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Related papers: Charmonium decays: J/psi --> e+e- and eta_c --> ga…

200 papers

For the vertex corrections to the partial decay rate $\Gamma(Z \to b\bar{b})$ involving the top quark only the leading terms of order $\alpha\alpha_s$ in the $1/M_t$ expansion are known. In this work we compute the missing next-to-leading…

High Energy Physics - Phenomenology · Physics 2009-10-30 R. Harlander , T. Seidensticker , M. Steinhauser

In this work, we study the radiative decay of heavy quarkonium states by using the effective Lagrangian approach. Firstly, we construct the spin-breaking terms in the effective Lagrangian for the $nP\leftrightarrow mS$ transitions and…

High Energy Physics - Phenomenology · Physics 2012-02-23 Zhi-Guo He

The decay psi(2S) --> eta J/psi is used to measure, for the first time, all prominent eta-meson branching fractions with the same experiment in the same dataset, thereby providing a consistent treatment of systematics across branching…

High Energy Physics - Experiment · Physics 2010-04-08 A. Lopez , CLEO Collaboration

Using data collected with the CLEO detector operating at the CESR e+e- collider at sqrt s = 3.97-4.26 GeV, we investigate 15 charmonium decay modes of the psi(4040), psi(4160), and Y(4260) resonances. We confirm, at 11$\sigma$ significance,…

High Energy Physics - Experiment · Physics 2010-04-08 T. E. Coan

I compute the leading color-octet contributions to the process $\gamma + p \to J/\psi + \gamma (+ X)$ within the non-relativistic QCD (NRQCD) factorization formalism. In the color-singlet model, $J/\psi + \gamma$ can only be produced when…

High Energy Physics - Phenomenology · Physics 2014-11-17 Thomas Mehen

The low $Q^2$ slopes of the the transition form factors provide a unique method to measure the sizes of the neutral pseudo-scalar mesons, since they do not have electromagnetic form factors. From the slope one obtains the "axial transition…

Nuclear Experiment · Physics 2015-11-23 A. M. Bernstein

The charmonium system provides an opportunity to explore a wide variety of topics in hadronic physics. Studies of the properties of and transitions among cc-bar states yield insight into relativistic and non-perturbative QCD effects. At the…

High Energy Physics - Experiment · Physics 2008-01-08 M. R. Shepherd

The inclusive light hadronic decays of 1D_2 heavy quarkonia are studied within the framework of NRQCD at the leading order in $v$ and up to the order of $\alpha_s^3$. With one-loop QCD corrections, the infrared divergences and Coulomb…

High Energy Physics - Phenomenology · Physics 2009-09-02 Ying Fan , Zhi-Guo He , Yan-Qing Ma , Kuang-Ta Chao

We present a new, simplified analysis of the low-energy electron-positron interaction, and use the resulting effective theory to calculate the binding effects that contribute to the decay rate, Gamma, of orthopositronium, through…

High Energy Physics - Phenomenology · Physics 2009-12-30 Richard J. Hill , G. Peter Lepage

The $W$-exchange process $B_{s}$ ${\to}$ ${\eta}_{c}(J/{\psi})D$ is studied with the perturbative QCD approach. Three kinds of wave functions for $B_{s}$ meson and two forms of wave functions for charmonium are considered. It is estimated…

High Energy Physics - Phenomenology · Physics 2015-06-15 Junfeng Sun , Zhengjun Xiong , Yueling Yang , Gongru Lu

The coupling constant of rho --> eta gamma decay is calculated in the framework of light cone QCD sum rules. A comparison of our prediction on the coupling constant with the result obtained from analysis of the experimental data is…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. M. Aliev , I. Kanik , A. Ozpineci

Mass spectrum of charmonium is computed in the framework of potential non-relativistic quantum chromodynamics. \textit{O}$(1/m)$ and \textit{O}$(1/m^2)$ relativistic corrections to the Cornell potential and spin-dependent potential have…

High Energy Physics - Phenomenology · Physics 2020-10-29 Raghav Chaturvedi , Ajay Kumar Rai

In heavy quarkonium production, the measured ratio $R_{c \bar c}=\sigma[J/\psi+ c\bar c + X]/\sigma[J/\psi +X]$ at B factories is much larger than existing theoretical predictions. To clarify this discrepancy, in nonrelativistic QCD (NRQCD)…

High Energy Physics - Phenomenology · Physics 2009-06-19 Yan-Qing Ma , Yu-Jie Zhang , Kuang-Ta Chao

Combining our results for various O(alpha_s^2) corrections to the weak radiative B-meson decay, we are able to present the first estimate of the branching ratio at the next-to-next-to-leading order in QCD. We find BR(B -> X_s gamma) = (3.15…

QCD corrections to all the allowed decays of superheavy groundstate quarkonia into electroweak gauge and Higgs bosons are presented. For quick estimates, approximations that reproduce the exact results within less than at worst two percent…

High Energy Physics - Phenomenology · Physics 2011-07-19 J. H. Kühn , M. Peter

After discussing the intrinsic ambiguity in determining the light quark mass ratio $m_u/m_d$, we reexamine the recent proposal that this ambiguity can be resolved by applying the QCD multipole expansion for the heavy quarkonium decays. It…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kiwoon Choi

The $O(\alpha)$ corrections to $\gamma\gamma --> f \bar f$ in the Standard Model are calculated for arbitrary, light fermions $f$. The relevant analytical results are listed in a form that is appropriate for practical applications, and…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Denner , S. Dittmaier

In the precedent paper of the authors (hep-ph/0510410), the $b\bar b$ states were treated in the framework of the spectral integral equation, together with simultaneous calculations of radiative decays of the considered bottomonia. In the…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. V. Anisovich , L. G. Dakhno , M. A. Matveev , V. A. Nikonov , A. V. Sarantsev

The decay rates for the exclusive B decays $B \rightarrow K \eta_c $ and $B \rightarrow K^* \eta_c$ are calculated in the context of the heavy quark effective theory. We obtain $\Gamma (B \rightarrow K \eta_c )/\Gamma (B\rightarrow K\psi…

High Energy Physics - Phenomenology · Physics 2009-10-28 Mohammad R. Ahmady , Roberto R. Mendel

In decays of the $Z^0$, the dominant mechanism for the direct production of charmonium states is the decay of the $Z^0$ into a charm quark or antiquark followed by its fragmentation into the charmonium state. We calculate the fragmentation…

High Energy Physics - Phenomenology · Physics 2014-11-17 Eric Braaten , Kingman Cheung , Tzu Chiang Yuan