High-speed, low-photodamage nonlinear imaging using passive pulse splitters

Pulsed lasers are key elements in nonlinear bioimaging techniques such as two-photon fluorescence excitation (TPE) microscopy. Typically, however, only a percent or less of the laser power available can be delivered to the sample before photoinduced damage becomes excessive. Here we describe a passive pulse splitter that converts each laser pulse into a fixed number of sub-pulses of equal energy. We applied the splitter to TPE imaging of fixed mouse brain slices labeled with GFP and show that, in different power regimes, the splitter can be used either to increase the signal rate more than 100-fold or to reduce the rate of photobleaching by over fourfold. In living specimens, the gains were even greater: a ninefold reduction in photobleaching during in vivo imaging of Caenorhabditis elegans larvae, and a six- to 20-fold decrease in the rate of photodamage during calcium imaging of rat hippocampal brain slices.     

Photobleaching in two-photon excitation microscopy

The intensity-squared dependence of two-photon excitation in laser scanning microscopy restricts excitation to the focal plane and leads to decreased photobleaching in thick samples. However, the high photon flux used in these experiments can potentially lead to higher-order photon interactions within the focal volume. The excitation power dependence of the fluorescence intensity and the photobleaching rate of thin fluorescence samples ( approximately 1 microm) were examined under one- and two-photon excitation. As expected, log-log plots of excitation power versus the fluorescence intensity and photobleaching rate for one-photon excitation of fluorescein increased with a slope of approximately 1. A similar plot of the fluorescence intensity versus two-photon excitation power increased with a slope of approximately 2. However, the two-photon photobleaching rate increased with a slope > or =3, indicating the presence of higher-order photon interactions. Similar experiments on Indo-1, NADH, and aminocoumarin produced similar results and suggest that this higher-order photobleaching is common in two-photon excitation microscopy. As a consequence, the use of multi-photon excitation microscopy to study thin samples may be limited by increased photobleaching.     

Dimethyl-pepep: a DNA probe in two-photon excitation cellular imaging

Dimethyl-pepep (D-pepep), a newly developed and very efficient two-photon absorber, has been tested here for two-photon excitation (TPE) cellular imaging. The spectral characteristics of the dye following one-photon excitation (OPE) and TPE (excitation and emission spectra, fluorescence lifetime, molecular brightness, saturation intensity) are reported. In vitro interaction studies with biomolecules show that dimethyl-pepep has a large affinity for DNA. A comparison with a widely used DNA stainer, 4-6-diamidino-2-phenylindole (DAPI) bound to DNA shows that the D-pepep brightness is one order of magnitude higher than that of DAPI, making this dye suitable for microscopy and imaging applications. TPE images taken from double-stained yeast Saccharomyces cerevisiae cells have revealed that D-pepep localizes mainly in the nucleus, similarly to DAPI, and in mitochondria, although to a minor extent. Preliminary tests have shown that the dye cellular toxicity is negligible.     

The Effect of Aspect Ratio of Gold Nanorods on Cell Imaging with Two-Photon Excitation

To make the gold nanorod (AuNR) a better photoluminescence (PL) probe for cell imaging under two-photon excitation (TPE), the effect of the aspect ratio of AuNRs was studied. The AuNRs with the aspect ratios of 2.7, 3.2, 4.1, and 4.5 and correlated longitudinal surface plasmon resonance (LSPR) bands of 710, 760, 820, and 870 nm were compared. The approach of two-photon excited PL was used to measure the two-photon absorption cross section (TPACS) of these AuNRs in aqueous solutions. Under TPE of an 800-nm femtosecond laser, the TPACS of AuNRs with an aspect ratio of 3.2 was found to be the highest (about 3?×?10⁹ GM), and that of AuNRs (aspect ratio of 2.7) was only 1.5?×?10⁹ GM. The probe function of these two AuNRs was further compared in cell imaging studies using the human liver cancer cell (QGY) as the cell model. Both TPE PL image and confocal reflectance image of AuNR-loaded cells were acquired comparatively in measurements. The brightness and contrast of confocal reflectance images for these two AuNRs in cells are similar. In contrast, the PL images of cellular AuNRs (2.7) under TPE of 800 nm are weak but that of cellular AuNRs (3.2) is much better. These results show that when the LSPR band of AuNRs is coincided with the excitation wavelength, the TPACS of these AuNRs will be enhanced ensuring a good quality of cell imaging under TPE. The LSPR band is correlated to the aspect ratio of AuNRs. Therefore, in cell imaging studies with TPE, the aspect ratio effect of AuNRs should be taken into consideration.     

