The use of optical parametric oscillator for harmonic generation and two-photon UV fluorescence microscopy

Ultrafast lasers have found increasing use in scanning optical microscopy due to their very high peak power in generating multiphoton excitations. A mode-locked Ti:sapphire laser is often employed for such purposes. Together with a synchronously pumped optical parametric oscillator (OPO), the spectral range available can be extended to 1,050-1,300 nm. This broader range available greatly facilitates the excitation of second harmonic generation (SHG) and third harmonic generation (THG) due to better satisfaction of phase matching condition that is achieved with a longer excitation wavelength. Dental sections are then investigated with the contrasts from harmonic generation. In addition, through intra-cavity doubling wavelengths from 525-650 nm are made available for effective two-photon (2-p) excitation with the equivalent photon energy in the UVB range (290-320 nm) and beyond. This new capacity allows UV (auto-) fluorescence excitation and imaging, for example, from some amino acids, such as tyrosine, tryptophan, and glycine.     

Second harmonic generation imaging of the deep shade plant Selaginella erythropus using multifunctional two‐photon laser scanning microscopy

Background : Multifunctional two‐photon laser scanning microscopy provides attractive advantages over conventional two‐photon laser scanning microscopy. For the first time, simultaneous measurement of the second harmonic generation (SHG) signals in the forward and backward directions and two photon excitation fluorescence were achieved from the deep shade plant Selaginella erythropus. Results : These measurements show that the S. erythropus leaves produce high SHG signals in both directions and the SHG signals strongly depend on the laser's status of polarization and the orientation of the dipole moment in the molecules that interact with the laser light. The novelty of this work is (1) uncovering the unusual structure of S. erythropus leaves, including diverse chloroplasts, various cell types and micromophology, which are consistent with observations from general electron microscopy; and (2) using the multifunctional two‐photon laser scanning microscopy by combining three platforms of laser scanning microscopy, fluorescence microscopy, harmonic generation microscopy and polarizing microscopy for detecting the SHG signals in the forward and backward directions, as well as two photon excitation fluorescence. Conclusions : With the multifunctional two‐photon laser scanning microscopy, one can use noninvasive SHG imaging to reveal the true architecture of the sample, without photodamage or photobleaching, by utilizing the fact that the SHG is known to leave no energy deposition on the interacting matter because of the SHG virtual energy conservation characteristic.     

Effects of aberrations and specimen structure in conventional, confocal and two-photon fluorescence microscopy

Specimen-induced aberrations cause a reduction in signal levels and resolution in fluorescence microscopy. Aberrations also affect the image contrast achieved by these microscopes. We model the effects of aberrations on the fluorescence signals acquired from different specimen structures, such as point-like, linear, planar and volume structures, when imaged by conventional, confocal and two-photon microscopes. From this we derive the image contrast obtained when observing combinations of such structures. We show that the effect of aberrations on the visibility of fine features depends upon the specimen morphology and that the contrast is less significantly affected in microscopes exhibiting optical sectioning. For example, we show that point objects become indistinguishable from background fluorescence in the presence of aberrations, particularly when imaged in a conventional fluorescence microscope. This demonstrates the significant advantage of using confocal or two-photon microscopes over conventional instruments when aberrations are present.     

Extension of imaging depth in two-photon fluorescence microscopy using a long-wavelength high-pulse-energy femtosecond laser source

We experimentally demonstrate, for the first time to the best of our knowledge, two-photon fluorescence imaging with a femtosecond optical parametric amplifier. In particular, we systematically compare the imaging depths of two-photon fluorescence microscopes based on three different excitation sources, including a femtosecond oscillator, a femtosecond regenerative amplifier and the optical parametric amplifier. The results show that the optical parametric amplifier can greatly extend the penetration depth by approximately 227% as compared with that obtained with the femtosecond oscillator due to effective suppression of scattering at longer wavelength and enhanced excitation efficiency enabled by higher pulse energy.     

