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Related papers: Weak phase alpha from B^0-> a_1^{+-}(1260) pi^{-+}

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The influence of strong and electroweak penguin amplitudes in $B/ \bar B \rightarrow \pi^+\pi^-$ is investigated in connection with the determination of the unitarity triangle angle $\alpha$ of the CKM matrix. A relation between the…

High Energy Physics - Phenomenology · Physics 2009-09-25 G. Kramer , W. Palmer , Y. L. Wu

A method is described which, under the assumption of SU(3) symmetry, allows one to determine the angle gamma=Arg(Vub^*) of the unitarity triangle from time-independent measurements of the branching ratios for the decays B^+ -> pi^0 K^+ and…

High Energy Physics - Phenomenology · Physics 2010-11-23 Matthias Neubert , Jonathan L. Rosner

We suggest two methods (based on flavor SU(3) symmetry) to determine the CKM angle $\gamma$ using the decays $B_d$, $B^+ \to K \eta (\eta')$ and $B_s \to \pi \eta (\eta')$, respectively. Rescattering effects are partly included -- we…

High Energy Physics - Phenomenology · Physics 2010-11-23 K. Agashe , N. G. Deshpande

We discuss implications of recent experimental data for B decays into two pseudoscalar mesons, with emphasis on those with $\eta$ and $\eta'$ in the final states. Applying a U-spin argument, we show that tree and penguin amplitudes, both in…

High Energy Physics - Phenomenology · Physics 2014-11-17 Cheng-Wei Chiang , Michael Gronau , Jonathan L. Rosner

Electroweak penguin (EWP) amplitudes are studied model-independently in $B$ meson decays to charmless final states consisting of a vector meson ($V$) and a pseudoscalar meson ($P$). A set of SU(3) relations is derived between EWP…

High Energy Physics - Phenomenology · Physics 2009-10-31 Michael Gronau

Penguin contributions, being not negligible in general, can hide the information on the CKM angle alpha coming from the measurement of the time-dependent B0(t) -> pi+pi- CP-asymmetry. Nevertheless, we show that this information can be…

High Energy Physics - Phenomenology · Physics 2016-08-25 Jérôme Charles

We present a method to measure the CKM phase $\alpha$ and the tree and penguin (strong and electroweak) amplitudes in $B \rightarrow \pi \pi$ decays, based on isospin consideration and the weak assumption that all tree amplitudes have a…

High Energy Physics - Phenomenology · Physics 2010-11-23 N. G. Deshpande , Xiao-Gang He , Sechul Oh

Isospin and flavor SU(3) set stringent bounds on penguin pollution in $B^0(t)\to \rho^+\rho^-$, providing a theoretically precise determination of $\alpha\equiv \phi_2 $, $\alpha = (91\pm 7_{\rm exp}\pm 3_{\rm th})^\circ$. Isospin breaking…

High Energy Physics - Phenomenology · Physics 2011-03-23 Michael Gronau

The decays of $B$ mesons to a pair of charmless pseudoscalar ($P$) mesons are analyzed within a framework of flavor SU(3). Symmetry breaking is taken into account in tree ($T$) amplitudes through ratios of decay constants; exact SU(3) is…

High Energy Physics - Phenomenology · Physics 2014-11-17 Cheng-Wei Chiang , Michael Gronau , Jonathan L. Rosner , Denis A. Suprun

Phases of elements of the Cabibbo-Kobayashi-Maskawa (CKM) matrix can be obtained using decays of $B$ mesons to $\pi^+ \pi^-$, $\pi^\pm K^\mp$, and $\pi^+ K^0$ or $\pi^- \overline{K}^0$. For $B^0~{\rm or}~ \overline{B}^0 \to \pi^+ \pi^-$,…

High Energy Physics - Phenomenology · Physics 2010-11-23 Amol S. Dighe , Michael Gronau , Jonathan L. Rosner

Though QCD Factorization(QCDF) could produce sufficiently large $B\to K\pi$ branching ratios close to experiments, the predicted direct CP asymmetry in ${\bar B}^{0}\to K^{+}\pi^{-}$ decay is however still quite below experiment, even with…

High Energy Physics - Phenomenology · Physics 2009-10-19 T. N. Pham

A new way of determining the phases of weak amplitudes in charged $B$ decays based on SU(3) symmetry is proposed. The CP violating phase $\gamma$ can now be determined without the previous difficulty associated with electroweak penguins.

High Energy Physics - Phenomenology · Physics 2009-10-28 N. G. Deshpande , Xiao-Gang He

The ratio of partial decay rates for charged and neutral $B$ mesons to $K \pi$ final states provides information on the weak phase $\gamma \equiv {\rm Arg} (V_{ub}^*)$ when augmented with information on the CP-violating asymmetry in the…

High Energy Physics - Phenomenology · Physics 2012-08-27 Michael Gronau , and Jonathan L. Rosner

In the presence of penguin contributions, the indirect CP asymmetry in B^0(t) --> pi^+ pi^- measures sin 2alpha_{eff}, where alpha_{eff} deviates from the true value of the CKM phase alpha by an amount theta, i.e. alpha_{eff} = alpha +…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. K. Giri , R. Mohanta

In charmless nonleptonic B decays to \pi\pi or \rho\rho, the "color allowed" and "color suppressed" tree amplitudes can be studied in a systematic expansion in \alphas(mb) and \Lambda/mb. At leading order in this expansion their relative…

High Energy Physics - Phenomenology · Physics 2014-11-18 Yuval Grossman , Andreas Hocker , Zoltan Ligeti , Dan Pirjol

The 2.5 sigma discrepancy between theory and experiment observed in the difference Delta ACP = ACP(B- --> pi0 K-) - ACP(Bb0 --> pi+ K-) can be explained by a new electroweak (EW) penguin amplitude. Motivated by this result, we have analyzed…

High Energy Physics - Phenomenology · Physics 2010-12-17 Lars Hofer , Dominik Scherer , Leonardo Vernazza

Current data of charmless B meson decays to two pseudoscalar mesons (PP) and one vector and one pseudoscalar mesons (VP) are analyzed within the framework of flavor SU(3) symmetry, a working principle that we have tested by allowing…

High Energy Physics - Phenomenology · Physics 2015-06-22 Hai-Yang Cheng , Cheng-Wei Chiang , An-Li Kuo

Recently Ciuchini, Pierini and Silvestrini proposed a method for constraining CKM parameters in B->K pi pi and B_s-> K pi pi through phase measurements of amplitudes involving I=3/2 K*pi final states. We show that complementary information…

High Energy Physics - Phenomenology · Physics 2008-11-26 Michael Gronau , Dan Pirjol , Amarjit Soni , Jure Zupan

The unitarity of the Cabibbo-Kobayashi-Maskawa (CKM) matrix has been well established by both direct and indirect measurements without any evidence of discrepancy. The CKM weak phase $\alpha$ is directly measured using an isospin analysis…

High Energy Physics - Phenomenology · Physics 2020-04-15 Abinash Kumar Nayak , Rahul Sinha , Anirban Karan , Benjamin Grinstein

Based on the most recent data in charmless B decays including the very recently reported large direct CP violations, it is shown that the weak phase gamma can well be extracted without two-fold ambiguity even only from two decay modes…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yue-Liang Wu , Yu-Feng Zhou