The effects of spherical aberration on multiphoton fluorescence excitation microscopy

Multiphoton fluorescence excitation microscopy is almost invariably conducted with samples whose refractive index differ from that of the objective immersion medium, conditions that cause spherical aberration. Due to the quadratic nature of multiphoton fluorescence excitation, spherical aberration is expected to profoundly affect the depth dependence of fluorescence excitation. In order to determine the effect of refractive index mismatch in multiphoton fluorescence excitation microscopy, we measured signal attenuation, photobleaching rates and resolution degradation with depth in homogeneous samples with minimal light scattering and absorption over a range of refractive indices. These studies demonstrate that signal levels and resolution both rapidly decline with depth into refractive index mismatched samples. Analyses of photobleaching rates indicate that the preponderance of signal attenuation with depth results from decreased rates of fluorescence excitation, even in a system with a descanned emission collection pathway. Similar results were obtained in analyses of fluorescence microspheres embedded in rat kidney tissue, demonstrating that spherical aberration is an important limiting factor in multiphoton fluorescence excitation microscopy of biological samples.     

A series of flexible design adaptations to the Nikon E‐C1 and E‐C2 confocal microscope systems for UV,multiphoton and FLIM imaging

Multiphoton microscopy is widely employed in the life sciences using extrinsic fluorescence of low‐ and high‐molecular weight labels with excitation and emission spectra in the visible and near infrared regions. For imaging of intrinsic and extrinsic fluorophores with excitation spectra in the ultraviolet region, multiphoton excitation with one‐ or two‐colour lasers avoids the need for ultraviolet‐transmitting excitation optics and has advantages in terms of optical penetration in the sample and reduced phototoxicity. Excitation and detection of ultraviolet emission around 300 nm and below in a typical inverted confocal microscope is more difficult and requires the use of expensive quartz optics including the objective. In this technical note we describe the adaptation of a commercial confocal microscope (Nikon, Japan E‐C1 or E‐C2) for versatile use with Ti‐sapphire and OPO laser sources and the addition of a second detection channel that enables detection of ultraviolet fluorescence and increases detection sensitivity in a typical fluorescence lifetime imaging microscopy experiment. Results from some experiments with this setup illustrate the resulting capabilities.     

The effects of refractive index heterogeneity within kidney tissue on multiphoton fluorescence excitation microscopy

Although multiphoton fluorescence excitation microscopy has improved the depth at which useful fluorescence images can be collected in biological tissues, the reach of multiphoton fluorescence excitation microscopy is nonetheless limited by tissue scattering and spherical aberration. Scattering can be reduced in fixed samples by mounting in a medium whose refractive index closely matches that of the fixed material. Using optical 'clearing', the effects of refractive index heterogeneity on signal attenuation with depth are investigated. Quantitative measurements show that by mounting kidney tissue in a high refractive index medium, less than 50% of signal attenuates in 100 μm of depth.     

Multiphoton microscopic imaging of adipose tissue based on second-harmonic generation and two-photon excited fluorescence

The fresh adipose tissue was investigated by the use of multiphoton microscopy (MPM) based on two-photon excited fluorescence and second-harmonic generation (SHG). Microstructure of collagen and adipose cells in the adipose tissue is clearly imaged at a subcellular level with the excitation light wavelengths of 850 and 730 nm, respectively. The emission spectrum of collagen SHG signal and NADH and FAD fluorescence signal can also be obtained, which can be used to quantify the content of collagen and adipose cells and reflect the degree of pathological changes when comparing normal tissue with abnormal adipose tissue in the same condition. The results indicate that MPM has the potential to be applied to investigate the adipose tissue and can be used in the research field of lipid and connective tissues.     

A simple introduction to multiphoton microscopy

Multiphoton microscopy is a powerful technique based on complex quantum mechanical effects. Thanks to the development of turnkey mode-locked laser systems, multiphoton microscopy is now available for everyone to use without extreme complexity. In this short introduction, we describe qualitatively the important concepts underlying the most commonly used type of multiphoton microscopy (two-photon excitation). We elucidate how those properties lead to the powerful results that have been achieved using this technique. As with any technique, two-photon excitation microscopy has limitations that we describe, and we provide examples of particular classes of experiments where two-photon excitation microscopy is advantageous over other approaches. Finally, we briefly describe other useful multiphoton microscopy approaches, such as three-photon excitation and second harmonic generation imaging.     