High-resolution simultaneous three-photon fluorescence and third-harmonic-generation microscopy

In recent years, nonlinear laser scanning microscopy has gained much attention due to its unique ability of deep optical sectioning. Based on our previous studies, a 1,200-1,300-nm femtosecond laser can provide superior penetration capability with minimized photodamage possibility. However, with the longer wavelength excitation, three-photon-fluorescence (3PF) would be necessary for efficient use of intrinsic and extrinsic visible fluorophores. The three-photon process can provide much better spatial resolution than two-photon-fluorescence due to the cubic power dependency. On the other hand, third-harmonic-generation (THG), another intrinsic three-photon process, is interface-sensitive and can be used as a general structural imaging modality to show the exact location of cellular membranes. The virtual-transition characteristic of THG prevents any excess energy from releasing in bio-tissues and, thus, THG acts as a truly noninvasive imaging tool. Here we demonstrated the first combined 3PF and THG microscopy, which can provide three-dimensional high-resolution images with both functional molecule specificity and sub-micrometer structural mapping capability. The simultaneously acquired 3PF and THG images based on a 1,230-nm Cr:forsterite femtosecond laser are shown with a Hoechst-labeled hepatic cell sample. Strong 3PF around 450 nm from DNA-bounded Hoechst-33258 can be observed inside each nucleus while THG reveals the location of plasma membranes and other membrane-based organelles such as mitochondria. Considering that the maximum-allowable laser power in common nonlinear laser microscopy is less than 10 mW at 800 nm, it is remarkable that even with a 100-mW 1,230-nm incident power, there is no observable photo damage on the cells, demonstrating the noninvasiveness of this novel microscopy technique.     

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.     

Imaging an optical disc by the combined use of scanning tunnelling microscopy and scanning electron microscopy

We present the data obtained by scanning tunnelling microscopy combined with scanning electron microscopy of the digitally encoded structure on a stamper used to fabricate optical discs. The combination allows us to focus the STM tip on a preselected spot with a precision of ?0·3 μm. The data show the superiority of STM for a more detailed characterization of shape, width, length, height and fine structure appearing on the sample. We also show the influence of tip shape on STM resolution. Simultaneous use of both microscopes is possible but high electron doses produce an insulating layer of contaminants thick enough to make STM operation impossible.     

Comparison of two-photon excitation laser scanning microscopy with UV-confocal laser scanning microscopy in three-dimensional calcium imaging using the fluorescence indicator Indo-1

Two-photon excitation laser scanning fluorescence microscopy (2p-LSM) was compared with UV-excitation confocal laser scanning fluorescence microscopy (UV-CLSM) in terms of three-dimensional (3-D) calcium imaging of living cells in culture. Indo-1 was used as a calcium indicator. Since the excitation volume is more limited and excitation wavelengths are longer in 2p-LSM than in UV-CLSM, 2p-LSM exhibited several advantages over UV-CLSM: (1) a lower level of background signal by a factor of 6–17, which enhances the contrast by a factor of 6–21; (2) a lower rate of photobleaching by a factor of 2–4; (3) slightly lower phototoxicity. When 3-D images were repeatedly acquired, the calcium concentration determined by UV-CLSM depended strongly on the number of data acquisitions and the nuclear regions falsely exhibited low calcium concentrations, probably due to an interplay of different levels of photobleaching of Indo-1 and autofluorescence, while the calcium concentration evaluated by 2p-LSM was stable and homogeneous throughout the cytoplasm. The spatial resolution of 2p-LSM was worse by 10% in the focal plane and by 30% along the optical axis due to the longer excitation wavelength. This disadvantage can be overcome by the addition of a confocal pinhole (two-photon excitation confocal laser scanning fluorescence microscopy), which made the resolution similar to that in UV-CLSM. These results indicate that 2p-LSM is preferable for repeated 3-D reconstruction of calcium concentration in living cells. In UV-CLSM, 0.18-mW laser power with a 2.φ pinhole (in normalized optical coordinate) gives better signal-to-noise ratio, contrast and resolution than 0.09-mW laser power with a 4.9-φ pinhole. However, since the damage to cells and the rate of photobleaching is substantially greater under the former condition, it is not suitable for repeated acquisition of 3-D images.     

