This PDF file contains the editorial “Special Section Guest Editorial: Multiphoton Microscopy” for JBO Vol. 8 Issue 03

Multiphoton microscopy is becoming a popular mode of live and fixed cell imaging. This mode of imaging offers several advantages due to the fact that fluorochrome excitation is a nonlinear event resulting in excitation only at the plane of focus. Multiphoton excitation is enhanced by the use of ultrafast lasers emitting in the near IR, offering better depth penetration coupled with efficient excitation. Because these lasers, such as titanium:sapphire lasers, offer tunable output it is possible to use them to collect multiphoton excitation spectra. We use the software-tunable Coherent Chameleon laser coupled to the Zeiss LSM 510 META NLO to acquire x-y images of biological samples at multiple excitation wavelengths, creating excitation lambda stacks. The mean intensity of pixels within the image plotted versus excitation wavelength reveals the excitation spectra. Excitation lambda stacks can be separated into individual images corresponding to the signal from different dyes using linear unmixing algorithms in much the same way that emission fingerprinting can be used to generate crosstalk free channels from emission lambda stacks using the META detector. We show how this technique can be used to eliminate autofluorescence and to produce crosstalk-free images of dyes with very close overlap in their emission spectra that cannot be separated using emission fingerprinting. Moreover, excitation finger- printing can be performed using nondescanned detectors (NDDs), offering more flexibility for eliminating autofluorescence or crosstalk between fluorochromes when imaging deep within the sample. Thus, excitation fingerprinting complements and extends the functions offered by the META detector and emission fingerprinting. We correct biases in the laser and microscope transmission to acquire realistic multiphoton excitation spectra for fluorochromes within cells using the microscope, which enables the optimization of the excitation wavelength for single and multilabel experiments and provides a means for studying the influence of the biological environment on nonlinear excitation.

One- and two-photon fluorescence resonance energy transfer (FRET) microscopy, using different bandwidth emission filters and a novel spectral spillover correction algorithm (PFRET algorithm), provides the basis for a quantitative approach to measure receptor clustering in endocytic membranes. Emission filters with wider bandwidth allow for an increased FRET signal and corresponding spillover. Treatment with the PFRET correction algorithm results in increasing correction levels and comparable energy transfer efficiency (E%) values, thus validating our algorithm-based approach. The relationship between E% and acceptor and donor levels and donor:acceptor (D:A) ratio is used to characterize the distribution of receptor-ligand complexes in endocytic membranes. In addition to the standard test for clustering (E%'s independence from acceptor levels), we describe a second parameter: the negative dependence of E% on increasing donor levels and D:A ratio. A donor geometric exclusion hypothesis is proposed to explain this phenomenon. One- and two-photon FRET microscopy assays show that polymeric IgA-receptor-ligand complexes are organized in clusters within apical endocytic membranes of polarized Madin-Darby canine kidney cells.

Traumatic brain injury (TBI) remains the most common cause of death in persons under age 45 in the Western world. One of the principal determinants of morbidity and mortality following TBI is traumatic axonal injury (TAI). Current hypotheses on the pathogenesis of TAI involve activation of apoptotic cascades secondary to TBI. While a number of studies have demonstrated direct evidence for the activation of apoptotic cascades in TAI, the precise pathway by which these cascades are initiated remains a subject of intense investigation. As axolemmal disruption with the subsequent intra-axonal influx of large molecular weight species has been demonstrated to occur in relation to local axonal breakdown, attention has focused on cascades that may occur as a result of loss of ionic homeostasis. One proposed pathway by which this has been hypothesized to occur is the Ca²⁺-mediated activation of calmodulin and subsequent activation of the phosphatase calcineurin with dephosphorylation of a protein known as BAD, leading to a proapoptotic interaction between BAD and the mitochondrial protein Bcl-xL. While this pathway is an intriguing route for traumatic axonal pathogenesis, neither conventional immunocytochemical/histochemical nor ultrastructural approaches have had the capacity to shed insight on whether BAD and Bcl-xL interact in TAI in vivo. We describe the implementation of confocal and two-photon excitation fluorescence resonance energy transfer (FRET) microscopy techniques through which we demonstrate interaction between the proapoptotic protein BAD and the prosurvival protein Bcl-xL within TAI following TBI. Further, we report on a method to reliably detect protein interactions within aldehyde fixed tissue sections through conventional immunohistochemical approaches.

