Light-Harvesting in Biophotonic Optofluidic Microcavities via Whispering-Gallery Modes.

Phycobiliproteins are a class of light-harvesting fluorescent proteins existing in cyanobacteria and microalgae, which harvest light and convert it into electricity. Owing to recent demands on environmental-friendly and renewable apparatuses, phycobiliproteins have attracted substantial interest in bioenergy and sustainable devices. However, converting energy from biological materials remains challenging to date. Herein, we report a novel scheme to enhance biological light-harvesting through light-matter interactions at the biointerface of whispering-gallery modes (WGMs), where phycobiliproteins were employed as the active gain material. By exploiting microdroplets as a carrier for light-harvesting biomaterials, strong local electric field enhancement and photon confinement at the cavity interface resulted in significantly enhanced bio-photoelectricity. A threshold-like behavior was discovered in photocurrent enhancement and the WGM modulated fluorescence. Systematic studies of biologically produced photoelectricity and optical mode resonance were carried out to illustrate the impact of the cavity quality factor, structural geometry, and refractive indices. Finally, a biomimetic system was investigated by exploiting cascade energy transfer in phycobiliprotein assembly composed of three light-harvesting proteins. The key findings not only highlight the critical role of optical cavity in light-harvesting but also offer deep insights into light energy coupling in biomaterials.

UV-induced phycobilisome dismantling in the marine picocyanobacterium Synechococcus sp. WH8102.

The marine picocyanobacterium Synechococcus sp. WH8102 was submitted to ultraviolet (UV-A and B) radiations and the effects of this stress on reaction center II and phycobilisome integrity were studied using a combination of biochemical, biophysical and molecular biology techniques. Under the UV conditions that were applied (4.3 W m(-2) UV-A and 0.86 W m(-2) UV-B), no significant cell mortality and little chlorophyll degradation occurred during the 5 h time course experiment. However, pulse amplitude modulated (PAM) fluorimetry analyses revealed a rapid photoinactivation of reaction centers II. Indeed, a dramatic decrease of the D1 protein amount was observed, despite a large and rapid increase in the expression level of the psbA gene pool. Our results suggest that D1 protein degradation was accompanied (or followed) by the disruption of the N-terminal domain of the anchor linker polypeptide LCM, which in turn led to the disconnection of the phycobilisome complex from the thylakoid membrane. Furthermore, time course analyses of in vivo fluorescence emission spectra suggested a partial dismantling of phycobilisome rods. This was confirmed by characterization of isolated antenna complexes by SDS-PAGE and immunoblotting analyses which allowed us to locate the disruption site of the rods near the phycoerythrin I-phycoerythrin II junction. In addition, genes encoding phycobilisome components, including alpha-subunits of all phycobiliproteins and phycoerythrin linker polypeptides were all down regulated in response to UV stress. Phycobilisome alteration could be the consequence of direct UV-induced photodamages and/or the result of a protease-mediated process.

Mediation of ultrafast light-harvesting by a central dimer in phycoerythrin 545 studied by transient absorption and global analysis.

We report ultrafast femtosecond transient absorption measurements of energy-transfer dynamics for the antenna protein phycoerythrin 545, PE545, isolated from a unicellular cryptophyte Rhodomonas CS24. The phycoerythrobilins are excited at both 485 and 530 nm, and the spectral response is probed between 400 and 700 nm. Room-temperature measurements are contrasted with measurements at 77 K. An evolution-associated difference spectra (EADS) analysis is combined with estimations of bilin spectral positions and energy-transfer rates to obtain a detailed kinetic model for PE545. It is found that sub pulse-width dynamics include relaxation between the exciton states of a chromophore dimer (beta 50/60) located in the core of the protein. Energy transfer from the lowest exciton state of the phycoerythrobilin (PEB) dimer to one of the periphery 15,16-dihydrobiliverdin (DBV) bilins is found to occur on a time scale of 250 fs at room temperature and 960 fs at 77 K. A host of energy-transfer dynamics involving the beta 158, beta 82, and alpha 19 bilins occur on a time scale of 2 ps at room temperature and 3 ps at 77 K. A final energy transfer occurs between the red-most DBV bilins with a time scale estimated to be approximately 30 ps. The role of the centrally located phycoerythrobilin dimer is seen as crucial-spectrally as it expands the cross-section of absorption of the protein; structurally as it sits in the middle of the protein acting as an intermediary trap; and kinetically, as the internal conversion and subsequent red-shift of the excitation is extremely fast.

Effect of heat on phycoerythrin fluorescence: Influence of thermal exposure on the fluorescence emission of R-phycoerythrin.