Frequency domain lifetime and spectral imaging microscopy

In the femtoliter observation volume of a two-photon microscope, multiple fluorophores can be present and complex photophysics can take place. Combined detection of the fluorescence emission spectra and lifetimes can provide deeper insight into specimen properties than these two imaging modalities taken separately. Therefore, we have developed a detection scheme based on a frequency-modulated multichannel photomultiplier, which measures simultaneously the spectrum and the lifetime of the emitted fluorescence. Experimentally, the efficiency of the frequency domain lifetime measurement was compared to a time domain set-up. The performance of this spectrally and lifetime-resolved microscope was evaluated on reference specimens and living cells labeled with three different stains targeting the membrane, the mitochondria, and the nucleus.     

Spectra and lifetimes of fluorescence resonance energy transfer fluorophores under two-photon excitation

We show two-photon spectra and lifetimes acquired using conventional confocal microscopes equipped with an ultra-short pulsed laser and a time-gated intensified charge coupled device. We report on the two-photon spectra and lifetimes of Alexa350, enhanced green fluorescent protein (EGFP), EGFP-CD46, and Cy3 labelled antibodies. Cellular and extracellular EGFP two-photon spectra and lifetimes are compared.     

Direct measurement of glutathione in epidermal cells of intact Arabidopsis roots by two-photon laser scanning microscopy

Two-photon laser scanning microscopy (TPLSM) was used to directly measure glutathione (GSH) as its fluorescent glutathione S-bimane conjugate (GSB) in developing root hair cells (trichoblasts) and non-root hair cells (atrichoblasts) of intact Arabidopsis roots. In comparison to confocal microscopy, TPLSM showed more detail deep within the tissue with less signal attenuation. The total level of GSB labelling reached a plateau after 60 min in both trichoblasts and atrichoblasts, reflecting depletion of GSH. GSB was formed initially in the cytoplasm and was subsequently transported into the vacuole. The volume ratio of vacuole to cytoplasm was determined using the Cavalieri estimator of volume and used to calculate the amount of GSB per volume of cytoplasm in each cell type. At the end of the time-course the cytoplasmic concentration of GSB was 2.7 ± 0.5 m m ( n  = 5) in trichoblasts and 5.5 ± 0.8 m m ( n  = 5) in atrichoblasts. In trichoblasts this value represents the initial concentration of GSH in the cytoplasm. Labelling of roots with monochlorobimane (MCB) on ice led to the formation of GSB in the cytoplasm, but prevented vacuolar sequestration. After washing prelabelled roots and transfer to room temperature, vacuolar transport resumed. Although no free MCB was present the total amount of GSB in atrichoblasts increased further, indicating that the higher values recorded in the atrichoblasts might reflect additional symplastic transport and sequestration of GSB from neighbouring cells.     

Fast scanning STED and two-photon fluorescence excitation microscopy with continuous wave beam

In this paper we report stimulated emission depletion (STED) and two-photon excitation (2PE) fluorescence microscopy with continuous wave (CW) laser beam using a new generation laser scanning confocal microscope equipped for STED-CW (TCS STED-CW, Leica Microsystems, Mannheim, Germany). We show the possibility to achieve CW-2PE with the very same beam used for STED-CW. This feature extends the performance of the microscope allowing multimodal imaging (CW-2PE, STED-CW, confocal).     

Imaging and colour coding of magnetic domains by kerr scanning optical microscopy

The imaging of ferromagnetic domains by the transverse Kerr effect using a scanning optical microscope (SOM) with two or four directions of light incidence (± x, ± y) allows the digital record of the B_y and B_x components of the magnetic induction B . These components can be used to calculate a two-dimensional colour-coded map of B , which can be superposed by vector arrows.     

A comparison study of detecting gold nanorods in living cells with confocal reflectance microscopy and two‐photon fluorescence microscopy

Two‐photon fluorescence microscopy and confocal reflectance microscopy were compared to detect intracellular gold nanorods in rat basophilic leukaemia cells. The two‐photon photoluminescence images of gold nanorods were acquired by an 800 nm fs laser with the power of milliwatts. The advantages of the obtained two‐photon photoluminescence images are high spatial resolution and reduced background. However, a remarkable photothermal effect on cells was seen after 30 times continuous scanning of the femto‐second laser, potentially affecting the subcellular localization pattern of the nanorods. In the case of confocal reflectance microscopy the images of gold nanorods can be obtained with the power of light source as low as microwatts, thus avoiding the photothermal effect, but the resolution of such images is reduced. We have noted that confocal reflectance images of cellular gold nanorods achieved with 50 μW 800 nm fs have a relatively poor resolution, whereas the 50 μW 488 nm CW laser can acquire reasonably satisfactory 3D reflectance images with improved resolution because of its shorter wavelength. Therefore, confocal reflectance microscopy may also be a suitable means to image intracellular gold nanorods with the advantage of reduced photothermal effect.     

