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J/ -Nucleon Scattering Length and In-Medium Mass Shift of J/ in QCD Sum Rule Analysis
Author(s) -
A. Hayashigaki
Publication year - 1999
Publication title -
progress of theoretical physics
Language(s) - English
Resource type - Journals
eISSN - 1347-4081
pISSN - 0033-068X
DOI - 10.1143/ptp.101.923
Subject(s) - physics , scattering , nucleon , sum rule in quantum mechanics , meson , scattering length , particle physics , quantum chromodynamics , scattering amplitude , omega , nuclear matter , amplitude , dimension (graph theory) , spin (aerodynamics) , nuclear physics , quantum mechanics , combinatorics , mathematics , thermodynamics
We calculate the spin-averaged $J/\psi$-nucleon scattering length$a_{J/\psi}$ by directly applying QCD sum rule to $J/\psi$-$N$ forwardscattering amplitude. Our result $a_{J/\psi} = - 0.10 \pm 0.02$ fm, predictsthe possibility of bound states with nuclei, though the force is weaker thanthat of the light vector mesons ($\rho,\omega,\phi$)-$N$ cases. Up todimension-4 gluonic operators, we evaluate the scattering length with twist-2contribution, which increases the absolute value of the scattering length about30%. If we apply $a_{J/\psi}$ to the effective mass of $J/\psi$ in nuclearmatter on the basis of the linear density approximation, it shows very slightdecrease ($4 \sim 7$ MeV) at normal matter density.Comment: 14 pages, latex, 2 figures included, uses epsf.st

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