Polarization-sensitive optical coherence tomography (PS-OCT) combines the high-resolution imaging capabilities of OCT with polarization contrast.1,2 Polarization of light thereby may provide additional image contrast based on inherent polarization properties related to the textural organization of tissues, such that structures can be distinguished for example based on their birefringent characteristics. PS-OCT has found widespread applications in many biomedical fields including imaging of dental, neural, osseous, and intravascular structures.1,2 The most prominent field of application of PS-OCT, however, has been ophthalmology.3 In the human eye, PS-OCT can be used to distinguish: (a) fibrous tissues exhibiting birefringence including the retinal nerve fiber layer, sclera, cornea, and tendons of extraocular muscles;188.8.131.52.184.108.40.206.–13 (b) pigmented structures exhibiting polarization scrambling including the retinal pigment epithelium, the choroid, and the pigment epithelium of the iris;5,14 and (c) polarization preserving tissues including the iridal stroma, conjunctive tissue, and most of the neurosensory retina such as the photoreceptor layer.5,15 PS-OCT has proven particularly useful for imaging and quantitative assessment of retinal pathology in age-related macular degeneration, glaucoma, central serous retinopathy, and diabetic retinopathy.8,16220.127.116.11.–21
In images of the anterior eye segment, PS-OCT provides additional contrast for collagenous, birefringent tissues such as the cornea, sclera, and tendons, as well as for the trabecular meshwork.9,12,15 The diagnostic potential of birefringence imaging by PS-OCT has been exploited in keratoconus patients.9,22 As alterations in corneal microstructure can lead to changes of the birefringent characteristics, PS-OCT was also proposed for imaging such changes during corneal crosslinking therapy.12,23 Following trabeculectomy—a surgical procedure for intraocular pressure (IOP) relieve in glaucoma patients—the evolution of filtering blebs was monitored by PS-OCT.12,2425.26.–27 Finally, PS-OCT was also used to investigate birefringence characteristics of the sclera.13
For advancing our knowledge and understanding of eye development, its physiology in health and disease, and for the development of new therapeutics, rodent models have been playing an essential role.28,29 The gold standard for such preclinical investigations has been histology. Histology enables the assessment of structural details with microscopic resolution and molecular specificity. However, it also requires enucleation of the eye, and therefore, does not permit longitudinal studies in the same animal. OCT—among other modalities—has been proposed as a noninvasive alternative to histology providing in vivo imaging capabilities with micrometer scale resolution and in real time. OCT has been applied for imaging the anterior murine eye in models of several ophthalmic diseases including a model of Axenfeld–Rieger malformations of the anterior segment related to PITX2 mutation,30 a DBA/2J model of glaucoma,31 a mouse model of glaucoma overexpressing bone morphogenetic protein 2,32 mouse models of elevated IOP,33,34 mice deficient in secreted protein acidic and rich in cysteine,35 and phenotypical investigations of genetic components of corneal and stromal thickness relevant for keratoconus.36
Even though standard (i.e., non-PS) OCT has obviously proven useful for imaging the anterior segment in preclinical studies, PS-OCT studies of the murine eye have thus far been limited to the posterior eye segment.3738.39.–40 In this paper, we aim to investigate the polarization properties of the healthy murine eye and demonstrate the potential of PS-OCT as a tool for imaging structural changes in the anterior mouse eye with enhanced contrast.
Materials and Methods
Pigmented C57BL/6 mice were purchased from the breeding facility at the Medical University of Vienna. The mice were fed a standard diet and were kept under controlled lighting conditions (12-h light, 12-h dark). For the OCT imaging experiments, mice (, age: 20 to 21 months) were anesthetized using ketamine (Ketasol, aniMedica GmbH, Germany; body weight; intraperitoneal) and xylazine (Rompun, Bayer Austria GmbH, Austria; body weight; intraperitoneal). One mouse (age 20 months) which presented an irregular cornea was imaged as a pathologic example, and one mouse (age 21 months) was used for a longitudinal investigation of the anterior eye during mydriasis. Anesthesia was required for immobilizing the animals during PS-OCT imaging. For imaging the murine lens in some animals, the pupils were dilated using phenylephrine (2.5%; topical) and tropicamide (Mydriaticum, Agepha Pharmaceuticals, Austria; topical). Under anesthesia, mice were placed in an adjustable mount in order to align the eye position with respect to the measurement beam and kept warm using heat pads. Artificial tear drops (Oculotect; Thea Pharma GmbH, Austria) were repeatedly applied to keep the cornea moist. All experiments were performed in accordance with the ARVO Statement for the Use of Animals in Ophthalmic and Vision Research and under a protocol approved by the ethics committee at Medical University of Vienna and the Austrian Federal Ministry of Science, Research and Economy (protocol number GZ 66.009/0131-V/3b/2018).
