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We studied the effect of momentum space anisotropy on heavy quarkonium statesusing an extended magnetized effective fugacity quasiparticle model (EQPM).Both the real and imaginary part of the potential has been modified through thedielectric function by including the anisotropic parameter $\xi$. The real partof the medium modified potential becomes more attractive in the presence of theanisotropy and constant magnetic field. The binding energy of the 1S, 2S, and1P quarkonium states including anisotropy effects for both the oblate and theisotropic case were studied. We find that the binding energy of quarkoniumstates becomes stronger in the presence of anisotropy. However, the magneticfield is found to reduce the binding energy. The thermal width of thecharmonium and bottomonium 1S states have been studied at constant magneticfield eB = 0.3 GeV2 for isotropic and prolate cases. The effect of magneticfield on the mass spectra of the 1P state for the oblate case was alsoexamined. The dissociation temperature for the 1S, 2S, and 1P charmonium andbottomonium have been determined to be higher for the oblate case with respectto the isotropic case

Anisotropic behavior of S-wave and P-wave states of heavy quarkonia at finite magnetic field