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Related papers: Extracting beta and the new D_{sJ} resonances

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We consider the possibility of measuring both $\sin (2 \beta)$ and $\cos (2 \beta)$ in the KM unitarity triangle using the process $B^0 \to D^{*+}D^{*-}K_s$. This decay mode has a higher branching fraction (O(1%)) than the mode $B^0 \to…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. E. Browder , A. Datta , Patrick. J. O'Donnell , S. Pakvasa

We study the nonresonant three-body decays of $B^{+}\to D^{(*)-}_{s} K^{+} \pi^{+}$ and $B_{d}\to D_{s}^{(*)-} K^{0} \pi^{+}$. We find that these decays can provide the information on the time-like form factors of $D^{(*)}_{s} K$. We also…

High Energy Physics - Phenomenology · Physics 2009-11-10 Chuan-Hung Chen

We study the contributions of the $B\rightarrow \psi(3770)K[\psi(3770)\rightarrow D\bar{D}]$, $B\rightarrow K^*(1410)\pi[K^*(1410)\rightarrow K\pi]$ and $B\rightarrow X(3872)K[X(3872)\rightarrow J/\psi\gamma, \psi(2S)\gamma, D\bar{D}\pi,…

High Energy Physics - Experiment · Physics 2023-11-14 Hossein. Mehraban , Behnam Mohammadi

We present a method to measure the weak phase 2beta+gamma in the three-body decay B0 -> D+- Ks pi-+. These decays are mediated by interfering amplitudes which are color-allowed and hence relatively large. In addition, the three-body decay…

High Energy Physics - Phenomenology · Physics 2010-11-23 R. Aleksan , T. C. Petersen

If the weak phase of B_s-anti B_s mixing (2 beta_s) is found to be significantly different from zero, this is a clear signal of new physics (NP). However, if such a signal is found, we would like an unambiguous determination of 2 beta_s in…

High Energy Physics - Phenomenology · Physics 2013-05-30 Soumitra Nandi , David London

We (re)examine CP violation in the decays B_d -> D K_s, where D represents D^0, D(bar), or one of their excited states. The quantity $\sin^2(2\beta + \gamma)$ can be extracted from the time-dependent rates for $B_d(t) -> {\bar D}^{**0} K_s$…

High Energy Physics - Phenomenology · Physics 2014-11-17 B. Kayser , D. London

I briefly describe the use of the three-body decay modes $B^0 \to D^{(*)-} D^{(*)0} K^+$ to investigate open issues in charmed meson spectroscopy, and of the time dependent $B^0 (\bar {B^0}) (t) \to D^{-} D^{+} \pi^0$ transitions for a…

High Energy Physics - Phenomenology · Physics 2009-11-07 P. Colangelo

We describe how the angular analysis of vector-vector final states in B decays provides theoretically clean techniques for determination of CP violating phases. The quantity $\sin^2 (2\beta + \gamma)$ can be cleanly obtained from the time…

High Energy Physics - Phenomenology · Physics 2007-05-23 David London , Nita Sinha , Rahul Sinha

We study the decay B0->D*+D*-Ks using (230 +/- 2) x 10^{6} BBbar pairs collected by the Babar detector at the PEP-II B factory. We measure a branching fraction B(B0->D*+D*-Ks)=(4.4\pm0.4\pm0.7)\times 10^{-3} and find evidence for the decay…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

Preliminary results are presented on a search for several exclusive charmless hadronic B decays, from data collected by the BABAR detector near the Upsilon(4S) resonance. These include two-body decay modes h^{+/-}h^{-/+} three-body decay…

High Energy Physics - Experiment · Physics 2007-05-23 Theresa J. Champion

The small P wave compoment of $B\to J/\psi K^*$ measured by CLEO makes it practical to measure $\sin2\beta$ using $B^0\to J/\psi K^{*0}\to J/\psi K_S \pi^0$, independent from $B^0\to J/\psi K_S$. Because these modes are color suppressed,…

High Energy Physics - Phenomenology · Physics 2009-10-31 Xiao-Gang He , Wei-Shu Hou

We consider the nonleptonic B decays $ B \to D^{(*)} D_s(2317)$ and $ B \to D^{(*)} D_s(2460)$, involving the newly discovered $D_s(2317)$ and the $D_s(2460)$ states. We find that experiments indicate disagreement with model calculations of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alakabha Datta , Patrick J. O'Donnell

We present a method to measure the weak phase gamma in the three-body decay of charged B mesons to the final states D K pi0. These decays are mediated by interfering amplitudes which are color-allowed and hence relatively large. As a…

High Energy Physics - Phenomenology · Physics 2010-11-23 Roy Aleksan , Troels Petersen , Abner Soffer

We compute energy distributions of three particles emerging from decaying many-body resonances. We reproduce the measured energy distributions from decays of two archetypal states chosen as the lowest $0^{+}$ and $1^{+}$-resonances in…

Nuclear Theory · Physics 2008-11-26 R. Alvarez-Rodriguez , A. S. Jensen , D. V. Fedorov , H. O. U. Fynbo , E. Garrido

We present the complete differential decay rates for the process B_s -> J/psi K^+ K^- including S-wave and P-wave angular momentum states for the K^+ K^- meson pair. We examine the effect of an S-wave component on the determination of the…

High Energy Physics - Phenomenology · Physics 2009-11-18 Yuehong Xie , Peter Clarke , Greig Cowan , Franz Muheim

In this work, we study the $S$, $P$ and $D$ wave resonance contributions to three-body decays $B_{(s)} \to [ D^{(*)}, \bar{D}^{(*)} ] K^+K^-$ by employing the perturbative QCD (PQCD) approach, where the kaon-kaon invariant mass spectra are…

High Energy Physics - Phenomenology · Physics 2020-09-23 Ya Li , Da-Cheng Yan , Zhou Rui , Lan Liu , Yue-Tong Zhang , Zhen-Jun Xiao

We report a measurement of the exclusive $B^+$ meson decay to the final state $D_s^- K^+\pi^+$ using $520 \times 10^{6} B\bar{B}$ pairs collected near the $\Upsilon(4S)$ resonance, with the Belle detector at the KEKB asymmetric-energy…

High Energy Physics - Experiment · Physics 2007-08-22 The Belle Collaboration , K. Abe

We make a detailed study of the three-body decays $B_{(s)}\rightarrow \chi_{c1} hh'$, where $h^{(')}$ is either a pion or kaon, by taking into account the $S$-wave states in the $hh'$ invariant mass distribution within the perturbative QCD…

High Energy Physics - Phenomenology · Physics 2021-10-13 Meng-Kun Jia , Chao-Qi Zhang , Jia-Ming Li , Zhou Rui

We suggest a novel method to determine the sign of cos(2 beta) in the decays B --> psi K, by creating interference between KL and KS final states via ``regeneration,'' that is propagation through a matter target region to convert some KL to…

High Energy Physics - Phenomenology · Physics 2010-11-23 Helen R. Quinn , Thomas Schietinger , Joao P. Silva , Arthur E. Snyder

We present a feasibility study of a method to measure the cosine of twice the CKM Unitarity Triangle angle beta using a time-dependent Dalitz plot analysis of B0 -> D pi+ pi- decays, where the neutral D meson is reconstructed in decays to…

High Energy Physics - Phenomenology · Physics 2008-12-18 Thomas Latham , Tim Gershon
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