-IntroductionThe exotic physical properties of mixed valence manganese oxides, known as manganites, have been fascinating and puzzling the scientific community for the last two decades [1]. The most striking phenomena are the colossal magnetoresistance, charge and orbital ordered states, and the coexistence at different length scales of ferromagnetic (FM) metallic and charge ordered antiferromagnetic (CO-AFM) insulating domains. The latter, known as phase separation, is currently viewed as an intrinsic feature of several strongly correlated electron systems [2], such as superconductors [3], multi-ferroics [4], and magnetocaloric materials [5].Intrinsic disorder and the coexistence of energetically near degenerate phases are key factors to understand this effect [2,6].Metamagnetic transitions, observed in measurements of isothermal magnetization versus magnetic field, M vs. H, are common in manganites [7,8]. The origin of these effects are caused by the field induced transformation of the metastable CO-AFM state at low fields to a homogeneous ferromagnet at high fields. In manganites both phases coexist in low magnetic fields, and the broad metamagnetic transitions observed, are the result of an increasing field dependent fraction of the ferromagnetic phase within the phase-separated material. But in addition, measurements at very low temperatures (< 4 K) have revealed a surprising and beautiful effect: the observation of a discontinuous metamagnetic transition at a critical magnetic field [9,10,11]. This phenomenon, referred to as ultrasharp magnetization jumps, avalanche-like or abrupt metamagnetic transition, has puzzled the scientific community since it was first reported [12]. Similar effects were later found on a variety of different systems [13,14], including spin ice [15] and iron-rich intermetallic compounds [16], and it is now established that these discontinuous transitions are not a peculiarity restricted to manganese oxides. More generally, the study of magnetic avalanches in manganites helps the understanding of phase transitions of mixed first order and continuous character, and from the study of this phenomena other fields can benefit, such as fracture theory in disordered media [17].Several aspects of these discontinuous transition were previously studied. It has been established that the critical field of the avalanche-like transition depends strongly on the magnetic field sweep rate [18,19,20,21]. This is a consequence of relaxation effects, which play a major role in the avalanche process, and yield the observation of a spontaneous transition 3 [10,11,13] at a fixed magnetic field. The main question was, and to some extent still is, what causes these discontinuous magnetization jumps? Initially, an interpretation was proposed within the framework of a martensitic transformation [19,22], associated with strain between the phase separated regions. However, various experimental findings rule out the martensitic scenario, such as the sharpness of the transition in inhomogeneous polycrystalline sam...