Fluorescence and excited state dynamics of the deprotonated Schiff base retinal in proteorhodopsin

Temperature Dependence of the Krokinobacter rhodopsin 2 Kinetics

We investigated the temperature-dependent kinetics of the light-driven Na⁺ pump Krokinobacter rhodopsin 2 (KR2) at Na⁺-pumping conditions. The recorded microsecond flash photolysis data were subjected to detailed global target analysis, employing Eyring constraints and spectral decomposition. The analysis resulted in the kinetic rates, the composition of the different photocycle equilibria, and the spectra of the involved photointermediates. Our results show that with the temperature increase (from 10 to 40°C), the overall photocycle duration is accelerated by a factor of 6, with the L-to-M transition exhibiting an impressive 40-fold increase. It follows from the analysis that in KR2 the chromophore and the protein scaffold are more kinetically decoupled than in other microbial rhodopsins. We link this effect to the rigidity of the retinal protein environment. This kinetic decoupling should be considered in future studies and could potentially be exploited for fine-tuning biotechnological applications.

A QM/MM study of the initial excited state dynamics of green-absorbing proteorhodopsin

The primary photochemical reaction of the green-absorbing proteorhodopsin is studied by means of a hybrid quantum mechanics/molecular mechanics (QM/MM) approach. The simulations are based on a homology model derived from the blue-absorbing proteorhodopsin crystal structure. The geometry of retinal and the surrounding sidechains in the protein binding pocket were optimized using the QM/MM method. Starting from this geometry the isomerization was studied with a relaxed scan along the C13[double bond, length as m-dash]C14 dihedral. It revealed an "aborted bicycle pedal" mechanism of isomerization that was originally proposed by Warshel for bovine rhodopsin and bacteriorhodopsin. However, the isomerization involved the concerted rotation about C13[double bond, length as m-dash]C14 and C15[double bond, length as m-dash]N, with the latter being highly twisted but not isomerized. Further, the simulation showed an increased steric interaction between the hydrogen at the C14 of the isomerizing bond and the hydroxyl group at the neighbouring tyrosine 200. In addition, we have simulated a nonadiabatic trajectory which showed the timing of the isomerization. In the first 20 fs upon excitation the order of the conjugated double and single bonds is inverted, consecutively the C13[double bond, length as m-dash]C14 rotation is activated for 200 fs until the S1-S0 transition is detected. However, the isomerization is reverted due to the specific interaction with the tyrosine as observed along the relaxed scan calculation. Our simulations indicate that the retinal - tyrosine 200 interaction plays an important role in the outcome of the photoisomerization.

Ultrafast excited state decay of natural UV filters: from intermolecular hydrogen bonds to a conical intersection

An unsaturated bond in the side chain leads to the ultrafast decay of the excited statesviaa conical intersection independent of solvent properties.

Ultrafast Photoinduced Deactivation Dynamics of Proteorhodopsin

We report femtosecond time-resolved absorption change measurements of the photoinduced deactivation dynamics of a microbial rhodopsin in the ultraviolet-visible and mid-infrared range. The blue light quenching process is recorded in green proteorhodopsin's (GPR) primary proton donor mutant E108Q from the deprotonated 13-cis photointermediate. The return of GPR to the dark state occurs in two steps, starting with the photoinduced 13-cis to all-trans reisomerization of the retinal. The subsequent Schiff base reprotonation via the primary proton acceptor (D97) occurs on a nanosecond time scale. This step is two orders of magnitude faster than that in bacteriorhodopsin, potentially because of the very high pK_A of the GPR primary proton acceptor.