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Ogilvy51 S.Okhrimenko O.Oldeman R.Onderwater G.Orlandea M.Otalora Goicochea J.M.Owen P.Oyanguren A.Pal B.K.Palano A.Palombo F.Palutan M.Panman J.Papanestis A.Pappagallo M.Pappalardo L.L.Parkes C.Parkinson C.J.Passaleva G.Patel G.D.Patel M.Patrignani C.Pazos Alvarez A.Pearce A.Pellegrino A.Pepe Altarelli M.Perazzini S.Perez Trigo E.Perret P.Perrin-Terrin M.Pescatore L.Pesen E.Petridis K.Petrolini A.Picatoste Olloqui E.Pietrzyk B.Pilař T.Pinci D.Pistone A.Playfer S.Plo Casasus M.Polci F.Poluektov A.Polycarpo E.Popov A.Popov1 D.Popovici B.Potterat C.Price E.Prisciandaro J.Pritchard A.Prouve C.Pugatch V.Puig Navarro A.Punzi G.Qian W.Rachwal B.Rademacker J.H.Rakotomiaramanana B.Rama M.Rangel M.S.Raniuk I.Rauschmayr N.Raven G.Reichert S.Reid M.M.Dos Reis A.C.Ricciardi S.Richards S.Rihl M.Rinnert K.Rives Molina V.Roa Romero D.A.Robbe P.Rodrigues A.B.Rodrigues E.Rodriguez Perez P.Roiser S.Romanovsky V.Romero Vidal A.Rotondo M.Rouvinet J.Ruf T.Ruiz H.Ruiz Valls P.Saborido Silva J.J.Sagidova N.Sail P.Saitta B.Salustino Guimaraes V.Sanchez Mayordomo C.Sanmartin Sedes B.Santacesaria R.Santamarina Rios C.Santovetti E.Sarti A.Satriano C.Satta A.Saunders D.M.Savrie M.Savrina D.Schiller M.Schindler H.Schlupp M.Schmelling M.Schmidt B.Schneider O.Schopper A.Schune M.-H.Schwemmer R.Sciascia B.Sciubba A.Seco M.Semennikov A.Sepp I.Serra N.Serrano J.Sestini L.Seyfert P.Shapkin M.Shapoval I.Shcheglov Y.Shears T.Shekhtman L.Shevchenko V.Shires A.Silva Coutinho R.Simi G.Sirendi M.Skidmore N.Skwarnicki T.Smith N.A.Smith E.Smith E.Smith J.Smith M.Snoek H.Sokoloff M.D.Soler F.Soomro F.Souza D.Souza De Paula B.Spaan B.Sparkes A.Spradlin P.Sridharan S.Stagni F.Stahl M.Stahl S.Steinkamp O.Stenyakin O.Stevenson S.Stoica S.Stone S.Storaci B.Stracka S.Straticiuc M.Straumann U.Stroili R.Subbiah V.K.Sun L.Sutcliffe W.Swientek K.Swientek S.Syropoulos V.Szczekowski M.Szczypka P.Szilard D.Szumlak T.T’Jampens S.Teklishyn M.Tellarini G.Teubert F.Thomas C.Thomas E.Van Tilburg J.Tisserand V.Tobin M.Tolk S.Tomassetti L.Tonelli D.Topp-Joergensen S.Torr N.Tournefier E.Tourneur S.Tran M.T.Tresch M.Tsaregorodtsev A.Tsopelas P.Tuning N.Ubeda Garcia M.Ukleja A.Ustyuzhanin A.Uwer U.Vagnoni V.Valenti G.Vallier A.Vazquez Gomez R.Vazquez Regueiro P.Vázquez Sierra C.Vecchi S.Velthuis J.J.Veltri M.Veneziano G.Vesterinen M.Viaud B.Vieira D.Vieites Diaz M.Vilasis-Cardona X.Vollhardt A.Volyanskyy D.Voong D.Vorobyev A.Vorobyev V.Voß C.Voss H.De Vries J.A.Waldi R.Wallace C.Wallace R.Walsh J.Wandernoth S.Wang J.Ward D.R.Watson N.K.Websdale D.Whitehead M.Wicht J.Wiedner D.Wilkinson G.Williams M.P.Williams M.Wilson F.F.Wimberley J.Wishahi J.Wislicki W.Witek M.Wormser G.Wotton S.A.Wright S.Wu S.Wyllie K.Xie Y.Xing Z.Xu Z.Yang Z.Yuan X.Yushchenko O.Zangoli M.Zavertyaev M.Zhang L.Zhang W.C.2024-07-222024-07-22201410298479http://akademikarsiv.cbu.edu.tr:4000/handle/123456789/16846A binned Dalitz plot analysis of B± → DK± decays, with D → KS π+π− and D → KS K+K−, is performed to measure the CP -violating observables x± and y±, which are sensitive to the Cabibbo-Kobayashi-Maskawa angle γ. The analysis exploits a sample of proton-proton collision data corresponding to 3.0 fb−1 collected by the LHCb experiment. Measurements from CLEO-c of the variation of the strong-interaction phase of the D decay over the Dalitz plot are used as inputs. The values of the parameters are found to be x+ = (−7.7 ± 2.4 ± 1.0 ± 0.4) × 10−2, x− = (2.5 ± 2.5 ± 1.0 ± 0.5) × 10−2, y+ = (−2.2 ± 2.5 ± 0.4 ± 1.0) × 10−2, and y− = (7.5 ± 2.9 ± 0.5 ± 1.4) × 10−2. The first, second, and third uncertainties are the statistical, the experimental systematic, and that associated with the precision of the strong-phase parameters. These are the most precise measurements of these observables and correspond to γ = (62 −14)◦, with a second solution at γ → γ + 180◦, and rB = 0.080−0.021, where rB is the ratio between the suppressed and favoured B decay amplitudes. © CERN 2014. All rights reserved.EnglishAll Open Access; Gold Open AccessArticle10.1007/JHEP10(2014)097