Polarization-Sensitive Optical Coherence Tomography
A sketch of the spectral domain PS-OCT system used for imaging the murine anterior segment is shown in Fig. 1. Detailed specifications of the system can be found elsewhere,41 hence only a brief description is provided here. A polarization-maintaining (PM) fiber-based Michelson interferometer was illuminated by a superluminescent diode with a central wavelength of 837 nm and a full-width-at-half-maximum bandwidth of 52 nm. The incident light was linearly polarized, launched into the slow axis channel of the PM fiber system, and split into sample and reference arms. A quarter wave plate (QWP, at 45 deg) then provided circularly polarized light for sample illumination. After passing a pair of galvanometer scanners, a 4:5 telescope relayed the pivot point of the fast scanning mirror into the back focal plane of the objective lens (Olympus E A10). The setup provided a transverse resolution of in the focal plane and an axial resolution of in air. The reference arm featured another QWP (at 22.5 deg) and glass blocks for dispersion balancing. The interfered light from sample and reference arm was split into two orthogonal components by a polarizing beam splitter. Each polarization component was then detected by a spectrometer unit comprising a collimator (), a transmission grating (), an achromatic doublet (), and a high-speed line scan camera (Basler sprint) operating at 70 kHz line rate using 2048 pixels per spectrum corresponding to a frame rate of B-scans per second. A real-time display providing B-scan images at 28 frames per second and a continuously updating OCT -projection image enabled speedy alignment of the mouse eye with respect to the beam. Data sets containing per polarization channel covering up to (, optical distance) were acquired in .
PS-OCT Image Processing
PS-OCT images were computed from the spectral data by first performing standard spectral domain OCT processing including background removal, resampling to -space, numerical dispersion compensation, zero-padding, and Fourier transformation.42 Compared to results from earlier imaging sessions in the rodent retina37 and in the human brain,43 OCT images of the murine anterior segment include structures with greatly varying reflectivity—from the corneal epithelium with signals close to the noise floor to the densely pigmented iris pigment epithelium with signals above the average noise level. Since the strong backscattering signals were accompanied by weaker ghost signals caused by distant side lobes of the point spread function, an additional spectral shaping step was implemented.44 For this purpose, all spectra of each B-scan acquisition were divided by their average spectrum, which had already served as the background spectrum for background removal. Then each 2048-pixel wide spectrum was multiplied by a Gaussian function with a width of 2200 pixels and by a normalization factor, namely the energy of the background spectrum divided by the energy of the Gaussian shaping function.