Major signal increase in fluorescence microscopy through dark-state relaxation

We report a substantial signal gain in fluorescence microscopy by ensuring that transient molecular dark states with lifetimes >1 micros, such as the triplet state relax between two molecular absorption events. For GFP and Rhodamine dye Atto532, we observed a 5-25-fold increase in total fluorescence yield before molecular bleaching when strong continuous-wave or high-repetition-rate pulsed illumination was replaced with pulses featuring temporal pulse separation >1 micros. The signal gain was observed both for one- and two-photon excitation. Obeying dark or triplet state relaxation in the illumination process signifies a major step toward imaging with low photobleaching and strong fluorescence fluxes.     

Characterization of a range of fura dyes with two-photon excitation

Two-photon excitation (TPE) spectra of Fura-2, -4F, -6F, -FF, and Furaptra were characterized using a tunable (750-850 nM) ultra-short pulse laser. Two-photon fluorescence of these dyes was studied in free solution and in the cytosol of isolated rabbit ventricular cardiomyocytes. The TPE spectra of the Ca(2+)-free and Ca(2+)-bound forms of the dyes were measured in free solution and expressed in terms of the two-photon fluorescence cross section (Goppert-Meyer units). The Fura dyes displayed the same Ca(2+)-free TPE spectrum in the intracellular volume of permeabilized and intact cardiomyocytes. Fluorescence measurements over a range of laser powers confirmed the TPE of both Ca(2+)-free and Ca(2+)-bound forms of the dyes. Single-wavelength excitation at 810 nM was used to determine the effective dissociation constants (K(eff)) and dynamic ranges (R(f)) of Fura-2, -4F, -6F, -FF, and Furaptra dyes (K(eff) = 181 +/- 52 nM, 1.16 +/- 0.016 micro M, 5.18 +/- 0.3 micro M, 19.2 +/- 1 micro M, and 58.5 +/- 2 micro M; and R(f) = 22.4 +/- 3.8, 12.2 +/- 0.34, 6.3 +/- 0.17, 16.1 +/- 2.8, and 25.4 +/- 4, respectively). Single-wavelength excitation of intracellular Fura-4F resolved diastolic and peak [Ca(2+)] in isolated stimulated cardiomyocytes after calibration of the intracellular signal using reversible exposure to low (100 micro M) extracellular [Ca(2+)]. Furthermore, TPE of Fura-4F allowed continuous, long-term (5-10 min) Ca(2+) imaging in ventricular cardiomyocytes using laser-scanning microscopy without significant cellular photodamage or photobleaching of the dye.     

Imaging living cells and tissues by two-photon excitation microscopy

Two-photon excitation microscopy provides attractive advantages over confocal microscopy for three-dimensionally resolved fluorescence imaging. Since two-photon excitation occurs only at the focal point of the microscope, it inherently provides three-dimensional resolution. This localization of excitation also minimizes photobleaching and photodamage, which are the ultimate limiting factors in imaging living cells. Furthermore, no pinhole is required to attain three-dimensional discrimination, so the efficiency of fluorescence collection is increased. These advantages allow experiments on thick living samples that would not be possible with other imaging techniques. The cost and complexity of the lasers required for two-photon excitation microscopy have limited its use, but appropriate turn-key lasers have now been introduced, and their cost should decrease. Finally, the recent introduction of commercial two-photon excitation laser-scanning microscope systems allows a much larger group of researchers access to this state-of-the-art methodology.     

