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.     

Fluorescence recovery after photobleaching and photoconversion in multiple arbitrary regions of interest using a programmable array microscope

Photomanipulation (photobleaching, photoactivation, or photoconversion) is an essential tool in fluorescence microscopy. Fluorescence recovery after photobleaching (FRAP) is commonly used for the determination of lateral diffusion constants of membrane proteins, and can be conveniently implemented in confocal laser scanning microscopy (CLSM). Such determinations provide important information on molecular dynamics in live cells. However, the CLSM platform is inherently limited for FRAP because of its inflexible raster (spot) scanning format. We have implemented FRAP and photoactivation protocols using structured illumination and detection in a programmable array microscope (PAM). The patterns are arbitrary in number and shape, dynamic and adjustable to and by the sample characteristics. We have used multispot PAM–FRAP to measure the lateral diffusion of the erbB3 (HER3) receptor tyrosine kinase labeled by fusion with mCitrine on untreated cells and after treatment with reagents that perturb the cytoskeleton or plasma membrane or activate coexpressed erbB1 (HER1, the EGF receptor EGFR). We also show the versatility of the PAM for photoactivation in arbitrary regions of interest, in cells expressing erbB3 fused with the photoconvertible fluorescent protein dronpa. dronpa. Microsc. Res. Tech., 2009. © 2009 Wiley-Liss, Inc.     

Ligand-conjugated quantum dots monitor antigen uptake and processing by dendritic cells

The dendritic cell (DC) specific pathogen-uptake receptor (DC-SIGN) internalizes antigens for degradation and presentation onto MHC molecules. At the cell membrane, DC-SIGN forms nanoclusters that facilitate virus capture. However, internalized viruses, such as HIV-1, escape degradation. Here, we exploit ligand-conjugated, virus-sized, highly photostable quantum dots (QDs) to monitor in living cells antigen binding, entry, and trafficking. The antigen-coated QDs specific uptake and persistence in live DCs open the possibility for tracking antigen-presenting cells in vivo.     

Minimizing light exposure with the programmable array microscope

The exposure of fluorophores to intense illumination in a microscope often results in photobleaching and phototoxicity, thus constituting a major limiting factor in time lapse live cell or single molecule imaging. Laser scanning confocal microscopes are particularly prone to this problem, inasmuch as they require high irradiances to compensate for the inherently low duty cycle of point scanning systems. In the attempt to maintain adequate speed and signal-to-noise ratios, the fluorophores are often driven into saturation, thereby generating a nonlinear response. One approach for reducing photodegradation in the laser scanning confocal microscope is represented by controlled light exposure microscopy, introduced by Manders and colleagues. The strategy is to reduce the illumination intensity in both background areas (devoid of information) as well as in bright foreground regions, for which an adequate signal-to-noise ratio can be achieved with lower excitation levels than those required for the less intense foreground pixels/voxels. Such a variable illumination scheme can also be exploited in widefield microscopes that employ lower irradiance but higher illumination duty cycles. We report here on the adaptation of the controlled light exposure microscopy principle to the programmable array microscope, which achieves optical sectioning by use of a spatial light modulator (SLM) in an image plane as a programmable mask for illumination and conjugate (and nonconjugate) detection. By incorporating the basic controlled light exposure microscopy concept for minimizing exposure, we have obtained a reduction in the rate of photobleaching of up to ~5-fold, while maintaining an image quality comparable to regular imaging with the programmable array microscope.     

A dual path programmable array microscope (PAM): simultaneous acquisition of conjugate and non-conjugate images

A programmable array microscope (PAM) incorporates a spatial light modulator (SLM) placed in the primary image plane of a widefield microscope, where it is used to define patterns of illumination and/or detection. We describe the characteristics of a special type of PAM collecting two images simultaneously. The conjugate image (I_c) is formed by light originating from the object plane and returning along the optical path of the illumination light. The non‐conjugate image (I_nc) receives light from only those regions of the SLM that are not used for illuminating the sample. The dual‐signal PAM provides much more time‐efficient excitation than the confocal laser scanning microscope (CLSM) and greater utilization of the available emission light. It has superior noise characteristics in comparison to single‐sided instruments. The axial responses of the system under a variety of conditions were measured and the behaviour of the novel I_nc image characterized. As in systems in which only I_c images are collected (Nipkow‐disc microscopes, and previously characterized PAMs), the axial response to thin fluorescent films showed a sharpening of the axial response as the unit cell of the repetitive patterns decreased in size. The dual‐signal PAM can be adapted to a wide range of data analysis and collection strategies. We investigated systematically the effects of patterns and unit cell dimensions on the axial response. Sufficiently sparse patterns lead to an I_c image formed by the superposition of the many parallel beams, each of which is equivalent to the single scanning spot of a CLSM. The sectioning capabilities of the system, as given by its axial responses, were similar for a given scan pattern and for processed pseudorandom sequence (PRS) scans with the same size of the unit cell. For the PRS scans, optical sectioning was achieved by a subtraction of an I_nc image or, alternatively, a scaled widefield image from the I_c image. Based on the comparative noise levels of the two methods, the non‐conjugate subtraction was significantly superior. A point spread function for I_c and I_nc was simulated and properties of the optical transfer functions (OTFs) were compared. Simulations of the OTF in non‐conjugate imaging did not suffer from the missing cone problem, enabling a high quality deconvolution of the non‐conjugate side alone. We also investigated the properties of images obtained by subjecting the I_c and I_nc data to a combined maximum likelihood deconvolution.     