After Fourier transforming the preprocessed spectra, the complex data from the two polarization channels were axially aligned in order to compensate for the path length difference caused by the difference in linear polarization mode dispersion of the two orthogonally polarized PM fiber modes.41 Finally, PS-OCT images displaying sample reflectivity, phase retardation, and birefringent axis orientation were computed from the amplitude and phase data.6 Further, images of the degree of polarization uniformity (DOPU)45,46 were calculated as described in the next section. PS-OCT images were displayed as cross-sectional B-scans and volume renderings using gray and color scales.47 In order to gate out regions with low reflectivity, which did not provide meaningful polarization data, pixels whose reflectivity did not exceed the mean noise level by 6 dB (4 dB for the depolarization analysis in Sec. 2.4) were displayed in light gray in the PS-OCT images. B-scan images with increased SNR were computed by averaging the complex OCT data of several frames repeated at the same -scan position.48
Depolarization Imaging Using a Simplified Noise Correction for DOPU
Depolarization of light is caused by several ocular tissues, in particular by those containing melanin pigments.49 In order to analyze depolarization in PS-OCT images, the DOPU has emerged as an appropriate and handy approach. DOPU essentially corresponds to a normalized measure of the length of an ensemble of spatially and/or temporally averaged Stokes vectors50 The most pronounced depolarization effects can be observed for circularly polarized light, which is used for sample illumination here. A variety of different algorithms have been developed to perform DOPU analysis including two- and three-dimensional (3-D) kernels as well as temporal Stokes vector averaging.41,45,51,52
One limitation of DOPU is its inaccuracy in case of pixels with low signal-to-noise ratio (SNR). Makita et al.46 recently proposed an approach to DOPU, which eliminates the noise bias for the first two Stokes vector elements before averaging, viz. and , where the primed elements are the noise-error-corrected Stokes parameters and is the noise power measured in the ’th polarization channel. The noise correction improves DOPU measurements in particular for weak signals close to the noise floor ( in reflectivity images).46
Now, as in many PS-OCT designs, the optical and electronical layout of the two polarization detection channels is identical, we may assume that . As a consequence, such that only is left to be corrected for the additive noise error. By plugging the expression for into Eq. (1) and using the relation for the SNR of the PS-OCT reflectivity signal, the expression for the noise-corrected quantity DOPU′ simplifies to read
Since usually in pixels containing meaningful PS-OCT data exceeding the noise floor, DOPU′ will in general be greater than DOPU. In other words, the DOPU observed without noise correction will be lower than the noise-corrected DOPU′, unless the SNR is high. In Fig. 2, we show a comparison of Stokes vector images and DOPU [kernel size: ] for the original DOPU approach [Fig. 2(a)],45,53 Makita’s modification [Fig. 2(b)],46 and for the simplified approach presented in this paper [Fig. 2(c)]. For the Stokes vector images, the linear magnitudes of Stokes vector elements , , and were fed into the R, G, and B channel of an RGB image and the logarithmically scaled was used for the alpha channel. In the DOPU images, pixels with low reflectivity were displayed in gray as described in the previous section. Aside from the more pronounced noise floor intensity in Fig. 2(a), the Stokes vector images look virtually identical for the three approaches, while obvious differences can be observed in the corresponding DOPU images. The polarization preserving or depolarizing characteristics strongly differ for pixels with low SNR (e.g., in deeper regions of the lens) but exhibit a rather similar appearance for pixels with high SNR (e.g., in the lens capsule). Depolarization in the melanin-laden iris leads to a pronounced local variation of the Stokes vectors which is visible as color changes between neighboring speckles in the magnified view of Fig. 2(c) shown in Fig. 2(d). In contrast, the RGB representation of the Stokes vectors in the lens [Fig. 2(e)] appears more uniformly red and orange, indicating a dominant component of backscattered light. The second Stokes vector element represents the linearly polarized light component, which would be expected to be detected for light scattered from rather polarization preserving tissue after double pass of the QWP in the sample arm. Consequently, the observed DOPU values are low for Fig. 2(d) and high for Fig. 2(e), respectively. Histograms of the four Stokes vector elements computed for the image region of Figs. 2(a)–2(c) including the lens are shown in Fig. 2(f). Here the distribution of is skewed toward higher values for the original DOPU approach as compared to the noise-corrected approaches which, in turn, appear similar. For the magnitudes of Stokes vector elements , , and , the distributions overlap tightly and no differences can be observed. For the DOPU images presented in the results section below, the modified DOPU approach using a rectangular kernel spanning was used.
For histological correlation, two mice were sacrificed by overdosing with sodium pentobarbital. Mouse eyes were enucleated postmortem after in vivo OCT imaging and fixed in 4% paraformaldehyde at 4°C overnight. Then the eyes were rinsed in phosphate-buffered saline, dehydrated with a series of ascending ethanol concentrations, and embedded in paraffin. Sections of thickness were created using a rotary microtome and subsequently stained with hematoxylin and eosin (H&E). Sections were digitized using the NanoZoomer slide scanner (C9600-12, Hamamatsu).
