The thermodynamic response of soft biological tissues to pulsed ultraviolet laser irradiation.

The physical mechanisms that enable short pulses of high-intensity ultraviolet laser radiation to remove tissue, in a process known as laser ablation, remain obscure. The thermodynamic response of biological tissue to pulsed laser irradiation was investigated by measuring and subsequently analyzing the stress transients generated by pulsed argon fluorine (ArF, lambda = 193 nm) and krypton fluorine (KrF, lambda = 248 nm) excimer laser irradiation of porcine dermis using thin-film piezoelectric transducers. For radiant exposures that do not cause material removal, the stress transients are consistent with rapid thermal expansion of the tissue. At the threshold radiant exposure for ablation, the peak stress amplitude generated by 248 nm irradiation is more than an order of magnitude larger than that produced by 193 nm irradiation. For radiant exposures where material removal is achieved, the temporal structure of the stress transient indicates that the onset of material removal occurs during irradiation. In this regime, the variation of the peak compressive stress with radiant exposure is consistent with laser-induced rapid surface vaporization. For 193 nm irradiation, ionization of the ablated material occurs at even greater radiant exposures and is accompanied by a change in the variation of peak stress with radiant exposure consistent with a plasma-mediated ablation process. These results suggest that absorption of ultraviolet laser radiation by the extracellular matrix of tissue leads to decomposition of tissue on the time scale of the laser pulse. The difference in volumetric energy density at ablation threshold between the two wavelengths indicates that the larger stresses generated by 248 nm irradiation may facilitate the onset of material removal. However, once material removal is achieved, the stress measurements demonstrate that energy not directly responsible for target decomposition contributes to increasing the specific energy of the plume (and plasma, when present), which drives the gas dynamic expansion of ablated material. This provides direct evidence that ultraviolet laser ablation of soft biological tissues is a surface-mediated process and not explosive in nature.     

用二次谐波成像技术研究经飞秒激光切削后角膜变化

本文用二次谐波成像技术（second harmonic generation SHG）来研究飞秒激光切削后角膜结构的变化.在生物学研究,材料科学等方面都有很广泛应用的SHG成像技术能在不破坏的角膜情况下获得高对比度的角膜层析图像,分辨率为500 nm,实验装置是利用现有的双光子显微镜.本文还根据成像结果评价了飞秒激光在角膜切削中的质量,为飞秒激光微米级的精确切削和临床应用提供了实验支持.     

Vector Alkaline Phosphatase Substrate Blue III: One Substrate for Brightfield Histochemistry and High-resolution Fluorescence Imaging by Confocal Laser Scanning Microscopy

A number of histochemical chromogenic substrates for alkaline phosphatase are commercially available and give reaction products with a range of colours for brightfield examination. Some of these reaction products are also fluorescent, exhibiting a wide excitation range and a broad emission peak. We report here that one of these substrates, Vector Blue III, yields a stable, strongly fluorescent reaction product with an excitation peak around 500 nm and a large Stokes shift to an emission peak at 680 nm. The reaction product can be excited using a mercury lamp with a fluorescein excitation filter or an argon ion laser at 488 nm or 568 nm, and the emission detected using a long-pass filter designed for Cy-5. Thus, a single substrate is suitable for brightfield imaging of tissue sections and high-resolution analysis of subcellular detail, using a confocal laser scanning microscope, in the same specimen.     

2′,7′-Bis-(2-carboxyethyl)-5(6)-carboxyfluorescein as a dual-emission fluorescent indicator of intracellular pH suitable for argon laser confocal microscopy

The widely used fluorescent probe 2',7'-bis-(2-carboxyethyl)-5(6)-carboxyfluorescein (BCECF) serves as a pH-sensitive indicator in classical microscopy. Characteristics of BCECF were studied and a way of employing the probe in a confocal laser scanning microscope equipped with an argon laser at 488 nm was developed, based on the fact that the emission fluorescence spectra are pH-dependent with spectral maximum shift from 518 to 529 nm. Optical filters for the dual-emission ratio method were set to 506 and 529 nm. pH values measured inside a single cell of Saccharomyces cerevisiae were similar to those obtained with other pH estimation methods.     