An optical sectioning programmable array microscope implemented with a digital micromirror device

The defining feature of a programmable array microscope (PAM) is the presence of a spatial light modulator in the image plane. A spatial light modulator used singly or as a matched pair for both illumination and detection can be used to generate an optical section. Under most conditions, the basic optical properties of an optically sectioning PAM are similar to those of rotating Nipkow discs. The method of pattern generation, however, is fundamentally different and allows arbitrary illumination patterns to be generated under programmable control, and sectioning strategies to be changed rapidly in response to specific experimental conditions. We report the features of a PAM incorporating a digital micromirror device, including the axial sectioning response to fluorescent thin films and the imaging of biological specimens. Three axial sectioning strategies were compared: line scans, dot lattice scans and pseudo-random sequence scans. The three strategies varied widely in light throughput, sectioning strength and robustness when used on real biological samples. The axial response to thin fluorescent films demonstrated a consistent decrease in the full width at half maximum (FWHM), accompanied by an increase in offset, as the unit cells defining the patterns grew smaller. Experimental axial response curves represent the sum of the response from a given point of illumination and cross-talk from neighbouring points. Cross-talk is minimized in the plane of best focus and when measured together with the single point response produces a decrease in FWHM. In patterns having constant throughput, there appears to be tradeoff between the FWHM and the size of the offset. The PAM was compared to a confocal laser scanning microscope using biological samples. The PAM demonstrated higher signal levels and dynamic range despite a shorter acquisition time. It also revealed more structures in x - z sections and less intensity drop-off with scanning depth.     

Three-dimensional spectral imaging by Hadamard transform spectroscopy in a programmable array microscope

We report the acquisition and deconvolution of three-dimensional spectrally resolved images in a programmable array microscope implementing a Hadamard transform fluorescence spectroscopy system with adjustable spectral resolution. A stack of 16 two-dimensional spectral images was collected at 400 nm intervals along the optical axis. The specimen consisted of a polytene chromosome spread from Drosophila melanogaster doubly labelled for the Polyhomeotic protein by indirect immunofluorescence labelling with Alexa594 and for DNA with YOYO-1. The resulting four-dimensional data set consisted of the xyz spatial dimensions (898 × 255 × 16) with a 26-point spectrum at each spatial location. The total exposure time to the sample was 34 min. The system requires the acquisition of multiple images, and thus works best with fluorophores that are resistant to photobleaching. Image deconvolution reduced the amount of out-of-focus blur by up to a factor of 8, resulting in a dramatic improvement in the visualization of the chromosome backbone and localization of the specific Polyhomeotic domains.     

Probing DNA structure and function with a multiwavelength fluorescence confocal laser microscope

Three levels of organization in DNA structure in the interphase cell nucleus are assessed by confocal laser scanning microscopy: (i) the conformational state of the double helix; (ii) the distribution of eu- and heterochromatin; and (iii) the localization of replication complexes throughout S phase. Multi-parameter measurements were carried out in each optical section using two laser sources and combined stereoscopic reconstructions were used to assess the co-localization of nuclear components. DNA is highly polymorphic and can adopt a variety of different helical conformations as well as unusual structures (curved, cruciform, multi-stranded). We have assessed by laser scanning microscopy the presence of left-handed Z-DNA in polytene chromosomes of Diptera as well as the spatio-temporal distribution of Z-DNA binding proteins in whole-mount Drosophila embryos and ovaries. We have determined the 3-D distribution of replication sites relative to heterochromatin regions, nucleoli and nuclear membrane by using short pulses of BrdU incorporation in synchronized mouse and human fibroblasts. Replication sites were visualized with a monoclonal anti-BrdU antibody combined with DNA fluorescent staining and antibody labelling of nuclear lamin. The implications of dynamic DNA movement and structural rearrangement to the organization of the nucleus in domains are discussed.