Browsing by Author "Abachi S."
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Institution PublicationConstraints on the CKM angle γ in B0→D̄0K*0 and B0→D0K*0 from a Dalitz analysis of D0 and D̄0 decays to KSπ+π-( 2009-04-01)
;Aubert B. ;Bona M. ;Karyotakis Y. ;Lees J.P. ;Poireau V. ;Prudent X. ;Tisserand V. ;Zghiche A. ;Tico J.G. ;Grauges E. ;Lopez L. ;Palano A. ;Pappagallo M. ;Eigen G. ;Stugu B. ;Sun L. ;Abrams G.S. ;Battaglia M. ;Brown D.N. ;Button-Shafer J. ;Cahn R.N. ;Jacobsen R.G. ;Kadyk J.A. ;Kerth L.T. ;Kolomensky Y.G. ;Kukartsev G. ;Lynch G. ;Osipenkov I.L. ;Ronan M.T. ;Tackmann K. ;Tanabe T. ;Wenzel W.A. ;Hawkes C.M. ;Soni N. ;Watson A.T. ;Koch H. ;Schroeder T. ;Walker D. ;Asgeirsson D.J. ;Cuhadar-Donszelmann T. ;Fulsom B.G. ;Hearty C. ;Mattison T.S. ;McKenna J.A. ;Barrett M. ;Khan A. ;Saleem M. ;Teodorescu L. ;Blinov V.E. ;Bukin A.D. ;Buzykaev A.R. ;Druzhinin V.P. ;Golubev V.B. ;Onuchin A.P. ;Serednyakov S.I. ;Skovpen Y.I. ;Solodov E.P. ;Todyshev K.Y. ;Bondioli M. ;Curry S. ;Eschrich I. ;Kirkby D. ;Lankford A.J. ;Lund P. ;Mandelkern M. ;Martin E.C. ;Stoker D.P. ;Abachi S. ;Buchanan C. ;Gary J.W. ;Liu F. ;Long O. ;Shen B.C. ;Vitug G.M. ;Yasin Z. ;Zhang L. ;Paar H.P. ;Rahatlou S. ;Sharma V. ;Campagnari C. ;Hong T.M. ;Kovalskyi D. ;Mazur M.A. ;Richman J.D. ;Beck T.W. ;Eisner A.M. ;Flacco C.J. ;Heusch C.A. ;Kroseberg J. ;Lockman W.S. ;Schalk T. ;Schumm B.A. ;Seiden A. ;Wilson M.G. ;Winstrom L.O. ;Chen E. ;Cheng C.H. ;Doll D.A. ;Echenard B.Fang F.We present constraints on the angle γ of the unitarity triangle with a Dalitz analysis of neutral D decays to KSπ+π- from the processes B0→D̄0K*0 (B̄0→D0K̄*0) and B0→D0K*0 (B̄0→D̄0K̄*0) with K*0→K+π- (K̄*0→K-π+). Using a sample of 371×106 BB̄ pairs collected with the BABAR detector at PEP-II, we constrain the angle γ as a function of rS, the magnitude of the average ratio between b→u and b→c amplitudes. © 2009 The American Physical Society. -
Institution PublicationExclusive initial-state-radiation production of the DD̄, D*D̄, and D*D̄* systems( 2009-05-01)
;Aubert B. ;Karyotakis Y. ;Lees J.P. ;Poireau V. ;Prencipe E. ;Prudent X. ;Tisserand V. ;Garra Tico J. ;Grauges E. ;Lopez L. ;Lopez L. ;Palano A. ;Palano A. ;Pappagallo M. ;Pappagallo M. ;Eigen G. ;Stugu B. ;Sun L. ;Battaglia M. ;Brown D.N. ;Kerth L.T. ;Kolomensky Y.G. ;Lynch G. ;Osipenkov I.L. ;Tackmann K. ;Tanabe T. ;Hawkes C.M. ;Soni N. ;Watson A.T. ;Koch H. ;Schroeder T. ;Asgeirsson D.J. ;Fulsom B.G. ;Hearty C. ;Mattison T.S. ;McKenna J.A. ;Barrett M. ;Khan A. ;Randle-Conde A. ;Blinov V.E. ;Bukin A.D. ;Buzykaev A.R. ;Druzhinin V.P. ;Golubev V.B. ;Onuchin A.P. ;Serednyakov S.I. ;Skovpen Y.I. ;Solodov E.P. ;Todyshev