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At least 19 recordsLinked to original sources
PubMed2001

Multiphoton fluorescence microscopy.

Multiphoton fluorescence microscopy has now become a relatively common tool among biophysicists and biologists. The intrinsic sectioning achievable by multiphoton excitation provides a simple means to excite a small volume inside cells and tissues. Multiphoton microscopes have a simplified optical path in the emission side due to the lack of an emission pinhole, which is necessary with normal confocal microscopes. This article illustrates examples in which this advantage in the simplified optics is exploited to achieve a new type of measurements. First, dual-emission wavelength measurements are used to identify regions of different phase domains in giant vesicles and to perform fluctuation experiments at specific locations in the membrane. Second, we show how dual-wavelength measurements are used in conjunction with scanning fluctuation analysis to measure the changes in the geometry of the domains and the incipient formation of gel domains when the temperature of the giant vesicles is gradually lowered.

Fluorescence Polarization↗
PubMed2003

Quantitative imaging of protein-protein interactions by multiphoton fluorescence lifetime imaging microscopy using a streak camera.

Fluorescence lifetime imaging microscopy (FLIM) using multiphoton excitation techniques is now finding an important place in quantitative imaging of protein-protein interactions and intracellular physiology. Recent developments in multiphoton FLIM methods are reviewed and a novel multiphoton FLIM system using a streak camera is described. An example of a typical application of the system is provided in which the fluorescence resonance energy transfer between a donor-acceptor pair of fluorescent proteins within a cellular specimen is measured.

Animals↗
PubMed2002

Fluorescence resonance energy transfer analysis of protein-protein interactions in single living cells by multifocal multiphoton microscopy.

Fluorescence resonance energy transfer (FRET) resolved by multifocal multiphoton microscopy (MMM) was successfully used to measure transport phenomena in living cells. We expressed different pairs of CFP-/YFP-fusion proteins involved in retrograde Golgi-to-ER transport to analyze sorting of the occupied KDEL-receptor into retrograde transport vesicles triggered by application of the external cholera toxin mutant CTXK63. FRET observed as a sensitized emission of the acceptor was confirmed by acceptor photobleaching and the dequenching of the donor was measured. FRET-MMM data obtained from single cells were compared with bulk cell experiments employing spectrofluorimetry. The importance of controlling the degree of overexpression of CFP-/YFP-fusion proteins for FRET analysis is stressed in this article. Using MMM we showed for the first time that FRET can be measured across the Golgi membrane. Finally, FRET-MMM records performed continuously over 2 h allowed to analyze intracellular retrograde transport and sorting events and to discuss these mechanisms on a single cell level.

Bacterial Proteins↗
PubMed2003

Nondiffusive mechanisms enhance protein uptake rates in ion exchange particles.

Scanning confocal fluorescence microscopy and multiphoton fluorescence microscopy were used to image the uptake of the protein lysozyme into individual ion exchange chromatography particles in a packed bed in real time. Self-sharpening concentration fronts penetrating into the particles were observed at low salt concentrations in all of the adsorbents studied, but persisted to 100 mM ionic strength only in some materials. In other adsorbents, diffuse profiles were seen at these higher salt concentrations, with the transition region exhibiting a pronounced fluorescence peak at the front at intermediate salt concentrations. These patterns in the uptake profiles are accompanied by significant increases in protein uptake rates that are also seen macroscopically in batch uptake experiments. The fluorescence peak appears to be a concentration overshoot that may develop, in part, from an electrokinetic contribution to transport that also enhances the uptake rate. Further evidence for an electrokinetic origin is that the effect is correlated with high adsorbent surface charge densities. Predictions of a mathematical model incorporating the electrokinetic effect are in qualitative agreement with the observations. These findings indicate that mechanisms other than diffusion contribute to protein transport in oppositely charged porous materials and may be exploited to achieve rapid uptake in process chromatography.

Diffusion↗
PubMed1997

Multiphoton excitation fluorescence microscopy and spectroscopy of in vivo human skin.

