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Updated branching fraction measurements of B0( s) → K0Sh+h′ − decays

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Abstract The charmless three-body decays B ( s) 0  → K S 0 h + h ′ − (where h (′) = π, K) are analysed using a sample of pp collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 3 fb−1. The branching fractions are measured relative to that of the B 0 → K S 0 π + π − decay, and are determined to be: $$ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{\pi}^{-}\right)}=0.123\pm 0.009\left(\mathrm{stat}\right)\pm 0.015\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.549\pm 0.018\left(\mathrm{stat}\right)\pm 0.033\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.191\pm 0.027\left(\mathrm{stat}\right)\pm 0.031\left(\mathrm{syst}\right)\pm 0.011\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=1.70\pm 0.07\left(\mathrm{stat}\right)\pm 0.11\left(\mathrm{syst}\right)\pm 0.10\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}\in \left[0.008-0.051\right]\kern0.5em \mathrm{at}\kern0.5em 90\%\kern0.5em \mathrm{confidence}\kern0.5em \mathrm{level},\hfill \end{array} $$ ℬ B 0 → K S 0 K ± π ∓ ℬ B 0 → K S 0 K + π − = 0.123 ± 0.009 stat ± 0.015 syst , ℬ B 0 → K S 0 K + K − ℬ B 0 → K S 0 π + π − = 0.549 ± 0.018 stat ± 0.033 syst , ℬ B s 0 → K S 0 π + π − ℬ B 0 → K S 0 π + π − = 0.191 ± 0.027 stat ± 0.031 syst ± 0.011 f s / f d , ℬ B s 0 → K S 0 K ± π ∓ ℬ B 0 → K S 0 π + π − = 1.70 ± 0.07 stat ± 0.11 syst ± 0.10 f s / f d , ℬ B s 0 → K S 0 K + K − ℬ B 0 → K S 0 π + π − ∈ 0.008 − 0.051 at 90 % confidence level , where f s /f d represents the ratio of hadronisation fractions of the B s 0 and B 0 mesons.
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R. Aaij B. Adeva M. Adinolfi Z. Ajaltouni S. Akar J. Albrecht F. Alessio M. Alexander S. Ali G. Alkhazov P. Alvarez Cartelle A. A. Alves S. Amato S. Amerio Y. Amhis L. An L. Anderlini G. Andreassi M. Andreotti J. E. Andrews R. B. Appleby F. Archilli P. d’Argent J. Arnau Romeu A. Artamonov M. Artuso E. Aslanides G. Auriemma M. Baalouch I. Babuschkin S. Bachmann J. J. Back A. Badalov C. Baesso S. Baker V. Balagura W. Baldini A. Baranov R. J. Barlow C. Barschel S. Barsuk W. Barter F. Baryshnikov M. Baszczyk V. Batozskaya B. Batsukh V. Battista A. Bay L. Beaucourt J. Beddow F. Bedeschi I. Bediaga A. Beiter L. J. Bel V. Bellee N. Belloli K. Belous I. Belyaev E. Ben-Haim G. Bencivenni S. Benson S. Beranek A. Berezhnoy R. Bernet A. Bertolin C. Betancourt F. Betti M.-O. Bettler M. van Beuzekom Ia. Bezshyiko S. Bifani P. Billoir A. Birnkraut A. Bitadze A. Bizzeti T. Blake F. Blanc J. Blouw S. Blusk V. Bocci T. Boettcher A. Bondar N. Bondar W. Bonivento I. Bordyuzhin A. Borgheresi S. Borghi M. Borisyak M. Borsato F. Bossu M. Boubdir T. J. V. Bowcock E. Bowen C. Bozzi S. Braun T. Britton J. Brodzicka E. Buchanan C. Burr A. Bursche J. Buytaert S. Cadeddu R. Calabrese M. Calvi M. Calvo Gomez A. Camboni P. Campana D. H. Campora Perez L. Capriotti A. Carbone G. Carboni R. Cardinale A. Cardini P. Carniti L. Carson K. Carvalho Akiba G. Casse L. Cassina L. Castillo Garcia M. Cattaneo G. Cavallero R. Cenci D. Chamont