We have employed a spectroscopic approach for monitoring fluorescence resonance energy transfer (FRET) in living cells. This method provides excellent spectral separation of green fluorescent protein (GFP) mutant signals within a subcellular imaging volume using two-photon excited fluorescence imaging and spectroscopy (TPIS-FRET). In contrast to current FRET-based methodologies, TPIS-FRET does not rely on the selection of optical filters, ratiometric image analysis, or bleedthrough correction algorithms. Utilizing the intrinsic optical sectioning capabilities of TPIS-FRET, we have identified protein–protein interactions within discrete subcellular domains. To illustrate the applicability of this technique to the detection of homodimer formation, we demonstrated the in vivo association of promyleocyte (PML) homodimers within their corresponding nuclear body.

Fluorescence lifetime imaging microscopy (FLIM) using multiphoton excitation techniques is now finding an important place in quantitative imaging of protein–protein interactions and intracellular physiology. Recent developments in multiphoton FLIM methods are reviewed and a novel multiphoton FLIM system using a streak camera is described. An example of a typical application of the system is provided in which the fluorescence resonance energy transfer between a donor-acceptor pair of fluorescent proteins within a cellular specimen is measured.

We describe the implementation of a commercial fluorescence lifetime imaging microscopy (FLIM) instrument used in conjunction with a commercial laser scanning multiphoton microscope. The femtosecond-pulsed near-infrared laser is an ideal excitation source for time-domain fluorescence lifetime measurements. With synchronization from the x-y scanners, fluorescence lifetimes can be acquired on a pixel-by-pixel basis, with high spatial resolution. Multiexponential curve fits for each pixel result in two-dimensional fluorescence resonance energy transfer (FRET) measurements that allow the determination of both proximity of fluorescent FRET pairs, as well as the fraction of FRET pairs close enough for FRET to occur. Experiments are described that characterize this system, as well as commonly used reagents valuable for FRET determinations in biological systems. Constructs of CFP and YFP were generated to demonstrate FRET between this pair of green fluorescent protein (GFP) color variants. The lifetime characteristics of the FRET pair fluorescein and rhodamine, commonly used for immunohistochemistry, were also examined. Finally, these fluorophores were used to demonstrate spatially resolved FRET with senile plaques obtained from transgenic mouse brain. Together these results demonstrate that FLIM allows sensitive measurements of protein–protein interactions on a spatial scale less than 10 nm using commercially available components.

Observations of cells or tissues with fluorescence microscopy can provide unique insights into cellular physiology and structure. Such information may reveal the pathological state of a tissue to the physician or information on cytoskeletal dynamics to the research scientist. However, problems of overlapping spectra, low signal, and light scatter impose serious limitations on what can be achieved in practice with fluorescence microscopy. These problems can be addressed in part by the development of new imaging modalities that make maximum use of the information present in the fluorescence signal. We describe the application of a new technology to the study of standard histological pathology specimens: a multiphoton excitation fluorescence microscope that incorporates a novel, photon-counting detector that measures the excited-state lifetimes of fluorescent probes. In initial investigations, we have applied this system to the observation of C. elegans embryos and primate histology specimens, with the objective of identifying potentially diagnostic signatures. Our findings demonstrate that lifetime multiphoton microscopy has considerable potential as a diagnostic tool for pathological investigations.

