2018
DOI: 10.1140/epja/i2018-12595-1
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Beautiful mathematics for beauty-full and other multi-heavy hadronic systems

Abstract: In most non-perturbative methods in hadron physics the calculations are started with a correlation function in terms of some interpolating and transition currents in x-space. For simplicity, the calculations are then transformed to the momentum space by a Fourier transformation. To suppress the contributions of the higher states and continuum; and enhance the ground state contribution, Borel transformation as well as continuum subtraction are applied by the help of quark-hadron duality assumption. In the prese… Show more

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Cited by 25 publications
(21 citation statements)
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“…The subtraction procedures for different systems are described in Ref. [44] in details. When the masses of the initial and final baryonic states are equal, as we stated previously, we set…”
Section: Qcd Sidementioning
confidence: 99%
“…The subtraction procedures for different systems are described in Ref. [44] in details. When the masses of the initial and final baryonic states are equal, as we stated previously, we set…”
Section: Qcd Sidementioning
confidence: 99%
“…There are several representations of the Bessel functions and it is shown in [43] that the cosine representation makes the calculations straightforward and more suitable for the Borel transformation. In this step, we perform the x-integration and use…”
Section: Q Qmentioning
confidence: 99%
“…We hope that not only we will be able to identify the ground state doubly heavy baryons predicted by the quark model [37][38][39], but also will find more information on the resonances beyond the ground state particles. Heretofore, lattice QCD [40], Quark Spin Symmetry [41,42], QCD Sum Rules [29][30][31]43,44] are just some of the attempts that have been made to predict masses, residues, decay modes, lifetimes, strong coupling constants, and other properties of doubly heavy baryons.…”
Section: Introductionmentioning
confidence: 99%
“…Then equating these two representations of the correlator via dispersion relation and carrying out double Borel transformations on the -p 2 and -(p + q) 2 to eliminate the contributions of higher resonances and continuum (the details of Borel transformations can be found in Refs. [32,33]). As a result, we get the requested LCSR for the MM as The   QCD function is very lengthy and not illuminating, therefore the explicit expression of this function are not presented here.…”
Section: S X S X Tr S X S X Tr S X S X (9)mentioning
confidence: 99%