PS-OCT of the Anterior Eye Segment in C57BL/6 Mice
PS-OCT imaging was performed in the anterior eye segments of C57BL/6 mice. PS-OCT tomograms of a frontal scan and of the chamber angle of a 20-month-old mouse are shown in Fig. 3. Similar to OCT scans of the human eye, the cornea is rather transparent at 840 nm and hyposcattering in the reflectivity image [Fig. 3(a)], whereas a strong signal can be observed in the iris. Also the lens provides an intense backscatter signal, which can be attributed to the cataract observed in the aged mouse eye as earlier investigations have shown that normal C57BL/6 mice may develop cataract at older age.54 Note that the focal plane was placed approximately at the iris and that due to light attenuation by the iridal melanin, no OCT signals can be observed from structures located posterior to the iris. In the PS-OCT retardation B-scan [Fig. 3(b)], most structures appear uniformly blue with low retardation, only the darkly pigmented iris and fur scramble the polarization and exhibit strongly varying retardation values. A similar picture is seen in the DOPU image in Fig. 3(c). Here most tissues have DOPU values close to unity, except for the iris and the fur whose DOPU values are much lower owing to their pigmentation.
PS-OCT images of the iridocorneal angle are shown in Figs. 3(d)–3(f). These images also provide access to the ciliary body which, similar to the iris, appears hyperscattering in the reflectivity image [Fig. 3(d)] and depolarizing in the retardation and DOPU images, respectively [Figs. 3(e) and 3(f)]. As the focal plane of the objective was placed closer to the cornea for this acquisition, the depolarizing behavior of the corneal stroma can be observed in Figs. 3(e) and 3(f) as well (see asterisks).
In order to compare the PS-OCT data to the gold standard, we show an H&E stained histological section of a 20-month-old C57BL/6 mouse in Fig. 3(g). The melanin pigments within tissue structures in the uvea—namely iris, ciliary body, and choroid—appear intrinsically dark brown. The magnified view on the panel’s right side shows that the pigments are distributed all across the murine iris—unlike the human iris, which only comprises melanin in a thin epithelial layer while its stroma is pigment-free.
A more detailed view of the polarization characteristic of the murine cornea is provided in Fig. 4. For these images, the cornea overlapped with the system’s focal plane and four images were averaged to enhance the SNR and improve the visualization of the corneal stroma. Similar to the human cornea,55 the reflectivity is weaker in the corneal epithelium than in the stroma [Fig. 4(a)]. Also in PS-OCT retardation and DOPU images, the mouse eye recapitulates the polarization characteristics of its human counterpart,56 while the anterior and posterior layers preserve the polarization state of backscattered light, the corneal stroma exhibits a depolarizing behavior [Figs. 4(c) and 4(d)]. Averaged axial profiles of reflectivity, retardation, and DOPU averaged over 120 A-lines are plotted in Fig. 4(f) in order to visualize the depolarizing character of the stroma via the increased spread of retardation values and the decreased DOPU values. Histological sections of the mouse cornea are shown for comparison in Figs. 4(b) and 4(e).
The depolarization characteristics of the central corneal stroma, iris, and the anterior part of the lens were evaluated in six C57BL/6 mouse eyes. In DOPU B-scan images, the average DOPU value was assessed in a manually selected region of interest spanning () for each tissue. Box plots of the results are shown in Fig. 4(g) for cornea, iris, and lens. The strongest depolarization was observed in the iris (, ), followed by the corneal stroma () and the lens (). Using Mann–Whitney U-tests with Bonferroni correction, the differences between DOPU measurements were found to be statistically significant when comparing cornea versus iris (), lens versus iris (), and between corneal stroma and lens ().
PS-OCT of Mydriasis
In order to investigate the effect of mydriasis on the mouse eye, longitudinal imaging was performed before and after applying dilating eye drops (phenylephrine, 2.5%) on the cornea of an anaesthetized mouse. No artificial tear drops were used in this experiment. Seventeen 3-D PS-OCT data sets were acquired between 24 and 57 min after inducing anesthesia. Volume renderings of the reflectivity data sets are shown in Figs. 5(a) and 5(d) for the undilated eye and 33 min after application of the mydriatic agent. Corresponding reflectivity and DOPU B-scans are shown in Figs. 5(b), 5(e) and 5(c), 5(f), respectively. Aside from the pupil dilation, spontaneous cataract formation can be observed as an increase of backscattering from the lens. Note that most of the lens appears polarization preserving while only a small fraction at the right-hand side of panel (f) exhibits decreased DOPU. The pupil area was assessed automatically from a depth projection image of the volumetric DOPU data and is plotted longitudinally in Fig. 5(g). An almost linear increase by 150% can be observed over a time span of 10 min following phenylephrine application; then a plateau leveling off at is reached. In order to test the hypothesis whether depolarization in the iris increases as the iris is compacted during mydriasis, the iris was segmented and histograms of DOPU within the iris were computed for every 3-D PS-OCT data set. The results are plotted as a function of time in Fig. 5(h). Although a slight modulation of the shape of the histograms can be observed over time, its maximum essentially stays constant at .