Fluorescence lifetime images are obtained with the laser scanning microscope using two methods: the time-correlated single-photon counting method and the frequency-domain method. In the same microscope system, we implement both methods. We perform a comparison of the performance of the two approaches in terms of signal-to-noise ratio (SNR) and the speed of data acquisition. While in our practical implementation the time-correlated single-photon counting technique provides a better SNR for low-intensity images, the frequency-domain method is faster and provides less distortion for bright samples.

Single-molecule spectroscopy and single-molecule detection are emerging areas that have many applications when combined with scanning, imaging, and spectroscopy techniques. We have combined a commercial confocal scanning head, to a Ti:sapphire laser and to an inverted microscope, for the detection of single molecule fluorescence of varies dyes by two-photon excitation. We collected spot images of fluorescent molecules that have been deposited on a substrate considering both blinking and photobleaching behavior of fluorescent spots. Here, we report data related to two-photon interactions that occur with the following fluorescent molecules: Indo-1, Rhodamine 6G, Fluorescein, and Pyrene. The choice of these specific dyes is based upon their wide use in biological and medical applications together with the varying complexity of their chemical structure that increases from Pyrene to Indo-1. Moreover, we report some data about single molecule studies related to denaturation of an enhanced green fluorescent protein, GFPmut2, under one photon excitation regime, that show a very similar trend to that observed for the already mentioned fluorescent molecules.

Sulfur mustard (SM; 2,2-dichloroethyl sulfide) is a percutaneous alkylating agent first used as a chemical weapon at Ypres, Belgium, in World War I. Despite its well-documented history, the primary lesions effecting dermal–epidermal separation and latent onset of incapacitating blisters remain poorly understood. By immunofluorescent imaging of human epidermal keratinocytes (HEK) and epidermal tissues exposed to SM (400 μM for 5 min), we have amassed unequivocal evidence that SM disrupts adhesion complex molecules, which are also disrupted by epidermolysis bullosa-type blistering diseases of the skin. Images of keratin 14 (K14) in control cells showed tentlike filament networks linking the HEK's basolateral anchoring sites to the dorsal surface of its nuclei. Images from 6-h postexposure profiles revealed early disruption (≤ 1 h) and progressive collapse of the K14 cytoskeleton. Collapse involved focal erosions, loss of functional asymmetry, and displacement of nuclei beneath a mat of jumbled filaments. In complementary studies, 1-h images showed statistically significant (p<0.01) decreases of 25 to 30% in emissions from labeled α₆β₄ integrin and laminin 5, plus disruption of their receptor–ligand organization. Results indicate that SM alkylation destabilizes dermal–epidermal attachments and potentiates vesication by disrupting adhesion complex molecules and associated signaling mechanisms required for their maintenance and repair.

Two-photon excitation photodynamic therapy (TPE-PDT) is being investigated as a clinical treatment for age-related macular degeneration (AMD). TPE-PDT has the potential to provide a more specific and therefore advantageous therapy regime than traditional one-photon excitation PDT. The highly vascularized 8 to 9-day-old chicken chorioallantoic membrane (CAM) is used to model the rapid growth of blood vessels in the wet form of AMD. Using an ex ovo model system for the CAM, ablation studies were successful in mimicking the leaky vessels found in AMD. In addition, the distribution and localization of liposomal Verteporfin were investigated in order to characterize the photosensitizing drug in vivo. Localization of the photosensitizer appears to be greatest on the upper vessel wall, which indicates a potentially strong treatment locale for TPE-PDT.

