with a Hitachi F-7000 spectrofluorometer (Tokyo, Japan) using 1 cm path length quartz cuvettes. Fluorescence anisotropy measurements were performed at room temperature (~25 °C) with a Hitachi F-7000 spectrofluorometer (Tokyo, Japan). Fluorescence anisotropy values were calculated using the following equation (Lakowicz, 2006) :
where IVV and IVH are the measured fluorescence intensities (after appropriate background subtraction) with the excitation polarizer vertically oriented and emission polarizer vertically and horizontally oriented, respectively. G is the grating correction factor and is the ratio of the efficiencies of the detection system for vertically and horizontally polarized light, and is equal to IHV/IHH. The excitation wavelength was set at 490 nm, and emission was monitored at 510 nm. Excitation and emission slits with slit widths of 3 nm were used for all measurements. The optical density of the samples measured at 490 nm was less than 0.15. Data shown in Fig. 2b represent means ± SE of at least three independent measurements.