Multiphoton excitation microscopy at 730 nm and 960 nm was used to image in vivo human skin autofluorescence from the surface to a depth of approximately 200 microm. The emission spectra and fluorescence lifetime images were obtained at selected locations near the surface (0-50 microm) and at deeper depths (100-150 microm) for both excitation wavelengths. Cell borders and cell nuclei were the prominent structures observed. The spectroscopic data suggest that reduced pyridine nucleotides, NAD(P)H, are the primary source of the skin autofluorescence at 730 nm excitation. With 960 nm excitation, a two-photon fluorescence emission at 520 nm indicates the presence of a variable, position-dependent intensity component of flavoprotein. A second fluorescence emission component, which starts at 425 nm, is observed with 960-nm excitation. Such fluorescence emission at wavelengths less than half the excitation wavelength suggests an excitation process involving three or more photons. This conjecture is further confirmed by the observation of the super-quadratic dependence of the fluorescence intensity on the excitation power. Further work is required to spectroscopically identify these emitting species. This study demonstrates the use of multiphoton excitation microscopy for functional imaging of the metabolic states of in vivo human skin cells.

Biophysical Phenomena↗
PubMed2003

Fluorescence resonance energy transfer determinations using multiphoton fluorescence lifetime imaging microscopy to characterize amyloid-beta plaques.

We describe the implementation of a commercial fluorescence lifetime imaging microscopy (FLIM) instrument used in conjunction with a commercial laser scanning multiphoton microscope. The femtosecond-pulsed near-infrared laser is an ideal excitation source for time-domain fluorescence lifetime measurements. With synchronization from the x-y scanners, fluorescence lifetimes can be acquired on a pixel-by-pixel basis, with high spatial resolution. Multiexponential curve fits for each pixel result in two-dimensional fluorescence resonance energy transfer (FRET) measurements that allow the determination of both proximity of fluorescent FRET pairs, as well as the fraction of FRET pairs close enough for FRET to occur. Experiments are described that characterize this system, as well as commonly used reagents valuable for FRET determinations in biological systems. Constructs of CFP and YFP were generated to demonstrate FRET between this pair of green fluorescent protein (GFP) color variants. The lifetime characteristics of the FRET pair fluorescein and rhodamine, commonly used for immunohistochemistry, were also examined. Finally, these fluorophores were used to demonstrate spatially resolved FRET with senile plaques obtained from transgenic mouse brain. Together these results demonstrate that FLIM allows sensitive measurements of protein-protein interactions on a spatial scale less than 10 nm using commercially available components.

Alzheimer Disease↗
PubMed2002

Imaging cells and extracellular matrix in vivo by using second-harmonic generation and two-photon excited fluorescence.

Multiphoton microscopy relies on nonlinear light-matter interactions to provide contrast and optical sectioning capability for high-resolution imaging. Most multiphoton microscopy studies in biological systems have relied on two-photon excited fluorescence (TPEF) to produce images. With increasing applications of multiphoton microscopy to thick-tissue "intravital" imaging, second-harmonic generation (SHG) from structural proteins has emerged as a potentially important new contrast mechanism. However, SHG is typically detected in transmission mode, thus limiting TPEF/SHG coregistration and its practical utility for in vivo thick-tissue applications. In this study, we use a broad range of excitation wavelengths (730-880 nm) to demonstrate that TPEF/SHG coregistration can easily be achieved in unstained tissues by using a simple backscattering geometry. The combined TPEF/SHG technique was applied to imaging a three-dimensional organotypic tissue model (RAFT). The structural and molecular origin of the image-forming signal from the various tissue constituents was determined by simultaneous spectroscopic measurements and confirming immunofluorescence staining. Our results show that at shorter excitation wavelengths (<800 nm), the signal emitted from the extracellular matrix (ECM) is a combination of SHG and TPEF from collagen, whereas at longer excitation wavelengths the ECM signal is exclusively due to SHG. Endogenous cellular signals are consistent with TPEF spectra of cofactors NAD(P)H and FAD at all excitation wavelengths. The reflected SHG intensity follows a quadratic dependence on the excitation power, decays exponentially with depth, and exhibits a spectral dependence in accordance with previous theoretical studies. The use of SHG and TPEF in combination provides complementary information that allows noninvasive, spatially localized in vivo characterization of cell-ECM interactions in unstained thick tissues.

Animals↗
PubMedDate not supplied

Mapping piezoelectric-field distribution in gallium nitride with scanning second-harmonic generation microscopy.