The goal of this work was to measure and model the effect of thermal exposure on the fluorescence emission of R-phycoerythrin (R-PE). The long-term objective of our work is to assess the feasibility of encapsulating R-PE for use as the critical component of a time-temperature integrator (TTI) for ascertaining the degree of inactivation of food pathogens such as Salmonella. In this article we present a study to measure and model the thermally induced fluorescence emission decay of R-PE in several isothermal experiments. We used the isothermal data to determine the kinetic parameters, based on a general n(th) order reaction, and evaluated the utility of the resulting model by using it to predict R-PE fluorescence emission decay for several nonisothermal experiments based on published USDA safe harbor guidelines for cooked beef products. The transient experiments were conducted over the same temperature range used in the isothermal study. Very good agreement was obtained between theory and experiment at temperatures of 62.8 degrees C and above, although the model slightly underpredicted the extent of fluorescence emission decay at 60 degrees C. Our results indicate that R-PE fluorescence emission decay kinetics is well behaved and that the protein is a strong candidate for use as a time-temperature integrator.

Photosensitized formation of singlet oxygen by phycobiliproteins in neutral aqueous solutions.

Phycobiliproteins (PBPs) are a type of promising sensitizers for photodynamic therapy (PDT). Upon irradiation (lambda>500nm) of an oxygen-saturated aqueous solution of phycobiliproteins, particularly, C-phycocyanin (C-PC), allophycocyanin (APC) or R-phycoerythrin (R-PE), the formation of singlet oxygen (1O2) was detected by using imidazole in the presence of p-nitrosodimethylaniline (RNO). The bleaching of RNO caused by the presence of imidazole in our system showed typical concentration dependence with a maximum at about 8mM imidazole, which is in agreement with the formation of 1O2. In addition, the generation of 1O2 was verified further in the presence of D2O and specific singlet oxygen quencher 1,4-diazabicyclo [2,2,2] octane (DABCO) and sodium azide (NaN3). Our experimental results indicated that APC possesses high ability to generate reactive oxygen species and the relative quantum yields of photogeneration of 1O2 by PBPs are as follows: APC > C-PC > R-PE.

Exciton splitting in phycoerythrin 545.

Phycoerythrin 545 is a biliprotein having a polypeptide structure of alpha 2 beta 2, and each alpha and beta polypeptide has chromophores. Circular dichroism (CD) and absorption spectroscopy in the visible region together with various biochemical protocols have been used to study these chromophores. The CD spectrum exhibits overlapping positive and negative bands. Exciton splitting between closely-spaced pairs of chromophores produces a CD spectrum that has positive and negative bands of equal rotational strengths, a conservative spectrum. Alternatively, any positive or negative band could arise from a single chromophore. The results of this study demonstrate that exciton splitting is the likely cause of the negative and corresponding positive bands. The CD spectra of the separated alpha and beta polypeptides, under conditions where the polypeptide structure is denatured, have no negative bands. When the polypeptides are allowed to refold individually, the chromophores on the beta polypeptide regain a combination of negative and positive CD bands. The spectrum of the alpha polypeptide shows no evidence of exciton splitting under these refolding conditions. In another approach, urea is added to the protein in low concentrations, which result in changes in the conformation and perhaps association of the protein. A difference CD spectrum of native protein minus protein in 0.8 M urea shows a spectrum characteristic of exciton splitting. Moreover, the remaining CD spectra in 0.8, 1.6, or 2.4 M urea still show the possibility of further exciton splitting, but a slightly different wavelengths from the spectrum that is deleted by 0.8 M urea. This finding may suggest that there are two types of exciton splitting.

Structure and interactions of phycocyanobilin chromophores in phycocyanin and allophycocyanin from an analysis of their resonance raman spectra.

Raman spectra of phycocyanobilin, phycocyanin, and allophycocyanin were obtained at resonance with their visible and near-UV transitions. These spectra were empirically assigned with the help of 14N- and 15N-isotopic substitutions and comparisons with resonance Raman spectra of phycoerythrin. These results confirm the previously suggested assignment of a conformation-sensitive band around 1239-1246 cm-1 to a mode involving nu CmH and nu CN coordinates. Computer-assisted decomposition of the complex, conformation-sensitive 1580-1670-cm-1 region yielded five components that we labeled I-V. The previously described spectral changes observed upon monomerization and denaturation in resonance Raman spectra of phycocyanin and allophycocyanin essentially arise from changes in the relative intensities of these components. Component I (around 1649-1651 cm-1) and component III (1621-1624 cm-1) originate predominantly from nu C=C at C15 of the chromophore. Their relative intensity ratio reflects the relative amounts of C15-Z-anti and C15-Z-syn methine bridge conformations, respectively. Component II (1633-1638 cm-1) is ascribed to a nu C=C mode of pyrrole rings; it is not sensitive to the chromophore conformation. Component IV is also conformation-insensitive and originates from nu C=N and nu C=C coordinates, most likely from ring C. Component V (1591-1594 cm-1) involves a nu C=N coordinate in ring D, coupled to a nu C=C coordinate of the C15 methine bridge. The implications of the present assignments on those of resonance Raman active modes of phytochrome are discussed. A consistent set of correlations between chromophore conformations and resonance Raman data is obtained for both phycobiliproteins and phytochrome.