Nuclear aggresomes form by fusion of PML-associated aggregates

Nuclear aggregates formed by proteins containing expanded poly-glutamine (poly-Q) tracts have been linked to the pathogenesis of poly-Q neurodegenerative diseases. Here, we show that a protein (GFP170*) lacking poly-Q tracts forms nuclear aggregates that share characteristics of poly-Q aggregates. GFP170* aggregates recruit cellular chaperones and proteasomes, and alter the organization of nuclear domains containing the promyelocytic leukemia (PML) protein. These results suggest that the formation of nuclear aggregates and their effects on nuclear architecture are not specific to poly-Q proteins. Using GFP170* as a model substrate, we explored the mechanistic details of nuclear aggregate formation. Fluorescence recovery after photobleaching and fluorescence loss in photobleaching analyses show that GFP170* molecules exchange rapidly between aggregates and a soluble pool of GFP170*, indicating that the aggregates are dynamic accumulations of GFP170*. The formation of cytoplasmic and nuclear GFP170* aggregates is microtubule-dependent. We show that within the nucleus, GFP170* initially deposits in small aggregates at or adjacent to PML bodies. Time-lapse imaging of live cells shows that small aggregates move toward each other and fuse to form larger aggregates. The coalescence of the aggregates is accompanied by spatial rearrangements of the PML bodies. Significantly, we find that the larger nuclear aggregates have complex internal substructures that reposition extensively during fusion of the aggregates. These studies suggest that nuclear aggregates may be viewed as dynamic multidomain inclusions that continuously remodel their components.     

Continual assembly of desmosomes within stable intercellular contacts of epithelial A-431 cells

Subclones of human carcinoma-derived A-431 cell line stably producing fusion proteins consisting of the enhanced green fluorescent protein and either human desmoglein 2 (Dsg-GFP) or human plakoglobin (GFP-Pg) were used to examine the behavior of desmosomes in living cells. Immunofluorescence microscopy of the fixed cells showed that both fusion proteins, which were expressed in significantly lower levels relative to their endogenous counterparts, were efficiently recruited into desmosomes. Time-lapse confocal imaging of these cells reveals that such GFP-labeled desmosomes (GFP desmosomes) are stable structures which exhibit various dynamic and motile activities. The most notable are independent lateral mobility and fusion. Furthermore, the continual assembly of new nascent desmosomes is observed within stable contacts located at the middle of the epithelial sheet. A new GFP desmosome appears as a closely apposed group of fine patches which after a few minutes aggregate into a single structure. These three dynamic processes resulted in constant changes of desmosome distribution, numbers, and sizes. In addition, fluorescence recovery after photobleaching experiments showed that fine patches of desmosomal proteins may participate in desmosome maintenance. Such a diverse range of dynamic activities of desmosomes apparently produces flexible but tight cell-cell adhesion required for different morphogenetic events in epithelial structures.This work was supported by grant AR44016-04 from the National Institutes of Health     

Continuous wave two-photon scanning near-field optical microscopy.

We have implemented continuous-wave two-photon excitation of near-UV absorbing fluorophores in a scanning near-field optical microscope (SNOM). The 647-nm emission of an Ar-Kr mixed gas laser was used to excite the UV-absorbing DNA dyes DAPI, the bisbenzimidazole Hoechst 33342, and ethidium bromide in a shared aperture SNOM with uncoated fiber tips. Polytene chromosomes of Drosophila melanogaster and the nuclei of 3T3 Balb/c cells labeled with these dyes were readily imaged. The fluorescence intensity showed the expected nonlinear (second order) dependence on the excitation power in the range of 8-180 mW. We measured the fluorescence intensity as a function of the tip-sample displacement in the direction normal to the sample surface in the single- and two-photon excitation modes (SPE, TPE). The fluorescence intensity decayed faster in TPE than in SPE.     

