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Measurement of D0-D0 mixing parameters using D0 → K(S)(0)π+ π- and D0 → K(S)(0)K+ K- decays.

del Amo Sanchez P,Lees J P,Poireau V,Prencipe E,Tisserand V,Garra Tico J,Grauges E,Martinelli M,Palano A,Pappagallo M,Eigen G,Stugu B,Sun L,Battaglia M,Brown D N,Hooberman B,Kerth L T,Kolomensky Yu G,Lynch G,Osipenkov I L,Tanabe T,Hawkes C M,Watson A T,Koch H,Schroeder T,Asgeirsson D J,Hearty C,Mattison T S,McKenna J A,Khan A,Randle-Conde A,Blinov V E,Buzykaev A R,Druzhinin V P,Golubev V B,Onuchin A P,Serednyakov S I,Skovpen Yu I,Solodov E P,Todyshev K Yu,Yushkov A N,Bondioli M,Curry S,Kirkby D,Lankford A J,Mandelkern M,Martin E C,Stoker D P,Atmacan H,Gary J W,Liu F,Long O,Vitug G M,Campagnari C,Hong T M,Kovalskyi D,Richman J D,Eisner A M,Heusch C A,Kroseberg J,Lockman W S,Martinez A J,Schalk T,Schumm B A,Seiden A,Winstrom L O,Cheng C H,Doll D A,Echenard B,Hitlin D G,Ongmongkolkul P,Porter F C,Rakitin A Y,Andreassen R,Dubrovin M S,Mancinelli G,Meadows B T,Sokoloff M D,Bloom P C,Ford W T,Gaz A,Hirschauer J F,Nagel M,Nauenberg U,Smith J G,Wagner S R,Ayad R,Toki W H,Karbach T M,Merkel J,Petzold A,Spaan B,Wacker K,Kobel M J,Schubert K R,Schwierz R,Bernard D,Verderi M,Clark P J,Playfer S,Watson J E,Andreotti M,Bettoni D,Bozzi C,Calabrese R,Cecchi A,Cibinetto G,Fioravanti E,Franchini P,Luppi E,Munerato M,Negrini M,Petrella A,Piemontese L,Baldini-Ferroli R,Calcaterra A,de Sangro R,Finocchiaro G,Nicolaci M,Pacetti S,Patteri P,Peruzzi I M,Piccolo M,Rama M,Zallo A,Contri R,Guido E,Lo Vetere M,Monge M R,Passaggio S,Patrignani C,Robutti E,Tosi S,Bhuyan B,Lee C L,Morii M,Adametz A,Marks J,Schenk S,Uwer U,Bernlochner F U,Lacker H M,Lueck T,Volk A,Dauncey P D,Tibbetts M,Behera P K,Mallik U,Chen C,Cochran J,Crawley H B,Dong L,Meyer W T,Prell S,Rosenberg E I,Rubin A E,Gao Y Y,Gritsan A V,Guo Z J,Arnaud N,Davier M,Derkach D,Firmino da Costa J,Grosdidier G,Le Diberder F,Lutz A M,Malaescu B,Perez A,Roudeau P,Schune M H,Serrano J,Sordini V,Stocchi A, Wang L,Wormser G,Lange D J,Wright D M,Bingham I,Burke J P,Chavez C A,Coleman J P,Fry J R,Gabathuler E,Gamet R,Hutchcroft D E,Payne D J,Touramanis C,Bevan A J,Di Lodovico F,Sacco R,Sigamani M,Cowan G,Paramesvaran S,Wren A C,Brown D N,Davis C L,Denig A G,Fritsch M,Gradl W,Hafner A,Alwyn K E,Bailey D,Barlow R J,Jackson G,Lafferty G D,West T J,Anderson J,Cenci R,Jawahery A,Roberts D A,Simi G,Tuggle J M,Dallapiccola C,Salvati E,Cowan R,Dujmic D,Fisher P H,Sciolla G,Zhao M,Lindemann D,Patel P M,Robertson S H,Schram M,Biassoni P,Lazzaro A,Lombardo V,Palombo F,Stracka S,Cremaldi L,Godang R,Kroeger R,Sonnek P,Summers D J,Zhao H W,Nguyen X,Simard M,Taras P,De Nardo G,Monorchio D,Onorato G,Sciacca C,Raven G,Snoek H L,Jessop C P,Knoepfel K J,LoSecco J M,Wang W F,Corwin L A,Honscheid K,Kass R,Morris J P,Rahimi A M,Blount N L,Brau J,Frey R,Igonkina O,Kolb J A,Rahmat R,Sinev N B, Strom D,Strube