A coupled quantum dot-nanocavity system in the weak coupling regime of cavityquantumelectrodynamics is dynamically tuned in and out of resonance by the coherent elastic field of a fSAW 800 MHz surface acoustic wave. When the system is brought to resonance by the sound wave, light-matter interaction is strongly increased by the Purcell effect. This leads to a precisely timed single photon emission as confirmed by the second order photon correlation function, g (2) . All relevant frequencies of our experiment are faithfully identified in the Fourier transform of g (2) , demonstrating high fidelity regulation of the stream of single photons emitted by the system. Solid state cavity-quantumelectrodynamics (cQED) systems formed by an exciton confined in a single semiconductor quantum dot (QD) and strongly localized optical modes in a photonic nanocavity (PhNCs) have been intensely studied over the past years [1,2]. Membranes patterned with two-dimensional photonic crystals represent a particularly attractive platform for the integration of large scale photonic networks on a chip [3]. In this architecture, both the weak[4] and strong coupling regime [5,6] of cQED have been demonstrated. These key achievements paved the way towards efficient sources of single photons [7,8] or optical switching operations controlled by single photons [9]. So far, the dynamic control of the spontaneous emission [10] or the coherent evolution of the coupled QD-PhNC cQED system [11,12] has relied mainly on all-optical approaches, although all-electrical approaches would be highly desirable for real-world applications due to their reduced level of complexity. However, to switch an electric field and induce a Stark effect [13] with sufficent bandwidth, nanoscale electric contacts are required [14]. In addition to light, these membrane structures guide [15] or confine vibronic excitations with strong optomechanical coupling strength [16,17]. These phononic modes can be directly employed to interface photonic crystal membranes by radio frequency surface acoustic waves (SAWs) [18,19]. As SAWs can be excited at GHz frequencies on piezoelectric materials [20,21], electrically induced and acoustically driven quantum gates are well within reach on this platform [22]. Moreover, SAWs have a long-standing tradition to control optically active semiconductors [23]. On one hand, acoustic charge transport [24] in piezoelectric semiconductors by these phononic modes have been proposed [25] and demonstrated [26][27][28] to regulate the carrier injection into QDs for precisely triggered single photon sources. On the other hand, the dynamic strain accompanying the SAW dynamically tunes optical modes in optical cavities [18,29] or excitons in QDs [30,31]. Here we demonstrate the dynamic, acousto-optic control of a prototypical QD-PhNC system by a f SAW 800 MHz SAW. We show that the acoustic field precisely modulates the energy detuning between the QD and PhNC on sub-nanosecond timescales switching the emission rate of the QD by a factor of 4. The photon statis...