Chromatic two-photon excitation fluorescence imaging

We report on a chromatic axial scanning method for two-photon excitation fluorescence imaging. Effective axial scanning is achieved by incorporating a Fresnel lens in the system, which has large chromatic aberration and can therefore focus the excitation beam to different axial positions depending on its wavelength. We experimentally demonstrated this technique and used it to image the cross-section of fluorescent microspheres.     

A computer-aided two-photon scanning microscope

A computer-aided digital microscope for studying microstructures at wavelengths of the second optical harmonic and two-photon luminescence is designed. In contrast to commercial instruments, the microscope is intended to study the image dependence on the angle of incidence, azimuth, and angle of the radiation receipt, as well as the polarization characteristics in organic and inorganic structures. As examples, results of studying nonlinearly optical properties of peptide tubes and microstructures based on zinc oxide are given.     

Adaptive aberration correction in a two-photon microscope

We demonstrate aberration correction in two-photon microscopy. Specimen-induced aberrations were measured with a modal wavefront sensor, implemented using a ferro-electric liquid crystal spatial light modulator (FLCSLM). Wavefront correction was performed using the same FLCSLM. Axial scanned ( x z ) images of fluorescently labelled polystyrene beads using an oil immersion lens show restored sectioning ability at a depth of 28 µm in an aqueous specimen.     

Antecedents of two-photon excitation laser scanning microscopy

In 1931, Maria G?ppert-Mayer published her doctoral dissertation on the theory of two-photon quantum transitions (two-photon absorption and emission) in atoms. This report describes and analyzes the theoretical and experimental work on nonlinear optics, in particular two-photon excitation processes, that occurred between 1931 and the experimental implementation of two-photon excitation microscopy by the group of Webb in 1990. In addition to Maria G?ppert-Mayer's theoretical work, the invention of the laser has a key role in the development of two-photon microscopy. Nonlinear effects were previously observed in different frequency domains (low-frequency electric and magnetic fields and magnetization), but the high electric field strength afforded by lasers was necessary to demonstrate many nonlinear effects in the optical frequency range. In 1978, the first high-resolution nonlinear microscope with depth resolution was described by the Oxford group. Sheppard and Kompfner published a study in Applied Optics describing microscopic imaging based on second-harmonic generation. In their report, they further proposed that other nonlinear optical effects, such as two-photon fluorescence, could also be applied. However, the developments in the field of nonlinear optical stalled due to a lack of a suitable laser source. This obstacle was removed with the advent of femtosecond lasers in the 1980s. In 1990, the seminal study of Denk, Strickler, and Webb on two-photon laser scanning fluorescence microscopy was published in Science. Their paper clearly demonstrated the capability of two-photon excitation microscopy for biology, and it served to convince a wide audience of scientists of the potential capability of the technique.     

Refractive-index-induced aberrations in two-photon confocal fluorescence microscopy

The effect of refractive index mismatch on the image quality in two-photon confocal fluorescence microscopy is investigated by experiment and numerical calculations. The results show a strong decrease in the image brightness using high-aperture objectives when the image plane is moved deeper into the sample. When exciting at 740 nm and recording the fluorescence around 460 nm in a glycerol-mounted sample using a lens of a numerical aperture of 1·4 (oil immersion), a 25% decrease in the intensity is observed at a depth of 9 μm. In an aqueous sample, the same decrease is observed at a depth of 3 μm. By reducing the numerical aperture to 1·0, the intensity decrease can be avoided at the expense of the overall resolution and signal intensity. The experiments are compared with the predictions of a theory that takes into account the vectorial character of light and the refraction of the wavefronts according to Fermat's principle. Advice is given concerning how the effects can be taken into account in practice.     

Wavelength division scanning for two-photon excitation fluorescence imaging

We investigate wavelength division scanning for two‐photon excitation fluorescence imaging. Two‐photon imaging using lateral wavelength division scanning is demonstrated. In addition, we theoretically analyse the spatial and temporal properties of a femtosecond laser beam focused by a Fresnel lens and investigate the feasibility of axial scanning using wavelength division.     

