Presented are magnetization measurements on a crystal of Cr7Ni antiferromagnetic rings. Irradiation with microwaves at frequencies between 1 and 10 GHz leads to observation of very narrow resonant photon absorption lines which are mainly broadened by hyperfin interactions. A two-pulse hole burning technique allowed us to estimate the characteristic energy diffusion time.PACS numbers: 75.50. Xx, 75.60.Jk, 75.75.+a, Magnetic molecules are currently considered among the most promising electron spin based quantum systems for the storing and processing of quantum information [1]. For this purpose, ferromagnetic [2] and antiferromagnetic [3,4] systems have attracted an increasing interest [5,6,7]. In the latter case the quantum hardware is thought of as a collection of coupled molecules, each corresponding to a different qubit. The main advantages would arise from the fact that they are extremely small and almost identical, allowing to obtain, in a single measurement, statistical averages of a larger number of qubits. The magnetic properties can be modelled with an outstanding degree of accuracy. And most importantly, the desired physical properties can be engineered chemically.Recently, the suitability of Cr-based antiferromagnetic molecular rings for the qubit implementation has been proposed [5,6,7]. The substitution of one metal ion in a Cr-based molecular ring with dominant antiferromagnetic couplings allowed to engineer its level structure and ground-state degeneracy [8,9]. A Cr 7 Ni molecular ring was characterized by means of low-temperature specificheat and torque-magnetometry measurements, thus determining the microscopic parameters of the corresponding spin Hamiltonian. The energy spectrum and the suppression of the leakage-inducing S-mixing render the Cr 7 Ni molecule a suitable candidate for the qubit implementation [6,7,10].In this paper we report the first micro-superconducting quantum interference device (micro-SQUID) [11] studies of the Cr 7 Ni molecular ring. Electron paramagnetic resonance (EPR) methods are combined with highsensitivity magnetization measurements. The magnetization detection could also be a Hall-probe magnetometer [12,13,14,15,16] The measurements were made in a dilution cryostat using a 20 µm sized single crystal of Cr 7 Ni. The magnetic probe was a micro-SQUID array [11,19] equipped with three coils allowing to apply a field in any direction and with sweep rates up to 10 T/s. The electromagnetic radiation was generated by a frequency synthesizer (Anritsu MG3694A) triggered with a nanosecond pulse generator. This setup allows to vary continuously the frequency from 0.1 Hz to 20 GHz, with pulse lengths form ∼1 ns to continuous radiation [20]. Using a 50 µm sized gold radio frequency (RF) loop, the RF radiation field was directed in a plane perpendicular to the applied static field µ 0 H. The microwave power of the generator could be varied from -80 to 20 dBm (10 −11 to 10 −1 W). The sample absorbes only a small fraction of the generator power. This fraction is however proportional t...