We demonstrate that the spin of optically addressable point defects can be coherently driven with AC electric fields. Based on magnetic-dipole forbidden spin transitions, this scheme enables spatially confined spin control, the imaging of high-frequency electric fields, and the characterization of defect spin multiplicity. While we control defects in SiC, these methods apply to spin systems in many semiconductors, including the nitrogen-vacancy center in diamond. Electrically driven spin resonance offers a viable route towards scalable quantum control of electron spins in a dense array. PACS number(s): 42.50.Ex, 71.70.Ej, 76.30.Mi, Optically addressable paramagnetic defects have proven to be powerful systems for solid-state quantum control. Research into the nitrogen-vacancy (NV) center in diamond has been driven by applications in quantum information and nanoscale sensing [1][2][3][4][5][6][7]. More recently, intrinsic defects in SiC [8] have been shown to have similar properties to the NV center in diamond, including long coherence times that persist up to room temperature [9], a high degree of optical polarization [10], and spin-dependent photoluminescence [9][10][11][12][13][14][15]. The technological maturity of SiC growth and processing combined with defect emissions near telecom wavelengths make SiC defects particularly amenable to integration with electronic, optoelectronic, electromechanical, and photonic devices.An important challenge in defect spin physics is to selectively manipulate individual spins at the nanometer scale. Localized spin control is particularly important since the inter-spin separation required for strong dipolar coupling is on the order of tens of nanometers [16,17]. Since electric fields are readily confined on similar length scales [18], electrically driven spin resonance [19][20][21][22][23][24][25] could be used to address this challenge. In this letter, we show that resonant electric fields can coherently drive spin transitions in optically addressable defects.We use AC electric fields to drive Rabi oscillations across a magnetic-dipole forbidden spin transition (Δm s =±2) of the optically addressable electronic spin of the QL1 defect in semiinsulating 6H-SiC. We then apply our electrically driven, optically detected magnetic resonance (E-ODMR) technique to spatially map the QL1 spin response to an AC electric field generated by our fabricated electrodes. This imaging applies to GHz-frequency resonant electric fields, 2 complementing non-resonant kHz-frequency AC electric field sensing previously demonstrated with NV centers in diamond [3]. Since the QL1 defect shares a ground-state spin Hamiltonian with many intrinsic defects in 13,15,[26][27][28][29] and the NV center in diamond [4], our results apply to a broad class of optically addressable solid-state defects.Our E-ODMR measurements determine that the optically addressable spin of QL1 has integervalue total spin (S), and long spin relaxation (T 1 ) times [10] suggest that it is the orbital ground state (see SI). Together...