Taking advantage of the electric field-enhanced second-harmonic generation effect in bulk gallium nitride (GaN) and indium gallium nitride (InGaN) quantum wells, we demonstrated the piezoelectric field distribution mapping in bulk GaN and InGaN multiple-quantum-well (MQW) samples using scanning second-harmonic generation (SHG) microscopy. Scanning SHG microscopy and the accompanying third-harmonic generation (THG) microscopy of the bulk GaN sample were demonstrated using a femtosecond Cr:forsterite laser at a wavelength of 1230 nm. Taking advantage of the off-resonant electric field-enhanced SHG effect and the bandtail state-resonance THG effect, the second- and third-harmonic generation microscopic images obtained revealed the piezoelectric field and bandtail state distributions in a GaN sample. Combined with 720 nm wavelength excited two-photon fluorescence microscopy in the same sample, the increased defect density around the defect area was found to suppress bandedge photoluminescence, to increase yellow luminescence, to increase bandtail state density, and to decrease residue piezoelectric field intensity. Scanning SHG microscopy of the InGaN MQW sample was resonant excited with 800 nm femtosecond pulses from a Ti:sapphire laser in order to suppress SHG contribution from the bulk GaN substrate. Taking advantage of the strong piezoelectric field inside the InGaN quantum well, the wavelength resonant effect, and the electric field-enhanced SHG effect of InGaN quantum wells, resonant scanning SHG microscopy revealed the piezoelectric field distribution inside the wells. Combined with accompanying three-photon fluorescence microscopy from the bulk GaN substrate underneath the quantum wells, the direct correspondence between the piezoelectric field strength inside the quantum well and the substrate quality can be obtained. According to our study, the GaN substrate area with bright bandedge luminescence corresponds to the area with strong SHG signals indicating a higher stained-induced piezoelectric field. These scanning harmonic generation microscopies exhibit superior images of the piezoelectric field and defect state distributions in GaN and InGaN MQWs not available before. Combining with scanning multiphoton fluorescence microscopy, these techniques open new ways for the physical property study of this important material system and can provide interesting details that are not readily available by other microscopic techniques.

Journal Article↗
PubMed2003

Multiphoton endoscopy.

Despite widespread use of multiphoton fluorescence microscopy, development of endoscopes for nonlinear optical imaging has been stymied by the degradation of ultrashort excitation pulses that occurs within optical fiber as a result of the combined effects of group-velocity dispersion and self-phase modulation. We introduce microendoscopes (350-1000 microm in diameter) based on gradient-index microlenses that effectively eliminate self-phase modulation within the endoscope. Laser-scanning multiphoton fluorescence endoscopy exhibits micrometer-scale resolution. We used multiphoton endoscopes to image fluorescently labeled neurons and dendrites.

Animals↗
PubMed2000

Single granule pH cycling in antigen-induced mast cell secretion.

The pH cycling of individual granules in secreting (serotonin-loaded) mast cells is quantitatively examined using multicolor multiphoton fluorescence microscopy. A typical exocytosis event consists of maximal calcium rise at time zero, granule alkalization a few seconds later and, finally, complete contents release at a fraction of a second after alkalization. Membrane fusion is either transient, as indicated by subsequent granule reacidification, or 'full', as indicated by a granule disappearance with a collapse of its membrane into the plasma membrane. The relative frequency of these two coexisting behaviors (the 'kiss-to-collapse' ratio) is approximately 2:1. A typical transiently fusing granule experiences multiple alkalization/acidification cycles after addition of exogenous antigen. Between recycling granules, coalescence events are frequent, with 80% resulting in a collapse of the formed granule complex to the plasma membrane. The full dynamics of secretion encompass a complex combination of these granule activities.

Acridine Orange↗
PubMed2003

Imaging the effects of anti-angiogenic treatments.

It is clear that various imaging modalities have given keen insight into the molecular mechanisms involved in anti-angiogenic treatments. A key to the advancement of anti-angiogenic therapy is not only the discovery of new drugs and treatments, but the analysis of the specific modes of action of these compounds in order to produce the next generation with greater effectiveness. While existing clinical methods incorporate the analysis of serum and urine to measure angiogenic factors, an imaging technique monitoring the effectiveness of anti-angiogenic therapy would be a convenient, noninvasive, cost effective technique to aid in treatment planning and disease management.

Angiogenesis Inhibitors↗
PubMed2003

Live tissue intrinsic emission microscopy using multiphoton-excited native fluorescence and second harmonic generation.