Two-photon excitation makes it possible to excite molecules in volumes of much less than 1 fl. In two-photon flash photolysis (TPFP) this property is used to release effector molecules from caged precursors with high three-dimensional resolution. We describe and examine the benefits of using TPFP in model solutions and in a number of cell systems to study their spatial and temporal properties. Using TPFP of caged fluorescein, we determined the free diffusion coefficient of fluorescein (D = 4×0^–6 cm²/s at 20°C, which is in close agreement with published values). TPFP of caged fluorescein in lens tissue in situ revealed spatial nonuniformities in intercellular fiber cell coupling by gap junctions. At the lens periphery, intercellular transport was predominantly directed along rows of cells, but was nearly isotropic further from the periphery. To test an algorithm aiming to reconstruct the Ca²⁺ release flux underlying physiological Ca²⁺ signals in heart muscle cells, TPFP of DM-Nitrophen was utilized to generate artificial microscopic Ca2+ signals with known underlying Ca²⁺ release flux. In an experiment with mouse oocytes, the recently developed Ca²⁺ cage dimethoxynitrophenyl-ethyleneglycol-bis-(β-aminoethylether)-N,N,N,N tetraacetic acid-4 (DMNPE-4) was released in the oocyte cytosol and inside a nucleolus. Analysis of the resulting fluorescence changes suggested that the effective diffusion coefficient within the nucleolus was half of that in the cytosol. These experiments demonstrate the utility of TPFP as a novel tool for the optical study of biomedical systems.

We characterize the transmembrane voltage response of a novel second-harmonic generation (SHG) marker using a screening protocol with giant unilamellar vesicles. Two mechanisms are found to contribute to the voltage response: (1) an electro-optic-induced alteration of the molecular hyperpolarizability and (2) an electric-field-induced alteration of the degree of molecular alignment. We quantify the relative weights and of these contributions and provide an upper limit to their response time, which is found to be submillisecond. The identification of two voltage response mechanisms leads to new strategies for the molecular design of membrane potential markers.

High-resolution four-dimensional (4-D) optical tomography of human skin based on multiphoton autofluorescence imaging and second harmonic generation (SHG) was performed with the compact femtosecond laser imaging system DermaInspect as well as a modified multiphoton microscope. Femtosecond laser pulses of 80 MHz in the spectral range of 750 to 850 nm, fast galvoscan mirrors, and a time-correlated single-photon counting module have been used to image human skin in vitro and in vivo with subcellular spatial and 250-ps temporal resolution. The nonlinear induced autofluorescence originates from naturally endogenous fluorophores and protein structures such as reduced nicotinamide adenine dinucleotide phosphate, flavins, collagen, elastin, porphyrins, and melanin. Second harmonic generation was used to detect collagen structures. Tissues of patients with dermatological disorders such as psoriasis, fungal infections, nevi, and melanomas have been investigated. Individual intratissue cells and skin structures could be clearly visualized. Intracellular components and connective tissue structures could be further characterized by fluorescence excitation spectra, by determination of the fluorescence decay per pixel, and by fluorescence lifetime imaging. The novel noninvasive multiphoton autofluorescence-SHG imaging technique provides 4-D (x,y,z,τ) optical biopsies with subcellular resolution and offers the possibility of introducing a high-resolution optical diagnostic method in dermatology.

Image resolution and signal level in fluorescence microscopy through inhomogeneous turbid media consisting of scatterers of multiple sizes under single- (1p), two- (2p), and three-photon (3p) excitation have been investigated based on a modified Monte Carlo model. The effects of the size distribution and the concentration distribution of scattering particles are explored. Simulation results reveal that the size and the concentration distribution both have an impact on image formation in media consisting of small particles and that 3p excitation has the most significant impact. In media with scatterers of a large size, both size and concentration distributions lead to a slight effect. Image formation in a mixed medium containing small and large scattering particles is more affected by the large particles.

In recent years, fluorescence microscopy based on two-photon excitation has become a popular tool for biological and biomedical imaging. Among its advantages is the enhanced depth penetration permitted by fluorescence excitation with the near-infrared photons, which is particularly attractive for deep-tissue imaging. To fully utilize two-photon fluorescence microscopy as a three-dimensional research technique in biology and medicine, it is important to characterize the two-photon imaging parameters in a turbid medium. We investigated the two-photon point spread functions (PSFs) in a number of scattering samples. Gel samples containing 0.1-μm fluorescent microspheres and Liposyn III were used as phantoms mimicking the turbid environment often found in tissue. A full characterization of the two-photon PSFs of a water and oil immersion objective was completed in samples composed of 0, 0.25, 0.5, 1, and 2% Liposyn III. Our results show that up to depths of about 100 (oil) and 200 µm (water), the presence of scatterers (up to 2% Liposyn III) does not appreciably degrade the PSF widths of the objectives.

