The quantum mechanical counterpart of the famous Stoner-Wohlfarth model -an easy-axis magnet in a tilted magnetic field -is studied theoretically and through simulations, as a function of the spin-size S in a sweeping longitudinal field. Beyond the classical Stoner-Wohlfarth transition, the sweeping field-induced adiabatic change of states slows down as S increases, leading to a dynamical quantum phase transition. This result is described as a critical phenomenon associated with Landau-Zener tunneling gaps at metastable quasi-avoided crossings. Furthermore, a beating of the magnetization is discovered after the Stoner-Wohlfarth transition. The period of the beating, obtained analytically, arises from a new type of quantum phase factor.PACS numbers: 75.10. Jm, 75.45.+j, 75.50.Xx, 75.60.Jk We study the reversal of a uniaxial magnet of spin S submitted to a fixed transverse field and a longitudinal sweeping field. This model had been studied for single-molecule magnets with moderate spins S=10, in which the Landau-Zener (LZ) transition plays an important role [1][2][3][4][5]. Some years ago, the parent model of an Ising spin-chain with ferromagnetic interactions and same longitudinal and transverse fields showed a quantum spinodal phase transition where a size (spin-chain length)-independent magnetization decay was observed and attributed to independent single-spin reversals [6].In this letter, we study the quantum aspects of the Stoner-Wohlfarth (SW) transition, and more particularly the relations between the quantum dynamics and classical irreversibility of a large quantum spin S in a uniaxial anisotropy broken by a transverse field, and submitted to a sweeping longitudinal field at zero Kelvin. In the S → ∞ limit, the spin becomes classical and exhibits the so-called SW transition [7]. This is a magnetization jump from a metastable to a stable state when the field, applied in the opposite hemisphere, reaches a critical value. We obtained two main results: (i) the classical SW transition (infinite spin) is given by a critical phenomenon of the spinodal type in the limit of a large spin S in the quantum regime, and (ii) when the sweeping field exceeds the SW point, magnetization beatings of quantum mechanical origin, which are analyzed and attributed to a new type of quantum phase factor, appear.In order to catch the properties of our model properly in the S → ∞ limit, we introduce the normalized quantum spin operators with a modified commutation relations:The corresponding SW Hamiltonian, with uniaxial anisotropy, transverse field (fixed) and longitudinal field (sweeping at the time-rate c), is written as [8]:In Eq. (2) and hereafter, we set gµ B = 1 and = 1. The time evolution of the normalized quantum spin operators, given byis obtained numerically by the standard Runge-Kutta method.The corresponding time-evolution of the usual (classical) SW model comes from the torque equation dm/dt = −m × H eff with the effective field H eff = −∂E SW /∂m = (H x , 0, 2Dm z + H z ). The energy of the SW model, E SW , is of ...