Abstract
The second order N-dimensional Schrödinger equation with Killingbeck
potential, namely V (r) = ar^2 + br -c/r ; a > 0 is examined via Laplace
transform approach.The stationary states are determined by good behavior of
eigenfunctions at the origin and at infinity. Energy eigenvalue equation has
been used to determine the mass spectra of heavy quarkonium system, specially
for lower dimension N = 3. The eigenfunctions are used to determine the radii
of the bound states.The present results suggest that the bound states 1P; 2S;
3S of (\Upsilon(bb),\psi(cc)) are more tightly bound than they are
supposed in non relativistic hadronic study.
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