Photonic bandgap cavities are prime solid-state systems to investigate light-matter interactions in the strong coupling regime. However, as the cavity is defined by the geometry of the periodic dielectric pattern, cavity control in a monolithic structure can be problematic. Thus, either the state coherence is limited by the read-out channel, or in a high Q cavity, it is nearly decoupled from the external world, making measurement of the state extremely challenging. We present here a method for ameliorating these difficulties by using a coupled cavity arrangement, where one cavity acts as a switch for the other cavity, tuned by control of the atomic transition.PACS numbers: 42.50. Pq, 42.70.Qs, 42.60.Gd, As the maturity and sophistication of quantum optics progresses, there is a growing movement to translate such effects into practical devices. This impetus suggests, for reasons of scalability and practicality, the need for viable solid-state technologies to produce and distribute single photons as an enabling technology for derivative quantum devices. In particular we are concerned with the role played by cavity Quantum Electro-Dynamics (CQED) in such devices.CQED has been used to great effect in the generation of deterministic, transform limited single (and higherorder Fock states) photon pulses [1], and schemes exist which incorporate CQED for quantum computing [2], and entanglement generation [3]. More recently 'hybrid' schemes for quantum computation have been suggested incorporating matter qubits in cavities with single photon generation, linear optics and high fidelity photon detection [4]. However many of these schemes (with notable exceptions) will be problematic to scale or to remove from laboratory environments.Given difficulties with implementing most present schemes in non-research environments, significant attention has turned towards photonic band gap (PBG) cavities as quantum cavities. This is due to their superb photonic confinement properties and the recent realization of high Q cavities with small mode volume (of order the wavelength 3 ) [5,6]. These successes have been fueled by a combination of technological imperatives and advances in fabrication.