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Studies of the resonance structure in D 0 → K ∓ π ± π ± π ∓ decays.

Authors :
Aaij R
Adeva B
Adinolfi M
Ajaltouni Z
Akar S
Albrecht J
Alessio F
Alexander M
Alfonso Albero A
Ali S
Alkhazov G
Alvarez Cartelle P
Alves AA Jr
Amato S
Amerio S
Amhis Y
An L
Anderlini L
Andreassi G
Andreotti M
Andrews JE
Appleby RB
Archilli F
d'Argent P
Arnau Romeu J
Artamonov A
Artuso M
Aslanides E
Atzeni M
Auriemma G
Baalouch M
Babuschkin I
Bachmann S
Back JJ
Badalov A
Baesso C
Baker S
Balagura V
Baldini W
Baranov A
Barlow RJ
Barschel C
Barsuk S
Barter W
Baryshnikov F
Batozskaya V
Battista V
Bay A
Beaucourt L
Beddow J
Bedeschi F
Bediaga I
Beiter A
Bel LJ
Beliy N
Bellee V
Belloli N
Belous K
Belyaev I
Ben-Haim E
Bencivenni G
Benson S
Beranek S
Berezhnoy A
Bernet R
Berninghoff D
Bertholet E
Bertolin A
Betancourt C
Betti F
Bettler MO
van Beuzekom M
Bezshyiko I
Bifani S
Billoir P
Birnkraut A
Bizzeti A
Bjørn M
Blake T
Blanc F
Blusk S
Bocci V
Boettcher T
Bondar A
Bondar N
Bordyuzhin I
Borghi S
Borisyak M
Borsato M
Bossu F
Boubdir M
Bowcock TJV
Bowen E
Bozzi C
Braun S
Brodzicka J
Brundu D
Buchanan E
Burr C
Bursche A
Buytaert J
Byczynski W
Cadeddu S
Cai H
Calabrese R
Calladine R
Calvi M
Calvo Gomez M
Camboni A
Campana P
Campora Perez DH
Capriotti L
Carbone A
Carboni G
Cardinale R
Cardini A
Carniti P
Carson L
Carvalho Akiba K
Casse G
Cassina L
Cattaneo M
Cavallero G
Cenci R
Chamont D
Chapman MG
Charles M
Charpentier P
Chatzikonstantinidis G
Chefdeville M
Chen S
Cheung SF
Chitic SG
Chobanova V
Chrzaszcz M
Chubykin A
Ciambrone P
Cid Vidal X
Ciezarek G
Clarke PEL
Clemencic M
Cliff HV
Closier J
Coco V
Cogan J
Cogneras E
Cogoni V
Cojocariu L
Collins P
Colombo T
Comerma-Montells A
Contu A
Coombs G
Coquereau S
Corti G
Corvo M
Costa Sobral CM
Couturier B
Cowan GA
Craik DC
Crocombe A
Cruz Torres M
Currie R
D'Ambrosio C
Da Cunha Marinho F
Da Silva CL
Dall'Occo E
Dalseno J
Davis A
De Aguiar Francisco O
De Bruyn K
De Capua S
De Cian M
De Miranda JM
De Paula L
De Serio M
De Simone P
Dean CT
Decamp D
Del Buono L
Dembinski HP
Demmer M
Dendek A
Derkach D
Deschamps O
Dettori F
Dey B
Di Canto A
Di Nezza P
Dijkstra H
Dordei F
Dorigo M
Dosil Suárez A
Douglas L
Dovbnya A
Dreimanis K
Dufour L
Dujany G
Durante P
Durham JM
Dutta D
Dzhelyadin R
Dziewiecki M
Dziurda A
Dzyuba A
Easo S
Ebert M
Egede U
Egorychev V
Eidelman S
Eisenhardt S
Eitschberger U
Ekelhof R
Eklund L
Ely S
Esen S
Evans HM
Evans T
Falabella A
Farley N
Farry S
Fazzini D
Federici L
Ferguson D
Fernandez G
Fernandez Declara P
Fernandez Prieto A
Ferrari F
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Ferreira Rodrigues F
Ferro-Luzzi M
Filippov S
Fini RA
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Firlej M
Fitzpatrick C
Fiutowski T
Fleuret F
Fontana M
Fontanelli F
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Franco Lima V
Frank M
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Funk W
Furfaro E
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Gabriel E
Gallas Torreira A
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Gambetta S
Gandelman M
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Gao Y
Garcia Martin LM
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Gascon D
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Gerick D
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Gibson V
Girard OG
Giubega L
Gizdov K
Gligorov VV
Golubkov D
Golutvin A
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Gotti C
Govorkova E
Grabowski JP
Graciani Diaz R
Granado Cardoso LA
Graugés E
Graverini E
Graziani G
Grecu A
Greim R
Griffith P
Grillo L
Gruber L
Gruberg Cazon BR
Grünberg O
Gushchin E
Guz Y
Gys T
Göbel C
Hadavizadeh T
Hadjivasiliou C
Haefeli G
Haen C
Haines SC
Hamilton B
Han X
Hancock TH
Hansmann-Menzemer S
Harnew N
Harnew ST
Hasse C
Hatch M
He J
Hecker M
Heinicke K
Heister A
Hennessy K
Henrard P
Henry L
van Herwijnen E
Heß M
Hicheur A
Hill D
Hopchev PH
Hu W
Huang W
Huard ZC
Hulsbergen W
Humair T
Hushchyn M
Hutchcroft D
Ibis P
Idzik M
Ilten P
Jacobsson R
Jalocha J
Jans E
Jawahery A
Jiang F
John M
Johnson D
Jones CR
Joram C
Jost B
Jurik N
Kandybei S
Karacson M
Kariuki JM
Karodia S
Kazeev N
Kecke M
Keizer F
Kelsey M
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Khairullin E
Khanji B
Khurewathanakul C
Kirn T
Klaver S
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Kolpin M
Kopecna R
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Kozeiha M
Kravchuk L
Kreps M
Kress F
Krokovny P
Krzemien W
Kucewicz W
Kucharczyk M
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Kuonen AK
Kvaratskheliya T
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Lafferty G
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Langenbruch C
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Le Gac R
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Lefrançois J
Lefèvre R
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Lemos Cid E
Leroy O
Lesiak T
Leverington B
Li PR
Li T
Li Y
Li Z
Likhomanenko T
Lindner R
Lionetto F
Lisovskyi V
Liu X
Loh D
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Longstaff I
Lopes JH
Lucchesi D
Lucio Martinez M
Luo H
Lupato A
Luppi E
Lupton O
Lusiani A
Lyu X
Machefert F
Maciuc F
Macko V
Mackowiak P
Maddrell-Mander S
Maev O
Maguire K
Maisuzenko D
Majewski MW
Malde S
Malecki B
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Maltsev T
Manca G
Mancinelli G
Marangotto D
Maratas J
Marchand JF
Marconi U
Marin Benito C
Marinangeli M
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Marks J
Martellotti G
Martin M
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Martinez Santos D
Martinez Vidal F
Massafferri A
Matev R
Mathad A
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Matteuzzi C
Mauri A
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Mazurov A
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McNab A
McNulty R
Mead JV
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Meaux C
Meier F
Meinert N
Melnychuk D
Merk M
Merli A
Michielin E
Milanes DA
Millard E
Minard MN
Minzoni L
Mitzel DS
Mogini A
Molina Rodriguez J
Mombächer T
Monroy IA
Monteil S
Morandin M
Morello MJ
Morgunova O
Moron J
Morris AB
Mountain R
Muheim F
Mulder M
Müller D
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Müller K
Müller V
Naik P
Nakada T
Nandakumar R
Nandi A
Nasteva I
Needham M
Neri N
Neubert S
Neufeld N
Neuner M
Nguyen TD
Nguyen-Mau C
Nieswand S
Niet R
Nikitin N
Nikodem T
Nogay A
O'Hanlon DP
Oblakowska-Mucha A
Obraztsov V
Ogilvy S
Oldeman R
Onderwater CJG
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Otalora Goicochea JM
Owen P
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Pais PR
Palano A
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Papanestis A
Pappagallo M
Pappalardo LL
Parker W
Parkes C
Passaleva G
Pastore A
Patel M
Patrignani C
Pearce A
Pellegrino A
Penso G
Pepe Altarelli M
Perazzini S
Pereima D
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Petridis K
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Piucci A
Placinta V
Playfer S
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Polci F
Lener MP
Poluektov A
Polyakov I
Polycarpo E
Pomery GJ
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Popov A
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Potterat C
Price E
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Pugatch V
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Rademacker JH
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Ravonel Salzgeber M
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Redi F
Reichert S
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Remon Alepuz C
Renaudin V
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Richards S
Rihl M
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Robert A
Rodrigues AB
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Rudolph MS
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Source :
The European physical journal. C, Particles and fields [Eur Phys J C Part Fields] 2018; Vol. 78 (6), pp. 443. Date of Electronic Publication: 2018 Jun 02.
Publication Year :
2018

