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J R Lakowicz

Publications and source records attributed to J R Lakowicz.

At least 109 records · Page 6Linked to original sources

Fluorescence anisotropy of tyrosine using one-and two-photon excitation.

We examined the emission spectra and steady-state anisotropy of tyrosyl fluorescence with two-photon excitation from 565 to 578 nm. The emission spectra of phenol and N-acetyl-L-tyrosinamide (NATyrA) were all the same for one-photon excitation (OPE) and two-photon excitation (TPE), and the tyrosine emission from ribonuclease A showed 10-nm shift to longer wavelengths with TPE. Surprisingly, the anisotropy of tyrosine, NATyrA and Leu5-enkephalin in frozen solution were near zero for TPE as compared to near 0.3 for OPE. Low values of the anisotropy near 0.05 were also found for phenol and ribonuclease A. A low anisotropy appears to be a basic characteristic of tyrosine or tyrosyl residues with two-photon excitation.

Biophysical Phenomena↗

Sensing oxygen through skin using a red diode laser and fluorescence lifetimes.

The most difficult impediments to transcutaneous optical sensing are the absorbance and scatter of light caused by skin and the lack of fluorescent sensing probes which can be excited at wavelengths over 600 nm. Furthermore, current optical sensing techniques rely on absorbance or fluorescence intensity measurements, both of which are sensitive to drifts in lamp intensity, changes in probe concentration and inner filter effects. We demonstrate oxygen sensing through a layer of skin by using red light which readily penetrates skin as diffusely scattered light. The oxygen sensitive osmium-ligand complex used in this study can be excited at 635-680 nm. In addition, we measure fluorescence lifetimes, which are inherently unaffected by factors that limit absorbance and fluorescence intensity measurements. By using phase fluorimetry and long lived fluorophores, we are able to demonstrate the potential for subdermal oxygen sensing with simple and inexpensive instrumentation. This work describes a paradigm for future non-invasive measurements of other analytes.

Biosensing Techniques↗

Metal-ligand complexes as a new class of long-lived fluorophores for protein hydrodynamics.

We describe the use of asymmetric Ru-ligand complexes as a new class of luminescent probes that can be used to measure rotational motions of proteins. These complexes are known to display luminescent lifetimes ranging from 10 to 4000 ns. In this report, we show that the asymmetric complex Ru(bpy)2(dcbpy) (PF6)2 displays a high anisotropy value when excited in the long wavelength absorption band. For covalent linkage to proteins, we synthesized the N-hydroxy succinimide ester of this metal-ligand complex. To illustrate the usefulness of these probes, we describe the intensity and anisotropy decays of [Ru(bpy)2(dcbpy)] when covalently linked to human serum albumin, concanavalin A (ConA), human immunoglobulin G (IgG), and Ferritin, and measured in solutions of increased viscosity. These data demonstrate that the probes can be used to measure rotational motions on the 10 ns to 1.5 microseconds timescale, which so far has been inaccessible using luminescence methods. The present probe [Ru(bpy)2(dcbpy)] can be regarded as the first of a class of metal-ligand complexes, each with different chemical reactivity and spectral properties, for studies of macromolecular dynamics.

Biophysical Phenomena↗

Fluorescence lifetime-based sensing in tissues: a computational study.

We have numerically solved the photon diffusion equation to predict the distribution of light in a tissue model system with a uniform concentration of fluorophore. Our results show that time-dependent measurements of light propagation can be used to monitor the fluorescent lifetimes of a uniformly distributed fluorophore in tissues. With proper referencing, frequency-domain measurements of phase-shift, theta, may allow quantitation of fluorescent lifetimes, tau, independent of changes in the local absorption and scattering properties. These results point to a new approach for noninvasive diagnostic monitoring through quantitation of fluorescent lifetime, tau, when the lifetime of the fluorophore is comparable with photon migration times.

Biophysical Phenomena↗

Potential applications of lifetime-based, phase-modulation fluorimetry in bioprocess and clinical monitoring.

The measurement of analyte concentration is a critical part of successful bioreactor and clinical monitoring. Although strategies exist for measuring the majority of relevant analytes, industrial on-line bioreactor control is carried out primarily by measurement and control of pH, pO2 and, in some cases, cell density. This is because the available technology cannot be easily and inexpensively adapted to (a) measure the analyte in an aseptic manner and/or allow for remote sensing, and (b) measure in real time so that on-line control is possible. Similar issues need to be addressed for biosensors for clinical applications. A rapidly emerging technology that has the potential of meeting these challenges is liftime-based phase-modulation fluorimetry, an optical technique that uses the measurement of fluorescence lifetime rather than intensity for determining the concentration of an analyte.

