1977
DOI: 10.1070/pu1977v020n09abeh005458
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Backward scattering of pions by nucleons

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Cited by 18 publications
(18 citation statements)
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“…where µ −1 = (0.9±0.2) fm = (4.56±1.01) GeV −1 , √ σ = 400 MeV and α = 0.21±0.01. We obtain bottomonium-like spectra by diagonalizing the Hamiltonian (3) with the potential (4). The number of bound states in the model is finite, and it decreases with increased screening µ.…”
Section: Heavy Quarkonia Modelmentioning
confidence: 99%
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“…where µ −1 = (0.9±0.2) fm = (4.56±1.01) GeV −1 , √ σ = 400 MeV and α = 0.21±0.01. We obtain bottomonium-like spectra by diagonalizing the Hamiltonian (3) with the potential (4). The number of bound states in the model is finite, and it decreases with increased screening µ.…”
Section: Heavy Quarkonia Modelmentioning
confidence: 99%
“…[39] for a similar form of the ρ trajectory from the analysis of πN charge-exchange scattering data. 4 Earlier analysis of ref. [40] found T ρ = 2.4 ± 0.4 GeV.…”
Section: Vector Mesonsmentioning
confidence: 99%
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“…Kaidalov has shown that the QGS model describes a large variety of experimental data on the exclusive and inclusive hadronic reactions at high energy very well [5,6,15]. However, due to the duality property of scattering amplitudes [13], this approach can also work in the intermediate-energy region [6].…”
Section: Introductionmentioning
confidence: 99%
“…In practice, since for each hadronic Regge trajectories at most only three lowest lying states are known[6], the observed Regge trajectories can be well approximated by the well-known linear form. Nevertheless, some experiments indicate a nonzero curvature, for example, the nucleon trajectory[7],…”
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confidence: 99%