Amplitude analysis of B-0 -> (D)over-bar0K(+)pi(-) decays
Aaij, R.;Adeva, B.;Adinolfi, M.;Affolder, A.;Ajaltouni, Z.;Akar, S.;Albrecht, J.;Alessio, F.;Alexander, M.;Ali, S.;Alkhazov, G.;Cartelle, P. Alvarez;Alves, A. A.;Amato, S.;Amerio, S.;Amhis, Y.;An, L.;Anderlini, L.;Anderson, J.;Andreotti, M.;Andrews, J. E.;Appleby, R. B.;Gutierrez, O. Aquines;Archilli, F.;D'Argent, P.;Artamonov, A.;Artuso, M.;Aslanides, E.;Auriemma, G.;Baalouch, M.;Bachmann, S.;Back, J. J.;Badalov, A.;Baesso, C.;Baldini, W.;Barlow, R. J.;Barschel, C.;Barsuk, S.;Barter, W.;Batozskaya, V.;Battista, V.;Bay, A.;Beaucourt, L.;Beddow, J.;Bedeschi, F.;Bediaga, I.;Bel, L. J.;Belyaev, I.;Ben Haim, E.;Bencivenni, G.;Benson, S.;Benton, J.;Berezhnoy, A.;Bernet, R.;Bertolin, A.;Bettler, M. O.;van Beuzekom, M.;Bien, A.;Bifani, S.;Bird, T.;Birnkraut, A.;Bizzeti, A.;Blake, T.;Blanc, F.;Blouw, J.;Blusk, S.;Bocci, V.;Bondar, A.;Bondar, N.;Bonivento, W.;Borghi, S.;Borsato, M.;Bowcock, T. J. V.;Bowen, E.;Bozzi, C.;Braun, S.;Brett, D.;Britsch, M.;Britton, T.;Brodzicka, J.;Brook, N. 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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.;de Vries, J. A.;Waldi, R.;Wallace, C.;Wallace, R.;Walsh, J.;Wandernoth, S.;Wang, J.;Ward, D. R.;Watson, N. K.;Websdale, D.;Weiden, A.;Whitehead, M.;Wiedner, D.;Wilkinson, G.;Wilkinson, M.;Williams, M.;Williams, M. P.;Williams, M.;Williams, T.;Wilson, F. F.;Wimberley, J.;Wishahi, J.;Wislicki, W.;Witek, M.;Wormser, G.;Wotton, S. A.;Wright, S.;Wyllie, K.;Xie, Y.;Xu, Z.;Yang, Z.;Yu, J.;Yuan, X.;Yushchenko, O.;Zangoli, M.;Zavertyaev, M.;Zhang, L.;Zhang, Y.;Zhelezov, A.;Zhokhov, A.;Zhong, L.
2015-01-01
Abstract
The Dalitz plot distribution of B0→D¯0K+π- decays is studied using a data sample corresponding to 3.0fb-1 of pp collision data recorded by the LHCb experiment during 2011 and 2012. The data are described by an amplitude model that contains contributions from intermediate K∗(892)0, K∗(1410)0, K2∗(1430)0 and D2∗(2460)- resonances. The model also contains components to describe broad structures, including the K0∗(1430)0 and D0∗(2400)- resonances, in the Kπ S-wave and the Dπ S- and P-waves. The masses and widths of the D0∗(2400)- and D2∗(2460)- resonances are measured, as are the complex amplitudes and fit fractions for all components included in the amplitude model. The model obtained will be an integral part of a future determination of the angle γ of the Cabibbo-Kobayashi-Maskawa quark mixing matrix using B0→DK+π- decays.
2015
Inglese
92
1
24
Esperti anonimi
internazionale
scientifica
sì
Aaij, R.; Adeva, B.; Adinolfi, M.; Affolder, A.; Ajaltouni, Z.; Akar, S.; Albrecht, J.; Alessio, F.; Alexander, M.; Ali, S.; Alkhazov, G.; Cartelle, P
...espandi
1.1 Articolo in rivista
info:eu-repo/semantics/article
1 Contributo su Rivista::1.1 Articolo in rivista
262
720
open
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