We describe novel approaches for compensating dispersion effects that arise when acousto-optic (AO) beam deflection of ultrafast laser pluses is used for multiphoton laser-scanning microscopy (MPLSM). AO deflection supports quick positioning of a laser beam to random locations, allowing high frame-rate imaging of user-selected sites of interest, in addition to conventional raster scanning. Compared to standard line-scan approaches, this results in improved signal strength (and thus increased signal-to-noise) as well as reduced photobleaching and photodamage. However, 2-D AO scanning has not yet been applied for multiphoton microscopy, largely because ultrafast laser pulses experience significant spatial and temporal dispersion while propagating through AO materials. We describe and quantify spatial dispersion, demonstrating it to be a significant barrier to achieving maximal spatial resolution. We also address temporal dispersion, which is a well-documented effect that limits multiphoton excitation efficacy, and is particularly severe for AO devices. To address both problems, we have developed a single diffraction grating scheme that reduces spatial dispersion more than three-fold throughout the field of view, and a novel four-pass stacked-prism prechirper that fully compensates for temporal dispersion while reducing by two-fold the required physical length relative to commonly employed designs. These developments enable the construction of a 2-D acousto-optic multiphoton laser-scanning microscope system.

Indocyanine green (ICG) is widely used in medical imaging and testing. Its complex spectral behavior and low quantum yield limits some applications. We show that proximity of ICG to a metallic silver particle increases its intensity approximately 20-fold and decreases the decay time. Since the rate of photobleaching is not increased, our results suggest that ICG-silver particle complexes can yield at least 20-fold more photons per ICG molecule for improved medical imaging.

Diagnostic algorithms can classify tissue samples as diseased or nondiseased based on fluorescence emission collected from the intact cervix. Such algorithms can distinguish high-grade squamous intraepithelial lesions from low-grade squamous intraepithelial lesions. An understanding of the effects of the values of biographical covariates, such as age, race, smoking, or menopausal status on the emission spectra for each patient could improve diagnostic efficiency. The analysis described was performed using data collected from two previously published clinical trials; one study measured spectra from 395 sites in 95 patients referred to a colposcopy clinic with abnormal Pap smears, and the second study measured spectra from 204 sites in 54 patients self-referred for screening and expected to have a normal Pap smear. For this analysis, data about age, race, menstrual cycle, and smoking were collected. The principal components from normalized data were compared. There are clear intensity differences observed with age and menopausal status; postmenopausal patients exhibit higher emission intensities. Differences associated with biographical variables need to be tested in larger studies, which stratify adequately for these variables. The addition of these biographical variables in the preprocessing of data could dramatically improve algorithm performance and applicability.

The finite-difference time-domain (FDTD) method provides a flexible approach to studying the scattering that arises from arbitrarily inhomogeneous structures. We implemented a three-dimensional FDTD program code to model light scattering from biological cells. The perfectly matched layer (PML) boundary condition has been used to terminate the FDTD computational grid. We investigated differences in angle-dependent scattering properties of normal and dysplastic cervical cells. Specifically, the scattering patterns and phase functions have been computed for normal and dysplastic cervical cells at three different epithelial depths, namely, basal/parabasal, intermediate, and superficial. Construction of cervical cells within the FDTD computational grid is based on morphological and chromatin texture features obtained from quantitative histopathology. The results show that angle-dependent scattering characteristics are different not only for normal and dysplastic cells but also for cells at different epithelial depths. The calculated scattering cross-sections are significantly greater for dysplastic cells. The scattering cross-sections of cells at different depths indicate that scattering decreases in going from the superficial layer to the intermediate layer, but then increases in the basal/parabasal layer. This trend for epithelial cell scattering has also been observed in confocal images of ex vivo cervical tissue.