K.Y. ;Bondioli M. ;Curry S. ;Eschrich I. ;Kirkby D. ;Lankford A.J. ;Lund P. ;Mandelkern M. ;Martin E.C. ;Stoker D.P. ;Abachi S. ;Buchanan C. ;Atmacan H. ;Gary J.W. ;Liu F. ;Long O. ;Vitug G.M. ;Yasin Z. ;Zhang L. ;Sharma V. ;Campagnari C. ;Hong T.M. ;Kovalskyi D. ;Mazur M.A. ;Richman J.D. ;Beck T.W. ;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. ;Fang F. ;Hitlin D.G. ;Narsky I. ;Piatenko T. ;Porter F.C. ;Andreassen R. ;Mancinelli G. ;Meadows B.T. ;Mishra K. ;Sokoloff M.D. ;Bloom P.C. ;Ford W.T. ;Gaz A. ;Hirschauer J.F. ;Nagel M. ;Nauenberg U.Smith J.G.We perform a study of the exclusive production of DD̄, D*D̄, and D*D̄* in initial-state-radiation events, from e+e- annihilations at a center-of-mass energy near 10.58. -
Institution PublicationMeasurement of D0-D̄0 Mixing from a Time-Dependent Amplitude Analysis of D0→K+π-π0 Decays( 2009-11-18)
;Aubert B. ;Bona M. ;Karyotakis Y. ;Lees J.P. ;Poireau V. ;Prencipe E. ;Prudent X. ;Tisserand V. ;Tico J.G. ;Grauges E. ;Lopez L. ;Lopez L. ;Palano A. ;Palano A. ;Pappagallo M. ;Pappagallo M. ;Eigen G. ;Stugu B. ;Sun L. ;Abrams G.S. ;Battaglia M. ;Brown D.N. ;Cahn R.N. ;Jacobsen R.G. ;Kerth L.T. ;Kolomensky Y.G. ;Lynch G. ;Osipenkov I.L. ;Ronan M.T. ;Tackmann K. ;Tanabe T. ;Hawkes C.M. ;Soni N. ;Watson A.T. ;Koch H. ;Schroeder T. ;Walker D. ;Asgeirsson D.J. ;Fulsom B.G. ;Hearty C. ;Mattison T.S. ;McKenna J.A. ;Barrett M. ;Khan A. ;Blinov V.E. ;Bukin A.D. ;Buzykaev A.R. ;Druzhinin V.P. ;Golubev V.B. ;Onuchin A.P. ;Serednyakov S.I. ;Skovpen Y.I. ;Solodov E.P. ;Todyshev K.Y. ;Bondioli M. ;Curry S. ;Eschrich I. ;Kirkby D. ;Lankford A.J. ;Lund P. ;Mandelkern M. ;Martin E.C. ;Stoker D.P. ;Abachi S. ;Buchanan C. ;Gary J.W. ;Liu F. ;Long O. ;Shen B.C. ;Vitug G.M. ;Yasin Z. ;Zhang L. ;Sharma V. ;Campagnari C. ;Hong T.M. ;Kovalskyi D. ;Mazur M.A. ;Richman J.D. ;Beck T.W. ;Eisner A.M. ;Flacco C.J. ;Heusch C.A. ;Kroseberg J. ;Lockman W.S. ;Schalk T. ;Schumm B.A. ;Seiden A. ;Wang L. ;Wilson M.G. ;Winstrom L.O. ;Cheng C.H. ;Doll D.A. ;Echenard B. ;Fang F. ;Hitlin D.G. ;Narsky I. ;Piatenko T. ;Porter F.C. ;Andreassen R. ;Mancinelli G. ;Meadows B.T. ;Mishra K.Sokoloff M.D.We present evidence of D0-D̄0 mixing using a time-dependent amplitude analysis of the decay D0→K+π-π0 in a data sample of 384fb-1 collected with the BABAR detector at the PEP-II e+e- collider at the Stanford Linear Accelerator Center. Assuming CP conservation, we measure the mixing parameters xKππ0′=[2.61-0.68+0.57(stat)±0.39(syst)]%, yKππ0′=[-0.06-0.64+0.55(stat)±0.34(syst)]%. This result is inconsistent with the no-mixing hypothesis with a significance of 3.2 standard deviations. We find no evidence of CP violation in mixing. © 2009 The American Physical Society. -