Multicolor nonlinear microscopy of living tissue using two- and three-photon-excited intrinsic fluorescence combined with second harmonic generation by supermolecular structures produces images with the resolution and detail of standard histology without the use of exogenous stains. Imaging of intrinsic indicators within tissue, such as nicotinamide adenine dinucleotide, retinol, indoleamines, and collagen provides crucial information for physiology and pathology. The efficient application of multiphoton microscopy to intrinsic imaging requires knowledge of the nonlinear optical properties of specific cell and tissue components. Here we compile and demonstrate applications involving a range of intrinsic molecules and molecular assemblies that enable direct visualization of tissue morphology, cell metabolism, and disease states such as Alzheimer's disease and cancer.

Alzheimer Disease↗
PubMed2002

Phase sensitive demodulation in multiphoton microscopy.

Multiphoton laser scanning microscopy offers advantages in depth of penetration into intact samples over other optical sectioning techniques. To achieve these advantages it is necessary to detect the emitted light without spatial filtering. In this nondescanned (nonconfocal) approach, ambient room light can easily contaminate the signal, forcing experiments to be performed in absolute darkness. For multiphoton microscope systems employing mode-locked lasers, signal processing can be used to reduce such problems by taking advantage of the pulsed characteristics of such lasers. Specifically, by recovering fluorescence generated at the mode-locked frequency, interference from stray light and other ambient noise sources can be significantly reduced. This technology can be adapted to existing microscopes by inserting demodulation circuitry between the detector and data collection system. The improvement in signal-to-noise ratio afforded by this approach yields a more robust microscope system and opens the possibility of moving multiphoton microscopy from the research lab to more demanding settings, such as the clinic.

Amplifiers, Electronic↗
PubMed2003

Monte Carlo simulation of multiphoton fluorescence microscopic imaging through inhomogeneous tissuelike turbid media.

Image resolution and signal level in fluorescence microscopy through inhomogeneous turbid media consisting of scatterers of multiple sizes under single- (1p), two- (2p), and three-photon (3p) excitation have been investigated based on a modified Monte Carlo model. The effects of the size distribution and the concentration distribution of scattering particles are explored. Simulation results reveal that the size and the concentration distribution both have an impact on image formation in media consisting of small particles and that 3p excitation has the most significant impact. In media with scatterers of a large size, both size and concentration distributions lead to a slight effect. Image formation in a mixed medium containing small and large scattering particles is more affected by the large particles.

Anisotropy↗
PubMed2002

Advantages and risks of multiphoton microscopy in physiology.

Multiphoton microscopy is based on the simultaneous absorption of two photons emitted by a pulsed infrared laser source. In this technique, the excitation is restricted to a very small focus and thus results in optical sectioning a priori without the need of a confocal aperture. Multiphoton microscopy was introduced in live cell imaging as an alternative to confocal microscopy due to its superior qualities, such as the deep penetration depth, the reduced photodamage and the lack of out-of-focus bleaching. However, during the past years, examinations revealed severe limitations to the initial expectations. In the focal plane, photodamage and photobleaching can be worse than in single photon microscopy. However, studies showed that with low excitation intensity and by special technical adaptations photodamage could be avoided successfully. For functional biological imaging multiphoton excitation provides an excellent tool such as the release of caged compounds in a diffraction-limited volume combined with multiphoton or confocal imaging.

Animals↗
PubMed2002

New modal wave-front sensor: application to adaptive confocal fluorescence microscopy and two-photon excitation fluorescence microscopy.

Confocal and multiphoton microscopes are particularly sensitive to specimen- or system-induced aberrations, which result in decreased resolution and signal-to-noise ratio. The inclusion of an adaptive optics correction system could help overcome this limitation and restore diffraction-limited performance, but such a system requires a suitable method of wave-front measurement. By extending the concept of a modal wave-front sensor previously described by Neil et al. [J. Opt. Soc. Am. A 17, 1098-1107 (2000)], we present a new sensor capable of measuring directly the Zernike aberration modes introduced by a specimen. This modal sensor is particularly suited to applications in three-dimensional microscopy because of its inherent axial selectivity; only those wave fronts originating in the focal region contribute to the measured signal. Four wave-front sensor configurations are presented and their input response is characterized. Sensitivity matrices and axial responses are presented.

Microscopy, Confocal↗