Endoscope apparatus

Surgery – Endoscope – Having imaging and illumination means

Reexamination Certificate

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C600S160000, C600S101000

Reexamination Certificate

active

06632172

ABSTRACT:

FIELD OF THE INVENTION
This invention relates to an endoscope apparatus with an insertion part having a small outer diameter which includes an object optical system to conduct measurements or stereoscopic-vision observations.
BACKGROUND OF THE INVENTION
Conventionally, an endoscope which includes a long and thin insertion part which is inserted into a cavity or the intra-corporeal of a human being for observation, etc., has been widely used in both the industrial field and the medical field. Furthermore in recent years, there have been a great need to measure the size and the depth of flaws and cracks in the industrial field, and to perform surgery using an endoscope in the medical field. Moreover in the medical field, using stereo images to recognize depth information is well known.
A conventional endoscope in which stereo observation are possible is described in Japanese Laid-open Patent Publication No. 8-29701. As shown in
FIG. 6
, two objective-lens systems are arranged in parallel and at the end of an endoscope insertion part. The endoscope conducts parallax stereoscopic vision by receiving an image from two image-pick-up devices (henceforth, CCD) and shifting the image due to the positional differences of the two CCDs.
In the optical system with two CCDs, since the number of pixels can be increased as compared to one CCD, it is effective in improving the image quality of stereo images and the precision of measurements. However, by arranging two CCDs in parallel, it then becomes difficult to reduce the size of an endoscope which makes it difficult to observe a narrow site or perform minimum invasive surgery.
A conventional endoscope having an optical system in which an image with a parallax is formed on one CCD is described in Japanese Laid-open Patent Publication No. 7-35989. As shown in
FIG. 7
, this optical system has one CCD on the extension line of the respective optical axis of the two object optical systems arranged in parallel to form two images. The distance between the two optical axes is hereinafter referred to as “the optic-axial distance”.
On the one hand, in recent years the trend has been toward smaller-sized CCDs. However, if the optimum optic-axial distance is determined such that a part of the object optical system nearest to the object has a moderate parallax, and an image is formed on the CCD with that optic-axial distance, as shown in
FIG. 8
, the center of an image will be positioned at the end of the CCD, if the CCD is small. That is, the area of the images at the right and left sides of the CCD, marked with diagonal lines in
FIG. 8
, decreases and causes interference with the stereoscopic vision and measurements.
Conversely, if the size of the CCD to be used and the optimum distance between the centers of the images on the CCD is also determined in accordance with the size of an endoscope, as shown in
FIG. 9
, there is a possibility that a parallax required for a measurement or for stereoscopic vision cannot be obtained if the optic-axial distance for the object optical system on the object side (nearest the object) is equal to the distance between the centers of the images on the CCD.
Therefore, in order to obtain a moderate parallax required for a measurement or a stereoscopic vision as well as an acceptable image on the CCD, the optic-axial distance of an object optical system, and the distance between the centers of the images on CCD need to be varied.
However, the optic-axial distance of an object optical system influences a parallax which is important at the time of a stereoscopic-vision observation and the precision at the time of measurement. If the optic-axial distance of the object optical system nearest to the object is narrow, a parallax will decrease so that depth information becomes hard to obtain when carrying out a stereoscopic vision and a measurement error becomes large when carrying out a measurement operation.
Conversely, if the optic-axial distance of the object optical system nearest to the object is wide, a parallax will become large. Although the precision of a measurement improves, the problem will arise that the end of an endoscope becomes large. And since a parallax is too large when carrying out a stereoscopic-vision observation, it is hard to observe on the contrary.
A parallax depends not only on the optic-axial distance of the object optical system nearest to the object but also on the distance to the object to be observed. In other words, the closer the object is, the larger the parallax becomes, and the farther it is, the smaller the parallax becomes.
Based on the above, in order to obtain a moderate parallax required for measurement and for a stereoscopic-vision observation depending on the observation distance, and in order not to make the size of an endoscope large, the optic-axial distance of the object optical system at a part thereof nearest to the object should be determined.
A conventional example in which the optic-axial distance of an object optical system is different from the distance between the centers of the images on the CCD is described in the Japanese Laid-open Patent Publication No. 62-215221.
In this example, as shown in
FIG. 10
, by sandwiching a parallel flat refractive element with a pair of optical systems, the optic-axial distance of an object optical system is narrowed towards the center of the image on the CCD. In such an optical system, if the CCD is small, the parallel flat dioptric element must be small. However, it is difficult to design and manufacture a small parallel flat dioptric element, and still more difficult to sandwich it with a pair of optical systems.
SUMMARY OF THE INVENTION
It is an object of the present invention to provide an object optical system with a moderate parallax and a moderate image size, without making the insertion part of the endoscope thick in diameter.
In an endoscope apparatus, according to the present invention, equipped with an object optical system to conduct a measurement or a stereoscopic-vision observation, as shown in
FIG. 1
, the object optical system comprises a pair of negative lenses; a first pair of positive-lenses; a brightness diaphragm; a second pair of positive-lenses; and an image-pick-up device for forming an object image. These elements are arranged in order from an object side. A pair of optical axes are defined by the pair of negative lenses, the first pair of positive-lenses and the brightness diaphragm. The second pair of positive-lenses are arranged eccentrically with respect to the pair of optical axes in a direction towards each other.
Each lens of the second pair of positive-lenses can be defined as a single-lens, plural single-lenses, or cemented lens or combination thereof.
The eccentric lenses may be provided on only one side of the second pair of positive-lenses, or on a part of the second pair of positive-lenses. It is noted that the centers, of the positive-lenses of the second pair, is the center of the circle if the lens shape is a circle, and it is the center of gravity of a polygon if the lens shape is a polygon.
The endoscope apparatus according to this invention, wherein the following conditional expression is satisfied:
0.2
≦x/d
≦0.9  (1)
wherein x represents an optic-axial distance of said pair of optical axes on the image-pick-up device side, and d represents the optic-axial distance of said pair of optical axes of the object side, the brightness diaphragm, respectively.
The positive-lenses of the second pair are arranged eccentrically with respect to a pair of optical axes in a direction in which the lenses come closer to each other symmetrically and by the same amount. According to this invention, the second pair of positive-lenses on the image-pick-up device side from a brightness diaphragm is arranged to be inwardly eccentric, with respect to each optical axis on the object side from a brightness diaphragm, towards the horizontal direction of the CCD surface.
The amount of the eccentricity of the second pair of positive-lenses does not necessarily need to be symmetrical. In a stereosco

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