Molecular photoswitches are utilized in the field of photopharmacology, where the energetics of a molecule can be reversibly controlled with light to achieve spatial and temporal resolution of a particular effect. Photoswitches may function by undergoing photoisomerization through which light is used to conformationally adapt a molecule to a biological site, or through an environmental effect where an external factor such as a solvent effect or hydrogen bonding can selectively allow or quench an emissive state within a molecule. To visualize photophysical processes, a useful depiction is the Jablonski diagram. This is a diagram which depicts electronic and vibrational energy levels within a molecule as vertical levels and shows the possible relaxation pathways from excited states. Typically, the ground state is referred to as S, and is drawn at the bottom of the figure with nearby vibrational excitations just above it. An absorption will promote an electron into the S state at any vibrational energy level, or into a higher order excited state if the absorbed energy has enough magnitude. The excited state can then undergo internal conversion which is the electronic relaxation to a lower state with the same vibrational energetics or vibrational relaxation within a state. This may be followed by an intersystem crossing wherein the electron undergoes a spin flip, or a radiative or nonradiative decay back to the ground state.
One example of an organic compound that undergoes photoisomerization is azobenzene. The structure is two phenyl rings joined with a N=N double bond and is the simplest aryl azo compound. Azobenzene and its derivatives have two accessible absorbance bands: the S state from a n-π* transition which can be excited into using blue light, and the S state from a π-π* transition that can be excited into using ultraviolet light. Azobenzene and its derivatives have two isomers, trans and cis. The trans isomer, having the phenyl rings on opposite sides of the azo double bond, is the thermally preferred isomer as there is less stereoelectronic distortion and more delocalization present. However, excitation of the trans isomer to the S state facilitates a shift to the cis isomer. The S absorption is associated with a conversion back to the trans isomer. In this way, azobenzene and its derivatives can act as reversible stores of energy by maintaining a strained configuration in the cis isomer. Modifications of the substituents on azobenzene allow the energetics of these absorptions to be tuned, and if they are engineered such that the two absorption bands overlap a single wavelength of light can be used to flip between them. There are a number of similar photoswitches which isomerize between E and Z configurations across an azo group (for instance, azobenzene and azopyrazole) or an ethylene bridge (for instance, stilbene and hemithioindigo).
Alternatively, photoswitches may themselves be emissive and exhibit environmental control over their properties. One such example is a class of ruthenium polypyridyl coordination complexes. Typically they contain two bidentate bipyridine or phenanthroline ligands and an extended phenanthroline-phenazine bidentate ligand such as dipyrido[3,2-a:2,3-c]phenazine (dppz).These complexes have an accessible metal to ligand charge transfer excited state (MLCT) which undergoes rapid intersystem crossing to a MLCT state due to the strong spin-orbit coupling of the ruthenium center. These excited states are localized on the extended ligand phenazine nitrogens, and emission occurs from the MLCT state. Hydrogen bonding interactions such as the presence of water around these nitrogen atoms stabilizes the MLCT state, quenching the emission process. Thus, by controlling whether an aqueous or otherwise protic polar solvent is present, emissive behaviors can be “turned on/off”, and alternation between “bright states” and “dark states” is facilitated. This light switch behavior makes these and similar complexes of recent interest in photopharmacological applications such as photodynamic therapy.