A fast spectroscopic system for superficial and local determination of the absorption and scattering properties of tissue (480 to 950 nm) is described. The probe can be used in the working channel of an endoscope. The scattering properties include the reduced scattering coefficient and a parameter of the phase function called γ, which depends on its first two moments. The inverse problem algorithm is based on the fit of absolute reflectance measurements to cubic B-spline functions derived from the interpolation of a set of Monte Carlo simulations. The algorithm's robustness was tested with simulations altered with various amounts of noise. The method was also assessed on tissue phantoms of known optical properties. Finally, clinical measurements performed endoscopically in vivo in the stomach of human subjects are presented. The absorption and scattering properties were found to be significantly different in the antrum and in the fundus and are correlated with histopathologic observations. The method and the instrument show promise for noninvasive tissue diagnostics of various epithelia.

Measurements of the spatial distributions of polarized light backscattered from a two-layer scattering medium are used to train a neural network. We investigated whether the absorption coefficients and thickness of the layer can be determined when the scattering properties are known. When determining the absorption of the upper layer or the layer's thickness, polarized light measurements provide better performance than unpolarized measurements, demonstrating the sensitivity of polarized light to superficial tissue. Determination of the lower layer's absorption coefficient is not improved by polarized light measurements. Prior knowledge of the tissue under investigation is also beneficial because errors are reduced if the range of absorption or thickness is restricted.

Limitations in the accuracy of measurements of optical properties (absorption and scattering coefficients) of strongly scattering media that are due to temporal dispersion inside the detection fibers of a time-of-flight setup were investigated for a tissue-like phantom. It is shown that the absorption and reduced scattering coefficients may be overestimated by up to 90% (depending on length and numerical aperture of the fibers) if the instrumental response measurements for the setup are performed by direct illumination of the tip of the detection fibers with collimated short laser pulses. However, the accuracy can be improved significantly if a thin layer of scattering media is used in front of the detection fibers during the response measurements. The relevance of the investigated dispersion effects is discussed with respect to frequency-domain measurements as well.

We present an image-processing method that enhances the detection of regions of higher absorbance in optical mammograms. At the heart of this method lies a second-derivative operator that is commonly employed in edge-detection algorithms. The resulting images possess a high contrast, an automatic display scale, and a greater sensitivity to smaller departures from the local background absorbance. Moreover, the images are free of artifacts near the breast edge. This second-derivative method enhances the display of structural information in optical mammograms and may be used to robustly select areas of interest to be further analyzed spectrally to determine the oxygenation level of breast lesions.

Pulse oximeters are widely used for noninvasive monitoring of oxygen saturation in arterial blood hemoglobin. We present a transmittance pulse oximetry system based on near-infrared (NIR) laser diodes (750 and 850 nm) for monitoring oxygen saturation of arterial blood hemoglobin. The pulse oximetry system is made up of the optical sensor, sensor electronics, and processing block. Also, we show experimental results obtained during the development of the whole NIR transmittance pulse oximetry system along with modifications in the sensor configuration, signal processing algorithm, and calibration procedure. Issues concerning wavelength selection and its implications for the improvement of the transmittance pulse oximetry technique are discussed. The results obtained demonstrate the proposed system's usefulness in monitoring a wide range of oxygen saturation levels.

We observed a difference in the thermal response of localized reflectance signal of human skin between type 2 diabetics and nondiabetics. We investigated the use of this thermo-optical behavior as the basis for a noninvasive method for the determination of the diabetic status of a subject. We used a two-site temperature differential method, which is predicated upon the measurement of localized reflectance from two areas on the surface of the skin. Each of these areas is subjected to a different thermal perturbation. The response of localized reflectance to temperature perturbation was measured and used in a classification algorithm. We used a discriminant function to classify subjects as diabetic or nondiabetic. In a prediction set of twenty-four noninvasive tests collected from six diabetic and six nondiabetic subjects, the sensitivity ranged between 73 and 100%, and the specificity ranged between 75 and 100%, depending on the thermal conditions and the probe–skin contact time. The difference in the thermo-optical response of the skin of the two groups is explained in terms of a difference in the response of cutaneous microcirculation, which is manifested as a difference in the near-infrared light absorption. Another factor is the difference in the temperature response of the scattering coefficient between the two groups, which may be caused by cutaneous structural differences induced by nonenzymatic glycation of skin protein fibers, and possibly by the difference in blood cell aggregation.