Saturation modified point spread functions in two-photon microscopy

Excitation saturation can dramatically alter the effective imaging point spread function (PSF) in two-photon fluorescence microscopy. The saturation-modified PSF can have important implications for resolution in fluorescence imaging as saturation leads to both an increased fluorescence observation volume and an altered spatial profile for the PSF. We introduce here a computational approach to accurately quantify molecular excitation profiles that represent the modified imaging PSF in two-photon microscopy under the influence of excitation saturation. An analytical model that accounts for pulsed laser excitation is developed to calculate the influence of saturation at any location within the excitation laser profile. The overall saturation modified molecular excitation profiles are then evaluated numerically. Our results demonstrate that saturation can play an important role in two-photon fluorescence microscopy even with relatively modest excitation levels.     

Probing nucleocytoplasmic transport by two-photon activation of PA-GFP

Two-photon activation of photoactivatable green fluorescent protein (PA-GFP) provides a unique tool for probing cellular transport processes, because activation is strictly limited to the sub-femtoliter optical volume of the two-photon spot. We demonstrate two-photon activation of PA-GFP immobilized in a gel and freely diffusing within cells and recover a quadratic power dependence. Illumination at 820 nm allows simultaneous activation and fluorescence monitoring by two-photon excitation. Alternatively, we activate PA-GFP using two-photon excitation and monitor the fluorescence of the photoconverted product with one-photon excitation. We probe nucleocytoplasmic transport through the nuclear pore complex of COS-1 cells, by observing the time-dependent fluorescence at various locations within the cell after two-photon activation of PA-GFP in the nucleus and in the cytoplasm. Two-photon activation of a tandem construct of two PA-GFPs showed a markedly slower rate of crossing through the nuclear pore. Analysis based on a restricted diffusion model yields a nuclear pore radius of 4.5 nm, which is in good agreement with previously reported values. This application demonstrates the attractive features of two-photon photoactivation over traditional techniques, such as photobleaching, for studying transport processes in cells.     

Real time two-photon absorption microscopy using multi point excitation

In this communication we present the development of a real time two-photon absorption microscope, based on parallel excitation with many foci. This pattern of foci is created by a two-dimensional microlens array. The fluorescence is detected by direct, non descanned detection on a CCD camera. Due to the parallel nature of both excitation and detection it is possible to speed up image acquisition significantly. This makes the instrument especially suitable for studying living specimens and/or real time processes. The optical design of the instrument is discussed and an imaging example is given. We specifically address the relation between the axial sectioning capability and the distance between the illumination foci at the sample.     

Effect of a confocal pinhole in two-photon microscopy.

We investigated the effect of a finite-sized confocal pinhole on the performance of nonlinear optical microscopes based on two-photon excited fluorescence and second-harmonic generation. These techniques were implemented using a modified inverted commercial confocal microscope coupled to a femtosecond Ti:sapphire laser. Both the transverse and axial resolutions are improved when the confocal pinhole is used, albeit at the expense of the signal level. Therefore, the routine use of a confocal pinhole of optimized size is recommended for two-photon microscopy wherever the fluorescence or harmonic signals are large.     

Imaging of optically thick specimen using two-photon excitation microscopy.

The in-depth imaging properties of two-photon excitation microscopy were investigated and compared with those of confocal microscopy. Confocal imaging enabled the recording of images from dental biofilm down to a depth of 40 microm, while two-photon excitation images could be recorded at depths greater than 100 microm. Two-photon excitation point spread functions (PSFs) were recorded at depths ranging from 0 to 90 microm depth using 220-nm diameter fluorescent beads immersed in water. PSFs were measured using both a high numerical aperture oil immersion objective and a water immersion objective. The experiments carried out using the oil immersion objective showed a rapid degradation of both the axial and lateral resolution due to spherical aberrations. In addition, the detected fluorescence intensity rapidly decreased as a function of depth. The experiments carried out using the water immersion objective showed no significant degradation of both the axial and lateral resolution and the fluorescence intensity.     

