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Related papers: The $\sqrt{m\Lambda_{QCD}$ scale in heavy quarkoni…

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We argue that consistency of the combined heavy quark and chiral effective lagrangian requires the QCD scale which multiplies $1/M$ in the heavy quark expansion to be the chiral symmetry breaking scale, $\Lambda_{CSB}$, rather than the QCD…

High Energy Physics - Phenomenology · Physics 2009-09-15 Lisa Randall , Eric Sather

A rigorous QCD analysis of the inclusive annihilation decay rates of heavy quarkonium states is presented. The effective-field-theory framework of nonrelativistic QCD is used to separate the short-distance scale of annihilation, which is…

High Energy Physics - Phenomenology · Physics 2014-11-17 Geoffrey T. Bodwin , Eric Braaten , G. Peter Lepage

We derive the imaginary part of the potential NRQCD Hamiltonian up to order 1/m^4, when the typical momentum transfer between the heavy quarks is of the order of Lambda_{QCD} or greater, and the binding energy E much smaller than…

High Energy Physics - Phenomenology · Physics 2009-11-07 Nora Brambilla , Dolors Eiras , Antonio Pineda , Joan Soto , Antonio Vairo

The decay widths of S-wave quarkonia ($\etc,\etb\to \gg{~~and~~} \J,\U\to\ee$) are calculated on the basis of a quasipotential approach. The nontrivial dependence on relative quark motion of decay amplitude is taken into consideration via…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. P. Martynenko , V. A. Saleev

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

We analyze the end-point region of the photon spectrum in semi-inclusive radiative decays of very heavy quarkonium (m alpha_s^2 >> Lambda_QCD). We discuss the interplay of the scales arising in the Soft-Collinear Effective Theory, m,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Xavier Garcia i Tormo , Joan Soto

We modify the calculation of quarkonium masses using the radial WKB and Pekeris-type approximations for the case of three-dimensional, rotationally invariant non-commutative space. We obtain corrections to the charmonium…

High Energy Physics - Phenomenology · Physics 2022-11-17 Benedek Bukor , Juraj Tekel

The leading nonperturbative effects to the fine and hyperfine splitting were calculated some time ago. Recently, they have been used in order to obtain realistic numerical results for the lower levels in bottomonium systems. We point out…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. Pineda

In the framework of a specific scheme of the QCD sum rules for $S$-wave levels of the heavy quarkonium, one derives an expression, relating the energetic density of quarkonium states and universal characteristics in the heavy quarkonium…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. V. Kiselev

In the framework of a specific scheme of the QCD sum rules for $S$-wave levels of the heavy quarkonium, one derives expressions, relating the leptonic constants, the energetic density of quarkonium states and universal characteristics in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kiselev V.

We review a number of results for the spectrum and inclusive decays of heavy quarkonium systems which can be derived from QCD under well controlled approximations. They essentially follow from the hierarchy of scales in these systems, which…

High Energy Physics - Phenomenology · Physics 2009-11-10 Joan Soto

In the NRQCD factorization for productions and decays of a quakonium the difference between the quarkonium mass and the twice of the heavy quark mass is neglected at the leading order of the small velocity expansion. The effect of this…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. P. Ma

The possible importance of threshold effects in heavy quarkonium spectroscopy is discussed. The starting point is the calculation of the spectrum of heavy quarkonium-like states with self-energy/threshold corrections. Two different…

High Energy Physics - Phenomenology · Physics 2020-08-26 J. Ferretti

We analyse the possible existence of non-perturbative contributions in heavy $\bar Q Q$ systems ($\bar Q$ and $Q$ need not have the same flavour) which cannot be expressed in terms of local condensates. Starting from QCD, with well defined…

High Energy Physics - Phenomenology · Physics 2016-09-01 A. Pineda , J. Soto

Using Nonrelativistic QCD on the lattice we studied the mass spectrum of quarkonium systems nonperturbatively for a range of the bar quark mass. We determined two products of the matrix elements involved in quarkonium decays and studied the…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. P. Ma , B. H. J. McKellar

Recent calculations of heavy quark cross sections near threshold at next-to-next-to-leading order have found second-order corrections as large as first-order ones. We analyse long-distance contributions to the heavy quark potential in…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Beneke

In this talk I review the calculation of the third order corrections to the heavy quarkonium spectrum in the nonrelativistic effective theory framework and its application to the phenomenology of top quark threshold production.

High Energy Physics - Phenomenology · Physics 2009-11-07 A. A. Penin

We briefly summarize some results obtained by potential NRQCD in the non perturbative regime: 1) a systematic procedure to obtain the heavy quarkonium potential in the 1/m expansion (with explicit expressions up to O(1/m^2) in terms of…

High Energy Physics - Phenomenology · Physics 2009-11-07 Antonio Pineda

In this contribution, we discuss the possible importance of continuum-coupling (or threshold) effects in heavy quarkonium spectroscopy. Our calculations are carried out in a coupled-channel model, where meson-meson higher Fock (or…

High Energy Physics - Phenomenology · Physics 2019-10-02 J. Ferretti

We obtain the Potential NRQCD Lagrangian relevant for S-wave states with next-next-to-next-to-leading logarithmic (NNNLL) accuracy. We compute the heavy quarkonium mass of spin-averaged $l= 0$ (angular momentum) states, with otherwise…

High Energy Physics - Phenomenology · Physics 2019-01-02 C. Anzai , D. Moreno , A. Pineda
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