PS-OCT of Corneal Pathology
PS-OCT imaging was performed in the eye of a C57BL/6 mouse, which had spontaneously developed corneal pathology, possibly scarring following a scratch. Figures 6(a)–6(c) show volume renderings of 3-D PS-OCT images. The cornea—a smooth, thin, and almost transparent structure in healthy mouse eyes—presents with a rough surface, substantial thickening, and pronounced backscattering in the reflectivity image [Fig. 6(a)]. With , the central corneal thickness of this mouse eye was substantially greater than those of healthy littermates (, average of eyes). Aside from several streak-like regions of increased retardation and low DOPU, the retardation and DOPU images in Figs. 6(b) and 6(c) depict rather uniform polarization states in the cornea. With an average DOPU value of 0.94 in this cornea, depolarization was less pronounced than in the stroma of normal corneas where an average DOPU of was measured. Similar to healthy eyes, strong depolarization can be observed in the iris as well as in the pigmented hairs and eye lashes. Compared to the volume renderings, which provide a plastic overview but integrate the PS-OCT signal along the direction of observation, a fairly different picture of the cornea is seen in the PS-OCT B-scans presented in Figs. 6(d)–6(m). Unlike in normal eyes, strong birefringence can be observed in the stroma of the swollen cornea, visible as a gradual increase of phase retardation with depth [Figs. 6(f) and 6(g)].
Corneal PS-OCT projection images of the same data set computed by averaging the signals in beam direction for a shallow tissue slab are shown in Fig. 7. The mean intensity projection image averaged over the image range in Fig. 7(a) reveals a highly scattering region in the center of the cornea. Abnormal corneal swelling and hyperscattering behavior is visualized in a side-by-side comparison with a reflectivity B-scan of a normal mouse cornea in Fig. 7(d). A phase retardation map of a deep slab located posterior to the surface of the corneal epithelium is shown in Fig. 7(b). Several regions exhibiting increased retardation as well as three highly birefringent streaks can be observed. The birefringent axis orientation map of the same slab reveals partially organized birefringent fiber orientations [Fig. 7(c)]. The retardation and axis orientation B-scans show a polarization preserving characteristic in the anterior cornea, whereas weak birefringence and defined axis orientations can be observed in the portion posterior to the epithelium [Figs. 7(e) and 7(f)]. Also a highly birefringent structure can be observed, which casts a shadow trail of increased retardation [in green and marked by the arrow in Fig. 7(e)].
The benefit of polarization contrast in OCT has been demonstrated in the literature for various diseases of the human eye.3 In disease models of human retinal pathology, PS-OCT has also proven a valuable contrast enhancement and an additional route toward the quantitative assessment of tissue parameters and lesion properties.39,40,57 Although PS-OCT has been successfully demonstrated for imaging the human anterior eye in health and disease by multiple experiments and studies, this is—to the best of our knowledge—the first presentation of PS-OCT in the anterior segment of murine eyes.
In analogy to the application of PS-OCT in human retinas and mouse models of retinal diseases, polarization provides access to additional contrast for preclinical imaging of the anterior eye. The mouse eye shares many similarities with the human eye. However, the ocular proportions differ between the two species: most apparently, the murine eye features a much larger lens compared to the overall eye size. Still, the different anatomical structures and tissue properties widely resemble those in humans. Also the polarization characteristics observed in the mouse eye (Figs. 3 and 4) and in human eyes12,56,58 are largely similar: the cornea features polarization preserving epithelial and endothelial layers, whereas light backscattered from the stroma exhibits strong local differences in the detected polarization states (Fig. 4). A different polarization pattern was observed in the pathologic cornea shown in Figs. 6 and 7. Other than the healthy case in Figs. 3 and 4, the swollen tissue enabled the visualization of the birefringent characteristics of the stroma, which may indicate altered tissue microstructure caused by an infection or scarring.
