Measurement of the branching fractions of the decays $D^+\rightarrow K^-K ^+K^+$, $D^+\rightarrow \pi^-\pi^+K^+$ and $D^+_s\rightarrow \pi^-K^+K^+$
2018
- Roel Aaij
- Gregory Ciezarek
- Paula Collins
- Ulrich Straumann
- Stefan Roiser
- W. Qian
- Achim Vollhardt
- Barbara Storaci
- Alessio Piucci
- Daniel Patrick OHanlon
- Marcel Merk
- S. Ricciardi
- Christopher Jones
- Konstantin Gizdov
- Marie-Noelle Minard
- Daniel Berninghoff
- Naomi Veronika
- Pavel Krokovny
- Gianfranco Morello
- Marco Corvo
- I. Polyakov
- Alessandro Camboni
- Peirong Li
- Florian Lemaitre
- Guillaume Pietrzyk
- L. Kravchuk
- Julian Wishahi
- Mikkel Bjørn
- Menglin Xu
- John Gordon Smeaton
- Max Neuner
- Veronika Chobanova
- Thomas Kirn
- Melody Ravonel Salzgeber
- Matteo Palutan
- Niels Tuning
- Adam Dendek
- A. Mogini
- Sebastian Bachmann
- Zhenzi Wang
- David Gascon
- Timothy Evans
- Matthew Kelsey
- Da Yu Tou
- Neville Harnew
- Olga Morgunova
- Stephan Escher
- Daniel Hynds
- Tatsiana Klimkovich
- Marcin Chrzaszcz
- O. Maev
- Guido Haefeli
- Sheldon Stone
- Marek Idzik
- Jennifer Brigitta Zonneveld
- Sergey Barsuk
- Florin Maciuc
- Tomasz Szumlak
- Edwige Tournefier
- Marcel Materok
- D. Pinci
- Miriam Lucio Martinez
- Angelo Di Canto
- Alexandra Paige Rollings
- Jeremy Dalseno
- Olivier Göran Girard
- Roland Waldi
- Nikolay Nikitin
- Michele Atzeni
- Oliver Grunberg
- Daniel Vieira
- Sascha Stahl
- Arseniy Vitkovskiy
- Sebastian Neubert
- Viktoriia Chekalina
- Eluned Smith
- Margarete Schellenberg
- Anna Danilina
- Jascha Peter Grabowski
- Matthew Needham
- Eduardo Enrique Sepulveda
- Burkhard Schmidt
- Domenico Galli
- Christoph Hasse
- Ivan Belyaev
- Aleksandr Petrov
- Iwan Thomas Smith
- Stefano Petrucci
- Monica Pepe Altarelli
- Stephen Farry
- Oleg Stenyakin
- Stephen Wotton
- Lars Eklund
- Luis Miguel Garcia Martin
- Daniele Marangotto
- Alvaro Gomes
- Matthew Kenzie
- Holger Stevens
- Denis Derkach
- Malte Hecker
- Angelo Carbone
- Olivier Deschamps
- D. Chamont
- Martinus van Beuzekom
- A. Merli
- M. Fiorini
- Patrick Spradlin
- Michael Brodski
- Liupan An
- Vanessa Müller
- Konstantin Belous
- A. Pearce
- Rudolf Oldeman
- Michal Dziewiecki
- F. Blanc
- Sarah Karodia
- Shanzhen Chen
- Zan Ren
- Florian Reiss
- Juan Jose Saborido Silva
- M. D. Sokoloff
- Josue Molina Rodriguez
- Wen Chao Zhang
- Federica Lionetto
- Zhipeng Tang
- Marco Petruzzo
- Luiz Gustavo Silva De Oliveira
- Nicola Serra
- Maxime Vernet
- Jaap Velthuis
- Marcelo Soares
- Giulia Tellarini
- Vladimir Gligorov
- Fabrice Desse
- Philippe Charpentier
- Rafael Tourinho Jadallah Aoude
- Emmy Gabriel
- Anna Ossowska
- Mengzhen Wang
- Alex Seuthe
- Andrey Ustyuzhanin
- Adlene Hicheur
- Matthieu Kecke
- Eric van Herwijnen
- Lucio Anderlini
- Zhuoming Li
- Roger Forty
- Y. H. Xie
- Roberta Santacesaria
- Laurent Dufour
- Xavier Vilasis-Cardona
- Lais Soares Lavra
- J. Bhom
- David Ward
- Andrea Valassi
- Barbara Sciascia
- Alexander Bondar
- Joao A B Coelho
- Simon Nieswand
- Meril Reboud
- Elisabetta Spadaro Norella
- Antonio Fernandez Prieto
- Barak Raimond Gruberg Cazon
- Yuanning Gao
- Luca Federici
- P. Billoir
- Chung Nguyen-Mau
- Joan Arnau Romeu
- Siim Tolk
- Dawid Gerstel
- Floris Keizer
- Brian Hamilton
- Thierry Gys
- Johannes Heuel
- Antonio Augusto Alves Jr
- Bartosz Malecki
- Eugeni Graugés
- Janine Müller
- Sophie Richards
- Patrick Mackowiak
- Matthew James Tilley
- Donal Murray
- Konstantinos Petridis
- Martino Borsato
- Balazs Voneki
- Evelina Gersabeck
- F. Muheim
- Franciole Da Cunha Marinho
- Nikita Kazeev
