinabro
Samuel Thomas Cunliffe
Sanjeeda Bharati Das
Nibedita Dash
Guglielmo de Nardo
Giacomo de Pietro
Rashmi Dhamija
Francesco Di Capua
Zdenek Dolezal
Thanh Van Dong
David Dossett
Denis Alexandrovich Epifanov
Ariane Frey
Bryan Gregory Fulsom
Renu Garg
Alexei Garmash
Vipin Gaur
Anjan Giri
Pablo Goldenzweig
Enrico Graziani
Daniel Greenwald
Tianping Gu
Yinghui Guan
Kristina Gudkova
Christos Hadjivasiliou
Kiyoshi Hayasaka
Hisaki Hayashii
Daniel Ricalde Herrmann
George Wei-Shu Hou
Chia-Ling Hsu
Kenji Inami
Akimasa Ishikawa
Ryosuke Itoh
Masako Iwasaki
William Jacobs
Sen Jia
Yifan Jin
Dibyajyoti Kalita
Abdul Basith Kaliyar
Kook Hyun Kang
Takeo Kawasaki
Christian Kiesling
Cheolhun Kim
Doris Yangsoo Kim
Kyung Tae Kim
Kyungho Kim
Yongkyu Kim
Kay Kinoshita
Peter Kodys
Tomoyuki Konno
Alexander Korobov
Samo Korpar
Evgeniy Kovalenko
Peter Krizan
Pavel Krokovny
Thomas Kuhr
Manish Kumar
Rajeev Kumar
Kospalage Janaka Kumara
Alexander Kuzmin
Young-Joon Kwon
Yun-Tsung Lai
Tommy Lam
Martina Laurenza
Seungcheol Lee
Luigi Li Gioi
Jin Li
Longke Li
Y.B. Li
Yang Li
James Frederick Libby
Kilian Adriano Lieret
Dmitri Liventsev
Alberto Martini
Masataka Masuda
Tatsuro Matsuda
Dmitry Matvienko
Shubhangi Krishan Maurya
Frank Meier
Mario Merola
Felix Metzner
Kenkichi Miyabayashi
Roman Mizuk
Gagan Bihari Mohanty
Hyunki Moon
Mikihiko Nakao
Zbigniew Natkaniec
Andrii Natochii
Lopamudra Nayak
Minakshi Nayak
Nisar Nellikunnummel
Shohei Nishida
Hiroaki Ono
Pavel Oskin
Pavel Pakhlov
Galina Pakhlova
Silvio Pardi
Hwan-Bae Park
Seokhee Park
Antonio Passeri
Sourav Patra
Stephan Martin Paul
Todd Kristofer Pedlar
Rok Pestotnik
L.E. Piilonen
Tomaz Podobnik
Elisabetta Prencipe
Markus Prim
Armine Rostomyan
Niharika Rout
Guido Russo
Debashis Sahoo
Saurabh Sandilya
Aman Sangal
Luka Santelj
Vladimir Savinov
Gunar Schnell
Jeff Schueler
Christoph Schwanda
Alan Jay Schwartz
Yoshiaki Seino
Katsumi Senyo
Martin Edmund Sevior
Mikhail Shapkin
Chanchal Sharma
Jing-Ge Shiu
Frank Simon
Jasbir Singh
Anatoly Sokolov
Elena Solovieva
Marko Staric
Zachary S. Stottler
Mizuki Sumihama
Makoto Takizawa
Umberto Tamponi
Kiyoshi Tanida
Francesco Tenchini
Makoto Uchida
Timofey Uglov
Kenta Uno
Shoji Uno
Yutaka Ushiroda
Yuri Usov
Raynette van Tonder
Gary Varner
Kevin Ernest Varvell
Anselm Georg Vossen
Eiasha Waheed
Erfei Wang
Min-Zu Wang
Xiaolong Wang
Shun Watanuki
Olga Werbycka
Jaroslaw Wiechczynski
Eunil Won
Bruce Yabsley
Wenbiao Yan
Seongbae Yang
Hua Ye
John Yelton
Junhao Yin
Changzheng Yuan
Ziping Zhang
Victor Zhilich
Valentina Zhukova
Publication date
1 January 2023
Publisher
HAL CCSD
Abstract
International audienceWe present measurements of the branching fractions for the singly Cabibbo-suppressed decays
D
+
→
K
+
K
−
π
+
π
0
D^+\to K^{+}K^{-}\pi^{+}\pi^{0}
D
+
→
K
+
K
−
π
+
π
0
and
D
s
+
→
K
+
π
−
π
+
π
0
D_s^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}
D
s
+
→
K
+
π
−
π
+
π
0
, and the doubly Cabibbo-suppressed decay
D
+
→
K
+
π
−
π
+
π
0
D^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}
D
+
→
K
+
π
−
π
+
π
0
, based on 980
f
b
−
1
{\rm fb}^{-1}
fb
−
1
of data recorded by the Belle experiment at the KEKB
