Structure and Principle of Angioscope



Fig. 1.1
Principle of the optical fiber. Circumference material should be a water-containing fluid, so that refractive-index matching is assumed. Refraction on the tip of fiber is omitted. Incident angle θ does not correspond to incident angle on the boundary between core and clad. Actual incident angle for this boundary should be (2/π)-θ. The reflectivity of the core and clad are n 1 and n 2, respectively. This figure is based on geometric optics. Surface-wave propagation in the clad can be explained by wave optics





1.1.3 Pixel Separation Method for Image Transmission


Optical images that contain information of color and figure can be transmitted through rigid optics, such as an objective lens and telescope, in general. Despite the optical fiber of which refractive-index distribution forms a quadratic function being equivalent to a series of convex lenses, this fiber is not able to deliver images precisely because of mode transformation, i.e., turbulent wave front by the bending of the optical fiber as well as imprecision of refractive-index distribution on radial direction of the optical fiber. Therefore, a picture element (pixel) separation method should be used to transmit images by the optical fiber. Each pixel in the picture can be delivered through an individual optical fiber. Figure 1.2 shows example of an image set at various pixel sizes. Obviously, fine pixel resolution is better for diagnostic use, but it is restricted by other factors, in particular the diameter of the optical fiber (image guide). The required amount of pixels is dependent on an observation area and desired resolution for an observation. Three or six thousand pixels have been used in the coronary angioscopic imaging.

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Fig. 1.2
Effect of pixel size on image quality. Number of pixels are 2.2 k, 5 k, 20 k, and 18 M, respectively, left to right



1.2 Optical Image Guides



1.2.1 Silica-Based Optical Waveguide


The production technology of silica-based image guide had been established by Japanese engineer Atsushi Utsumi who had been working with Mitsubishi Cable, Co. Ltd [2]. A cross-sectional schematic structure of his waveguide is illustrated in Fig. 1.3, comparing it to conventional optical fiber bundle used in a fiber endoscope. The optical fiber bundle is basically a human-work assembling fiber, which contains several thousands of independent pixel fibers. Because the optical fiber bundle was expensive and its pixel size is limited to 20,000–40,000 pixels, a CCD endoscope had been replaced. In contrast, the silica-based image guide is a unified fiber, which contains several thousands of independent core in a common clad region. Since this silica-based image guide can be fabricated by a wiredrawing process corresponding to fit large-lot production, it should be very thin and inexpensive. Despite pixel size being limited to approximately 10 k, this silica-based image guide has been used in an angioscope due to its thinness and inexpensiveness. Technical challenges in the fabrication of this image guide are core diameter stability/distribution and optimization to suppress optical leakage between each core. When the core diameter distribution is scattered, some core has a specific color due to the mode difference in small amount of the transmission mode (see 1.1.2). Moreover, because the clad region is common for all cores, the optical leakage exists as close-set pixel to pixel. This leakage reduces image quality to be a bleary image. A few Japanese optical fiber fabricators only can produce a high-quality silica-based image guide so far.

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Fig. 1.3
The schematic structures of the silica-based image guide and optical fiber bundle


1.2.2 Specifications of Optical Image Guides


The specification of the silica-based image guides for the coronary angioscope is summarized in Table 1.1 with one particular new image guide made of a plastic material. The information of this table is based on specification catalogs from each fabricator [35]. The author also tries to predict and indicate undisclosed information in Table 1.1. Three thousand or six thousand pixels are employed in general. The minimum bending radius should be less than 15 mm for the coronary angioscope. The outer diameter of the image guide should be less than around 0.4 mm because of both stiffness and size. The glass fibers need a coating layer to avoid a scratch of the fiber outside to keep their bending capability because of the brittle fracture characteristics of glass materials. The angioscope image taken in the 1990s was dark and not sharp because of low pixel density (equal to low pixel size in the image) using a low-NA image guide in the early years [6, 7]. The standard pixel size in an angioscope image in the 1990s was 3000, but a 6000 pixel image is generally used in recent years. The recent advance of high-NA silica-based image guide can make bright and sharp angioscopic image by increasing pixel density as well as suppressing cross leakage. Another advantage of the high-NA image guide is a wide view angle of the image. Since edge distortion is observed in the wide view angle image, in general, an observer feels spatial effect even from a two-dimensional image. One particular waveguide made of plastic material in Table 1.1 has the obvious capability to be applied in the coronary angioscope but has not been applied yet. The cost of plastic fiber might be less than tenth part of the silica-based image guide. Moreover, plastic material has lower stiffness than silica glass. These characteristics are helpful to make ideal coronary angioscope.


Table 1.1
Image guide specifications applicable to the angioscope














Image fiber

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May 26, 2017 | Posted by in CARDIOLOGY | Comments Off on Structure and Principle of Angioscope

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