Search PubMed⌕ Search

PubMed · 10652007

Multiple frequency fluorescence lifetime imaging microscopy.

Abstract

The experimental configuration and the computational algorithms for performing multiple frequency fluorescence lifetime imaging microscopy (mfFLIM) are described. The mfFLIM experimental set-up enables the simultaneous homodyne detection of fluorescence emission modulated at a set of harmonic frequencies. This was achieved in practice by using monochromatic laser light as an excitation source modulated at a harmonic set of frequencies. A minimum of four frequencies were obtained by the use of two standing wave acousto-optic modulators placed in series. Homodyne detection at each of these frequencies was performed simultaneously by mixing with matching harmonics present in the gain characteristics of a microchannel plate (MCP) image intensifier. These harmonics arise as a natural consequence of applying a high frequency sinusoidal voltage to the photocathode of the device, which switches the flow of photoelectrons 'on' and 'off' as the sinus voltage swings from negative to positive. By changing the bias of the sinus it was possible to control the duration of the 'on' state of the intensifier relative to its 'off' state, enabling the amplitude of the higher harmonic content in the gain to be controlled. Relative modulation depths of 400% are theoretically possible from this form of square-pulse modulation. A phase-dependent integrated image is formed by the sum of the mixed frequencies on the phosphor of the MCP. Sampling this signal over a full period of the fundamental harmonic enables each harmonic to be resolved, provided that the Nyquist sampling criterion is satisfied for the highest harmonic component in the signal. At each frequency both the phase and modulation parameters can be estimated from a Fourier analysis of the data. These parameters enable the fractional populations and fluorescence lifetimes of individual components of a complex fluorescence decay to be resolved on a pixel-by-pixel basis using a non-linear fit to the dispersion relationships. The fitting algorithms were tested on a simulated data set and were successful in disentangling two populations having 1 ns and 4 ns fluorescence lifetimes. Spatial invariance of the lifetimes was exploited to improve the accuracy significantly. Multiple frequency fluorescence lifetime imaging microscopy was then successfully applied to resolve the fluorescence lifetimes and fluorescence intensity contributions in a rhodamine dye mixture in solution, and green fluorescent protein variants co-expressed in live cells.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

A Squire, P J Verveer, P I Bastiaens. 2000. Multiple frequency fluorescence lifetime imaging microscopy.. https://doi.org/10.1046/j.1365-2818.2000.00651.x

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related citations

Rational synthesis of beta-substituted chlorin building blocks.

Chlorins bearing synthetic handles at specific sites about the perimeter of the macrocycle constitute valuable building blocks. We previously developed methodology for preparing meso-substituted chlorin building blocks and now present methodology for preparing several complementary beta-substituted chlorin building blocks. The chlorins bear one or two beta substituents, one meso substituent, a geminal dimethyl group to lock in the chlorin hydrogenation level, and no flanking meso and beta substituents. The synthesis involves convergent joining of an Eastern half and a Western half. New routes have been developed to two beta-substituted bromo-dipyrromethane monocarbinols (Eastern halves). A new beta-substituted Western half was prepared following the method for preparing an unsubstituted Western half (3,3-dimethyl-2,3-dihydrodipyrrin). Chlorin formation is achieved by a two-flask process of acid-catalyzed condensation followed by metal-mediated oxidative cyclization. beta-Substituted chlorins have been prepared in 18-24% yield bearing a 4-iodophenyl group at the 8-position, a 4-iodophenyl group or a 4-[2-(trimethylsilyl)ethynyl]phenyl group at the 12-position, and a 4-iodophenyl group and a 4-[2-(trimethylsilyl)ethynyl]phenyl group at diametrically opposed beta-positions (2, 12). The latter building block makes possible the stepwise construction of linear multi-chlorin architectures. The chlorins exhibit typical absorption and fluorescence spectra. A systematic shift in the absorption maximum (637-655 nm for the free base chlorins, 606-628 nm for the zinc chlorins) and intensity of the chlorin Q(y)() band (epsilon up to 79 000 M(-)(1) cm(-)(1)) is observed depending on the location of the substituents. The characteristic spectral features and location of substituents in defined positions make these chlorins well suited for a variety of applications in biomimetic and materials chemistry.

Fluorescence↗

Pathogenic alpha 1-antitrypsin polymers are formed by reactive loop-beta-sheet A linkage.

alpha(1)-Antitrypsin is the most abundant circulating protease inhibitor and the archetype of the serine protease inhibitor or serpin superfamily. Members of this family may be inactivated by point mutations that favor transition to a polymeric conformation. This polymeric conformation underlies diseases as diverse as alpha(1)-antitrypsin deficiency-related cirrhosis, thrombosis, angio-edema, and dementia. The precise structural linkage within a polymer has been the subject of much debate with evidence for reactive loop insertion into beta-sheet A or C or as strand 7A. We have used site directed cysteine mutants and fluorescence resonance energy transfer (FRET) to measure a number of distances between monomeric units in polymeric alpha(1)-antitrypsin. We have then used a combinatorial approach to compare distances determined from FRET with distances obtained from 2.9 x 10(6) different possible orientations of the alpha(1)-antitrypsin polymer. The closest matches between experimental FRET measurements and theoretical structures show conclusively that polymers of alpha(1)-antitrypsin form by insertion of the reactive loop into beta-sheet A.

Fluorescence↗

Rapid kinetics of regulator of G-protein signaling (RGS)-mediated Galphai and Galphao deactivation. Galpha specificity of RGS4 AND RGS7.

Regulator of G-protein signaling (RGS) proteins accelerate GTP hydrolysis by Galpha subunits speeding deactivation. Galpha deactivation kinetics mediated by RGS are too fast to be directly studied using conventional radiochemical methods. We describe a stopped-flow spectroscopic approach to visualize these rapid kinetics by measuring the intrinsic tryptophan fluorescence decrease of Galpha accompanying GTP hydrolysis and Galpha deactivation on the millisecond time scale. Basal k(cat) values for Galpha(o), Galpha(i1), and Galpha(i2) at 20 degrees C were similar (0.025-0.033 s(-1)). Glutathione S-transferase fusion proteins containing RGS4 and an RGS7 box domain (amino acids 305-453) enhanced the rate of Galpha deactivation in a manner linear with RGS concentration. RGS4-stimulated rates could be measured up to 5 s(-1) at 3 microm, giving a catalytic efficiency of 1.7-2.8 x 10(6) m(-1) s(-1) for all three Galpha subunits. In contrast, RGS7 showed catalytic efficiencies of 0.44, 0.10, and 0.02 x 10(6) m(-1) s(-1) toward Galpha(o), Galpha(i2), and Galpha(i1), respectively. Thus RGS7 is a weaker GTPase activating protein than RGS4 toward all Galpha subunits tested, but it is specific for Galpha(o) over Galpha(i1) or Galpha(i2). Furthermore, the specificity of RGS7 for Galpha(o) does not depend on N- or C-terminal extensions or a Gbeta(5) subunit but resides in the RGS domain itself.

Fluorescence↗