The photocycle of channelrhodopsin-2 is investigated in a comprehensive study by ultrafast absorption and fluorescence spectroscopy as well as flash photolysis in the visible spectral range. The ultrafast techniques reveal an excited-state decay mechanism analogous to that of the archaeal bacteriorhodopsin and sensory rhodopsin II from Natronomonas pharaonis. After a fast vibrational relaxation of the excited-state population with 150 fs its decay with mainly 400 fs is observed. Hereby, both the initial all-trans retinal ground state and the 13-cis-retinal K photoproduct are populated. The reaction proceeds with a 2.7 ps component assigned to cooling processes. Small spectral shifts are observed on a 200 ps timescale. They are attributed to conformational rearrangements in the retinal binding pocket. The subsequent dynamics progresses with the formation of an M-like intermediate (7 and 120 μs), which decays into red-shifted states within 3 ms. Ground-state recovery including channel closing and reisomerization of the retinal chromophore occurs in a triexponential manner (6 ms, 33 ms, 3.4 s). To learn more about the energy barriers between the different photocycle intermediates, temperature-dependent flash photolysis measurements are performed between 10 and 30°C. The first five time constants decrease with increasing temperature. The calculated thermodynamic parameters indicate that the closing mechanism is controlled by large negative entropy changes. The last time constant is temperature independent, which demonstrates that the photocycle is most likely completed by a series of individual steps recovering the initial structure.

The conformational dynamics induced by ligand binding to the tetracycline-binding aptamer is monitored via stopped-flow fluorescence spectroscopy and time-correlated single photon counting experiments. The fluorescence of the ligand is sensitive to changes within the tertiary structure of the aptamer during and after the binding process. In addition to the wild-type aptamer, the mutants A9G, A13U and A50U are examined, where bases important for regulation are changed to inhibit the aptamer’s function. Our results suggest a very fast two-step-mechanism for the binding of the ligand to the aptamer that can be interpreted as a binding step followed by a reorganization of the aptamer to accommodate the ligand. Binding to the two direct contact points A13 and A50 was found to occur in the first binding step. The exchange of the structurally important base A9 for guanine induces an enormous deceleration of the overall binding process, which is mainly rooted in an enhancement of the back reaction of the first binding step by several orders of magnitude. This indicates a significant loss of tertiary structure of the aptamer in the absence of the base A9, and underlines the importance of pre-organization on the overall binding process of the tetracycline-binding aptamer.

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A series of short RNA duplexes containing one or two 1-ethynylpyrene-modified adenine bases was synthesised. The melting behaviour of these duplexes was examined by monitoring temperature-dependent pyrene fluorescence. In the singly modified RNA duplexes, the bases flanking the ethynylpyrene-rA were varied to examine the sequence specificity of the fluorescence change of pyrene upon RNA hybridisation. Because an increase in pyrene fluorescence upon melting of the duplex can be correlated with intercalation of pyrene, and a decrease is usually associated with the position of pyrene outside the strand, a relationship between the flanking bases and the tendency of the dye to intercalate has been established. It was found that pyrene intercalation is less likely to take place if the modified base is flanked only by A-U base pairs. Flanking G-C base pairs, even only in the 5'-direction of the modified base, will favour intercalation. In addition, we examined a doubly modified compound that had a pyrene located on each strand. The spectra indicated that the two pyrenes were close enough for interaction. Upon melting of the strand, a fluorescence blue shift corresponding to the dissociation of the pyrene-pyrene complex could be observed in addition to the intensity effect already known from the singly modified compounds. Two melting curves based on the different properties of the fluorophore could be extracted, leading to different melting points corresponding to the global duplex melting and to the change of local pyrene environment, respectively.

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The photophysics of pyrene attached to an adenine base within RNA single strands and duplexes is examined with respect to the position of the pyrene within the strand and the number of pyrenes attached to one duplex. Compounds with pyrenes intercalating sequence specifically are examined, as well as a doubly modified compound, where the two pyrenes are located close enough to each other for significant excimer interaction. Femtosecond transient absorption measurements and time correlated single photon counting measurements allow a thorough examination of the local influences on the pyrene photophysics. Our results suggest that optical excitation establishes an equilibration between two molecular states of different spectroscopic properties and lifetimes that are coupled only via the excited state as a gateway. One of them is a neutral pyrene-adenine excited state, S*, while the second one is connected to an excited charge transfer state, S*(CT). In all compounds, an ultrafast sub-ps decay from a higher excited state into the lowest excited state S* occurs, and an excited charge transfer species S*(CT) is formed within picoseconds. The fluorescence behavior of the pyrene-modified adenine, however, is strongly dependent on RNA conformation. Both S* and S*(CT) states are fluorescent, and decay within hundreds of picoseconds and approximately 2 ns, respectively. The ratio between S* and S*(CT) fluorescence depends strongly on pyrene intercalation, and it is found that the S* state is quenched selectively upon intercalation of the pyrene into RNA. The doubly modified duplex exhibits an additional fluorescent state with a lifetime of 18.7 ns, which is associated with the pyrene excimer state. This state coexists with a significant population of the pyrene monomer, since the characteristic features of the latter can still be observed. Formation of the excimer occurs on femtosecond time scales. The pyrene label thus provides a sensitive tool to monitor the local structural dynamics of RNA with the chromophore acting as a molecular beacon.

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