Recent developments in optical coherence tomography for imaging the retina

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Abstract

Optical coherence tomography (OCT) was introduced in ophthalmology a decade ago. Within a few years in vivo imaging of the healthy retina and optic nerve head and of retinal diseases was a fact. In particular the ease with which these images can be acquired considerably changed the diagnostic strategy used by ophthalmologists. The OCT technique currently available in clinical practice is referred to as time-domain OCT, because the depth information of the retina is acquired as a sequence of samples, over time. This can be done either in longitudinal cross-sections perpendicular to, or in the coronal plane parallel to the retinal surface. Only recently, major advances have been made as to image resolution with the introduction of ultrahigh resolution OCT and in imaging speed, signal-to-noise ratio and sensitivity with the introduction of spectral-domain OCT. Functional OCT is the next frontier in OCT imaging. For example, polarization-sensitive OCT uses the birefringent characteristics of the retinal nerve fibre layer to better assess its thickness. Blood flow information from retinal vessels as well as the oxygenation state of retinal tissue can be extracted from the OCT signal. Very promising are the developments in contrast-enhanced molecular optical imaging, for example with the use of scattering tuneable nanoparticles targeted at specific tissue or cell structures. This review will provide an overview of these most recent developments in the field of OCT imaging focussing on applications for the retina.

Introduction

In 1991, optical coherence tomography (OCT) was reported for the first time (Huang et al., 1991). Owing to the clear optical system of the eye itself, OCT soon found its way to ophthalmology. Within a few years in vivo imaging of the healthy retina and optic nerve head and of retinal diseases and in particular the ease with which these images can be acquired considerably changed the diagnostic strategy used by ophthalmologists (Hee et al., 1995a, Hee et al., 1995b, Hee et al., 1995c, Hee et al., 1995d, Hee et al., 1996). Today, OCT is widely used for imaging the vitreoretinal interface, for monitoring (cystoid) macular oedema (CMO) and retinal thickness in a wide variety of patients and for monitoring retinal nerve fibre layer (RNFL) thickness and optic nerve head parameters in glaucoma patients.

OCT provides cross-sectional images of the macula or optic nerve head, analogous to ultrasonography. Instead of sound OCT uses light waves to obtain a reflectivity profile of the tissue under investigation (Huang et al., 1991). The use of light inherently leads to a one-to-two order magnitude improvement in axial resolution. In the eye it allows for visualization of structures and lesions at all levels of the retina (Hee et al., 1995a), obtained in a non-contact mode.

The OCT technique currently available in clinical practice is also referred to as time-domain OCT (TD-OCT), because the depth information of the retina is acquired as a sequence of samples, over time. Several efforts have been made to improve TD-OCT imaging quality. Some have tried to optimize the image quality post-acquisition (Adler et al., 2004; Sander et al., 2005), others by using different light sources to increase real-time image resolution (Drexler et al., 2001). Modifying image acquisition was also attempted using single flying spot raster scanning in the coronal plane parallel to the retinal surface (Podoleanu et al., 1997, Podoleanu et al., 1998a; Hitzenberger et al., 2003), or using full field capturing of a sample (Dubois et al., 2004a). Only recently, major advances in both imaging speed and sensitivity have been achieved with the introduction of spectral-domain (SD) OCT (Nassif et al., 2004; Wojtkowski et al., 2004). This review will provide an overview of the most recent developments in the field of OCT imaging of the eye, focussing on applications for the posterior segment of the eye.

Section snippets

Image formation

OCT is the optical analogue of ultrasound imaging. Using light instead of ultrasound is advantageous since shorter wavelengths permit imaging at higher resolution. Moreover, no contact medium is required, as the difference in optical impedance, the refractive index between air and tissue, is not as large as the difference in acoustic impedance between air and tissue. Unfortunately, the speed of light exceeds that of sound by a factor 150.000, which means that, in contrast to ultrasonic echoes

Combined OCT and scanning laser ophthalmoscopy (OCT/SLO)

Podoleanu et al., 1997, Podoleanu et al., 1998a pioneered the development of a different approach to OCT imaging. This method involves en-face scanning in the XY plane, and combines high-resolution tomographic images with the surface imaging capability of the scanning laser ophthalmoscope (SLO). Similar to the standard-resolution, conventional OCT, this system is build around a Michelson interferometer, and uses a SLD with a central wavelength of 820 nm and a spectral bandwidth of 20 nm. To allow

Basic principles

In TD-OCT the location of the coherence gate (l) is varied as a function of time by moving the reference mirror, i.e. the OCT signal is collected in the l-domain. In spectral-domain (SD−)OCT the reference mirror is stationary, and the OCT signal is acquired as function of wave number k, either by using a spectrometer as detector or by varying the (narrowband) wavelength of the light source in time (i.e. the OCT signal is collected in the k-domain). The wave number k is related to wavelength

Adaptive optics in OCT

One can wonder about the value of an OCT scan with a 1 μm axial resolution if the transversal resolution remains 15–20 μm. While major strides have been made in improving axial resolution and image acquisition speed, less has been achieved in transverse image resolution. As mentioned earlier, transversal resolution depends on the NA of the system optics including the eye itself and the spot size on the retina. A smaller spot size on the retina can be achieved by expanding the beam and the pupil

Polarization-sensitive OCT

Although this review has so far focused mainly on OCT developments in macular imaging, another important use is the follow-up of glaucoma patients. Ganglion cells and nerve fibres are lost before any change is detected in the visual field (Quigley and Addicks, 1982; Sommer et al., 1991). OCT is capable of measuring the thickness of the RNFL, and can discriminate between healthy subjects and glaucomatous patients (Soliman et al., 2002; Carpineto et al., 2003; Medeiros et al., 2004; Budenz et

Molecular imaging with OCT

One of the big advantages of OCT over conventional imaging techniques like FA and ICG angiography is the fact that it is capable of non-invasive imaging of retinal anatomy and morphology. However, because functional changes precede morphological ones, diagnostic modalities which combine conventional imaging with quantitative visualization of the involved molecular processes is of paramount importance. Molecular imaging (MI) combines molecular contrast agents with traditional imaging techniques.

Future directions

In the past decade, through the use of longitudinal TD-OCT, ophthalmologists have gained new insights in the pathophysiology of a multitude of ocular diseases. In particular, OCT visualizes the detailed morphological changes and progress of these ocular diseases with or without therapy (Schuman et al., 2004). In this regard, the OCT/SLO may become an interesting addition or alternative to the conventional TD-OCT system available. T-scan based coronal scanning provides an overview of any area of

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