Surgery – Endoscope – Having imaging and illumination means
Reexamination Certificate
2001-12-19
2003-12-09
Leubecker, John P. (Department: 3739)
Surgery
Endoscope
Having imaging and illumination means
C600S176000, C359S833000
Reexamination Certificate
active
06659942
ABSTRACT:
FIELD OF THE INVENTION
The invention relates to an endoscope comprising a relay system defining an endoscope axis, and a deflection system for deflecting a beam entering the endoscope at an angle of up to 30 degrees with respect to said endoscope axis, while the deflection system contains deflection elements provided with reflecting surfaces.
Endoscopes have at their distal end a lens which forms an image of the scene under observation. This image is relayed optically or electronically to the proximal end, where it is accessible to observation. Endoscope lenses must be designed in such a way that they can be accommodated within a narrow tube.
It is often desirable for the field of view not to be arranged symmetrically, with respect to the axis of the endoscope, but rather for the direction of view to form a fairly small or even significant angle with the axis of the endoscope. In this case it is necessary for deflecting elements to be provided which divert light from the field of view that is to be pictured in the direction of the endoscope axis. Which deflecting elements are appropriate is determined chiefly by the desired visual angle of the endoscope, that is, by the angle of deflection.
In known endoscopes, at small angles of deflection up to about 15 degrees, use is made of refracting elements like wedge plates, a non-centered frontal lens, a non-centered eyepiece unit, or combinations of the same, as deflecting elements. At larger angles of deflection, starting at about 25 degrees, use is made, on the other hand, of reflecting elements such as prisms with reflected surfaces.
Wedge plates or the decentering of imaging optical elements have the disadvantage of worsening the image quality through a distortion of the field of view that increases with the angle of deflection. If the eyepiece unit is non-centered, then in addition the size of the image field must be reduced, in order to avoid vignetting. Refracting elements, moreover, cause color errors in principle, which must be corrected at considerable expense.
Reflecting optical elements do not have these deficiencies. A deflection system, in which two reflecting surfaces are provided, is described in DE 35 37 155 A1. Here the lens has a lens system which forms the lens field in the image plane, which is arranged vertically to the axis of the endoscope. Between the plano-concave front lenses and the other lenses of the lens system, a deflection unit is installed, consisting of two prisms cemented together, in which unit the light entering from the lens field is reflected onto an external surface of one of the prisms, which surface is parallel to the endoscope axis, and the light is reflected on the interface between the prisms.
BACKGROUND OF THE INVENTION
In a similarly built system known from U.S. Pat. No. 4,684,224, a plano-parallel plate is installed on the entering surface of the deflection unit, onto which surface a plano-concave lens is cemented. This deflection unit provides two reflecting surfaces, both of which are at an angle to the axis of the endoscope.
From WO 99/10762, an endoscope lens is known in which the deflection unit consists of just one prism with two reflecting surfaces, and onto which the plano-concave frontal lens is cemented directly. A plane-parallel plate or a second prism is not necessary here, because a totally reflecting layer is applied on the side turned toward the frontal lens.
An endoscope lens known from DE 24 58 306 C3 consists of two prisms, where the deflected beam entering the endoscope axis are reflected not more than twice on two interfaces of one of the prisms. The U.S. Pat. No. 4,730,909 discloses a deflection system for angles of deflection of more than 90 degrees where the entering reflected more than twice.
The said endoscope lenses comprising the reflective deflection elements both show that they are not suitable for deflection angles of less than about 30 degrees, or can only be used at the price of accepting restrictions in the available image field diameter, a distortion of the field of view, or any other reduction in the image quality.
It is the purpose of the present invention to provide a deflection system for an endoscope which does not have the above-mentioned disadvantages of the refracting elements, and which is also suitable for deflection angles of less than 30 degrees, as well as to provide an endoscope comprising a deflection system of this type. A deflection system for deflection angles of 5 to 25 degrees, especially in the range of about 15 degrees, is preferable.
In accordance with the present invention, this objective is fulfilled by the features defined in claim 1. Since the deflection system comprises deflection elements containing reflecting surfaces, while said reflecting surfaces are arranged in such a way that the beam deflected into the optical axis is reflected more than twice, it is possible to obtain deflection angles between 0 and 30 degrees within a restricted space of the deflection system. This is made possible without any of the disadvantages associated with refractive deflecting elements. Here the optical axis is the axis of the endoscope, especially the optical axis of the optical elements connected in series to the deflection system; for example, optical elements of the lens.
According to a preferred embodiment of the present invention, at least one reflecting surface is used in transmission as well as in reflection. This takes advantage of the fact that transmissions occur at small angles of incidence, whereas large angles of incidence cause a reflection. This feature allows an especially compact design, since the reflecting surface may extend over the entire cross-section without reducing the surface available for transmission.
According to another preferred embodiment of the present invention, the said reflecting surface is used only once for transmission, whereas one or more reflections may occur on this surface. This makes it possible to obtain deflection angles within the desired range with relatively fewer optical elements as well as with a relatively few reflections.
According to another preferred embodiment of the present invention, the reflected on said reflecting surface against a thin layer, whereas said layer may also consist of a coating of several thin layers. Depending on the angle of incidence, a transparent coating permits both transmission and reflection. Although the reflection may also be obtained against another glass material or even air, the advantage of the reflection on a thin layer is that said reflection is only determined by the materials which the carrier is made of and within which the reflection occurs, as well as by the layer itself. An air gap or another means may be provided on the side of the layer opposite to the carrier without considerably affecting the reflection.
According to another preferred embodiment of the present invention, the beam deflected into the optical axis is totally reflected on at least one reflecting surface. The advantage of this is a virtually loss-free reflection.
If the refractive index of a totally reflecting layer is n(layer), and the index of the carrier is n(glass), the following equation applies for the limiting angle_(limit) of the total reflection against the layer:
sin_(limit)=
n
(layer)/
n
(glass)
This means that it is necessary that
n
(layer)<
n
(glass)
in order for a total reflection even to be possible. Moreover, the following equation applies for the thickness d of the layer:
d>
1.2
—
(layer)
where_is the wave length of the light in use so as to obtain a loss-free total reflection.
A layer of this type can be designed as a single-layer or multi-layer system and can be applied by means of known coating processes as disclosed in WO 99/10762. For multi-layer systems, the above-mentioned condition must prevail for at least one of the layers applied.
The refractive indices and the angles of the optically effective surfaces to one another must be selected so that all the other beams from the field of view under observation will be subjected as much as
Karl Storz GmbH & Co. KG
Leubecker John P.
St. Onge Steward Johnston & Reens LLC
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