M. Charles Ph. Charpentier G. Chatzikonstantinidis M. Chefdeville S. Chen S. F. Cheung V. Chobanova M. Chrzaszcz A. Chubykin X. Cid Vidal G. Ciezarek P. E. L. Clarke M. Clemencic H. V. Cliff J. Closier V. Coco J. Cogan E. Cogneras V. Cogoni L. Cojocariu P. Collins A. Comerma-Montells A. Contu A. Cook G. Coombs S. Coquereau G. Corti M. Corvo C. M. Costa Sobral B. Couturier G. A. Cowan D. C. Craik A. Crocombe M. Cruz Torres S. Cunliffe R. Currie C. D’Ambrosio F. Da Cunha Marinho E. Dall’Occo J. Dalseno A. Davis K. De Bruyn S. De Capua M. De Cian J. M. De Miranda L. De Paula M. De Serio P. De Simone C. T. Dean D. Decamp M. Deckenhoff L. Del Buono H.-P. Dembinski M. Demmer A. Dendek D. Derkach O. Deschamps F. Dettori B. Dey A. Di Canto P. Di Nezza H. Dijkstra F. Dordei M. Dorigo A. Dosil Suárez A. Dovbnya K. Dreimanis L. Dufour G. Dujany K. Dungs P. Durante R. Dzhelyadin M. Dziewiecki A. Dziurda A. Dzyuba N. Déléage S. Easo M. Ebert U. Egede V. Egorychev S. Eidelman S. Eisenhardt U. Eitschberger R. Ekelhof L. Eklund S. Ely S. Esen H. M. Evans T. Evans A. Falabella N. Farley S. Farry R. Fay D. Fazzini D. Ferguson G. Fernandez A. Fernandez Prieto F. Ferrari F. Ferreira Rodrigues M. Ferro-Luzzi S. Filippov R. A. Fini M. Fiore M. Fiorini M. Firlej C. Fitzpatrick T. Fiutowski F. Fleuret K. Fohl M. Fontana F. Fontanelli D. C. Forshaw R. Forty V. Franco Lima M. Frank C. Frei J. Fu W. Funk E. Furfaro C. Färber E. Gabriel A. Gallas Torreira D. Galli S. Gallorini S. Gambetta M. Gandelman P. Gandini Y. Gao L. M. Garcia Martin J. García Pardiñas J. Garra Tico L. Garrido P. J. Garsed D. Gascon C. Gaspar L. Gavardi G. Gazzoni D. Gerick E. Gersabeck M. Gersabeck T. Gershon Ph. Ghez S. Gianì V. Gibson O. G. Girard L. Giubega K. Gizdov V. V. Gligorov D. Golubkov A. Golutvin A. Gomes I. V. Gorelov C. Gotti E. Govorkova R. Graciani Diaz L. A. Granado Cardoso E. Graugés E. Graverini G. Graziani A. Grecu R. Greim P. Griffith L. Grillo L. Gruber B. R. Gruberg Cazon O. Grünberg E. Gushchin Yu. Guz T. Gys C. Göbel T. Hadavizadeh C. Hadjivasiliou G. Haefeli C. Haen S. C. Haines B. Hamilton X. Han S. Hansmann-Menzemer N. Harnew S. T. Harnew J. Harrison M. Hatch J. He T. Head A. Heister K. Hennessy P. Henrard L. Henry E. van Herwijnen M. Heß A. Hicheur D. Hill C. Hombach P. H. Hopchev Z.-C. Huard W. Hulsbergen T. Humair M. Hushchyn D. Hutchcroft M. Idzik P. Ilten R. Jacobsson J. Jalocha E. Jans A. Jawahery F. Jiang M. John D. Johnson C. R. Jones C. Joram B. Jost N. Jurik S. Kandybei M. Karacson J. M. Kariuki S. Karodia M. Kecke M. Kelsey M. Kenzie T. Ketel E. Khairullin B. Khanji C. Khurewathanakul T. Kirn S. Klaver K. Klimaszewski T. Klimkovich S. Koliiev M. Kolpin I. Komarov R. Kopecna P. Koppenburg A. Kosmyntseva S. Kotriakhova A. Kozachuk M. Kozeiha L. Kravchuk M. Kreps P. Krokovny F. Kruse W. Krzemien W. Kucewicz M. Kucharczyk V. Kudryavtsev A. K. Kuonen K. Kurek T. Kvaratskheliya D. Lacarrere G. Lafferty A. Lai G. Lanfranchi C. Langenbruch T. Latham C. Lazzeroni R. Le Gac J. van Leerdam A. Leflat J. Lefrançois R. Lefèvre F. Lemaitre E. Lemos Cid O. Leroy T. Lesiak B. Leverington T. Li Y. Li Z. Li T. Likhomanenko R. Lindner F. Lionetto X. Liu D. Loh I. Longstaff