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.     

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.     

Optimizing multiphoton fluorescence microscopy light collection from living tissue by noncontact total emission detection (epiTED)

A benefit of multiphoton fluorescence microscopy is the inherent optical sectioning that occurs during excitation at the diffraction-limited spot. The scanned collection of fluorescence emission is incoherent; that is, no real image needs to be formed on the detector plane. The nearly isotropic emission of fluorescence excited at the focal spot allows for new detection schemes that efficiently funnel all attainable photons to detector(s). We previously showed [Combs, C.A., et al. (2007) Optimization of multiphoton excitation microscopy by total emission detection using a parabolic light reflector. J. Microsc. 228, 330-337] that parabolic mirrors and condensers could be combined to collect the totality of solid angle around the excitation spot for tissue blocks, leading to ～8-fold signal gain. Using a similar approach, we have developed an in vivo total emission detection (epiTED) instrument modified to make noncontact images from outside of living tissue. Simulations suggest that a ～4-fold enhancement may be possible (much larger with lower NA objectives than the 0.95 NA used here) with this approach, depending on objective characteristics, imaging depth and the characteristics of the sample being imaged. In our initial prototype, 2-fold improvements were demonstrated in the mouse brain and skeletal muscle as well as the rat kidney, using a variety of fluorophores and no compromise of spatial resolution. These results show this epiTED prototype effectively doubles emission signal in vivo; thus, it will maintain the image signal-to-noise ratio at two times the scan rate or enable full scan rate at approximately 30% reduced laser power (to minimize photo-damage).     

Characterization of uniform ultrathin layer for z-response measurements in three-dimensional section fluorescence microscopy

Layer‐by‐layer technique is used to adsorb a uniform ultrathin layer of fluorescently labelled polyelectrolytes on a glass cover slip. Due to their thickness, uniformity and fluorescence properties, these ultrathin layers may serve as a simple and applicable standard to directly measure the z‐response of different scanning optical microscopes. In this work we use ultrathin layers to measure the z‐response of confocal, two‐photon excitation and 4Pi laser scanning microscopes. Moreover, due to their uniformity over a wide region, i.e. cover slip surface, it is possible to quantify the z‐response of the system over a full field of view area. This property, coupled with a bright fluorescence signal, enables the use of polyelectrolyte layers for representation on sectioned imaging property charts: a very powerful method to characterize image formation properties and capabilities (z‐response, off‐axis aberration, spherical aberration, etc.) of a three‐dimensional scanning system. The sectioned imaging property charts method needs a through‐focus dataset taken from such ultrathin layers. Using a comparatively low illumination no significant bleaching occurs during the excitation process, so it is possible to achieve long‐term monitoring of the z‐response of the system. All the above mentioned properties make such ultrathin layers a suitable candidate for calibration and a powerful tool for real‐time evaluation of the optical sectioning capabilities of different three‐dimensional scanning systems especially when coupled to sectioned imaging property charts.     

Parameters and mechanisms governing image contrast in scanning electron microscopy of single-walled carbon nanotubes

Image formation of single-walled carbon nanotubes (SWNTs) in the scanning electron microscope (SEM) is peculiarly sensitive to primary electron landing energy, imaging history, sample/substrate geometry, electrical conductivity, sample contamination, and substrate charging. This sensitivity is probably due to the extremely small interaction volume of the SWNTs' monolayered, nanoscale structures with the electron beam. Traditional electron beam/bulk specimen interaction models appear unable to explain the contrast behavior when directly applied to SWNTs. We present one systematic case study of SWNT SEM imaging with special attention to the above parameters and propose some physical explanations for the effect of each. We also demonstrate that it is possible to employ voltage biasing to counteract this extrinsic behavior, gain better control of the image contrast, and facilitate the interpretation of SWNT images in the SEM.