We present a microfabricated optical cavity, which combines a very small mode volume with high finesse. In contrast to other micro-resonators, such as microspheres, the structure we have built gives atoms and molecules direct access to the high-intensity part of the field mode, enabling them to interact strongly with photons in the cavity for the purposes of detection and quantum-coherent manipulation. Light couples directly in and out of the resonator through an optical fiber, avoiding the need for sensitive coupling optics. This renders the cavity particularly attractive as a component of a lab-on-a-chip, and as a node in a quantum network. © 2005 American Institute of Physics. ͓DOI: 10.1063/1.2132066͔ High-finesse optical cavities are central to many techniques and devices in atomic physics, 1 optoelectronics, 2 chemistry, 3 and biosensing. 4 As well as selecting spectral and spatial distributions of the classical electromagnetic field, optical cavities make it possible to harness quantum effects for applications in quantum information science. 1,5 For example, it is possible to produce single photons on demand using atoms 6,7 or ions 8 inside a cavity and to create entanglement between those that share a cavity photon. 9-11 Similar ideas are being pursued with quantum dots. 12,13 Microscopic cavities are of particular interest 14 because small volume gives the photon a large field and because they offer the possibility of integration with micro-opto-electro-mechanical systems 15 and atom chips. [16][17][18] Here we present a simple and innovative method for fabricating microscopic, broadly-tuneable, high-finesse cavities. These have the significant new feature that their structure is open, giving an atom, molecule or quantum dot direct access to an antinode of the cavity mode. This structure is therefore ideally suited for detecting small numbers of particles, 19 and miniaturizing quantum devices based on strong dipole-cavity coupling.We have made high-finesse, open optical cavities that operate in length at a range of approximately 20-200 m. Each cavity is formed by a concave micro-mirror and the plane tip of an optical fiber, both coated for reflection, as illustrated in Fig. 1͑a͒. Arrays of concave mirrors are fabricated in silicon by wet-etching isotropically through circular apertures in a lithographic mask using a mixture of HF and HNO 3 in acetic acid. The etch bath in which the wafer is immersed undergoes continuous agitation during the etching process, resulting in an approximately spherical surface profile, as shown in Fig. 1͑b͒. The etch rate and the final morphology of the silicon surface are highly dependent on the agitation and on the concentration of each component in the etchant. 20 Precise control over these factors gives us repeatable surface profiles in the silicon with 6 nm rms roughness. In our first experiment, gold is sputtered onto an array of mirror templates to form a layer 100 nm thick with a surface roughness of 10 nm. The plane mirror of the cavity is a dielectric multilayer, w...