Biosensing Techniques↗

Fluorescence of tyrosine and tryptophan in proteins using one- and two-photon excitation.

We examined the emission spectra of tyrosine- and tryptophan-containing proteins using one-photon (270-310 nm) and two-photon (565-610 nm) excitation. Emission spectra for two-photon excitation of native and denatured human serum albumin and of three purine nucleoside phosphorylases indicated an absence of the tyrosine emission normally seen for one-photon excitation below 290 nm. We examined the one-photon and two-photon excitation spectra of tyrosine-tryptophan mixtures to determine the origin of selective excitation of the tryptophan residues. These results confirmed a short-wavelength shift of the tyrosine two-photon excitation spectrum relative to that of tryptophan, as recently reported by Rehms and Callis (1993) Chem. Phys. Lett. 208, 276-282.

Animals↗

On the possibility of calcium imaging using Indo-1 with three-photon excitation.

We show that the calcium fluorophore Indo-1 can be excited by simultaneous absorption of three-photons at 885 nm, a wavelength readily available from Ti:sapphire lasers. Three-photon excitation was demonstrated by the emission intensity of Indo-1 which depended on the cube of the laser power, and by a higher anisotropy than was observed for two-photon excitation. Excitation of Indo-1 becomes a two-photon process when the wavelength is decreased to 820 nm. Three-photon excitation was accomplished at a low 17 microM concentration of Indo-1. Examination of the spatial profile of the excited Indo-1 showed a smaller volume for three- versus two-photon excitation. These results suggest that three-photon excitation may be useful in fluorescence microscopy using the long wavelength output of Ti:sapphire lasers, and may provide higher spatial resolution than available using two-photon excitation.

Calcium↗

Distribution of distances between the tryptophan and the N-terminal residue of melittin in its complex with calmodulin, troponin C, and phospholipids.

We used frequency-domain measurements of fluorescence resonance energy transfer to measure the distribution of distances between Trp-19 of melittin and a 1-dimethylamino-5-sulfonylnaphthalene (dansyl) residue on the N-terminal-alpha-amino group. Distance distributions were obtained for melittin free in solution and when complexed with calmodulin (CaM), troponin C (TnC), or palmitoyloleoyl-L-alpha-phosphatidylcholine (POPC) vesicles. A wide range of donor (Trp-19)-to-acceptor (dansyl) distances was found for free melittin, which is consistent with that expected for the random coil state, characterized by a Gaussian width (full width at half maxima) of 28.2 A. In contrast, narrow distance distributions were found for melittin complexed with CaM, 8.2 A, or with POPC vesicles, 4.9 A. A somewhat wider distribution was found for the melittin complex with TnC, 12.8 A, suggesting the presence of heterogeneity in the mode of binding between melittin and TnC. For all the complexes the mean Trp-19 to dansyl distance was near 20 A. This value is somewhat smaller than expected for the free alpha-helical state of melittin, suggesting that binding with CaM or TnC results in a modest decrease in the length of the melittin molecule.

Calmodulin↗

Synthesis of squaraine-N-hydroxysuccinimide esters and their biological application as long-wavelength fluorescent labels.

We describe the synthesis and the fluorescence spectral characterization of two conjugatable long-wavelength fluorescence probes. These probes consist of a squaraine moiety, which is a cyanine-type chromophore with a central squarate bridge, and a reactive N-hydroxysuccinimide group for coupling with amino functions. One form is water soluble due to the presence of a sulfobutyl group; the other is water insoluble. The water-insoluble form was reacted with taurine to achieve water solubility and this squaraine-taurine conjugate displayed a very high affinity for bovine serum albumin. The squaraines exhibit short lifetimes and low quantum yields in water, with a significant increase in lifetime and quantum yield when bound to proteins. Their absorption maxima around 635 nm in water and 640 nm when bound to proteins allow excitation with the newly commercially available diode laser sources at 635, 645, and 650 nm. The spectral properties and photostabilities of the water-soluble squaraine probes are compared with those of the commercially available CY5-NHS ester.

Cyclobutanes↗

Fluorescence lifetime imaging of intracellular calcium in COS cells using Quin-2.

