Fluorescent protein (FP) variants that can be reversibly converted between fluorescent and nonfluorescent states have proven to be a catalyst for innovation in the field of fluorescence microscopy. However, the structural basis of the process remains poorly understood. High-resolution structures of a FP derived from Clavularia in both the fluorescent and the light-induced nonfluorescent states reveal that the rapid and complete loss of fluorescence observed upon illumination with 450-nm light results from cistrans isomerization of the chromophore. The photoinduced change in configuration from the well ordered cis isomer to the highly nonplanar and disordered trans isomer is accompanied by a dramatic rearrangement of internal side chains. Taken together, the structures provide an explanation for the loss of fluorescence upon illumination, the slow light-independent recovery, and the rapid light-induced recovery of fluorescence. The fundamental mechanism appears to be common to all of the photoactivatable and reversibly photoswitchable FPs reported to date.crystallography ͉ fluorescence ͉ photoswitching ͉ protein structure G reen fluorescent protein (GFP) from the jellyfish Aequorea victoria (1) and more recently, cyan, yellow, and red fluorescent proteins (FPs), isolated from coral reef organisms (2), have become standard research tools in cellular biology. Structural studies have revealed a universally conserved fold for FPs: an 11-stranded -barrel with a central and axial ␣-helix (3, 4). A sequence of three amino acid residues on this central ␣-helix (Ser-65-Tyr-66-Gly-67 in Aequorea GFP) undergoes a series of autocatalytic posttranslational modifications to form the chromophore. Despite overall structural similarity across FPs from a variety of species and a variety of hues, members of the GFP family are quite diverse with respect to their photophysical properties. For example, properties such as emission color, extinction coefficient, quantum yield, and fluorescence lifetime can vary dramatically among FP variants. These properties are determined by both the influence of the protein matrix on the chromophore environment and the particular covalent chemical structure of the chromophore (5).Another photophysical property common to all FPs is wavelength-dependent change in their f luorescence emission properties upon illumination. In most cases, these changes appear to result from irreversible covalent modification of the chromophore structure or its local protein environment. Examples of such permanent changes include light-induced transition from a f luorescent to a nonf luorescent state (photobleaching), transition from a nonf luorescent to a f luorescent state (photoactivation), or a change in excitation or emission wavelength maxima (photoconversion). Photobleaching, photoactivation, and photoconversion are well documented and can be advantageous for f luorescence imaging applications such as in vivo tracking of fusion protein movements (6 -9). A less well documented process, occasionally described as ''re...