Institution PublicationSearch for the Z(4430)- at B A B AR( 2009-06-01)
;Aubert B. ;Bona M. ;Karyotakis Y. ;Lees J.P. ;Poireau V. ;Prencipe E. ;Prudent X. ;Tisserand V. ;Tico J.G. ;Grauges E. ;Lopez L. ;Lopez L. ;Palano A. ;Palano A. ;Pappagallo M. ;Pappagallo M. ;Eigen G. ;Stugu B. ;Sun L. ;Abrams G.S. ;Battaglia M. ;Brown D.N. ;Cahn R.N. ;Jacobsen R.G. ;Kerth L.T. ;Kolomensky Y.G. ;Lynch G. ;Osipenkov I.L. ;Ronan M.T. ;Tackmann K. ;Tanabe T. ;Hawkes C.M. ;Soni N. ;Watson A.T. ;Koch H. ;Schroeder T. ;Walker D. ;Asgeirsson D.J. ;Fulsom B.G. ;Hearty C. ;Mattison T.S. ;McKenna J.A. ;Barrett M. ;Khan A. ;Blinov V.E. ;Bukin A.D. ;Buzykaev A.R. ;Druzhinin V.P. ;Golubev V.B. ;Onuchin A.P. ;Serednyakov S.I. ;Skovpen Y.I. ;Solodov E.P. ;Todyshev K.Y. ;Bondioli M. ;Curry S. ;Eschrich I. ;Kirkby D. ;Lankford A.J. ;Lund P. ;Mandelkern M. ;Martin E.C. ;Stoker D.P. ;Abachi S. ;Buchanan C. ;Atmacan H. ;Gary J.W. ;Liu F. ;Long O. ;Vitug G.M. ;Yasin Z. ;Zhang L. ;Sharma V. ;Campagnari C. ;Hong T.M. ;Kovalskyi D. ;Mazur M.A. ;Richman J.D. ;Beck T.W. ;Eisner A.M. ;Flacco C.J. ;Heusch C.A. ;Kroseberg J. ;Lockman W.S. ;Martinez A.J. ;Schalk T. ;Schumm B.A. ;Seiden A. ;Wilson M.G. ;Winstrom L.O. ;Cheng C.H. ;Doll D.A. ;Echenard B. ;Fang F. ;Hitlin D.G. ;Narsky I. ;Piatenko T. ;Porter F.C. ;Andreassen R. ;Mancinelli G. ;Meadows B.T. ;Mishra K.Sokoloff M.D.We report the results of a search for Z(4430)- decay to J/ψπ- or ψ(2S)π- in B-,0→J/ψπ-K0,+ and B-,0→ψ(2S)π-K0,+ decays. The data were collected with the BABAR detector at the SLAC PEP-II asymmetric-energy e+e- collider operating at center-of-mass energy 10.58 GeV, and the sample corresponds to an integrated luminosity of 413fb-1. Each Kπ- mass distribution exhibits clear K*(892) and K2*(1430) signals, and the efficiency-corrected spectrum is well described by a superposition of the associated Breit-Wigner intensity distributions, together with an S-wave contribution obtained from the LASS I=1/2 Kπ- scattering amplitude measurements. Each Kπ- angular distribution varies significantly in structure with Kπ- mass, and is represented in terms of low-order Legendre polynomial moments. We find that each J/ψπ- or ψ(2S)π- mass distribution is well described by the reflection of the measured Kπ- mass and angular distribution structures. We see no significant evidence for a Z(4430)- signal for any of the processes investigated, neither in the total J/ψπ- or ψ(2S)π- mass distribution, nor in the corresponding distributions for the regions of Kπ- mass for which observation of the Z(4430)- signal was reported. We obtain branching-fraction upper limits B(B-→Z-K̄0,Z- →J/ψπ-)<1.5×10-5, B(B0→Z-K+,Z-→J/ψπ-) <0.4×10-5, B(B-→Z-K̄0,Z-→ψ(2S)π-)<4. 7×10-5, and B(B0→Z-K+,Z-→ψ(2S)π-)<3.1×10-5 at 95% confidence level, where the Z(4430)- mass and width have been fixed to the reported central values. © 2009 The American Physical Society. -