We describe the first fluorescence lifetime images of cells. To demonstrate this new capability we measured intracellular images of Ca2+ in COS cells based on the Ca(2+)-dependent fluorescence lifetime of Quin-2. Apparent fluorescence lifetimes were measured by the phase-modulation method using a gain-modulated image intensifier and a slow-scan CCD camera. We describe methods to correct the images for photobleaching during acquisition of the data, and to correct for the position-dependent response of the image intensifier. The phase angle Quin-2 images were found to yield lower than expected Ca2+ concentrations, which appears to be the result of the formation of fluorescent photoproducts by Quin-2. Fluorescence lifetime imaging (FLIM) does not require wavelength-radiometric probes and appears to provide new opportunities for chemical imaging of cells.

Animals↗

Light quenching and depolarization of fluorescence observed with laser pulses. A new experimental opportunity in time-resolved fluorescence spectroscopy.

We report the first time-resolved studies of quenching of fluorescence by light, i.e., "light quenching". The dye 4-(dicyanomethylene)-2-methyl-6-(p-dimethamino)-4H-pyrane (DCM) was excited in the anti-Stokes region from 560-600 nm. At high illumination power the intensities of DCM were sub-linear with incident power. The extent of light quenching was proportional to the emission spectrum at the incident wavelength, as expected for light-stimulated decay from the excited state. The frequency-domain intensity decays indicated the effect was not due to heating or other photochemical effects. Importantly, the decay time was unchanged, as expected for light quenching with a single pulsed laser beam, while the time-zero anisotropy was decreased due to orientation-dependent quenching of the excited state population. Light quenching of fluorescence provides a new method to control the excited state population and orientation of fluorophores, and offers new experimental opportunities for biophysical applications of time-resolved fluorescence.

Anisotropy↗

Analysis of anisotropy decays in terms of correlation time distributions, measured by frequency-domain fluorometry.

We describe the theory and practical aspects of analyzing fluorescence anisotropy decays in terms of correlation times distributions. In our model the rotational motions of the fluorophores were described using Gaussian or Lorentzian distributions of the correlation times. The theory is presented both for time and frequency-domain measurements, although the simulations and measurements are focused on the frequency-domain measurements of the anisotropy decays. Analysis of simulated data is presented to illustrate the nature of the data and the resolution which can be expected with presently available frequency-domain measurements. Additionally, we describe experimental data for samples where one can reasonably expect a single exponential and/or discrete multi-exponential correlation time distributions, and for samples where the anisotropy decay might be expected to display a distribution of correlation times. These samples include small single tryptophan peptides in propylene glycol, the single tryptophan residue in S. Nuclease, and the single tryptophan residue in the native and partially unfolded states of ribonuclease T1.

Amino Acid Sequence↗

Theory of light quenching: effects of fluorescence polarization, intensity, and anisotropy decays.

Experimental studies have recently demonstrated that fluorescence emission can be quenched by laser light pulses from modern high repetition rate lasers, a phenomenon we call "light quenching." We now describe the theory of light quenching and some of its effects on the steady-state and time-resolved intensity and anisotropy decays of fluorophores. Light quenching can decrease or increase the steady-state or time-zero anisotropy. Remarkably, the light quenching can break the usual z axis symmetry of the excited-state population, and the emission polarization can range from -1 to +1 under selected conditions. The measured anisotropy (or polarization) depends upon whether the observation axis is parallel or perpendicular to the propagation direction of the light quenching beam. The effects of light quenching are different for a single pulse, which results in both excitation and quenching, as compared with a time-delayed quenching pulse. Time-delayed light quenching pulses can result in step-like changes in the time-dependent intensity or anisotropy and are predicted to cause oscillations in the frequency-domain intensity and anisotropy decays. The increasing availability of pulsed laser sources offers the opportunity for a new class of two-pulse or multiple-pulse experiments where the sample is prepared by an excitation pulse, the excited state population is modified by the quenching pulse(s), followed by time- or frequency-domain measurements of the resulting emission.

Biophysical Phenomena↗

Fluorescence lifetime imaging microscopy: homodyne technique using high-speed gated image intensifier.