Alkaline phosphatase cytochemistry in confocal scanning light microscopy for imaging the bone marrow stroma

This paper reports on the use of alkaline phosphatase cytochemistry and combined conventional and confocal reflection and fluorescence scanning light microscopic modes in the study of human marrow stroma. It was found that the end product of the enzyme reaction using Napthol AS phosphate as substrate and Fast Blue BB as coupler reflected the 633 nm (red) light from a Helium-Neon laser. Serial optical sections suitable for 3-D reconstruction and selectively depicting the marrow reticulum cells could be obtained from thick glycol methacrylate sections reacted for Alkaline phosphatase. Furthermore, the yellow background of uncoupled diazonium salt over cytochemically unreactive structures in the same specimens and fields was used for imaging haemopoietic cell mass by operating the microscope at 488 nm (argon ion laser, blue-green). These methods may offer advantages in the investigation of the bone marrow stroma and its interplay with haemopoiesis and osteogenesis in normal and disease conditions.     

Receptor-mediated calcium signal playing a nuclear third messenger in the activation of antigen-specific B cells.

We have studied receptor-mediated calcium signals in antigen-specific B cells (trinitrophenol-specific B cell clone, TP67.21) using a confocal fluorescence microscope with an argon ion laser (488 nm) and a He-Cd laser (325 nm). Confocal fluorescence images of fluo-3 loaded B cells, excited by an argon ion laser, became much brighter and more nonhomogeneous than those before antigen stimulation. Time-dependent fluorescence changes in intensities were abrupt and quite similar to the patterns of the intracellular calcium ion concentration [Ca2+]i observed by a conventional fluorescence microscope using fura-2. From the morphological patterns of the calcium images, the parts of the bright fluorescence seemed to belong to the nucleus in B cells. To confirm the above events we measured the confocal fluorescence images of the nucleus. From the fluorescence images of co-loaded Hoechst 33342 (a DNA-specific fluorescent probe), which excited by a He-Cd laser, the brighter parts of the fluo-3 fluorescence intensities were identified to the nucleus in B cells. This suggested the possibility that the increased intranuclear calcium ions may play a nuclear third messenger in B cells.     

Second-harmonic imaging microscopy for visualizing biomolecular arrays in cells, tissues and organisms

Although the nonlinear optical effect known as second-harmonic generation (SHG) has been recognized since the earliest days of laser physics and was demonstrated through a microscope over 25 years ago, only in the past few years has it begun to emerge as a viable microscope imaging contrast mechanism for visualization of cell and tissue structure and function. Only small modifications are required to equip a standard laser-scanning two-photon microscope for second-harmonic imaging microscopy (SHIM). Recent studies of the three-dimensional in vivo structures of well-ordered protein assemblies, such as collagen, microtubules and muscle myosin, are beginning to establish SHIM as a nondestructive imaging modality that holds promise for both basic research and clinical pathology. Thus far the best signals have been obtained in a transmitted light geometry that precludes in vivo measurements on large living animals. This drawback may be addressed through improvements in the collection of SHG signals via an epi-illumination microscope configuration. In addition, SHG signals from certain membrane-bound dyes have been shown to be highly sensitive to membrane potential. Although this indicates that SHIM may become a valuable tool for probing cell physiology, the small signal size would limit the number of photons that could be collected during the course of a fast action potential. Better dyes and optimized microscope optics could ultimately lead to the imaging of neuronal electrical activity with SHIM.     

Dual‐color STED super‐resolution microscope using a single laser source

STED (stimulated emission depletion) microscopy is one of the most promising super‐resolution fluorescence microscopies，due to its fast imaging and ultra‐high resolution. In this paper, we present a dual‐color STED microscope with a single laser source. Polarization beam splitters are used to separate the output from a supercontinuum laser source into four laser beams, including two excitation beams (488, 635 nm) and two depletion beams (592, 775 nm). These four laser beams are then used to build a low cost dual‐color STED system to achieve a spatial resolution of 75 nm in cell samples.     