A new nonablative laser device, Smoothbeam, has been under evaluation for nonablative wrinkle reduction in skin with minimal side effects. This device incorporates a laser at 1450-nm wavelength to heat the dermis and cryogen spray cooling to prevent epidermal damage. The thermal injury created is internal and imperceptible. The wound-healing response to this internal injury causes improvement in the appearance of skin wrinkles. Biopsies taken immediately after treatment showed mild residual thermal damage (RTD) at a depth range of 150 to 400 μm, which is the dermal zone where most solar elastosis resides. Biopsies from two months after treatment showed fibroplasia extending over a range of depths similar to the acute RTD zones. An improvement in wrinkle severity was noted on the treated side compared with the control side.

A long-period grating (LPG) was written into a progressive three-layered single-mode fiber that was embedded into a flexible platform as a curvature sensor. The spectral location and profile of the LPGs were unaltered after implantation in the platform. The curvature sensitivity was 3.747 nm m with a resolution of ∓1.1×10^–2 m^–1. The bend sensor is intended to be part of a respiratory monitoring system and was tested on a resuscitation training manikin.

A two-dimensional map of blood flow is crucial for physiological studies. We present a modified laser speckle imaging method (LSI) that is based on the temporal statistics of a time-integrated speckle. A model experiment was performed for the validation of this technique. The spatial and temporal resolutions of this method were studied in theory and compared with current laser speckle contrast analysis (LASCA); the comparison indicates that the spatial resolution of the modified LSI is five times higher than that of current LASCA. Cerebral blood flow under different temperatures was investigated by our modified LSI. Compared with the results obtained by LASCA, the blood flow map obtained by the modified LSI possessed higher spatial resolution and provided additional information about changes in blood perfusion in small blood vessels. These results suggest that this is a suitable method for imaging the full field of blood flow without scanning and provides much higher spatial resolution than that of current LASCA and other laser Doppler perfusion imaging methods.

We are investigating the possibility of a frequency compounding method for speckle reduction in optical coherence tomography. The method is based on incoherent summation of the magnitudes of two independent interferometric signals, which were recorded at two different center wavelengths simultaneously. We derive the corresponding statistics and compare the theoretical results with measurements obtained in a uniformly scattering sample. Finally we demonstrate our method by comparing images of human skin recorded in vivo with and without frequency compounding. The compounding method results in an increased contrast and improved image quality without loss of resolution.

Optical coherence tomography (OCT) acquires cross-sectional images of tissue by measuring back-reflected light. Images from in vivo OCT systems typically have a resolution of 10 to 15 mm, and are thus best suited for visualizing structures in the range of tens to hundreds of microns, such as tissue layers or glands. Many normal and abnormal tissues lack visible structures in this size range, so it may appear that OCT is unsuitable for identification of these tissues. However, examination of structure-poor OCT images reveals that they frequently display a characteristic texture that is due to speckle. We evaluated the application of statistical and spectral texture analysis techniques for differentiating tissue types based on the structural and speckle content in OCT images. Excellent correct classification rates were obtained when images had slight visual differences (mouse skin and fat, correct classification rates of 98.5 and 97.3%, respectively), and reasonable rates were obtained with nearly identical-appearing images (normal versus abnormal mouse lung, correct classification rates of 64.0 and 88.6%, respectively). This study shows that texture analysis of OCT images may be capable of differentiating tissue types without reliance on visible structures.