Abstract

Amplitude models are constructed to describe the resonance structure of D 0 → K - π + π + π - and D 0 → K + π - π - π + decays using pp collision data collected at centre-of-mass energies of 7 and 8 TeV with the LHCb experiment, corresponding to an integrated luminosity of 3.0  f b - 1 . The largest contributions to both decay amplitudes are found to come from axial resonances, with decay modes D 0 → a 1 ( 1260 ) + K - and D 0 → K 1 ( 1270 / 1400 ) + π - being prominent in D 0 → K - π + π + π - and D 0 → K + π - π - π + , respectively. Precise measurements of the lineshape parameters and couplings of the a 1 ( 1260 ) + , K 1 ( 1270 ) - and K ( 1460 ) - resonances are made, and a quasi model-independent study of the K ( 1460 ) - resonance is performed. The coherence factor of the decays is calculated from the amplitude models to be R K 3 π = 0.459 ± 0.010 ( stat ) ± 0.012 ( syst ) ± 0.020 ( model ) , which is consistent with direct measurements. These models will be useful in future measurements of the unitary-triangle angle γ and studies of charm mixing and C P violation.

Details

Language :
English
ISSN :
1434-6044
Volume :
78
Issue :
6
Database :
MEDLINE
Journal :
The European physical journal. C, Particles and fields
Publication Type :
Academic Journal
Accession number :
30956546
Full Text :
https://doi.org/10.1140/epjc/s10052-018-5758-4