Computed tomography-based spectral imaging for fluorescence microscopy

The computed tomography imaging spectrometer (CTIS) is a non-scanning instrument capable of simultaneously acquiring full spectral information (450-750 nm) from every position element within its field of view (75 microm x 75 microm). The current spatial and spectral sampling intervals of the spectrometer are 1.0 microm and 10 nm, respectively. This level of resolution is adequate to resolve signal responses from multiple fluorescence probes located within individual cells or different locations within the same cell. Spectral imaging results are presented from the CTIS combined with a commercial inverted fluorescence microscope. Results demonstrate the capability of the CTIS to monitor the spatiotemporal evolution of pH in rat insulinoma cells loaded with SNARF-1. The ability to analyze full spectral information for two-dimensional (x, y) images allows precise evaluation of heterogeneous physiological responses within cell populations. Due to low signal levels, integration times up to 2 s were required. However, reasonable modifications to the instrument design will provide higher system transmission efficiency with increased temporal and spatial resolution. Specifically, a custom optical design including the use of a larger format detector array is under development for a second-generation system.     

A high-resolution, confocal laser-scanning microscope and flash photolysis system for physiological studies

We describe the construction of a high-resolution confocal laser-scanning microscope, and illustrate its use for studying elementary Ca²⁺ signalling events in cells. An avalanche photodiode module and simple optical path provide a high efficiency system for detection of fluorescence signals, allowing use of a small confocal aperture giving near diffraction-limited spatial resolution (< 300 nm lateral and < 400 nm axial). When operated in line-scan mode, the maximum temporal resolution is 1 ms, and the associated computer software allows complete flexibility to record lines-cans continuously for long (minutes) periods or to obtain any desired pixel resolution in x-y scans. An independent UV irradiation system permits simultaneous photolysis of caged compounds over either a uniform, wide field (arc lamp source) or at a tightly focussed spot (frequency-tripled Nd:YAG laser). The microscope thus provides a versatile tool for optical studies of dynamic cellular processes, as well as excellent resolution for morphological studies. The confocal scanner can be added to virtually any inverted microscope for a component cost that is only a small fraction of that of comparable commercial instruments, yet offers better performance and greater versatility.     

Helium-neon laser preirradiation induces protection against UVC radiation in wild-type E. coli strain K12AB1157

We have observed that preirradiation with a helium-neon laser (632.8 nm) induces protection against UVC radiation in wild-type E. coli strain K12AB1157. The magnitude of protection was found to depend on the helium-neon laser irradiance, exposure time, and period of incubation between helium-neon laser exposure and subsequent UVC irradiation. The optimum values for dose, irradiance and interval between the two exposures were found to be 7 kJ/m(2), 100 W/m(2) and 1 h, respectively. The possible involvement of singlet oxygen in the helium-neon laser-induced protection is also discussed.     

Quantitative two-photon Ca2+ imaging via fluorescence lifetime analysis

Two-photon microscopy (TPM) revolutionized Ca2+ imaging by allowing recordings in the depth of intact tissue and live organisms. A serious limitation in TPM, however, is the lack of an accurate and straightforward approach for the quantification of Ca2+ signals, an ability that became an invaluable tool in fluorescence microscopy. Here, we present time-correlated fluorescence lifetime imaging (tcFLIM) as a ratiometric method for the quantification of Ca2+ signals in TPM. The fluorescence lifetime of the Ca2+-indicator dye Oregon Green BAPTA-1 (OGB-1) can be recorded using the approximately 80 MHz excitation pulses utilized in TPM. It shows a Ca2+ dependence that can be explained by the Ca2+-affinity, spectral properties and purity of the dye. Pixel-wise lifetime recordings, controlled by a laser-scanning microscope, allowed quantitative Ca2+ imaging in full-frame and linescan mode. Although we focused on the high-affinity Ca2+ indicator OGB-1, our tcFLIM-based quantification is applicable to other Ca2+ dyes and to fluorescence indicators in general.     