- Simon Stemmle
- Achille Stocchi
- Martina Pili
- Mika Vesterinen
- Umberto Marconi
- Tomasz Skwarnicki
- Maarten van Veghel
- Steven Blusk
- Yanxi Zhang
- Zehua Xu
- Mikhail Shapkin
- Rolf Lindner
- Sergey Filippov
- Stephan Eisenhardt
- H. F. Schreiner
- Stefan Schael
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- S. Monteil
- Dongliang Zhang
- Christopher Burr
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- Bartlomiej Rachwal
- Wenqian Huang
- Biplab Dey
- Julien Cogan
- Eddy Jans
- Franco Bedeschi
- Maximo Plo Casasus
- Tenglin Li
- Adam Davis
- V. Shevchenko
- Alessio Sarti
- Iain Longstaff
- Wojciech Krupa
- Maurizio Martinelli
- Antimo Palano
- Carla Marin Benito
- Mirco Andreotti
- A. Bay
- Hang Yin
- David Gerick
- F. Ratnikov
- Thomas Harrison
- Benjamin Audurier
- Constantin Weisser
- Dominik Stefan Mitzel
- Andreas Weiden
- Maria Elena Stramaglia
- Ekaterina Govorkova
- Marco Santimaria
- Ana Barbara Rodrigues
- Cameron Thomas Dean
- Arno Heister
- Kazuyoshi Carvalho Akiba
- Egor Khairullin
- Valery Pugatch
- Kyung Eun Kim
- Mirco Dorigo
- Michele Veltri
- Scott Ely
- Evgenii Shmanin
- Antonio Pellegrino
- Renata Kopecna
- James Mwangi Kariuki
- Daniel Decamp
- Abhijit Mathad
- Boleslaw Pietrzyk
- Marina Artuso
- Anna Lupato
- Clara Gaspar
- Andrei Tsaregorodtsev
- Carla Göbel
- Ziad Ajaltouni
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- F. Dordei
- Alexander Malinin
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- Diego Martinez Santos
- Michael Wilkinson
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- Giulio Gazzoni
- Gennady Panshin
- Lennaert Bel
- Christian Joram
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- U. Uwer
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- Marta Calvi
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- George Lafferty
- Laurence Carson
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- Adalberto Sciubba
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- S Cadeddu
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- Annarita Buonaura
- Vladimir Romanovskiy
- Eric Thomas
- John Beddow
- Jia-Jia Qin
- Olivier Leroy
- S. Perazzini
- Edward James Millard
- Elena Graverini
- Preema Rennee Pais
- Beatriz Garcia Plana
- Tomasz Fiutowski
- Donal Hill
- Rosen Matev
- Carlos Sanchez Mayordomo
- Daniel Lacarrere
- Valerie Gibson
- Paolo Carniti
- Raja Nandakumar
- Rafael Silva Coutinho
The branching fractions of the doubly Cabibbo-suppressed decays $D^+\rightarrow K^-K^+K^+$, $D^+\rightarrow \pi^-\pi^+K^+$ and $D^+_s\rightarrow\pi^-K^+K^+$ are measured using the decays $D^+\rightarrow K^-\pi^+\pi^+$ and $D^+_s\rightarrow K^-K^+\pi^+$ as normalisation channels. The measurements are performed using proton-proton collision data collected with the LHCb detector at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 2.0 fb$^{-1}$. The results are
\begin{align}
\frac {\mathcal{B}(D^+\rightarrow K^-K^+K^+)} {\mathcal{B}(D^+\rightarrow K^-\pi^+\pi^+)}& = (6.541 \pm 0.025 \pm 0.042) \times 10^{-4},\nonumber
\frac {\mathcal{B}(D^+\rightarrow \pi^-\pi^+K^+)} {\mathcal{B}(D^+\rightarrow K^-\pi^+\pi^+)}& = (5.231 \pm 0.009 \pm 0.023) \times 10^{-3}, \nonumber
\frac {\mathcal{B}(D^+_s\rightarrow\pi^-K^+K^+)} {\mathcal{B}(D^+_s\rightarrow K^-K^+\pi^+)}& = (2.372 \pm 0.024 \pm 0.025) \times 10^{-3},\nonumber
\end{align} where the uncertainties are statistical and systematic, respectively. These are the most precise measurements up to date.
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