J,Torrence E,Castelli G,Feltresi E,Gagliardi N,Margoni M,Morandin M,Posocco M,Rotondo M,Simonetto F,Stroili R,Ben-Haim E,Bonneaud G R,Briand H,Calderini G,Chauveau J,Hamon O,Leruste Ph,Marchiori G,Ocariz J,Prendki J,Sitt S,Biasini M,Manoni E,Angelini C,Batignani G,Bettarini S,Carpinelli M,Casarosa G,Cervelli A,Forti F,Giorgi M A,Lusiani A,Neri N,Paoloni E,Rizzo G,Walsh J J,Lopes Pegna D,Lu C,Olsen J,Smith A J S,Telnov A V,Anulli F,Baracchini E,Cavoto G,Faccini R,Ferrarotto F,Ferroni F,Gaspero M,Li Gioi L,Mazzoni M A,Piredda G, Renga F,Ebert M,Hartmann T,Leddig T,Schröder H,Waldi R,Adye T,Franek B,Olaiya E O,Wilson F F,Emery S,Hamel de Monchenault G,Vasseur G,Yèche Ch,Zito M,Aitchison I J R,Allen M T,Aston D,Bard D J,Bartoldus R,Benitez J F,Cartaro C,Convery M R,Dorfan J,Dubois-Felsmann G P,Dunwoodie W,Field R C,Franco Sevilla M,Fulsom B G,Gabareen A M,Graham M T,Grenier P,Hast C,Innes W R,Kelsey M H,Kim H,Kim P,Kocian M L,Leith D W G S,Li S,Lindquist B,Luitz S,Luth V,Lynch H L,MacFarlane D B,Marsiske H,Muller D R,Neal H,Nelson S,O'Grady C P,Ofte I,Perl M,Pulliam T,Ratcliff B N,Roodman A,Salnikov A A,Santoro V,Schindler R H,Schwiening J,Snyder A,Su D,Sullivan M K,Sun S,Suzuki K,Thompson J M,Va'vra J,Wagner A P,Weaver M, West C A,Wisniewski W J,Wittgen M,Wright D H,Wulsin H W,Yarritu A K,Young C C,Ziegler V,Chen X R,Park W,Purohit M V,White R M,Wilson J R,Sekula S J,Bellis M,Burchat P R,Edwards A J,Miyashita T S,Ahmed S,Alam M S,Ernst J A,Pan B,Saeed M A,Zain S B,Guttman N,Soffer A,Lund P,Spanier S M,Eckmann R,Ritchie J L,Ruland A M,Schilling C J,Schwitters R F,Wray B C,Izen J M,Lou X C,Bianchi F,Gamba D,Pelliccioni M,Bomben M,Lanceri L,Vitale L,Lopez-March N,Martinez-Vidal F,Milanes D A,Oyanguren A,Albert J,Banerjee Sw,Choi H H F,Hamano K,King G J,Kowalewski R,Lewczuk M J,Nugent I M,Roney J M,Sobie R J,Gershon T J,Harrison P F,Ilic J,Latham T E,Puccio E M T,Band H R,Chen X,Dasu S,Flood K T,Pan Y,Prepost R,Vuosalo C O,Wu S L, Null Null

Physical review letters(2010)

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摘要
We report a direct measurement of D0-D0 mixing parameters through a time-dependent amplitude analysis of the Dalitz plots of D(0) → K(S)(0) π+ π- and, for the first time, D0 → K(S)(0)K+ K- decays. The low-momentum pion π(s)(+) in the decay D*+ → D0 π(s)(+) identifies the flavor of the neutral D meson at its production. Using 468.5 fb(-1) of e+ e- colliding-beam data recorded near square root(s)=10.6 GeV by the BABAR detector at the PEP-II asymmetric-energy collider at SLAC, we measure the mixing parameters x = [1.6 ± 2.3(stat) ± 1.2(syst) ± 0.8(model)] × 10(-3), and y = [5.7 ± 2.0(stat) ± 1.3(syst) ± 0.7(model)] × 10(-3). These results provide the best measurement to date of x and y. The knowledge of the value of x, in particular, is crucial for understanding the origin of mixing.
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