Multiphoton fluorescence lifetime imaging of human hair

In vivo and in vitro multiphoton imaging was used to perform high resolution optical sectioning of human hair by nonlinear excitation of endogenous as well as exogenous fluorophores. Multiphoton fluorescence lifetime imaging (FLIM) based on time-resolved single photon counting and near-infrared femtosecond laser pulse excitation was employed to analyze the various fluorescent hair components. Time-resolved multiphoton imaging of intratissue pigments has the potential (i) to identify endogenous keratin and melanin, (ii) to obtain information on intrahair dye accumulation, (iii) to study bleaching effects, and (iv) to monitor the intratissue diffusion of pharmaceutical and cosmetical components along hair shafts.     

Optimization of multiphoton excitation microscopy by total emission detection using a parabolic light reflector

We have constructed a device that maximizes the probability of collecting all of the scattered and ballistic light isotropically generated at the focal spot of multiphoton excited emissions (MPE) to optimize the signal-to-noise ratio (SNR) for micro-imaging. This was accomplished by optically coupling a parabolic reflector (that surrounds the sample and top of the objective) to a pair of collimating lenses (above the sample) that redirects emitted light to a separate detector. These additional optics, combined with the objective, allow the total emission detection (TED) condition to be approached. Numerical simulations suggest an approximately 10-fold improvement in SNR with TED. Comparisons between the objective detection and TED reveal an enhancement of 8.9 in SNR (77% of predicted) for GFP-labelled brain slices and similar results for fluorescent beads. This increase in SNR can be used to improve time resolution, reduce laser power requirements/photodynamic damage, and, in certain cases, detection depth, for MPE imaging techniques.     

Two-photon fluorescence and second-harmonic generation imaging of collagen in human tissue based on multiphoton microscopy

Multiphoton microscopic imaging of collagen plays an important role in noninvasive diagnoses of human tissue. In this study, two-photon fluorescence and second-harmonic generation (SHG) imaging of collagen in human skin dermis and submucosa of colon and stomach tissues were investigated based on multiphoton microscopy (MPM). Our results show that multiphoton microscopic image of collagen bundles exhibits apparently different pattern in human tissues. The collagen bundles can simultaneously reveal its SHG and two-photon excited fluorescence images in the submucosa of colon and stomach, whereas it solely emit SHG signal in skin dermis. The intensity spectral information from tissues further demonstrated the above results. This indicates that collagen bundles have completely different space arrangement in these tissues. Our experimental results bring more detailed information of collagen for the application of MPM in human noninvasive imaging.     

Image scanning fluorescence emission difference microscopy based on a detector array

We propose a novel imaging method that enables the enhancement of three‐dimensional resolution of confocal microscopy significantly and achieve experimentally a new fluorescence emission difference method for the first time, based on the parallel detection with a detector array. Following the principles of photon reassignment in image scanning microscopy, images captured by the detector array were arranged. And by selecting appropriate reassign patterns, the imaging result with enhanced resolution can be achieved with the method of fluorescence emission difference. Two specific methods are proposed in this paper, showing that the difference between an image scanning microscopy image and a confocal image will achieve an improvement of transverse resolution by approximately 43% compared with that in confocal microscopy, and the axial resolution can also be enhanced by at least 22% experimentally and 35% theoretically. Moreover, the methods presented in this paper can improve the lateral resolution by around 10% than fluorescence emission difference and 15% than Airyscan. The mechanism of our methods is verified by numerical simulations and experimental results, and it has significant potential in biomedical applications.     

