SPECTRAL PROPERTIES OF PHYCOBILISOMES AND PHYCOBILIPROTEINS FROM THE BLUE-GREEN ALGA-NOSTOC SP.*

Abstract— An improved method for phycobilisome isolation from a blue-green alga Nostoc sp. was developed using 1% Triton X-100. The phycobilisome preparations showed little fragmentation and had structures similar in size to those observed in thin sections of the organism. Phycobiliproteins isolated from phycobilisomes and examined by sodium dodecyl sulfate polyacrylamide gel electrophoresis, had subunits with the following molecular weights: phycoerythrin (PE), 20,000 and 16,900; phycocyanin (PC), 14,700 and 16,300; and allophycocyanin (APC), 14,000. Isoelectric focusing of each phycobiliprotein resulted in major bands isoelectric at the following pH values: PE, 4.43, 4.45; PC 4.32; APC, 4.38. Absorption spectra at -196°c showed maxima at 551 and 566 nm for PE; 598 and 631 nm for PC; and 590, 600, 629 and 650 nm for APC. Concentrated vs dilute difference spectra of phycobiliproteins showed increased absorption at 574 nm (PE), 630 nm (PC) and 651 nm (APC) suggesting that spectral changes resulted from aggregation. Fluorescence analysis of each phycobiliprotein and of intact phycobilisome preparations showed that energy absorbed by phycoerythrin is transferred to allophycocyanin, possibly by a resonance transfer mechanism. These observations support a model where allophycocyanin forms the base of the phycobilisome which is attached to the photosynthetic membrane. The next layer is assumed to be phycocyanin, which in turn is followed by a phycoerythrin layer that is the outermost layer (on the stroma side) of the phycobilisome.     

Wright's formulae for the number of connected sparsely edged graphs

We have written computer programs to determine exactly the coefficients in Wright's formula for f(n, n + k), the number of connected sparsely edged labeled graphs (see preceding paper), and used them up to k = 24. We give the results up to k = 7.     

A new upper limit for the branching ratio (Ξ− → nπ−)(Ξ− → Λπ−)

From a sample of 735 000 Ξ^? decays, we have obtained a new upper limit for the branching ratio $\text{(Ξ}{}^{\mathrm{?}}\text{→}\text{n}\text{π}{}^{\mathrm{?}}\text{)}\text{(Ξ}{}^{\mathrm{?}}\text{→ Λπ}{}^{\mathrm{?}}\text{)}$. The result is 1.9 × 10^?5 at the 90% confidence level.     

Simulating the Performance of Michelson- and Sagnac-based Laser Interferometric Gravitational Wave Detectors in the Presence of Mirror Tilt and Curvature Errors

We model the behaviour of single-bounce delay-line dual recycled Sagnac-based interferometer and compare its performance with that of single-bounce Michelson-based system. Geometric imperfections such as mirror tilt and curvature mismatch can strongly influence the performance of the Sagnac device due to the inherently smaller free spectral range (FSR) and higher order mode spacing. This leads to a greater number of higher order modes near, or within the signal band in the signal recycling cavity of the instrument. The important consequence of that is, in general, a greater sensitivity of a Sagnac system to nonideal parameters and imperfections of various kind affecting the performance of a real interferometer. A number of optical configurations have also been examined numerically to determine the best possible optical arrangement, in the presence of such geometric imperfections. We show that there is an optimum choice for the nominal radius of curvature of the end mirrors which results from balancing the loss due to mirror tilt against that due to curvature mismatch.