Rapid three-dimensional isotropic imaging of living cells using Bessel beam plane illumination

A key challenge when imaging living cells is how to noninvasively extract the most spatiotemporal information possible. Unlike popular wide-field and confocal methods, plane-illumination microscopy limits excitation to the information-rich vicinity of the focal plane, providing effective optical sectioning and high speed while minimizing out-of-focus background and premature photobleaching. Here we used scanned Bessel beams in conjunction with structured illumination and/or two-photon excitation to create thinner light sheets (<0.5 μm) better suited to three-dimensional (3D) subcellular imaging. As demonstrated by imaging the dynamics of mitochondria, filopodia, membrane ruffles, intracellular vesicles and mitotic chromosomes in live cells, the microscope currently offers 3D isotropic resolution down to ～0.3 μm, speeds up to nearly 200 image planes per second and the ability to noninvasively acquire hundreds of 3D data volumes from single living cells encompassing tens of thousands of image frames.     

Second harmonic generation imaging of endogenous structural proteins

We show that structural protein arrays consisting largely of collagen, myosin, and tubulin, and their associated proteins can be imaged in three dimensions with high contrast and resolution by laser-scanning second harmonic generation (SHG) microscopy. SHG is a nonlinear optical scheme and this form of microscopy shares several common advantages with multiphoton excited fluorescence, namely, intrinsic three-dimensionality and reduced out-of-plane photobleaching and phototoxicity. SHG does not arise from absorption and in-plane photodamage considerations are therefore also greatly reduced. In particular, structural protein arrays that are highly ordered and birefringent produce large SHG signals without the need for any exogenous labels. We demonstrate that thick tissues including muscle and bone can be imaged and sectioned through several hundred micrometers of depth. Combining SHG with two-photon excited green fluorescent protein (GFP) imaging allows inference of the molecular origin of the SHG contrast in Caenorhabditis elegans sarcomeres. Symmetry and organization of microtubule structures in dividing C. elegans embryos are similarly studied by comparing the endogenous tubulin contrast with that of GFP::tubulin fluorescence. It is found that SHG provides molecular level data on radial and lateral symmetries that GFP constructs cannot. The physical basis of SHG is discussed and compared with that of two-photon excitation as well as that of polarization microscopy. Due to the intrinsic sectioning, lack of photobleaching, and availability of molecular level data, SHG is a powerful tool for in vivo imaging.     

Imaging plant cells by two-photon excitation

Summary. Along the past recent years, two-photon excitation (TPE) microscopy has moved from the realms of technical curiosity to be a standard application in many advanced cell biology laboratories. The growing body of literature covered in this review points out the obvious advantages of TPE over any other imaging method based on fluorescence, clearly improving signal-to-noise ratio and thick-tissue penetration and showing added potential for vital imaging. Like any new technology that has to gain its own space, TPE microscopy is still going through the growing pains in which reproducible protocols, probes, and applications are scarce. Yet, the published reports and unpublished results covered in this review point out that TPE can eventually accommodate most available protocols and probes, most of the times with evident advantages. Further, the potential for plant sciences is obvious, as plant cells possess many absorbing molecules and structures and are routinely more opaque than tissues of other organisms. Since prices make it one of the most expensive microscopies, TPE is coming slow to be a generalised technology, but enough data are emerging to establish it as a method with no alternative for some objectives.Correspondence and reprints: Instituto Gulbenkian de Ciência. 2780-156 Oeiras, Portugal.     