The murine lens mostly maintained the polarization state in our PS-OCT data. When severe cataracts formed under anesthesia, the lens visually became opaque and exhibited gradually increased backscattering. Also some small areas with reduced DOPU were observed in the lens, which otherwise did not markedly differ in terms of reflectivity (see Fig. 5). As anesthesia induced cataracts are reversible, no histological examination to explore the cause of the depolarizing signals was performed for the mouse eye imaged here. Nonetheless, PS-OCT may be an interesting modality to image cataractous lenses in mouse models of age-related and/or congenital lens pathology with additional contrast.
Melanin pigmentation in anterior eye tissues depolarizes backscattered light and thus can be detected by PS-OCT. Polarization scrambling was observed in the ciliary body and the iris, which may be considered the extensions of the pigmented uvea from the posterior eye’s choroid. However, unlike the human iris, whose backside is covered by a single-cell layer of epithelial pigment cells, we observed depolarization in PS-OCT images and accordingly melanin granules in histologic sections all across the murine iris. As PS-OCT can be used to quantify melanin density via depolarization,49,59 we also assessed DOPU in the iris during drug-induced pupil dilation. In our longitudinal PS-OCT imaging experiment, however, we could not observe any marked changes of iridal depolarization. While iris contraction may not suffice to distinctly alter pigment density within the tissue, PS-OCT powered depolarization imaging may be a potent tool for noninvasively assessing pigmented uveal tumors in a transgenic mouse model.60 Also in the popular DBA/2J mouse model, PS-OCT could be useful to image iris atrophy and pigment dispersion.61
Quantitative DOPU measurements in cornea, lens, and iris revealed statistically significant differences between the three tissues [see Fig. 4(g)], which may be exploited for automated segmentation of these structures. Compared to the DOPU values measured in normal mouse corneas, corneal depolarization was less pronounced in the pathologic cornea shown in Fig. 6. This cornea was also substantially thicker than normal corneas. Although the central corneal thicknesses of measured with our PS-OCT system in normal C57BL/6 mice were much thinner than those published in a histological report (),62 only slightly greater thicknesses () have been observed using OCT at 1310 nm.63 The quite substantial difference between corneal thickness measured using OCT and histology, respectively, may be attributed to morphological changes caused by tissue processing. This is also supported by a comparative study published by Hanlon et al. who compared corneal thickness measurements by OCT and conventional histology and found 30% to 35% greater thickness for standard histological workup.64
There are some technological limitations to the PS-OCT approach presented in this paper. A spectral domain PS-OCT prototype operating in the 840-nm regime was used for imaging. With standard OCT resolution of in tissue (), the system was able to resolve all major structures in the anterior mouse eye. In order to resolve more subtle cellular features and to decrease speckle size for improved depolarization imaging, higher axial resolution would be required.65,66 Using a light source with broader bandwidth, OCT reflectivity imaging of the anterior segment with ultrahigh axial resolution has been presented in the literature and recently enabled the visualization of single corneal nerves and the limbal palisades of Vogt.55,67 Ultrahigh resolution PS-OCT imaging has been demonstrated in the human cornea68 and may facilitate the identification of small structures such as corneal lamellae or ciliary processes in the mouse eye.
Another limitation is the rather shallow image depth that can be utilized for covering anterior eye structures. Despite the prototype’s ranging depth of 2.7 mm in tissue, which in general would be more than sufficient to image the murine anterior segment, the shallow depth of field and the strong sensitivity roll-off limit the useful image depth to . Moreover, the cornea has distinct directional scattering properties, which reduce the signal for nonorthogonal beam-cornea geometries. The latter drawback could be overcome by implementing a nontelecentric scanning approach.56 In order to increase the utilizable image depth, PS-OCT based on swept source OCT can provide a shallower sensitivity roll-off and deeper light penetration through cataract can be achieved by using a longer-wavelength light source.69 Also the depth of field could be increased by using Bessel beams.70 Swept source PS-OCT may then enable imaging of the entire anterior chamber and lens, and even whole eye imaging in rodents.71,72 Another strategy to achieve high lateral resolution over a long depth range would be the fusion of several 3-D data sets acquired at different focus positions, which could be enabled by rapidly tunable optics as recently proposed by Grulkowski et al.73 Finally, in addition to PS-OCT imaging of mouse models, it would be particularly interesting to investigate ocular structures in rats, which have larger eyes and may allow studies of further experimental models for diseases such as glaucoma.29
In conclusion, we have demonstrated the use of PS-OCT for imaging the murine anterior segment. Our results revealed anterior eye tissues with polarization properties similar to their human counterparts. Given the wide variety of mouse models of anterior eye pathology such as keratoconus or cataract, PS-OCT might be an interesting candidate for noninvasive, real-time 3-D imaging in longitudinal studies and experimental eye research.
