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Related papers: Non-factorizable effects on $\Bbar^0\to D^{(*)0}\p…

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For the color-suppressed $\bar{B}^0\longrightarrow D^{0}\pi^{0}$ decay, nonfactorizable contributions are expected to be leading and naive factorization description breaks down. We estimate $1/m_b$ power-suppressed nonfactorizable effect in…

High Energy Physics - Phenomenology · Physics 2011-07-19 Jian-Ying Cui , Zuo-Hong Li

The decay modes of the type $B \rightarrow \pi \, \pi $ are dynamically different. For the case $\bar{B_{d}^0} \rightarrow \, \pi^+ \pi^- $ there is a substantial factorized contribution which dominates. In contrast, the decay mode…

High Energy Physics - Phenomenology · Physics 2011-03-22 Jan O. Eeg , Teresa Palmer

The decay modes of the type $B \to \pi \, D $ are dynamically different. For the case $\bar{B_{d}^0} \to \pi^- D^{+} $ there is a substantial factorized contribution which dominates. In contrast, the decay mode $\bar{B_{d}^0} \to \pi^0…

High Energy Physics - Phenomenology · Physics 2014-11-20 Lars E. Leganger , Jan O. Eeg

Recent experimental results on the color-suppressed nonleptonic decays B^0 -> D^{(*)0} pi^0 provide evidence for a failure of the naive factorization model and for sizeable relative strong-interaction phases between class-1 and class-2 B ->…

High Energy Physics - Phenomenology · Physics 2009-11-07 Matthias Neubert , Alexey A. Petrov

Nonleptonic decays B to D pi- or B to D* pi- are dominated by factorizable contributions. In the heavy quark limit, nonfactorizable contribution arises from strong radiative correction and power corrections in 1/m_b. I calculate the decay…

High Energy Physics - Phenomenology · Physics 2011-01-27 Junegone Chay

We consider the color suppressed (nonfactorizable) amplitude for the decay mode $\bar{B_{d}^0} \rightarrow \pi^0 \pi^{0} $. We treat the $b$-quark in the heavy quark limit and the energetic light ($u,d,s$) quarks within a variant of Large…

High Energy Physics - Phenomenology · Physics 2012-12-10 J. O. Eeg

$\bar B \to D\pi$, $D^*\pi$, $J/\psi\bar K$ and $J/\psi\pi$ decays are studied. Their amplitude is given by a sum of factorized and non-factorizable ones. The latter which is estimated by using a hard pion approximation is rather small in…

High Energy Physics - Phenomenology · Physics 2009-10-30 K. Terasaki

While the factorization assumption works well for many two-body nonleptonic $B$ meson decay modes, the recent measurement of $\bar B\to D^{(*)0}M^0$ with $M=\pi$, $\rho$ and $\omega$ shows large deviation from this assumption. We analyze…

High Energy Physics - Phenomenology · Physics 2009-11-10 Yong-Yeon Keum , T. Kurimoto , H. -n. Li , C. -D. Lu , A. I. Sanda

The first observation of the color-suppressed decay mode \bar{B}^0_d --> D^(*)0 \pi^0 by the Belle and CLEO Collaborations makes a quantitative analysis of the isospin relations for the amplitudes of B --> D^(*)\pi possible. The strong…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zhi-zhong Xing

Working within the framework of the QCD light cone sum rules (LCSR), we compute and discuss the nonfactorizable higher twist effect in $\bar{B}^0\to D^{*0}\pi^0$ to make an all-around examination of its role in the charmed color-suppressed…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zuo-Hong Li , Zhong-Qian Su , Jian-Ying Cui

We prove a factorization theorem in QCD for the color suppressed decays B0-> D0 M0 and B0-> D*0 M0 where M is a light meson. Both the color-suppressed and W-exchange/annihilation amplitudes contribute at lowest order in LambdaQCD/Q where…

High Energy Physics - Phenomenology · Physics 2009-09-29 Sonny Mantry , Dan Pirjol , Iain W. Stewart

We point out that the decay modes B^0 --> D_s^+ D_s^- and B_s^0 --> D^+ D^- have no factorized contribution. At quark level these dacays can only proceed through the annihilation mechanism, which in the factorized limit give zero amplitude…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. O. Eeg , S. Fajfer , A. Hiorth

We analyze the decay processes B \to DK, DK^*, D\pi, and D\rho in a model-independent way. Using the quark diagram approach, we determine the magnitudes of the relevant amplitudes and the relative strong phase shifts. In order to find the…

High Energy Physics - Phenomenology · Physics 2009-11-10 C. S. Kim , Sechul Oh , Chaehyun Yu

The recent measurements of the color-suppressed modes $\bar B^0\to D^{(*)0}\pi^0$ imply non-vanishing relative final-state interaction (FSI) phases among various $\bar B\to D\pi$ decay amplitudes. Depending on whether or not FSIs are…

High Energy Physics - Phenomenology · Physics 2009-11-07 Hai-Yang Cheng

Nonfactorizable contributions to exclusive two-body nonleptonic weak decays of heavy mesons arising from color octet currents, characterized by the parameter $r_2$, are extracted from the data. It is found that $r_2$ is equal to $\sim…

High Energy Physics - Phenomenology · Physics 2009-10-28 Hai-Yang Cheng

The decay mode D^0 -> K^0 \bar{K^0} has no factorizable contribution. We calculate the nonfactorizable chiral loop contributions of order O(p^3)and then we use a heavy-light type chiral quark model to calculate nonfactorizable tree level…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. 0. Eeg , S. Fajfer , J. Zupan

We investigate to what extent the experimental information on $B \to \pi\pi$ branching fractions and CP asymmetries can be used to better understand the QCD dynamics in these decays. For this purpose we decompose the independent isospin…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thorsten Feldmann , Tobias Hurth

We investigate the possibility of testing factorization hypothesis in non-leptonic exclusive decays of B-meson. In particular, we considered the non factorizable \bar{B^0} -> D^{(*)+} D_s^{(*)-} modes and \bar{B^0} -> D^{(*)+} (\pi^-,…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. S. Kim , Y. Kwon , Jake Lee , W. Namgung

The various decay modes of the type $B \to \gamma D^* $ are dynamically different. In general there are factorizable contributions, and there are pole diagrams and pseudoscalar exchange contributions at meson level. The purpose of this…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. O. Eeg J. A. Macdonald Sørensen

We point out that the decay mode D^0 -> K^0 \bar{K^0} has no factorizable contribution. In the chiral perturbation language, treating D^0 as heavy, the O(p) contribution is zero. We calculate the nonfactorizable chiral loop contributions of…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. O. Eeg , S. Fajfer , J. Zupan
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