We report controlled ignition of magnetization reversal avalanches by surface acoustic waves in a single crystal of Mn 12 acetate. Our data show that the speed of the avalanche exhibits maxima on the magnetic field at the tunneling resonances of Mn 12 . Combined with the evidence of magnetic deflagration in Mn 12 acetate [Y. Suzuki et al., Phys. Rev. Lett. 95, 147201 (2005)], this suggests a novel physical phenomenon: deflagration assisted by quantum tunneling. DOI: 10.1103/PhysRevLett.95.217205 PACS numbers: 75.50.Xx, 45.70.Ht Magnetic properties of Mn 12 acetate have been intensively studied after the magnetic bi-stability of this molecular cluster below 3.5 K was demonstrated [1]. The bistability is caused by a large spin of the cluster, S 10, and by strong uniaxial magnetic anisotropy that provides a 65 K energy barrier between spin-up and spin-down states. At low temperature a magnetized Mn 12 crystal exhibits two modes of magnetic relaxation. The first mode is a slow one. It manifests itself in a staircase hysteresis curve which is due to thermally assisted quantum tunneling of the magnetization [2]. The second relaxation mode, exhibited by sufficiently large crystals, is a much more rapid magnetization reversal that typically lasts less than 1 ms. It was initially studied by Paulsen and Park [3] and attributed to a thermal runaway or avalanche [see also Ref. [4]]. In the avalanche, the initial relaxation of the magnetization towards the direction of the field results in the release of heat that further accelerates the magnetic relaxation. Recent local magnetic measurements of Mn 12 crystals [5] have demonstrated that during an avalanche the magnetization reversal occurs inside a narrow interface that propagates through a crystal at a constant speed of a few meters per second. It has been argued that this process is analogous to the propagation of a flame front (deflagration) through a flammable chemical substance. The conventional theory of deflagration, in the first approximation, yields the following expression for the velocity of the flame front [5-7]:Here U, 0 , and T f are the energy barrier, the attempt frequency, and the temperature of the ''flame'' in the expression 0 expU=k B T f for the ''chemical reaction'' time, and is thermal diffusivity. In the case of Mn 12 , 10 ÿ5 m 2 =s, 0 10 ÿ7 s, and the field dependence of the energy barrier, UH, is well known.In a flammable chemical substance the potential barrier is a constant determined by the nature of the chemical reaction that transforms a metastable chemical into a stable chemical (e.g., a mixture of hydrogen and oxygen transforms into water). On the contrary, in molecular magnets the energy barrier, as well as the released energy, can be controlled by the magnetic field. At certain values of the magnetic field the spin levels on the two sides of the energy barrier come to resonance and thermally assisted quantum spin tunneling under the barrier takes place; see Fig. 1. Therefore, the effect of the tunneling is roughly equivalent to cutting ...