In the previous sections we demonstrated imaging of intracellular Ca2+ using our approach to FLIM. What other analytes can be imaged using FLIM? We have now characterized the lifetime of a good number of ion indicators. Based on these studies we know that Cl- can be imaged using FLIM with probes such as SPQ or MQAE, pH can be imaged using resorufin and probes of the SNAFL and SNARF (Molecular Probes) series, and Mg2+ can be imaged using Magnesium Green, Mag-quin-2, or Mag-quin-1 (Molecular Probes). At present, the probe for K+, as PBFI, are just adequate as a lifetime probe, but it seems likely that newer probes for Na+ (Sodium Green) and K+ will be practical for effective imaging. Of course, imaging of oxygen is possible using a wide variety of fluorophores. It should be noted that a wide variety of substances and/or phenomena are known to alter decay times, acting as quenchers. These include the phenomena of resonance energy transfer, collisional quenching, temperature effects, and viscosity effects. Also, the FLIM method is not limited to microscopic objects but can be possibly used in remote imaging of any object. Hence, FLIM will allow the imaging of the chemical and physical properties of objects based on the effects of the local environment on the decay kinetics of fluorophores. The instrumentation for FLIM is presently complex and requires a moderately complex laser source, a gain-modulated image intensifier, and a slow-scan CCD camera. However, one can readily imagine the instrumentation becoming rather compact, and even all solid-state, owing to advances in laser and CCD technologies and, more importantly, advances in probe chemistry. To be specific, the dye laser shown in Fig. 1 may be replaced by a simpler UV laser, such as the 354 nm HeCd laser which has become available (Fig. 11). Intensity modulation of a continuous wave sources can be accomplished with acoustooptic modulators. The scientific slow-scan CCD cameras are presently rather expensive, but they are used in the present instrumentation because of their linearity and high dynamic range. However, the increasing use of CCD detectors suggest that even the scientific-grade CCD cameras will soon become less costly. Additionally, the frame rates of these detectors continue to increase in response to the need for faster imaging. Furthermore, the performance of the video CCD cameras is increasing, as seen by the introduction of 10-bit video analog-to-digital (A/D) converters.(ABSTRACT TRUNCATED AT 400 WORDS)

Aminoquinolines↗

Site-to-site diffusion in proteins as observed by energy transfer and frequency-domain fluorometry.

We report measurements of the site-to-site diffusion coefficients in proteins and model compounds, which were measured using time-dependent energy transfer and frequency-domain fluorometry. The possibility of measuring these diffusion coefficients were shown from simulations, which demonstrate that donor (D)-to-acceptor (A) diffusion alters the donor frequency response, and that this effect is observable in the presence of a distribution of donor-to-acceptor distances. For decay times typical of tryptophan fluorescence, the simulations indicate that D-A diffusion coefficients can be measured ranging from 10(-7) to 10(-5) cm2/s. This possibility was verified by studies of a methylene-chain linked D-A pair in solutions of varying viscosity. The D-A diffusion was also measured for two labeled peptides and two proteins, melittin and troponin I. In most cases we used global analysis of data sets obtained with varying amounts of collisional quenchers to vary the donor decay time. Unfolding of troponin I results in more rapid D-A diffusion, whereas for melittin more rapid diffusion was observed in the alpha-helical state but over a limited range of distances.

Diffusion↗

Distance-dependent fluorescence quenching of tryptophan by acrylamide.

We used GHz frequency-domain fluorometry to investigate the time-dependent intensity decays of N-acetyl-L-trytophanamide (NATA) when collisionally quenched by acrylamide in propylene glycol at 20 degrees C. The intensity decays of NATA became increasingly heterogeneous in the presence of acrylamide. The NATA intensity decays were not consistent with the Collins-Kimball radiation boundary condition (RBC) model for quenching. The steady-state Stern-Volmer plots show significant upward curvature. At low temperature in vitrified propylene glycol (-60%), where translational diffusion cannot occur during the lifetime of the excited state, quenching of NATA by acrylamide was observed. The Smoluchowski and RBC quenching models do not predict any quenching in the absence of translational diffusion. Hence, these frequency-domain and steady-state data indicate a through-space quenching interaction between NATA and acrylamide. The rate for quenching of NATA by acrylamide appears to depend exponentially on the fluorophore-quencher separation distance. Comparison of the time-resolved and steady-state data provides a sensitive method to determine the distance dependence of the fluorophore-quencher interaction. The distance-dependent rate of quenching also explains the upward curvature of the Stern-Volmer plot, which is often observed for quenching by acrylamide. These results suggest that the distance-dependent quenching rates need to be considered in the interpretation of quenching data of proteins by acrylamide.

Acrylamide↗