We study the de Haas-van Alphen (dHvA) oscillations in the two-dimensional compensated metal with overtilted Dirac cones near the Lifshitz transition. We employ the tight-binding model of α-(BEDT-TTF)2I3, in which the massless Dirac fermions are realized. When a uniaxial pressure (P) along the y-axis is applied above P 0.2 kbar in α-(BEDT-TTF)2I3, one electron pocket, which encloses the overtilted Dirac points, is changed to two electron pockets, i.e., Lifshitz transition happens, while a hole pocket does not change a topology. We show that the Fourier components corresponding to the 3/2 and 5/2 areas of the hole pocket are anomalously enhanced in the region of pressure where the Lifshitz transition occurs. This phenomenon will be observed in the twodimensional overtilted Dirac fermions near the Lifshitz transition.