Mutations conferring SO42- pumping ability on the cyanobacterial anion pump rhodopsin and the resultant unique features of the mutant.

Membrane transport proteins can be divided into two types: those that bind substrates in a resting state and those that do not. In this study, we demonstrate that these types can be converted by mutations through a study of two cyanobacterial anion-pumping rhodopsins, Mastigocladopsis repens halorhodopsin (MrHR) and Synechocystis halorhodopsin (SyHR). Anion pump rhodopsins, including MrHR and SyHR, initially bind substrate anions to the protein center and transport them upon illumination. MrHR transports only smaller halide ions, Cl- and Br-, but SyHR also transports SO42-, despite the close sequence similarity to MrHR. We sought a determinant that could confer SO42- pumping ability on MrHR and found that the removal of a negative charge at the anion entrance is a prerequisite for SO42- transport by MrHR. Consistently, the reverse mutation in SyHR significantly weakened SO42- pump activity. Notably, the MrHR and SyHR mutants did not show SO42- induced absorption spectral shifts or changes in the photoreactions, suggesting no bindings of SO42- in their initial states or the bindings to the sites far from the protein centers. In other words, unlike wild-type SyHR, these mutants take up SO42- into their centers after illumination and release it before the ends of the photoreactions.

Second thresholds in BEC-BCS-laser crossover of exciton-polariton systems.

The mechanism of second thresholds observed in several experiments is theoretically revealed by studying the BEC-BCS-laser crossover in exciton-polariton systems. We find that there are two different types of second thresholds: one is a crossover within quasiequilibrium phases and the other is into nonequilibrium (lasing). In both cases, the light-induced band renormalization causes gaps in the conduction and valence bands, which indicates the existence of bound electron-hole pairs in contrast to earlier expectations. We also show that these two types can be distinguished by the gain spectra.