Intact corneal stroma visualization of GFP mouse revealed by multiphoton imaging

The aim of this work is to demonstrate that multiphoton microscopy is a preferred technique to investigate intact cornea structure without slicing and staining. At the micron resolution, multiphoton imaging can provide both large morphological features and detailed structure of epithelium, corneal collagen fibril bundles and keratocytes. A large area multiphoton cross-section across an intact eye excised from a GFP mouse was obtained by a homebuilt multiphoton microscope. The broadband multiphoton fluorescence (435-700 nm) and second harmonic generation (SHG, 360-400 nm) signals were generated by the 760 nm output of a femtosecond titanium-sapphire laser. A water immersion objective (Fluor, 40X, NA 0.8; Nikon) was used to facilitate imaging the curve ocular surface. The multiphoton image over entire cornea provides morphological information of epithelial cells, keratocytes, and global collagen orientation. Specifically, our planar, large area multiphoton image reveals a concentric pattern of the stroma collagen, indicative of the laminar collagen organization throughout the stroma. In addition, the green fluorescence protein (GFP) labeling contributed to fluorescence contrast of cellular area and facilitated visualizing of inactive keratocytes. Our results show that multiphoton imaging of GFP labeled mouse cornea manifests both morphological significance and structural details. The second harmonic generation imaging reveals the collagen orientation, while the multiphoton fluorescence imaging indicates morphology and distribution of cells in cornea. Our results support that multiphoton microscopy is an appropriate technology for further in vivo investigation and diagnosis of cornea.     

Ultrafast photon counting applied to resonant scanning STED microscopy

To take full advantage of fast resonant scanning in super‐resolution stimulated emission depletion (STED) microscopy, we have developed an ultrafast photon counting system based on a multigiga sample per second analogue‐to‐digital conversion chip that delivers an unprecedented 450 MHz pixel clock (2.2 ns pixel dwell time in each scan). The system achieves a large field of view (～50 × 50 μm) with fast scanning that reduces photobleaching, and advances the time‐gated continuous wave STED technology to the usage of resonant scanning with hardware‐based time‐gating. The assembled system provides superb signal‐to‐noise ratio and highly linear quantification of light that result in superior image quality. Also, the system design allows great flexibility in processing photon signals to further improve the dynamic range. In conclusion, we have constructed a frontier photon counting image acquisition system with ultrafast readout rate, excellent counting linearity, and with the capacity of realizing resonant‐scanning continuous wave STED microscopy with online time‐gated detection.     

Configurations of the Re‐scan Confocal Microscope (RCM) for biomedical applications

The new high‐sensitive and high‐resolution technique, Re‐scan Confocal Microscopy (RCM), is based on a standard confocal microscope extended with a re‐scan detection unit. The re‐scan unit includes a pair of re‐scanning mirrors that project the emission light onto a camera in a scanning manner. The signal‐to‐noise ratio of Re‐scan Confocal Microscopy is improved by a factor of 4 compared to standard confocal microscopy and the lateral resolution of Re‐scan Confocal Microscopy is 170 nm (compared to 240 nm for diffraction limited resolution, 488 nm excitation, 1.49 NA). Apart from improved sensitivity and resolution, the optical setup of Re‐scan Confocal Microscopy is flexible in its configuration in terms of control of the mirrors, lasers and filters. Because of this flexibility, the Re‐scan Confocal Microscopy can be configured to address specific biological applications. In this paper, we explore a number of possible configurations of Re‐scan Confocal Microscopy for specific biomedical applications such as multicolour, FRET, ratio‐metric (e.g. pH and intracellular Ca²⁺ measurements) and FRAP imaging.     

Multiphoton versus confocal high resolution z-sectioning of enhanced green fluorescent microtubules: increased multiphoton photobleaching within the focal plane can be compensated using a Pockels cell and dual widefield detectors

Multiphoton excitation was originally projected to improve live cell fluorescence imaging by minimizing photobleaching effects outside the focal plane, yet reports suggest that photobleaching within the focal plane is actually worse than with one photon excitation. We confirm that when imaging enhanced green fluorescent protein, photobleaching is indeed more acute within the multiphoton excitation volume, so that whilst fluorescence increases as predicted with the square of the excitation power, photobleaching rates increase with a higher order relationship. Crucially however, multiphoton excitation also affords unique opportunities for substantial improvements to fluorescence detection. By using a Pockels cell to minimize exposure of the specimen together with multiple nondescanned detectors we show quantitatively that for any particular bleach rate multiphoton excitation produces significantly more signal than one photon excitation confocal microscopy in high resolution Z‐axis sectioning of thin samples. Both modifications are readily implemented on a commercial multiphoton microscope system.     

