The spinel M nV2O4 is a two-sublattice ferrimagnet, with site A occupied by the M n 2+ ion and site B by the V 3+ ion. The magnon of the system, the transversal fluctuation of the total magnetization, is a complicated mixture of the sublattice A and B transversal magnetic fluctuations. As a result, the magnons' fluctuations suppress in a different way the manganese and vanadium magnetic orders and one obtains two phases. At low temperature (0, T * ) the magnetic orders of the M n and V ions contribute to the magnetization of the system, while at the high temperature (T * , TN ), the vanadium magnetic order is suppressed by magnon fluctuations, and only the manganese ions have non-zero spontaneous magnetization. A modified spin-wave theory is developed to describe the two phases and to calculate the magnetization as a function of temperature. The anomalous M (T ) curve reproduces the experimentally obtained ZFC magnetization.PACS numbers: 75.50. Gg, 75.30.Ds, 75.60.Ej, This Letter is inspired from the experimental measurements of the ZFC magnetization of M nV 2 O 4 [1, 2, 3]. The profile of the experimental curve reproduces the anomalous magnetization curve predicted by L. Neel [4,5] for ferrimagnets with equal sublattice spins. This stimulates to model the manganese vanadate spinel in the spirit of the Neel's theory. By comparing and contrasting ZFC and FC magnetization one gains insight into a magnetism of the manganese vanadate oxide.The spinel M nV 2 O 4 is a two-sublattice ferrimagnet, with site A occupied by the M n 2+ ion, which is in the 3d 5 high-spin configuration with quenched orbital angular momentum, which can be regarded as a simple s = 5/2 spin. The B site is occupied by the V 3+ ion, which takes the 3d 2 high-spin configuration in the triply degenerate t 2g orbital, and has orbital degrees of freedom. The measurements show that the set in of the magnetic order is at Neel temperature T N = 56K [1], and that the magnetization has a maximum near T * = 50K. Below this temperature the magnetization sharply decreases and goes to zero when temperature approaches zero.We consider a system which obtains its magnetic properties from M n and V magnetic moments. It is shown that the true magnons in this system, which are the transversal fluctuations corresponding to the total magnetization, are complicated mixtures of the M n and V transversal fluctuations. The magnons interact with manganese and vanadium ions in a different way, and the magnons fluctuations suppress the M n and V ordered moments at different temperatures. As a result, the ferrimagnetic phase is divided into two phases: low temperature phase 0 < T < T * , where the magnetic orders of the M n and V ions contribute to the magnetization of the system, and high temperature phase (T * , T N ), where the vanadium magnetic order is suppressed by magnon fluctuations, and only the manganese ions have non-zero spontaneous magnetization. A modified spin-wave theory is developed to describe the two phases and to calculate the magnetization as a function ...