The reversible photoswitching between the 'on' and 'off' states of the fluorescent protein Dronpa involves photoisomerization as well as protein side-chain rearrangements, but the process of interconversion remains poorly characterized. Here we use time-resolved infrared measurements to monitor the sequence of these structural changes, but also of proton transfer events, which are crucial to the development of spectroscopic contrast. Light-induced deprotonation of the chromophore phenolic oxygen in the off state is a thermal ground-state process, which follows ultrafast (9 ps) trans-cis photoisomerization, and so does not involve excited-state proton transfer. Steady-state infrared difference measurements exclude protonation of the imidazolinone nitrogen in both the on and off states. Pump-probe infrared measurements of the on state reveal a weakening of the hydrogen bonding between Arg66 and the chromophore C ¼ O, which could be central to initiating structural rearrangement of Arg66 and His193 coinciding with the low quantum yield cis-trans photoisomerization
We compare visible-pump mid-infrared-probe femtosecond measurement of electron injection on dye-sensitized mesoporous TiO2 films immersed in neat solvent or in I–/I3 – electrolyte. Results are presented for the Ru-polypyridyl dyes N3 and N719 and the organic dye D149. Using N719 and the type of electrolyte required to make efficient and stable dye sensitized solar cells (DSSCs), we find multiple exponential injection dynamics, ranging from <300 fs to 0.5 ns for the ruthenium metal-centered dyes. The organic dye D149 shows double exponential <300 fs to 30 ps injection kinetics. We show that this result is not dependent on our pulse intensity, average intensity, or dye aggregates deposited during dyeing. We find the N3 dye immersed in neat solvent shows dominantly ultrafast, <300 fs, injection kinetics, as previously reported. Ultrafast kinetics were also observed for all samples when pulse intensity was increased above a given range. We discuss the implication of the results for rational design of future NIR absorbing dyes for DSSCs.
The fast-switching M159T mutant of the reversibly photoswitchable fluorescent protein Dronpa has an enhanced yield for the on-to-off reaction. The forward and reverse photoreactions proceed via cis-trans and trans-cis photoisomerization, yet protonation and deprotonation of the hydroxyphenyl oxygen of the chromophore is responsible for the majority of the resulting spectroscopic contrast. Ultrafast visible-pump, infrared-probe spectroscopy was used to detect the picosecond, nanosecond, as well as metastable millisecond intermediates. Additionally, static FTIR difference measurements of the Dronpa-M159T mutant correspond very closely to those of the wild type Dronpa, identifying the p-hydroxybenzylidene-imidazolinone chromophore in the cis anion and trans neutral forms in the bright "on" and dark "off" states, respectively. Green excitation of the on state is followed by dominant radiative decay with characteristic time constants of 1.9 ps, 185 ps, and 1.1 ns, and additionally reveals spectral changes belonging to the species decaying with a 1.1 ns time constant, associated with both protein and chromophore modes. A 1 ms measurement of the on state identifies bleach features that correspond to those seen in the static off-minus-on Fourier transform infrared (FTIR) difference spectrum, indicating that thermal protonation of the hydroxyphenyl oxygen proceeds within this time window. Blue excitation of the off state directly resolves the formation of the primary photoproduct with 0.6 and 14 ps time constants, which is stable on the nanosecond time scale. Assignment of the primary photoproduct to the cis neutral chromophore in the electronic ground state is supported by the frequency positions expected relative to those for the nonplanar distorted geometry for the off state. A 1 ms measurement of the off state corresponds closely with the on-minus-off FTIR difference spectrum, indicating thermal deprotonation and rearrangement of the Arg66 side chain to be complete.
Photosystem I (PSI) from Chroococcidiopsis thermalis PCC 7203 grown under far-red light (FRL; >725 nm) contains both chlorophyll a and a small proportion of chlorophyll f. Here, we investigated excitation energy transfer and charge separation using this FRL-grown form of PSI (FRL-PSI). We compared femtosecond transient visible absorption changes of normal, white-light (WL)-grown PSI (WL-PSI) with those of FRL-PSI using excitation at 670 nm, 700 nm, and (in the case of FRL-PSI) 740 nm. The possibility that chlorophyll f participates in energy transfer or charge separation is discussed on the basis of spectral assignments. With selective pumping of chlorophyll f at 740 nm, we observe a final ∼150 ps decay assigned to trapping by charge separation, and the amplitude of the resulting P700A charge-separated state indicates that the yield is directly comparable to that of WL-PSI. The kinetics shows a rapid 2 ps time constant for almost complete transfer to chlorophyll f if chlorophyll a is pumped with a wavelength of 670 nm or 700 nm. Although the physical role of chlorophyll f is best supported as a low-energy radiative trap, the physical location should be close to or potentially within the charge-separating pigments to allow efficient transfer for charge separation on the 150 ps timescale. Target models can be developed that include a branching in the formation of the charge separation for either WL-PSI or FRL-PSI.
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