MRT letter: high speed scanning has the potential to increase fluorescence yield and to reduce photobleaching

True confocal microscopy requires point-shaped illumination and detection. To generate an image, a diffraction limited spot is moved over the sample. Single spot scanning has suffered in the past from low image rates; a solution is the employment of very fast scanning devices (resonant scanners) for x-movement. In the process of introducing resonant scanning devices, it was found that both signal yield is improved and bleaching is decreased-in contrary to the assumed performance. This article will show by a simple and well understood model a straightforward explanation for the potential increase of signal yield and decrease in photobleaching. The time that is ruling the dose-rate effects is the effective time; a fluorochrome is illuminated. This time depends on the diameter of the spot that is moved over the sample and the speed at which the spot moves. In essence, the scan process causes a pulsed illumination of the fluorochromes. Various schemes of pulsed illumination are simulated with a fluorescence model. The model includes a dark state, where fluorochromes will exit the fluorescence process and slowly decay back into the ground state. Upon splitting a single dose into two pulses separated by a dark time-reflecting an increased scan speed-the amount of fluorescence emission is increased and bleaching is reduced. These results show a potential increase of fluorescence and a lower photobleaching upon higher scan speed. As illumination during the bleach-phase in a FRAP-experiment is similar to a light pulse, the findings also suggest to critically consider the very beginning of fluorescence recovery in terms of triplet relaxation process that potentially could falsify the measurements.     

Recent research on stimulated emission depletion microscopy for reducing photobleaching

Stimulated emission depletion (STED) microscopy is a useful tool in investigation for super‐resolution realm. By silencing the peripheral fluorophores of the excited spot, leaving only the very centre zone vigorous for fluorescence, the effective point spread function (PSF) could be immensely squeezed and subcellular structures, such as organelles, become discernable. Nevertheless, because of the low cross‐section of stimulated emission and the short fluorescence lifetime, the depletion power density has to be extremely higher than the excitation power density and molecules are exposed in high risk of photobleaching. The existence of photobleaching greatly limits the research of STED in achieving higher resolution and more delicate imaging quality, as well as long‐term and dynamic observation. Since the first experimental implementation of STED microscopy, researchers have lift out variety of methods and techniques to alleviate the problem. This paper would present some researches via conventional methods which have been explored and utilised relatively thoroughly, such as fast scanning, time‐gating, two‐photon excitation (TPE), triplet relaxation (T‐Rex) and background suppression. Alternatively, several up‐to‐date techniques, especially adaptive illumination, would also be unveiled for discussion in this paper. The contrast and discussion of these modalities would play an important role in ameliorating the research of STED microscopy.     

EXAMINATION OF ORAL TISSUES BY FOURIER TRANSFORM SPECTRAL IMAGING FLUORESCENCE

Fourier transform imaging spectroscopy was combined with fluorescence microscopy and a cooled CCD detector for examination of human oral tissues. Oral tissue fragments, obtained from patients, were irradiated at 365 nm by a mercury lamp through the microscope objectives. Microscope images were transferred to an imaging Fourier transform spectrometer and to a CCD camera for simultaneous recording of the fluorescence spectra at each image pixel. Detailed information was observed at a microscopic resolution. Oral tissue fragments were also treated with aluminum phthalocyanine tetrasulfonatre (AlPcS₄) prior to irradiation and imaging. Since the latter is preferentially retained in proliferating vascular tissue such as oral tumors, its effect upon the fluorescence imaging is of practical importance. AlPcS₄ is highly soluble in biological solutions and has a strong absorbance at our excitation wavelength and a strong emission peak at λ = 680 nm; therefore, it was found suitable for detection of malignant tumors by this method. It was found that the proposed spectral imaging method, when combined with fluorescence labeling, allows for direct, in vivo, medical examination of oral tissues with detailed spatial resolution.     

Compact non‐contact total emission detection for in vivo multiphoton excitation microscopy

We describe a compact, non‐contact design for a total emission detection (c‐TED) system for intra‐vital multiphoton imaging. To conform to a standard upright two‐photon microscope design, this system uses a parabolic mirror surrounding a standard microscope objective in concert with an optical path that does not interfere with normal microscope operation. The non‐contact design of this device allows for maximal light collection without disrupting the physiology of the specimen being examined. Tests were conducted on exposed tissues in live animals to examine the emission collection enhancement of the c‐TED device compared to heavily optimized objective‐based emission collection. The best light collection enhancement was seen from murine fat (5×–2× gains as a function of depth), whereas murine skeletal muscle and rat kidney showed gains of over two and just under twofold near the surface, respectively. Gains decreased with imaging depth (particularly in the kidney). Zebrafish imaging on a reflective substrate showed close to a twofold gain throughout the entire volume of an intact embryo (approximately 150 μm deep). Direct measurement of bleaching rates confirmed that the lower laser powers, enabled by greater light collection efficiency, yielded reduced photobleaching in vivo. The potential benefits of increased light collection in terms of speed of imaging and reduced photo‐damage, as well as the applicability of this device to other multiphoton imaging methods is discussed.     