e
+
e
−
e^{+}e^{-}
e
+
e
−
collider. We measure these modes relative to the Cabibbo-favored modes
D
+
→
K
−
π
+
π
+
π
0
D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0}
D
+
→
K
−
π
+
π
+
π
0
and
D
s
+
→
K
+
K
−
π
+
π
0
D_s^{+}\to K^{+}K^{-}\pi^{+}\pi^{0}
D
s
+
→
K
+
K
−
π
+
π
0
. Our results for the ratios of branching fractions are
B
(
D
+
→
K
+
K
−
π
+
π
0
)
/
B
(
D
+
→
K
−
π
+
π
+
π
0
)
=
(
11.32
±
0.13
±
0.26
)
%
B(D^{+}\to K^{+}K^{-}\pi^{+}\pi^{0})/B(D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0}) = (11.32 \pm 0.13 \pm 0.26)\%
B
(
D
+
→
K
+
K
−
π
+
π
0
)
/
B
(
D
+
→
K
−
π
+
π
+
π
0
)
=
(
11.32
±
0.13
±
0.26
)
%
,
B
(
D
+
→
K
+
π
−
π
+
π
0
)
/
B
(
D
+
→
K
−
π
+
π
+
π
0
)
=
(
1.68
±
0.11
±
0.03
)
%
B(D^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0})/B(D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0}) = (1.68 \pm 0.11\pm 0.03)\%
B
(
D
+
→
K
+
π
−
π
+
π
0
)
/
B
(
D
+
→
K
−
π
+
π
+
π
0
)
=
(
1.68
±
0.11
±
0.03
)
%
, and
B
(
D
s
+
→
K
+
π
−
π
+
π
0
)
/
B
(
D
s
+
→
K
+
K
−
π
+
π
0
)
=
(
17.13
±
0.62
±
0.51
)
%
B(D_s^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0})/B(D_s^{+}\to K^{+}K^{-}\pi^{+}\pi^{0}) = (17.13 \pm 0.62 \pm 0.51)\%
B
(
D
s
+
→
K
+
π
−
π
+
π
0
)
/
B
(
D
s
+
→
K
+
K
−
π
+
π
0
)
=
(
17.13
±
0.62
±
0.51
)
%
, where the uncertainties are statistical and systematic, respectively. The second value corresponds to
(
5.83
±
0.42
)
×
tan
4
θ
C
(5.83\pm 0.42)\times\tan^4\theta_C
(
5.83
±
0.42
)
×
tan
4
θ
C
, where
θ
C
\theta_C
θ
C
is the Cabibbo angle; this value is larger than other measured ratios of branching fractions for a doubly Cabibbo-suppressed charm decay to a Cabibbo-favored decay. Multiplying these results by world average values for
B
(
D
+
→
K
−
π
+
π
+
π
0
)
B(D^{+}\to K^{-}\pi^{+}\pi^{+}\pi^{0})
B
(
D
+
→
K
−
π
+
π
+
π
0
)
and
B
(
D
s
+
→
K
+
K
−
π
+
π
0
)
B(D_s^{+}\to K^{+}K^{-}\pi^{+}\pi^{0})
B
(
D
s
+
→
K
+
K
−
π
+
π
0
)
yields
B
(
D
+
→
K
+
K
−
π
+
π
0
)
=
(
7.08
±
0.08
±
0.16
±
0.20
)
×
1
0
−
3
B(D^{+}\to K^{+}K^{-}\pi^{+}\pi^{0})= (7.08\pm 0.08\pm 0.16\pm 0.20)\times10^{-3}
B
(
D
+
→
K
+
K
−
π
+
π
0
)
=
(
7.08
±
0.08
±
0.16
±
0.20
)
×
1
0
−
3
,
B
(
D
+
→
K
+
π
−
π
+
π
0
)
=
(
1.05
±
0.07
±
0.02
±
0.03
)
×
1
0
−
3
B(D^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0})= (1.05\pm 0.07\pm 0.02\pm 0.03)\times10^{-3}
B
(
D
+
→
K
+
π
−
π
+
π
0
)
=
(
1.05
±
0.07
±
0.02
±
0.03
)
×
1
0
−
3
, and
B
(
D
s
+
→
K
+
π
−
π
+
π
0
)
=
(
9.44
±
0.34
±
0.28
±
0.32
)
×
1
0
−
3
B(D_s^{+}\to K^{+}\pi^{-}\pi^{+}\pi^{0}) = (9.44\pm 0.34\pm 0.28\pm 0.32)\times10^{-3}
B
(
D
s
+
→
K
+
π
−
π
+
π
0
)
=
(
9.44
±
0.34
±
0.28
±
0.32
)
×
1
0
−
3
, where the third uncertainty is due to the branching fraction of the normalization mode. The first two results are consistent with, but more precise than, the current world averages. The last result is the first measurement of this branching fraction
Similar works
Full text
Available Versions
HAL-IN2P3
See this paper in CORE
Go to the repository landing page
Download from data provider
oai:HAL:hal-03897820v1
Last time updated on 03/03/2023