J. H. Lopes D. Lucchesi M. Lucio Martinez H. Luo A. Lupato E. Luppi O. Lupton A. Lusiani X. Lyu F. Machefert F. Maciuc O. Maev K. Maguire S. Malde A. Malinin T. Maltsev G. Manca G. Mancinelli P. Manning J. Maratas J. F. Marchand U. Marconi C. Marin Benito M. Marinangeli P. Marino J. Marks G. Martellotti M. Martin M. Martinelli D. Martinez Santos F. Martinez Vidal D. Martins Tostes L. M. Massacrier A. Massafferri R. Matev A. Mathad Z. Mathe C. Matteuzzi A. Mauri E. Maurice B. Maurin A. Mazurov M. McCann A. McNab R. McNulty B. Meadows F. Meier D. Melnychuk M. Merk A. Merli E. Michielin D. A. Milanes M.-N. Minard D. S. Mitzel A. Mogini J. Molina Rodriguez I. A. Monroy S. Monteil M. Morandin M. J. Morello O. Morgunova J. Moron A. B. Morris R. Mountain F. Muheim M. Mulder M. Mussini D. Müller J. Müller K. Müller V. Müller P. Naik T. Nakada R. Nandakumar A. Nandi I. Nasteva M. Needham N. Neri S. Neubert N. Neufeld M. Neuner T. D. Nguyen C. Nguyen-Mau S. Nieswand R. Niet N. Nikitin T. Nikodem A. Nogay D. P. O’Hanlon A. Oblakowska-Mucha V. Obraztsov S. Ogilvy R. Oldeman C. J. G. Onderwater A. Ossowska J. M. Otalora Goicochea P. Owen A. Oyanguren P. R. Pais A. Palano M. Palutan A. Papanestis M. Pappagallo L. L. Pappalardo C. Pappenheimer W. Parker C. Parkes G. Passaleva A. Pastore M. Patel C. Patrignani A. Pearce A. Pellegrino G. Penso M. Pepe Altarelli S. Perazzini P. Perret L. Pescatore K. Petridis A. Petrolini A. Petrov M. Petruzzo E. Picatoste Olloqui B. Pietrzyk M. Pikies D. Pinci A. Pistone A. Piucci V. Placinta S. Playfer M. Plo Casasus T. Poikela F. Polci M. Poli Lener A. Poluektov I. Polyakov E. Polycarpo G. J. Pomery S. Ponce A. Popov D. Popov B. Popovici S. Poslavskii C. Potterat E. Price J. Prisciandaro C. Prouve V. Pugatch A. Puig Navarro G. Punzi C. Qian W. Qian R. Quagliani B. Rachwal J. H. Rademacker M. Rama M. Ramos Pernas M. S. Rangel I. Raniuk F. Ratnikov G. Raven M. Ravonel Salzgeber M. Reboud F. Redi S. Reichert A. C. dos Reis C. Remon Alepuz V. Renaudin S. Ricciardi S. Richards M. Rihl K. Rinnert V. Rives Molina P. Robbe A. B. Rodrigues E. Rodrigues J. A. Rodriguez Lopez P. Rodriguez Perez A. Rogozhnikov S. Roiser A. Rollings V. Romanovskiy A. Romero Vidal J. W. Ronayne M. Rotondo M. S. Rudolph T. Ruf P. Ruiz Valls J. J. Saborido Silva E. Sadykhov N. Sagidova B. Saitta V. Salustino Guimaraes D. Sanchez Gonzalo C. Sanchez Mayordomo B. Sanmartin Sedes R. Santacesaria C. Santamarina Rios M. Santimaria E. Santovetti A. Sarti C. Satriano A. Satta D. M. Saunders D. Savrina S. Schael M. Schellenberg M. Schiller H. Schindler M. Schlupp M. Schmelling T. Schmelzer B. Schmidt O. Schneider A. Schopper H. F. Schreiner K. Schubert M. Schubiger M.-H. Schune R. Schwemmer B. Sciascia A. Sciubba A. Semennikov A. Sergi N. Serra J. Serrano L. Sestini P. Seyfert M. Shapkin I. Shapoval Y. Shcheglov T. Shears L. Shekhtman V. Shevchenko B. G. Siddi R. Silva Coutinho L. Silva de Oliveira G. Simi S. Simone M. Sirendi N. Skidmore T. Skwarnicki E. Smith I. T. Smith J. Smith M. Smith l. Soares Lavra M. D. Sokoloff F. J. P. Soler B. Souza De Paula B. Spaan P. Spradlin S. Sridharan F. Stagni M. Stahl S. Stahl P. Stefko S. Stefkova O. Steinkamp