  We studied the effect of momentum space anisotropy on heavy quarkonium states
using an extended magnetized effective fugacity quasiparticle model (EQPM).
Both the real and imaginary part of the potential has been modified through the
dielectric function by including the anisotropic parameter $\xi$. The real part
of the medium modified potential becomes more attractive in the presence of the
anisotropy and constant magnetic field. The binding energy of the 1S, 2S, and
1P quarkonium states including anisotropy effects for both the oblate and the
isotropic case were studied. We find that the binding energy of quarkonium
states becomes stronger in the presence of anisotropy. However, the magnetic
field is found to reduce the binding energy. The thermal width of the
charmonium and bottomonium 1S states have been studied at constant magnetic
field eB = 0.3 GeV2 for isotropic and prolate cases. The effect of magnetic
field on the mass spectra of the 1P state for the oblate case was also
examined. The dissociation temperature for the 1S, 2S, and 1P charmonium and
bottomonium have been determined to be higher for the oblate case with respect
to the isotropic case
