Abstract

We present the results of quenched charmonium spectrum for S- and P-states, obtained by a relativistic heavy quark method on anisotropic lattices. Simulations are carried out using the standard plaquette gauge action and a meanfield-improved clover quark action at at−1=3a_t^{-1} = 3--6 GeV with the renormalized anisotropy fixed to ξ≡as/at=3ξ\equiv a_s/a_t =3. We study the scaling of our fine and hyperfine mass splittings, and compare with previous results.

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