Institution PublicationTime-dependent amplitude analysis of B0→KS0π+π-( 2009-12-02)
;Aubert B. ;Karyotakis Y. ;Lees J.P. ;Poireau V. ;Prencipe E. ;Prudent X. ;Tisserand V. ;Tico J.G. ;Grauges E. ;Martinelli M. ;Martinelli M. ;Palano A. ;Palano A. ;Pappagallo M. ;Pappagallo M. ;Eigen G. ;Stugu B. ;Sun L. ;Battaglia M. ;Brown D.N. ;Kerth L.T. ;Kolomensky Y.G. ;Lynch G. ;Osipenkov I.L. ;Tackmann K. ;Tanabe T. ;Hawkes C.M. ;Soni N. ;Watson A.T. ;Koch H. ;Schroeder T. ;Asgeirsson D.J. ;Fulsom B.G. ;Hearty C. ;Mattison T.S. ;McKenna J.A. ;Barrett M. ;Khan A. ;Randle-Conde A. ;Blinov V.E. ;Bukin A.D. ;Buzykaev A.R. ;Druzhinin V.P. ;Golubev V.B. ;Onuchin A.P. ;Serednyakov S.I. ;Skovpen Y.I. ;Solodov E.P. ;Todyshev K.Y. ;Bondioli M. ;Curry S. ;Eschrich I. ;Kirkby D. ;Lankford A.J. ;Lund P. ;Mandelkern M. ;Martin E.C. ;Stoker D.P. ;Abachi S. ;Buchanan C. ;Atmacan H. ;Gary J.W. ;Liu F. ;Long O. ;Vitug G.M. ;Yasin Z. ;Zhang L. ;Sharma V. ;Campagnari C. ;Hong T.M. ;Kovalskyi D. ;Mazur M.A. ;Richman J.D. ;Beck T.W. ;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. ;Fang F. ;Hitlin D.G. ;Narsky I. ;Piatenko T. ;Porter F.C. ;Andreassen R. ;Mancinelli G. ;Meadows B.T. ;Mishra K. ;Sokoloff M.D. ;Bloom P.C. ;Ford W.T. ;Gaz A. ;Hirschauer J.F. ;Nagel M. ;Nauenberg U.Smith J.G.We perform a time-dependent amplitude analysis of B0→KS0π+π- decays to extract the CP violation parameters of f0(980)KS0 and ρ0(770)KS0 and the direct CP asymmetry of K*+(892)π-. The results are obtained from a data sample of (383±3)×106 BB̄ decays, collected with the BABAR detector at the PEP-II asymmetric-energy B factory at SLAC. We find two solutions, with an equivalent goodness-of-fit. Including systematic and Dalitz plot model uncertainties, the combined confidence interval for values of the CP parameter βeff in B0 decays to f0(980)KS0 is 18°<β eff<76° at 95% confidence level (C.L). CP conservation in B0 decays to f0(980)KS0 is excluded at 3.5 standard deviations including systematic uncertainties. For B0 decays to ρ0(770)KS0, the combined confidence interval is -9°<βeff<57° at 95% C.L. In decays to K*+(892)π- we measure the direct CP asymmetry to be ACP=-0.20±0.10±0. 01±0.02. The measured phase difference (including B0B̄0 mixing) between decay amplitudes of B0→K*+(892)π- and B̄0→K *-(892)π+, excludes the interval -137°<ΔΦ(K*+(892) π-)<-5° at 95% C.L. © 2009 The American Physical Society.