S. Stemmle O. Stenyakin H. Stevens S. Stoica S. Stone B. Storaci S. Stracka M. E. Stramaglia M. Straticiuc U. Straumann L. Sun W. Sutcliffe K. Swientek V. Syropoulos M. Szczekowski T. Szumlak S. T’Jampens A. Tayduganov T. Tekampe G. Tellarini F. Teubert E. Thomas J. van Tilburg M. J. Tilley V. Tisserand M. Tobin S. Tolk L. Tomassetti D. Tonelli S. Topp-Joergensen F. Toriello R. Tourinho Jadallah Aoude E. Tournefier S. Tourneur K. Trabelsi M. Traill M. T. Tran M. Tresch A. Trisovic A. Tsaregorodtsev P. Tsopelas A. Tully N. Tuning A. Ukleja A. Ustyuzhanin U. Uwer C. Vacca V. Vagnoni A. Valassi S. Valat G. Valenti R. Vazquez Gomez P. Vazquez Regueiro S. Vecchi M. van Veghel J. J. Velthuis M. Veltri G. Veneziano A. Venkateswaran T. A. Verlage M. Vernet M. Vesterinen J. V. Viana Barbosa B. Viaud D. Vieira M. Vieites Diaz H. Viemann X. Vilasis-Cardona M. Vitti V. Volkov A. Vollhardt B. Voneki A. Vorobyev V. Vorobyev C. Voß J. A. de Vries C. Vázquez Sierra R. Waldi C. Wallace R. Wallace J. Walsh J. Wang D. R. Ward H. M. Wark N. K. Watson D. Websdale A. Weiden M. Whitehead J. Wicht G. Wilkinson M. Wilkinson M. Williams M. P. Williams M. Williams T. Williams F. F. Wilson J. Wimberley M. A. Winn J. Wishahi W. Wislicki M. Witek G. Wormser S. A. Wotton K. Wraight K. Wyllie Y. Xie Z. Xing Z. Xu Z. Yang Z. Yang Y. Yao H. Yin J. Yu X. Yuan O. Yushchenko K. A. Zarebski M. Zavertyaev L. Zhang Y. Zhang A. Zhelezov Y. Zheng X. Zhu V. Zhukov J. B. Zonneveld S. Zucchelli
Title: Updated branching fraction measurements of B0( s) → K0Sh+h′ − decays
Description:
Abstract The charmless three-body decays B ( s) 0  → K S 0 h + h ′ − (where h (′) = π, K) are analysed using a sample of pp collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 3 fb−1.
The branching fractions are measured relative to that of the B 0 → K S 0 π + π − decay, and are determined to be: $$ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{\pi}^{-}\right)}=0.
123\pm 0.
009\left(\mathrm{stat}\right)\pm 0.
015\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.
549\pm 0.
018\left(\mathrm{stat}\right)\pm 0.
033\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.
191\pm 0.
027\left(\mathrm{stat}\right)\pm 0.
031\left(\mathrm{syst}\right)\pm 0.
011\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=1.
70\pm 0.
07\left(\mathrm{stat}\right)\pm 0.
11\left(\mathrm{syst}\right)\pm 0.
10\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}\in \left[0.
008-0.
051\right]\kern0.
5em \mathrm{at}\kern0.
5em 90\%\kern0.
5em \mathrm{confidence}\kern0.
5em \mathrm{level},\hfill \end{array} $$ ℬ B 0 → K S 0 K ± π ∓ ℬ B 0 → K S 0 K + π − = 0.
123 ± 0.
009 stat ± 0.
015 syst , ℬ B 0 → K S 0 K + K − ℬ B 0 → K S 0 π + π − = 0.
549 ± 0.
018 stat ± 0.
033 syst , ℬ B s 0 → K S 0 π + π − ℬ B 0 → K S 0 π + π − = 0.
191 ± 0.
027 stat ± 0.
031 syst ± 0.
011 f s / f d , ℬ B s 0 → K S 0 K ± π ∓ ℬ B 0 → K S 0 π + π − = 1.
70 ± 0.
07 stat ± 0.
11 syst ± 0.
10 f s / f d , ℬ B s 0 → K S 0 K + K − ℬ B 0 → K S 0 π + π − ∈ 0.
008 − 0.
051 at 90 % confidence level , where f s /f d represents the ratio of hadronisation fractions of the B s 0 and B 0 mesons.

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