mEosFP-based green-to-red photoconvertible subcellular probes for plants

Photoconvertible fluorescent proteins (FPs) are recent additions to the biologists' toolbox for understanding the living cell. Like green fluorescent protein (GFP), monomeric EosFP is bright green in color but is efficiently photoconverted into a red fluorescent form using a mild violet-blue excitation. Here, we report mEosFP-based probes that localize to the cytosol, plasma membrane invaginations, endosomes, prevacuolar vesicles, vacuoles, the endoplasmic reticulum, Golgi bodies, mitochondria, peroxisomes, and the two major cytoskeletal elements, filamentous actin and cortical microtubules. The mEosFP fusion proteins are smaller than GFP/red fluorescent protein-based probes and, as demonstrated here, provide several significant advantages for imaging of living plant cells. These include an ability to differentially color label a single cell or a group of cells in a developing organ, selectively highlight a region of a cell or a subpopulation of organelles and vesicles within a cell for tracking them, and understanding spatiotemporal aspects of interactions between similar as well as different organelles. In addition, mEosFP probes introduce a milder alternative to fluorescence recovery after photobleaching, whereby instead of photobleaching, photoconversion followed by recovery of green fluorescence can be used for estimating subcellular dynamics. Most importantly, the two fluorescent forms of mEosFP furnish bright internal controls during imaging experiments and are fully compatible with cyan fluorescent protein, GFP, yellow fluorescent protein, and red fluorescent protein fluorochromes for use in simultaneous, multicolor labeling schemes. Photoconvertible mEosFP-based subcellular probes promise to usher in a much higher degree of precision to live imaging of plant cells than has been possible so far using single-colored FPs.     

One- and two-photon excited fluorescence lifetimes and anisotropy decays of green fluorescent proteins

We have used one- (OPE) and two-photon (TPE) excitation with time-correlated single-photon counting techniques to determine time-resolved fluorescence intensity and anisotropy decays of the wild-type Green Fluorescent Protein (GFP) and two red-shifted mutants, S65T-GFP and RSGFP. WT-GFP and S65T-GFP exhibited a predominant approximately 3 ns monoexponential fluorescence decay, whereas for RSGFP the main lifetimes were approximately 1.1 ns (main component) and approximately 3.3 ns. The anisotropy decay of WT-GFP and S65T-GFP was also monoexponential (global rotational correlation time of 16 +/- 1 ns). The approximately 1.1 ns lifetime of RSGFP was associated with a faster rotational depolarization, evaluated as an additional approximately 13 ns component. This feature we attribute tentatively to a greater rotational freedom of the anionic chromophore. With OPE, the initial anisotropy was close to the theoretical limit of 0.4; with TPE it was higher, approaching the TPE theoretical limit of 0.57 for the colinear case. The measured power dependence of the fluorescence signals provided direct evidence for TPE. The general independence of fluorescence decay times, rotation correlation times, and steady-state emission spectra on the excitation mode indicates that the fluorescence originated from the same distinct excited singlet states (A*, I*, B*). However, we observed a relative enhancement of blue fluorescence peaked at approximately 440 nm for TPE compared to OPE, indicating different relative excitation efficiencies. We infer that the two lifetimes of RSGFP represent the deactivation of two substates of the deprotonated intermediate (I*), distinguished by their origin (i.e., from A* or B*) and by nonradiative decay rates reflecting different internal environments of the excited-state chromophore.     

Expanding Two-Photon Intravital Microscopy to the Infrared by Means of Optical Parametric Oscillator

Chronic inflammation in various organs, such as the brain, implies that different subpopulations of immune cells interact with the cells of the target organ. To monitor this cellular communication both morphologically and functionally, the ability to visualize more than two colors in deep tissue is indispensable. Here, we demonstrate the pronounced power of optical parametric oscillator (OPO)-based two-photon laser scanning microscopy for dynamic intravital imaging in hardly accessible organs of the central nervous and of the immune system, with particular relevance for long-term investigations of pathological mechanisms (e.g., chronic neuroinflammation) necessitating the use of fluorescent proteins. Expanding the wavelength excitation farther to the infrared overcomes the current limitations of standard Titanium:Sapphire laser excitation, leading to 1), simultaneous imaging of fluorophores with largely different excitation and emission spectra (e.g., GFP-derivatives and RFP-derivatives); and 2), higher penetration depths in tissue (up to 80%) at higher resolution and with reduced photobleaching and phototoxicity. This tool opens up new opportunities for deep-tissue imaging and will have a tremendous impact on the choice of protein fluorophores for intravital applications in bioscience and biomedicine, as we demonstrate in this work.     