Ultrafast optical pulse delivery with fibers for nonlinear microscopy

Nonlinear microscopies including multiphoton excitation fluorescence microscopy and multiple-harmonic generation microscopy have recently gained popularity for cellular and tissue imaging. The optimization of these imaging methods for minimally invasive use requires optical fibers to conduct light into tight space, where free-space delivery is difficult. The delivery of high-peak power laser pulses with optical fibers is limited by dispersion resulting from nonlinear refractive index responses. In this article, we characterize a variety of commonly used optical fibers in terms of how they affect pulse profile and imaging performance of nonlinear microscopy; the following parameters are quantified: spectral bandwidth and temporal pulse width, two-photon excitation efficiency, and optical resolution. A theoretical explanation for the measured performance of these fibers is also provided.     

Imaging modes for bilateral confocal scanning microscopy

The bilateral scanning approach to confocal microscopy is characterized by the direct generation of the image on a two-dimensional (2-D) detector. This detector can be a photographic plate, a CCD detector or the human eye, the human eye permitting direct visualization of the confocal image. Unlike Nipkow-type systems, laser light sources can be used for excitation. A design called a carousel has been developed, in which the bilateral confocal scan capability can be added to an existing microscope so that rapid exchange and comparison between confocal and non-confocal imaging conditions is possible. The design permits independent adjustment of confocal sectioning properties with lateral resolutions better than, or, in the worst case equivalent to, those available in conventional microscopy. The carousel can be considered as a stationary optical path in which certain imaging conditions, such as confocality, are defined and operate on part of the imaging field. The action of the bilateral scan mirror then extends this image condition over the whole field. A number of optical arrangements for the carousel are presented which realize various forms of confocal fluorescence and reflection imaging, with point, multiple point or slit confocal detection arrangements. Through the addition of active elements to the carousel direct stereoscopic, ratio, time-resolved and other types of imaging can be achieved, with direct image formation on a CCD, eye or other 2-D detectors without the need to modify the host microscope. Depending on the photon flux available, these imaging modes can run in real-time or can use a cooled CCD at (very) low light level for image integration over an extended period.     

Potential of ultraviolet wide-field imaging and multiphoton microscopy for analysis of dehydroergosterol in cellular membranes

Dehydroergosterol (DHE) is an intrinsically fluorescent sterol with absorption/emission in the ultraviolet (UV) region and biophysical properties similar to those of cholesterol. We compared the potential of UV-sensitive low-light-level wide-field (UV-WF) imaging with that of multiphoton (MP) excitation microscopy to monitor DHE in living cells. Significantly reduced photobleaching in MP microscopy of DHE enabled us to acquire three-dimensional z-stacks of DHE-stained cells and to obtain high-resolution maps of DHE in surface ruffles, nanotubes, and the apical membrane of epithelial cells. We found that the lateral resolution of MP microscopy is ～1.5-fold higher than that of UV-WF deconvolution microscopy, allowing for improved spatiotemporal analysis of plasma membrane sterol distribution. Surface intensity patterns of DHE with a diameter of 0.2 μm persisting over several minutes could be resolved by MP time-lapse microscopy. Diffusion coefficients of 0.25-μm-diameter endocytic vesicles containing DHE were determined by MP spatiotemporal image correlation spectroscopy. The requirement of extremely high laser power for visualization of DHE by MP microscopy made this method less potent for multicolor applications with organelle markers like green fluorescent protein-tagged proteins. The signal-to-noise ratio obtainable by UV-WF imaging could be significantly improved by pixelwise bleach rate fitting and calculation of an amplitude image from the decay model and by frame averaging after pixelwise bleaching correction of the image stacks. We conclude that UV-WF imaging and MP microscopy of DHE provide complementary information regarding membrane distribution and intracellular targeting of sterols.