Time-gated fluorescence lifetime imaging and microvolume spectroscopy using two-photon excitation

A scanning microscope utilizing two-photon excitation in combination with fluorescence lifetime contrast is presented. The microscope makes use of a tunable femtosecond titanium:sapphire laser enabling the two-photon excitation of a broad range of fluorescent molecules, including UV probes. Importantly, the penetration depth of the two-photon exciting (infra)red light is substantially greater than for the corresponding single-photon wavelength while photobleaching is significantly reduced. The time structure of the Ti:Sa laser can be employed in a straightforward way for the realization of fluorescence lifetime imaging. The fluorescence lifetime is sensitive to the local environment of the fluorescent molecule. This behaviour can be used for example to quantify concentrations of ions, such as pH and Ca²⁺, or pO₂ and pCO₂. In the set-up presented here the fluorescence lifetime imaging is accomplished by time-gated single photon counting. The performance and optical properties of the microscope are investigated by a number of test measurements on fluorescent test beads. Point-spread functions calculated from measurements on 230-nm beads using an iterative restoration procedure compare well with theoretical expectations. Lifetime imaging experiments on a test target containing two different types of test bead in a fluorescent buffer all with different lifetimes (2.15 ns, 2.56 ns and 3.34 ns) show excellent quantitative agreement with reference values obtained from time correlated single photon counting measurements. Moreover, the standard deviation in the results can be wholly ascribed to the photon statistics. Measurements of acridine orange stained biofilms are presented as an example of the potential of two-photon excitation combined with fluorescence lifetime contrast. Fluorescence lifetime and intensity images were recorded over the whole sample depth of 100 μm. Fluorescence intensity imaging is seriously hampered by the rapid decrease of the fluorescence signal as a function of the depth into the sample. Fluorescence lifetime imaging on the other hand is not affected by the decrease of the fluorescence intensity.     

Femtosecond pulse width control in microscopy by two-photon absorption autocorrelation

A technique for both the measurement and the control of the pulse width at the focal point of a high-NA lens, based on two-photon absorption interferometric autocorrelation, is presented. The technique is applied to measuring the pulse broadening induced on a pulse propagating through a high-NA lens system for several objectives. It is known that the pulse width may increase by up to ?50% of its original value by propagation through an objective which has wide field compensation for spherical and chromatic aberrations. The two-photon absorption autocorrelation technique allows adjustment of the actual pulse width in the focus of a high-NA lens through pre-chirp compensation. The pulse width is shown to be almost independent of penetration depth into the sample, while the amplitude of the autocorrelation signal shows a strong decrease with depth. The ability to both measure and control the actual pulse width under strong focusing conditions is of direct importance to, among others, two-photon absorption imaging approaches.     

Quasi-spherical focal spot in two-photon scanning microscopy by three-ring apodization

We present a beam-shaping technique for two-photon excitation (TPE) fluorescence microscopy. We show that by inserting a properly designed three-ring pupil filter in the illumination beam of the microscope, the effective optical sectioning capacity of such a system improves so that the point spread function gets a quasi-spherical shape. Such an improvement, which allows the acquisition of 3D images with isotropic quality, is obtained at the expense of only a small increase of the overall energy in the axial sidelobes. The performance of this technique is illustrated with a scanning TPE microscopy experiment in which the image of small beads is obtained. We demonstrate an effective narrowing of 12.5% in the axial extent of the point spread function, while keeping the 82% of the spot-fluorescence efficiency.     

Notes on theory and experimental conditions behind two-photon excitation microscopy

This report deals with the fundamental quantum physics behind two-photon excitation also providing a link to the experimental consequences exploited in microscopy. The optical sectioning effect is demonstrated as well as the distribution of excitation and of fluorescence emission.     

Wide-band acousto-optic deflectors for large field of view two-photon microscope

Acousto-optic deflector (AOD) is an attractive scanner for two-photon microscopy because it can provide fast and versatile laser scanning and does not involve any mechanical movements. However, due to the small scan range of available AOD, the field of view (FOV) of the AOD-based microscope is typically smaller than that of the conventional galvanometer-based microscope. Here, we developed a novel wide-band AOD to enlarge the scan angle. Considering the maximum acceptable acoustic attenuation in the acousto-optic crystal, relatively lower operating frequencies and moderate aperture were adopted. The custom AOD was able to provide 60 MHz 3-dB bandwidth and 80% peak diffraction efficiency at 840 nm wavelength. Based on a pair of such AOD, a large FOV two-photon microscope was built with a FOV up to 418.5 μm (40× objective). The spatiotemporal dispersion was compensated simultaneously with a single custom-made prism. By means of dynamic power modulation, the variation of laser intensity within the FOV was reduced below 5%. The lateral and axial resolution of the system were 0.58-2.12 μm and 2.17-3.07 μm, respectively. Pollen grain images acquired by this system were presented to demonstrate the imaging capability at different positions across the entire FOV.