Amplitude analysis of B-0 -> (D)over-bar0K(+)pi(-) decays
2015
- Roel Aaij
- Bernardo Adeva
- Marco Adinolfi
- A. A. Affolder
- Ziad Ajaltouni
- Simon Akar
- Johannes Albrecht
- Federico Alessio
- Michael Alexander
- S Ali
- Georgy Alkhazov
- P. Alvarez Cartelle
- Antonio Augusto Alves Jr
- Sandra Amato
- S. Amerio
- Yasmine Amhis
- Liupan An
- Lucio Anderlini
- Mirco Andreotti
- Jason Andrews
- Robert Appleby
- O. Aquines Gutierrez
- Flavio Archilli
- Philippe d'Argent
- A Artamonov
- Marina Artuso
- Elie Aslanides
- Giulio Auriemma
- Giulio Auriemma
- Marouen Baalouch
- Sebastian Bachmann
- J. J. Back
- Alexey Badalov
- Clarissa Baesso
- Wander Baldini
- Roger Barlow
- Colin Barschel
- Sergey Barsuk
- William Barter
- V. Batozskaya
- Vincenzo Battista
- Leo Beaucourt
- John Beddow
- F. Bedeschi
- Ignacio Bediaga
- Lennaert Bel
- I. Belyaev
- E. Ben-Haim
- Giovanni Bencivenni
- Sean Benson
- Jack Benton
- Alexander Berezhnoy
- Roland Bernet
- A. Bertolin
- M.-O. Bettler
- M van Beuzekom
- A. Bien
- Simone Bifani
- T. Bird
- A. Birnkraut
- A Bizzeti
- Thomas Blake
- F. Blanc
- Johan Blouw
- Steven Blusk
- Valerio Bocci
- Alexander Bondar
- Nikolay Bondar
- Nikolay Bondar
- W. Bonivento
- Silvia Borghi
- Martino Borsato
- Tjv Bowcock
- Espen Eie Bowen
- C Bozzi
- Svende Braun
- D. Brett
- M. Britsch
- Thomas Britton
- Jolanta Brodzicka
- N. H. Brook
- Albert Bursche
- Jan Buytaert
- Sandro Cadeddu
- Roberto Calabrese
- Marta Calvi
- M. Calvo Gomez
- P. Campana
- D. Campora Perez
- Lorenzo Capriotti
- Angelo Carbone
- G. Carboni
- Roberta Cardinale
- Alessandro Cardini
- P Carniti
- Laurence Carson
- K. Carvalho Akiba
- K. Carvalho Akiba
- R. Casanova Mohr
- Gianluigi Casse
- L. Cassina
- L. Castillo Garcia
- Marco Cattaneo
- Ch. Cauet
- Giovanni Cavallero
- R. Cenci
- Matthew Charles
- Ph. Charpentier
- Maximilien Chefdeville
- Shu Faye Cheung
- N. Chiapolini
- M. Chrzaszcz
- X. Cid Vidal
- Gregory Ciezarek
- P. E. L. Clarke
- Marco Clemencic
- Harry Cliff
- Joel Closier
- Victor Coco
- Julien Cogan
- Eric Cogneras
- Violetta Cogoni
- Lucian Cojocariu
- G. Collazuol
- Paula Collins
- Albert Comerma Montells
- A. Contu
- A. Cook
- M. Coombes
- S. Coquereau
- Gloria Corti
- Marco Corvo
- Benjamin Couturier
- Glen Cowan
- Daniel Charles Craik
- Andrew Crocombe
- M. Cruz Torres
- Samuel Cunliffe
- R Currie
- Carmelo DAmbrosio
- Jeremy Dalseno
- P. N. Y. David
- Adam Davis
- K. de Bruyn
- S. De Capua
- M. De Cian
- J.M. de Miranda
- L. De Paula
- W. De Silva
- P. De Simone
- C. T. Dean
- D. Decamp
- Mirko Deckenhoff
- L. Del Buono
- Nicolas Déléage
- Denis Derkach
- Olivier Deschamps
- Francesco Dettori
- Biplab Dey
- A. Di Canto
- F. Di Ruscio
- S. Donleavy
- F Dordei
- Marco Dorigo
- A. Dosil Suárez
- D. Dossett
- Anatoliy Dovbnya
- Karlis Dreimanis
- Laurent Dufour
- Giulio Dujany
- F. Dupertuis
- Paolo Durante
- Rustem Dzhelyadin
- A. Dziurda
- Alexey Dzyuba
- S. Easo
- S. Easo
- Ulrik Egede
- Victor Egorychev
- Semen Eidelman
- Stephan Eisenhardt
- Ulrich Eitschberger
- Robert Ekelhof
- Lars Eklund
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- Ch. Elsasser
- S. Ely
- Sevda Esen
- H.M. Evans
- T. M. Evans
- Antonio Falabella
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- C. Farinelli
- Nathanael Farley
- Stephen Farry
- Robert Fay
- Dianne Ferguson
- V. Fernandez Albor
- Frank Ferrari
- F Ferreira Rodrigues
- M. Ferro-Luzzi
- Sergey Filippov
- Marco Fiore
- M. Fiorini
- Miroslaw Firlej
- Conor Fitzpatrick
- Tomasz Fiutowski
- Klaus Fohl
- Philip Fol
- Marianna Fontana
- Flavio Fontanelli
- Roger Forty
- Oscar De Aguiar Francisco
- Christoph Frei
- M. Frosini
- Emiliano Furfaro
- A. Gallas Torreira
- Domenico Galli
- S. Gallorini
- Silvia Gambetta
