Abstract. -Spin relaxation between the two lowest-lying spin-states has been studied in the S = 4 single molecule magnet Ni4 under steady state conditions of low amplitude and continuous microwave irradiation. The relaxation rate was determined as a function of temperature at two frequencies, 10 and 27.8 GHz, by simultaneously measuring the magnetization and the absorbed microwave power. A strong temperature dependence is observed below 1.5 K, which is not consistent with a direct single-spin-phonon relaxation process. The data instead suggest that the spin relaxation is dominated by a phonon bottleneck at low temperatures and occurs by an Orbach mechanism involving excited spin-levels at higher temperatures. Experimental results are compared with detailed calculations of the relaxation rate using the universal density matrix equation.Quantum tunneling of magnetization (QTM) [1,2] and quantum phase interference [3,4] have been intensively studied in single molecule magnets (SMMs). These materials have also been suggested as candidates for qubits in quantum processors [5] and for applications in molecular spintronics [6]. Quantum manipulation of the spin in such materials can be envisioned provided they have sufficiently long spin relaxation (T 1 ) and dephasing times (T 2 ). A first step has been the study of coherent QTM, in which the tunneling rates are faster than the rate of decoherence [7,8]. These studies provided a lower bound on T 2 of about 0.5 ns. In SMM crystals dipolar interactions may limit the dephasing time, making it necessary to work with dilute SMM ensembles [9-11] or even individual molecules. For instance, a recent study of dilute doped antiferromagnetic wheels demonstrated a phase relaxation time of several microseconds at 1.8 K [12].The phase relaxation rate Γ 2 = 1/T 2 is generally much greater than the energy relaxation rate Γ. For instance, an upper bound on T 2 of 50 ns was found in dilute Ni 4 solutions at 130 GHz and 5.5 K, where energy relaxation, rather than dipolar or hyperfine interactions, may be the limiting mechanism [10]. Interestingly, the relaxation rate Γ due to a direct spin-phonon process of a SMM embedded in an elastic medium can be derived without any unknown coupling constant [13,14]. Moreover, collective relaxation effects are expected in SMM single crystals, such as phonon superradiance [15].Direct measurements of the magnetization under pulse microwave (MW) irradiation enable study of spindynamics in SMM crystals [16][17][18][19]. In Fe 8 , long pulses (> 10 µs) of resonant MW radiation drive spins and phonons out of equilibrium, and heating effects or phonon bottleneck (PB) preclude the observation of fast dynamics [16,18]. However, using very short high power MW pulses, refs.[17] and [19] showed that these effects can be circumvented, enabling the observation of spin-dynamics on microsecond time scales. Ref. [17] explains the observed temperature dependence of the level lifetimes with direct spin-phonon coupling whereas ref. [19] concludes that a PB develops and p...