We explored the photoisomerization mechanisms in novel homologues of photoactive yellow protein (PYP) from Leptospira biflexa (Lbif) to identify conserved features and functional diversity in the primary photochemistry of this family of photoreceptors. In close agreement with the prototypical PYP from Halorhodospira halophila (Hhal), we observe excited-state absorbance near 375 nm and stimulated emission near 500 nm, with triphasic excited-state decay. While the excited-state decay for Lbif PYP is the slowest among those of known PYPs due to the redistribution of the amplitudes of the three decay components, the quantum yield for productive photocycle entry is very similar to that of Hhal PYP. Pro68 is highly conserved in PYPs and is important for the high photochemical quantum yield in Hhal PYP, but this residue is Ile in wild-type Lbif PYP. The level of photoproduct formation is slightly increased in I68P Lbif PYP, indicating that this residue regulates the photochemical quantum yield in the entire PYP family. Lbif PYP also exhibited a blue-shifted photoproduct previously undiscovered in ultrafast studies of PYP, which we have named pUV. We posit that pUV is a detour in the PYP photocycle with a twisted protonated pCAH configuration. Cryokinetic experiments with Hhal PYP confirmed the presence of pUV, but the population of this state in room-temperature ultrafast experiments is very small. These results resolve the long-standing inconsistency in the literature regarding the existence of a bifurcation in the room-temperature photocycle of PYP.

Phytochrome proteins utilize ultrafast photoisomerization of a linear tetrapyrrole chromophore to detect the ratio of red to far-red light. Femtosecond photodynamics in the PAS-GAF-PHY photosensory core of the Cph1 phytochrome from Synechocystis sp. PCC6803 (Cph1Δ) were resolved with a dual-excitation-wavelength-interleaved pump-probe (DEWI) approach with two excitation wavelengths (600 and 660 nm) at three pH values (6.5, 8.0, and 9.0). Observed spectral and kinetic heterogeneity in the excited-state dynamics were described with a self-consistent model comprised of three spectrally distinct populations with different protonation states (P-I, P-II, and P-III), each composed of multiple kinetically distinct subpopulations. Apparent partitioning among these populations is dictated by pH, temperature, and excitation wavelength. Our studies provide insight into photocycle initiation dynamics at physiological temperatures, implicate the low-pH/low-temperature P-I state as the photoactive state in vitro, and implicate an internal hydrogen-bonding network in regulating the photochemical quantum yield.

Controlling the photoexcited properties and behavior of hybrid perovskites by halide doping has the potential to impact a wide range of emerging technologies, including solar cells and radiation detectors. Crystalline samples of methylammonium lead bromide substituted with chlorine (MAPbBr3–x Cl x ) were examined by transient reflectivity spectroscopy and nonadiabatic molecular dynamics simulations. At picosecond time scales, the addition of chlorine to the perovskite crystal increased the observed rate of hot carrier cooling and the calculated electron–phonon coupling constants. Chlorine-doped samples also exhibit a slower surface recombination velocity and a smaller ambipolar mobility.

The photoactive yellow protein (PYP) from Halorhodospira halophila (Hhal) is a bacterial photoreceptor and model system for exploring functional protein dynamics. We report ultrafast spectroscopy experiments that probe photocycle initiation dynamics in the PYP domain from the multidomain PYP-phytochrome-related photoreceptor from Rhodospirillum centenum (Rcen). As with Hhal PYP, Rcen PYP exhibits similar excited-state dynamics; in contrast, Rcen PYP exhibits altered photoproduct ground-state dynamics in which the primary I intermediate as observed in Hhal PYP is absent. This property is attributed to a tighter, more sterically constrained binding pocket around the p-coumaric acid chromophore due to a change in the Rcen PYP protein structure that places Phe98 instead of Met100 in contact with the chromophore. Hence, the I state is not a necessary step for the initiation of productive PYP photocycles and the ubiquitously studied Hhal PYP may not be representative of the broader PYP family of photodynamics.