The authors thank Stanislava Fialová, Erich Götzinger, Harald Sattmann, Siegfried Gollubits, Roberto Plasenzotti, and Jasmin Rezek at the Medical University of Vienna for excellent technical support. Financial support by the Austrian Science Fund (FWF Grant Nos. P19624-B02 and P25823-B24), the European Union (FP7 HEALTH Program Grant No. 201880, FUN-OCT), and the European Research Council (ERC Starting Grant No. 640396, OPTIMALZ) is gratefully acknowledged. This work was presented in part at ARVO Imaging in the Eye Conference 2017 and SPIE Photonics West 2018.74
Bernhard Baumann studied physics at the University of Vienna and received his PhD in medical physics from the Medical University of Vienna in 2009. He is an associate professor at the Center for Medical Physics and Biomedical Engineering of the Medical University of Vienna. His research interests are the development of innovative optical methods for biomedical imaging—in particular optical coherence tomography (OCT)—and their application for improved diagnostics of diseases in both clinical and preclinical research.
Marco Augustin received his master’s degree in medical informatics from Vienna University of Technology in 2014 and his PhD in medical physics from the Medical University of Vienna in 2018, respectively. Currently, he is enrolled as a postdoctoral associate at the Center for Medical Physics and Biomedical Engineering of the Medical University of Vienna. His interests include optical imaging techniques, especially optical coherence tomography, and its functional extensions, as well as image processing and pattern recognition particularly in life sciences.
Antonia Lichtenegger received her master’s degree in technical mathematics and biomedical engineering from the Technical University of Vienna in 2014 and 2015, respectively. Currently, she is a PhD candidate at the Center for Medical Physics and Biomedical Engineering of the Medical University of Vienna. Her interests include designing and setting up optical coherence microscopy systems and image processing in biomedical optics and neuroscience.
Danielle J. Harper received her master’s degree in physics at the University of St. Andrews in the United Kingdom in 2015. As a PhD student at the Medical University of Vienna, she is currently working to design an innovative OCT system, which is tailored for the in vivo functional imaging of the retina of animal models. Her main interests lie in optical imaging, particularly in the optical designs that make techniques such as OCT possible.
Martina Muck received her BSc degree in biomedical science and her master’s degree in tissue engineering and regenerative medicine from the University of Applied Sciences, FH Campus Wien and Technikum in Vienna. As a biomedical analyst, she is working on the preparation of brain samples for OCM imaging and histology.
Pablo Eugui received his master’s degree in biomedical engineering from the Universidad Publica de Navarra, Spain, in 2015. Currently, he is enrolled as a PhD student of the Medical University of Vienna and is working on fiber-based optical coherence tomography systems. His interests are optical imaging with different techniques, signal and image processing applied to the medical field, and the study of different neurological diseases.
Andreas Wartak received his PhD in medical physics from the Medical University of Vienna, Austria, in 2018. He is currently enrolled as a postdoctoral researcher at Wellman Center for Photomedicine, Harvard Medical School and Massachusetts General Hospital, Boston, Massachusetts, USA. His research focuses on OCT, in particular on the improvement and development of multichannel techniques for application in ophthalmology with emphasis on retinal imaging.
Michael Pircher received his PhD in technical sciences from Vienna University of Technology and completed his habilitation degree in medical physics at the Medical University of Vienna. He is an associate professor at the Center for Medical Physics and Biomedical Engineering of the Medical University of Vienna and an associate editor of Biomedical Optics Express.
Christoph K. Hitzenberger is a professor of medical physics and a vice-chair of the Center for Medical Physics and Biomedical Engineering at the Medical University of Vienna, and editor-in-chief of Biomedical Optics Express. He works in biomedical optics since 1987 and is one of the pioneers of low-coherence ocular biometry and OCT. He is a fellow of SPIE and OSA. His pioneering contributions to OCT were awarded with the Russ Prize of the National Academy of Engineering in 2017.