- Miriam Gandelman
- P. Gandini
- J. García Pardiñas
- J. Garofoli
- J. Garra Tico
- L. Garrido
- David Gascon
- C. Gaspar
- Ugo Gastaldi
- R. Gauld
- Laura Gavardi
- Giulio Gazzoni
- Angelo Geraci
- David Gerick
- Evelina Gersabeck
- Marco Gersabeck
- T. J. Gershon
- Ph. Ghez
- Alessio Gianelle
- Sebastiana Gianì
- V. Gibson
- Olivier Göran Girard
- Lavinia-Helena Giubega
- Vladimir Gligorov
- C. Goebel
- D. Golubkov
- A. Golutvin
- A. Golutvin
- A. Golutvin
- C. Gotti
- M. Grabalosa Gándara
- R. Graciani Diaz
- L. A. Granado Cardoso
- E. Grauges
- Elena Graverini
- G Graziani
- Alexandru Grecu
- E. Greening
- S. Gregson
- Peter Griffith
- Lucia Grillo
- O. Gruenberg
- O. Gruenberg
- B. Gui
- Evgeny Gushchin
- Yu. Guz
- T. Gys
- Christos Hadjivasiliou
- G. Haefeli
- Christophe Haen
- Susan Haines
- Samuel Hall
- B. Hamilton
- T. Hampson
- Xiaoxue Han
- Stephanie Hansmann-Menzemer
- Neville Harnew
- Samuel Harnew
- J. Harrison
- J. He
- Timothy Head
- V. Heijne
- Karol Hennessy
- Pierre Henrard
- Louis Henry
- J. A. Hernando Morata
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- M. Hess
- M. Hess
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- Donal Hill
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- Nazim Hussain
- D. E. Hutchcroft
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- A. Jawahery
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- Malcolm John
- Daniel Johnson
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- C. Joram
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- Nathan Jurik
- Sergii Kandybei
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- Matthias Karacson
- T. M. Karbach
- Sarah Karodia
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- I. R. Kenyon
- Matthew Kenzie
- Tjeerd Ketel
- Basem Khanji
- Basem Khanji
- Chitsanu Khurewathanakul
- Suzanne Klaver
- Konrad Klimaszewski
- O. Kochebina
- Michael Kolpin
- Ilya Komarov
- P. Koppenburg
- M. Korolev
- Leonid Kravchuk
- K. Kreplin
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- G. Krocker
- Pavel Krokovny
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- R. W. Lambert
- Gaia Lanfranchi
- Christoph Langenbruch
- Benedikt Langhans
- Thomas Latham
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- A. Leflat
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- Olivier Leroy
- Tadeusz Lesiak
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- Tatiana Likhomanenko
- Tatiana Likhomanenko
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- Yuehong Xie
- Zishuo Yang
- J. Yu
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- Xuhao Yuan
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- Mikhail Zavertyaev
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- L. Zhong
The Dalitz plot distribution of B-0 -> (D) over bar K-0(+)pi(-) decays is studied using a data sample corresponding to 3.0 fb(-1) of pp collision data recorded by the LHCb experiment during 2011 and 2012. The data are described by an amplitude model that contains contributions from intermediate K* (892)(0), K*(1410)(0), K-2*(1430)(0) and D-2(*)(2460)(-) resonances. The model also contains components to describe broad structures, including the K-0(*)(1430)(0) and D-0(*)(2400)(-) resonances, in the K pi S-wave and the D pi S-and P-waves. The masses and widths of the D-0*(2400)(-) and D-2(*)(2460)(-) resonances are measured, as are the complex amplitudes and fit fractions for all components included in the amplitude model. The model obtained will be an integral part of a future determination of the angle gamma of the Cabibbo-Kobayashi-Maskawa quark mixing matrix using B-0 -> DK+pi(-) decays.
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