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Related papers: QCD Corrections to Charmless $b \to s$ Processes

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We calculate the total and differential decay rates for the semi-inclusive nonleptonic decays $B\to D_s^{(*)} X_q$ ($q=c$ or $u$) under the factorization hypothesis. The initial bound state effect is treated using the light-cone expansion…

High Energy Physics - Phenomenology · Physics 2009-11-07 Changhao Jin

We give a more complete calculation of $b \to s\gamma $ decay in 2-Higgs doublet model, including leading log QCD corrections from $m_{top}$ to $M_W$ in addition to corrections from $M_{W}$ to $m_b$. The inclusive decay rate in the first…

High Energy Physics - Phenomenology · Physics 2009-10-28 Cai-Dian Lu

We calculate the ${\cal O}(\alpha_s^2 \beta_0 )$ corrections to the decay rate $b\rightarrow c\bar c s$. For reasonable values of $m_c/m_b$ this term is of the same order as both the one-loop and $\CO(\alpha_s^2 \log^2 m_W/m_b)$ corrections…

High Energy Physics - Phenomenology · Physics 2014-11-17 Ming Lu , Michael Luke , Martin J. Savage , Brian H. Smith

Some recent progress in China in the study of charmless B decays with QCD factorization is reviewed. Chirally enhanced power corrections and infrared divergence problem are stressed.

High Energy Physics - Phenomenology · Physics 2009-11-11 Dongsheng Du

The short distance QCD corrections to $b\to s\gamma \gamma$ are calculated in the leading logarithmic approximation. The equivalence of operator basis reduction for S-matrix elements by using the equations of motion or by proving a low…

High Energy Physics - Phenomenology · Physics 2009-10-30 Chia-Hung V. Chang , Guey-Lin Lin , York-Peng Yao

QCD corrections are evaluated to FCNC processes like $B \to X_s \nu \bar{\nu}$, $K \to \pi \nu \bar{\nu}$, $B \to l^+ l^-$ or $K_L \to \mu^+ \mu^-$, i.e. to processes mediated by effective operators containing neutrino currents or axial…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mikolaj Misiak , Joerg Urban

Within the framework of QCD factorization (QCDF), power corrections due to penguin annihilation can account for theobserved rates of penguin-dominated two-body decays of $B$ mesons and direct CP asymmetries $A_{CP}(K^-\pi^+)$,…

High Energy Physics - Phenomenology · Physics 2011-02-11 Hai-Yang Cheng , Chun-Khiang Chua

We present results on the NLO (alpha_s^2) spectator-scattering corrections to the topological penguin amplitudes for charmless hadronic two-body B-decays in QCD factorization. The corrections can be sizable for the colour-suppressed…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sebastian Jager

Using the factorization approach and considering the contributions of the current-current, QCD penguin and electroweak penguin operators at the leading approximation, the decay amplitudes and decay widths of $B_q\to D_q(D_q^*) P$ and…

High Energy Physics - Phenomenology · Physics 2010-02-01 K. Azizi , R. Khosravi , F. Falahati

A calculation of the leading isospin-breaking contributions to the B -> K^* gamma decay amplitudes based on the QCD factorization approach is presented. They arise at order Lambda/m_b in the heavy-quark expansion and are due to annihilation…

High Energy Physics - Phenomenology · Physics 2014-11-17 Alexander L. Kagan , Matthias Neubert

The next-to-leading order (NLO) quantum chromodynamics (QCD) corrections for $\chi_{cJ}(^3P_J^{[1]},^3S_1^{[8]})$, the P-wave charmoniums inclusive production at $B$ factories are calculated utilizing the non-relativistic QCD (NRQCD)…

High Energy Physics - Phenomenology · Physics 2015-06-03 Long-Bin Chen , Jun Jiang , Cong-Feng Qiao

We study the radiative charmless $B_{(s)}\to V(A)\gamma $ decays in perturbative QCD (pQCD) approach to the leading order in $\alpha_s$ (here $V$ and $A$ denotes vector mesons and two kinds of axial-vector mesons: $^3P_1$ and $^1P_1$…

High Energy Physics - Phenomenology · Physics 2007-11-08 Wei Wang , Run-Hui Li , Cai-Dian Lü

Exclusive semileptonic B decays to the lightest excited charmed mesons are investigated at order $\Lambda_{QCD}/m_Q$ in the heavy quark effective theory. At zero recoil, $\Lambda_{QCD}/m_Q$ corrections to the matrix elements of the weak…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zoltan Ligeti

Two-body charmless nonleptonic decays of the B_s meson are studied within the framework of generalized factorization in which factorization is applied to the tree level matrix elements while the effective Wilson coefficients are $\mu$ and…

High Energy Physics - Phenomenology · Physics 2016-08-25 Yaw-Hwang Chen , Hai-Yang Cheng , B. Tseng

We calculate the leading nonperturbative contributions to the effective Wilson coefficient of the four-fermion operators arising from the QCD penguin, and we demonstrate how the usual perturbative one loop contribution is augmented by…

High Energy Physics - Phenomenology · Physics 2016-09-06 Mohammad R. Ahmady , Victor Elias

Theoretical predictions for B decay rates are rewritten in terms of the Upsilon(1S) meson mass instead of the b quark mass, using a modified perturbation expansion. The theoretical consistency of this expansion is shown both at low and high…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andre H. Hoang , Zoltan Ligeti , Aneesh V. Manohar

We calculate the complete ${\cal O}(\alpha_s)$ corrections to the quark decay $b\to ccs$ taking full account of the quark masses, but neglecting penguin contributions. For a c to the b quark mass ratio $m_c/m_b= 0.3$ and a strange quark…

High Energy Physics - Phenomenology · Physics 2016-09-01 E. Bagan , Patricia Ball , B. Fiol , P. Gosdzinsky

We provide a systematic study of charmless $B_s \to PP, PV, VV$ decays ($P$ and $V$ denote pseudoscalar and vector mesons, respectively) based on an approximate six-quark operator effective Hamiltonian from QCD. The calculation of the…

High Energy Physics - Phenomenology · Physics 2015-05-28 Fang Su , Yue-Liang Wu , Ci Zhuang , Yi-Bo Yang

We study the charmless decays $B\to K_h\eta$ and $B\to K_h\eta'$ within the framework of QCD factorization (QCDF) for $K_h= K,K^*,K_0^*(1430)$ and naive factorization for $K_h=K_2^*(1430)$. There are three distinct types of penguin…

High Energy Physics - Phenomenology · Physics 2014-11-21 Hai-Yang Cheng , Chun-Khiang Chua

Using the QCD sum rules approach and the complete leading--logarithmic short--distance coefficients determining the penguin--amplitude, we obtain $B(B\to K^*\gamma) = (6.8\pm 2.4)\cdot 10^{-5}$ for top--quark masses in the range (150--200)…

High Energy Physics - Phenomenology · Physics 2007-05-23 Patricia Ball