Biodistribution of indocyanine green in a porcine burn model: light and fluorescence microscopy.

BACKGROUND: Infrared-excited fluorescence of intravenously administered indocyanine green (ICG) is being used as a method of early determination of burn depth. METHODS: Fluorescence microscopy and tissue fluorescence were recorded in a porcine burn model and correlated to burn severity and age. RESULTS: Recently placed superficial burns show significant fluorescence compared with adjacent normal tissue as a result of a strong inflammatory reaction in the superficial dermis with minimal vascular occlusion. The magnitude of the inflammatory reaction decreases with time. For deeper burns, vascular occlusion prevents transport of ICG into the burn and the intensity of ICG fluorescence in burn eschar is negligible. CONCLUSION: The intensity of ICG fluorescence measured at the surface of the wound for burns of similar age was shown to decrease exponentially with the depth of the burn. The enhanced fluorescence of partial-thickness burns is attributable to increased permeability, and the decreased signal associated with deeper injuries is attributable to vascular occlusion. These results suggest that it is possible to differentiate burns that will heal spontaneously with minimal granulation from those that will not by measuring the intensity of ICG fluorescence.

Quantitative comparison of background rejection, signal-to-noise ratio, and resolution in confocal and full-field laser scanning microscopes.

Development of a laser scanning microscope for simultaneous three-dimensional imaging in both a full-field laser scanning mode (FLSM) and a confocal laser scanning mode (CLSM) permits the direct comparison of axial resolution and out-of-focus background rejection as a function of sample thickness for both FLSM and CLSM with varying detector aperture (pinhole) radii. The sample-dependent detector aperture radii that optimize the signal-to-noise ratio (S/N) in the CLSM are experimentally determined. The results verify earlier calculations [Appl. Opt. 33, 603 (1994)]. Using these results, we discuss the practical and theoretical limits on the S/N in the CLSM and compare them with those of a full-field epifluorescence microscope (FEM) that is enhanced by image deconvolution. The specimen volume over which the FLSM exhibits imaging properties that are equivalent to a FEM is calculated in the appendices.

Imaging of total intracellular calcium and calcium influx and efflux in individual resting and stimulated tumor mast cells using ion microscopy.

Ion microscopy was employed to investigate intracellular total calcium concentrations and calcium influx, and efflux in resting and antigen-stimulated tumor mast cells (RBL-2H3 cells). The nucleus, a perinuclear region which included the Golgi apparatus (Golgi region), and the remaining cytoplasm were spatially resolved with the Cameca IMS-3f ion microscope in cryogenically prepared cells. In resting cells the nucleus contained about 0.60 mM, the Golgi region about 1.2 mM, and the remaining cytoplasm about 1.0 mM total calcium. Antigen stimulation of rat basophilic leukemia cells resulted in a significant loading of calcium in all three cellular compartments. Antigen stimulation in the absence of extracellular calcium resulted in a significant loss of total calcium from all three intracellular compartments. Influx and efflux of calcium were measured simultaneously in resting and stimulated cells by using stable 44Ca in the extracellular solution, and by imaging mass 40 to determine the native intracellular calcium (40Ca) and mass 44 to localize the 44Ca that entered the cell from extracellular solution. After a 10-min incubation, 0.240 fmol of the total calcium per cell had been replaced with 44Ca, which amounts to about 33% of the total cell calcium. If antigen was present during this incubation there was an additional loss of 0.229 fmol of 40Ca and an added gain of 0.476 fmol of 44Ca per cell, which corresponds to a net increase in total intracellular calcium of 0.247 fmol.

A confocal laser scanning microscope designed for indicators with ultraviolet excitation wavelengths.

In this paper we describe the modifications necessary to upgrade, at affordable cost, a commercially available confocal laser scanning microscope for use with ultraviolet (UV) excitation. The optical problems associated with these modifications are described in detail, and easy solutions to solve them are suggested. The optical resolution of the instrument was tested with fluorescent beads and was found to be close to diffraction limited. The light losses due to lateral chromatic aberration were assessed in a thick fluorescent specimen and were found to be comparable to those usually observed with visible light. For a more visual example of the resolution of this instrument, isolated ventricular heart muscle cells were loaded with the fluorescent Ca2+ indicator indo 1. This allowed us to visualize subcellular structural detail and to illustrate the optical sectioning capability of the UV confocal microscope when recording indo 1 emission. Dual-emission line scans were used to perform ratiometric time-resolved detection of Ca2+ transients in voltage-clamped heart muscle cells loaded with the salt form of indo 1. The system presented in this paper should significantly broaden the range of fluorescent indicators that can be used in confocal microscopy.

Background rejection and signal-to-noise optimization in confocal and alternative fluorescence microscopes.

In the confocal microscope, tightly focused illumination and spatially filtered detection are combined to reduce out-of-focus background and to produce high-quality images that display thin optical sections within thick fluorescent specimens. We define background as the detected light that originates outside a resolution volume and signal as the detected light that originates within the same volume. Background rejection is measured by the signal-to-background ratio (S/B) and is calculated for confocal, spinning-disk, line-illumination, slit-detection, and conventional fluorescence microscopes as a function of both the spatial filter size and the specimen thickness. Spatial filter sizes that reject background and optimize the signal-to-noise ratio (S/N) are calculated for each microscope. These calculations are normalized so that the time-averaged illumination at each point in the specimen is the same for each microscope. For thick specimens, we show that the S/B obtained with a confocal microscope can be more than 100 times greater than the S/B available with a conventional microscope, and we find that the optimal confocal S/N can be a factor of 10 greater than the S/N in the conventional microscope.