Live Imaging of Dense-core Vesicles in Primary Cultured Hippocampal Neurons

Observing and characterizing dynamic cellular processes can yield important information about cellular activity that cannot be gained from static images. Vital fluorescent probes, particularly green fluorescent protein (GFP) have revolutionized cell biology stemming from the ability to label specific intracellular compartments and cellular structures. For example, the live imaging of GFP (and its spectral variants) chimeras have allowed for a dynamic analysis of the cytoskeleton, organelle transport, and membrane dynamics in a multitude of organisms and cell types [1-3]. Although live imaging has become prevalent, this approach still poses many technical challenges, particularly in primary cultured neurons. One challenge is the expression of GFP-tagged proteins in post-mitotic neurons; the other is the ability to capture fluorescent images while minimizing phototoxicity, photobleaching, and maintaining general cell health. Here we provide a protocol that describes a lipid-based transfection method that yields a relatively low transfection rate (~0.5%), however is ideal for the imaging of fully polarized neurons. A low transfection rate is essential so that single axons and dendrites can be characterized as to their orientation to the cell body to confirm directionality of transport, i.e., anterograde v. retrograde. Our approach to imaging GFP expressing neurons relies on a standard wide-field fluorescent microscope outfitted with a CCD camera, image capture software, and a heated imaging chamber. We have imaged a wide variety of organelles or structures, for example, dense-core vesicles, mitochondria, growth cones, and actin without any special optics or excitation requirements other than a fluorescent light source. Additionally, spectrally-distinct, fluorescently labeled proteins, e.g., GFP and dsRed-tagged proteins, can be visualized near simultaneously to characterize co-transport or other coordinated cellular events. The imaging approach described here is flexible for a variety of imaging applications and can be adopted by a laboratory for relatively little cost provided a microscope is available.     

Photobleaching GFP reveals protein dynamics inside live cells

Cell biologists have used photobleaching to investigate the lateral mobility of fluorophores on the cell surface since the 1970s. Fusions of green fluorescent protein (GFP) to specific proteins extend photobleaching techniques to the investigation of protein dynamics within the cell, leading to renewed interest in photobleaching experiments. This article revisits general photobleaching concepts, reviews what can be learned from them and discusses applications illustrating the potential of photobleaching GFP fusion proteins inside living cells.     

Multiple bond-conjugated photoinduced nitric oxide releaser working with two-photon excitation

Four novel nitric oxide (NO) releasers working via two-photon excitation (TPE), based on an acceptor–donor–acceptor (A–D–A) molecular design, were synthesized. Their decomposition and NO release in response to one-photon excitation, and their decomposition in response to two-photon excitation were examined. Their photoinduced decomposition characteristics are discussed.     

Living cell functions and morphology revealed by two-photon microscopy in intact neural and secretory organs

Laser light microscopy enables observation of various simultaneously occurring events in living cells. This capability is important for monitoring the spatiotemporal patterns of the molecular interactions underlying such events. Two-photon excited fluorescence microscopy (two-photon microscopy), a technology based on multiphoton excitation, is one of the most promising candidates for such imaging. The advantages of two-photon microscopy have spurred wider adoption of the method, especially in neurological studies. Multicolor excitation capability, one advantage of two-photon micro-scopy, has enabled the quantification of spatiotemporal patterns of [Ca(2+)](i) and single episodes of fusion pore openings during exocytosis. In pancreatic acinar cells, we have successfully demonstrated the existence of "sequential compound exocytosis" for the first time, a process which has subsequently been identified in a wide variety of secretory cells including exocrine, endocrine and blood cells. Our newly developed method, the two-photon extracellular polar-tracer imaging-based quantification (TEPIQ) method, can be used for determining fusion pores and the diameters of vesicles smaller than the diffraction-limited resolution. Furthermore, two-photon microscopy has the demonstrated capability of obtaining cross-sectional images from deep layers within nearly intact tissue samples over long observation times with excellent spatial resolution. Recently, we have successfully observed a neuron located deeper than 0.9 mm from the brain cortex surface in an anesthetized mouse. This microscopy also enables the monitoring of long-term changes in neural or glial cells in a living mouse. This minireview describes both the current and anticipated capabilities of two-photon microscopy, based on a discussion of previous publications and recently obtained data.