Microscopic instrumentation and analysis of laser-tissue interaction in a skin flap model

A dorsal skin flap model for microcirculatory studies has been modified for "in vivo" studies of laser-tissue interaction with microcirculation. An experimental apparatus has been built implementing a laser delivery system, video microscopy during irradiation, and thermal recordings. This model has been used to study irradiation effects on microcirculation using the argon laser (488 and 514.5 nm) and the argon pumped dye laser at 577 nm. The results include: measurements of the optical properties of the model; dosimetry measurements for the production of embolized and stationary coaguli in arterioles and venules; and focal vessel disappearance of venules irradiated with the argon or the argon pumped dye laser at 577 nm; a method to determine light attenuation in the model; a unique method for measurements of blood flow velocity in arterioles and venules and measurements obtained with this method; measurements of transient and steady state temperatures during irradiation and a study of laser induced photorelaxation phenomena in venules.     

Construction of a confocal microscope for real-time x-y and x-z imaging

We describe the construction of a simple 'real-time' laser-scanning confocal microscope, and illustrate its use for rapid imaging of elementary intracellular calcium signaling events. A resonant scanning galvanometer (8 kHz) allows x-y frame acquisition rates of 15 or 30 Hz, and the use of mirrors to scan the laser beam permits use of true, pin-hole confocal detection to provide diffraction-limited spatial resolution. Furthermore, use of a piezoelectric device to rapidly focus the objective lens allows axial (x-z) images to be obtained from thick specimens at similar frame rates. A computer with image acquisition and graphics cards converts the output from the microscope to a standard video signal, which can then be recorded on videotape and analyzed by regular image processing systems. The system is largely made from commercially available components and requires little custom construction of mechanical parts or electronic circuitry. It costs only a small fraction of that of comparable commercial instruments, yet offers greater versatility and similar or better performance.     

Construction of a two-photon microscope for video-rate Ca imaging

We describe the construction of a video-rate two-photon laser scanning microscope, compare its performance to a similar confocal microscope, and illustrate its use for imaging local Ca(2+) transients from cortical neurons in brain slices. Key features include the use of a Ti-sapphire femtosecond laser allowing continuous tuning over a wide (700-1000 nm) wavelength range, a resonant scanning mirror to permit frame acquisition at 30 Hz, and efficient wide-field fluorescence detection. Two-photon imaging provides compelling advantages over confocal microscopy in terms of improved imaging depth and reduced phototoxicity and photobleaching, but the high cost of commercial instruments has limited their widespread adoption. By constructing one's own system the expense is greatly reduced without sacrifice of performance, and the microscope can be more readily tailored to specific applications.     

Protein profiled features patterned via confocal microscopy

Protein patterns were printed using conventional microlithographic materials in a bilayer arrangement and unconventional exposure tools. The bilayer resist stack consisted of a lower poly(tert-butyl methacrylate) layer and an upper diazonaphtoquinone/novolak layer. The protein features were printed in either 'contact printing', or 'step and repeat' mode. The latter printing mode can be managed in a flow-cell consisting of a standard microscope slide and cover slip, spaced apart by about 20 microm, as follows: (i) the exposure step is carried out in the cell using focused 488 nm beam of a confocal laser scanning microscope; (ii) the development step is performed by flowing the photoresist developer through the cell; (iii) the selective deposition of the protein (FITC-labelled avidin) is achieved via the flow of the protein solution through the cell until a desired contrast has been reached; (iv) the control of the process is assured using on-line monitoring of the photo-activated red fluorescence of the developing resist layer, and of the green fluorescence of the FITC-protein patterns, respectively. The protein printing technique uses equipment routinely available in biological laboratory. The 'step and repeat' patterning yields high and controllable resolution. The process can be applied in the fabrication of medical microanalysis devices.     

A photoreactive fluorescent marker for identifying eosinophils and their cytoplasmic granules in tissues.

Here we describe a simple histochemical technique that provides an improved approach to identifying eosinophil components in tissues through the formation of photoreactive complexes that produce stable fluorescent emissions. This method worked readily with histological tissue sections 6-60 microm thick, which were fixed in neutral buffered formalin (NBF), and with cell suspensions similarly fixed and unfixed. Deep red (>605 nm) fluorescent emissions were produced by eosinophil-specific granules when exposed to broadband excitation spectra from a 100-W mercury lamp source (510-590 nm), as well as single-wavelength excitations from both an argon laser (488 nm) and a UV-visible laser (514 nm). The fluorophore-granule complex emissions increased in intensity during the first minute of continuous photoexcitation, then remained stable (>10 min). All nonspecific autofluorescence phenomena associated with these tissues were photobleached in the first minute, including areas of background Biebrich scarlet binding where photoreactive complexes were not formed (i.e., collagen), indicating environmental influences on the fluorophore. This technique allows the visualization of eosinophil granules over a greater period of time than is usually permissible with standard fluorescent markers. Therefore, techniques such as confocal microscopy can be utilized to their fullest extent, providing much more detailed information on the location and distribution of the cytoplasmic contents of eosinophils.     

A proteasomal stress response: pre-treatment with proteasome inhibitors increases proteasome activity and reduces neuronal vulnerability to oxidative injury

We report here that exposure to low concentrations of proteasome inhibitors (e.g. 10-100 nm MG-132, 0.1-3 nm epoxomicin or 10-30 nm clasto-lactacystin beta-lactone) resulted in an enhancement, rather than an inhibition, of proteasome activity in cultured neocortical neurons. Size-fractionation chromatography confirmed that the enhanced peptide cleavage activity was associated with proteasome-sized complexes. This sub toxic exposure reduced neuronal death caused by subsequent exposure to oxidative stress (100-200 microm H(2)O(2) for 30 min, 24-h exposure to 100 microm paraquat or 7.5 microm menadione), but did not alter vulnerability to excitotoxicity (5-min exposure to 30-100 microm NMDA or 24 exposure to 12 microm NMDA). Sub toxic proteasome inhibitor exposure caused an increase in levels of proteasome core subunit proteins and mRNAs, but not in levels of potentially cytoprotective heat shock proteins (hsp70, hsp90 and hsp40). The neuroprotective effects of proteasome inhibitor pre-treatment were blocked by coapplication of proteasome inhibitors during the oxidative insult. These findings support a model in which sublethal proteasome inhibition induces neurons to increase proteasome activity and promotes resistance to oxidative injury and suggests that enhancement of proteasome activity is a potential therapeutic target for diseases in which oxidative stress has been implicated.     

siRNA release from gold nanoparticles by nanosecond pulsed laser irradiation and analysis of the involved temperature increase

Nanosecond pulsed laser irradiation can trigger a release of nucleic acids from gold nanoparticles, but the involved nanoeffects are not fully understood yet. Here we investigate the release of coumarin labeled siRNA from 15 to 30 nm gold particles after nanosecond pulsed laser irradiation. Temperatures in the particle and near the surface were calculated for the different radiant exposures. Upon irradiation with laser pulses of 4 nanosecond duration release started for both particle sizes at a calculated temperature increase of approximately 500 K. Maximum coumarin release was observed for 15 nm particles after irradiation with radiant exposure of 80 mJ cm^?2 and with 32 mJ cm^?2 for 30 nm particles. This corresponds to a temperature increase of 815 and 900 K, respectively. Our results show that the molecular release by nanosecond pulsed irradiation is based on a different mechanism compared to continuous or femtosecond irradiation. Local temperatures are considerably higher and it is expected that bubble formation plays a crucial role in release and damage to cellular structures.