JPH06130325A - Surface division projecting element - Google Patents

Surface division projecting element

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Publication number
JPH06130325A
JPH06130325A JP30590192A JP30590192A JPH06130325A JP H06130325 A JPH06130325 A JP H06130325A JP 30590192 A JP30590192 A JP 30590192A JP 30590192 A JP30590192 A JP 30590192A JP H06130325 A JPH06130325 A JP H06130325A
Authority
JP
Japan
Prior art keywords
light
image
tab
plane
convex lenses
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP30590192A
Other languages
Japanese (ja)
Other versions
JP3258097B2 (en
Inventor
Noriji Ooishi
則司 大石
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Rayon Co Ltd
Original Assignee
Mitsubishi Rayon Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Rayon Co Ltd filed Critical Mitsubishi Rayon Co Ltd
Priority to JP30590192A priority Critical patent/JP3258097B2/en
Publication of JPH06130325A publication Critical patent/JPH06130325A/en
Application granted granted Critical
Publication of JP3258097B2 publication Critical patent/JP3258097B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To obtain the surface division projecting element which is a projecting element formed by combining a tab prism assembly and a convex lens array together and has a reducing and enlarging function. CONSTITUTION:Two convex lenses 1 and 2 which are different in focal distance are arranged on the light incidence/projection surface of an array of plural tab prism assemblies each formed by joining two section symmetrical trapezoidal tab prisms 3 with their light reflecting surfaces out so that the ratio of the array interval D of convex lenses 1 arranged on the light incidence side and the array interval (d) of convex lenses 2 arranged on the light projection side is equal to the ratio of the focal distance F of the convex lenses 1 arrayed on the light incidence side and the focal distance (f) of the convex lenses 2 arrayed on the light projection side.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はスリット露光方式のアナ
ログ複写機に使われる拡大、縮小機能をもつ面分割投影
素子に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a plane-division projection element having an enlargement / reduction function used in a slit exposure type analog copying machine.

【0002】[0002]

【従来の技術】スリット露光方式のアナログ複写機に
は、読取りライン上の複写体を感光体上に投影する投影
素子が使われており、とくに小型の複写機には屈折率分
布型棒状レンズの配列体であるロッドレンズアレイに代
表される面分割型投影素子が便利に使われている。この
ような面分割素子は、コンパクトな光学系であり、その
組立や焦点距離の調整が行いやすいという長所がある反
面、等倍率の結像しか得られないため、拡大、縮小コピ
ーの必要な面分割投影素子とはならないという難点があ
る。
2. Description of the Related Art A slit exposure type analog copying machine uses a projection element for projecting a copying body on a reading line onto a photosensitive body. Especially, in a small copying machine, a gradient index rod lens is used. A plane-division type projection element represented by a rod lens array which is an array is conveniently used. Such a surface-splitting element is a compact optical system and has the advantage that it is easy to assemble and adjust the focal length, but on the other hand, it can only form an image of equal magnification, so it is necessary to enlarge or reduce the copy. There is a drawback that it does not serve as a split projection element.

【0003】[0003]

【発明が解決しようとする課題】上述したごとく、ロッ
ドレンズアレイ等の面分割投影素子では、拡大、縮小機
能を付与することが極めて難しく、拡大、縮小機能を備
えた面分割投影素子の開発が待たれている。
As described above, it is extremely difficult to give the enlargement / reduction function to the plane-division projection element such as the rod lens array, and the development of the plane-division projection element having the enlargement / reduction function has been developed. I'm waiting.

【0004】[0004]

【課題を解決するための手段】そこで本発明者は、画像
の拡大、縮小機能を備えた面分割素子を開発することを
目的として検討した結果、本発明を完成したものであ
り、その要旨とするところは、断面対称台形のタブプリ
ズム2つを、その光反射面が外側となるように、対称型
に組立たタブプリズム組立体複数個を、その光反射面が
対面するように直線状に配列し、直線状に配列したタブ
プリズム組立体の光入・出射端面に焦点距離の異なる2
種の凸レンズを、光入射端側に配設する凸レンズの配列
間隔Dと、光出射端側に配設する凸レンズの配列間隔d
との比を、光入射端側に配設する凸レンズの焦点距離
と、光出射端側に配設する凸レンズの焦点距離の比に等
しくなるように配設したことを特徴とする面分割投影素
子にある。
Therefore, the present inventor has completed the present invention as a result of an examination for the purpose of developing a surface division element having an image enlarging / reducing function. In order to do so, two tab prisms having symmetrical trapezoidal cross sections are symmetrically assembled so that their light reflecting surfaces are on the outside, and a plurality of tab prism assemblies are linearly arranged so that their light reflecting surfaces face each other. Arrayed and linearly arranged tab prism assemblies with different focal lengths on the light input and output end faces 2
An array interval D of the convex lenses disposed on the light incident end side and an array interval d of the convex lenses disposed on the light emission end side of the kind of convex lens.
And a convex lens disposed on the light incident end side and a focal length of the convex lens disposed on the light emitting end side are equal to each other. It is in.

【0005】本発明で用いる断面対称台形のタブプリズ
ム3の断面を図5に示した。このタブプリズムの軸との
角αをもって入射した光はタブプリズムの斜辺で、その
光反射面側へ屈折され、光反射面で反射した光は、タブ
プリズムの光出射面側の斜辺より、その軸とのなす角度
αで出射する。
FIG. 5 shows a cross section of a tab prism 3 having a symmetrical trapezoidal cross section used in the present invention. The light incident at an angle α with the axis of the tab prism is refracted to the light reflecting surface side of the tab prism, and the light reflected on the light reflecting surface is It emits at an angle α with the axis.

【0006】タブプリズムの斜辺と底面とのなす角度は
θであり、このθはできるだけ大きくすることが好まし
い。この角度θがあまり小さすぎると、物体面より発し
た光がタブプリズムの光反射面で反射せず、直接出射面
から出射する迷光を生ずるようになり、得られる像のコ
ントラストが低下する。このような観点より、角度θは
θ≦90°−sin-1(1/n)、(ただし、nはタブプリズムを
構成する素材の屈折率)なる条件を満足させておくこと
が好ましい。
The angle formed by the hypotenuse and the bottom surface of the tab prism is θ, and this θ is preferably as large as possible. If this angle θ is too small, the light emitted from the object surface will not be reflected by the light reflecting surface of the tab prism, and stray light will be emitted directly from the emission surface, and the contrast of the obtained image will be reduced. From such a viewpoint, it is preferable that the angle θ satisfies the condition of θ ≦ 90 ° −sin −1 (1 / n) (where n is the refractive index of the material forming the tab prism).

【0007】またタブプリズムの巾方向の長さbと、軸
方向の底辺の長さaとの比a/bは[数1]を満足せし
めることにより、レンズの収差の少ない光軸付近が最も
明るくなる意味で好ましいが、全体的な像の明るさはa
/bが[数1]よりやや小さい方が明るくなる。また、
像の均一さはa/bに敏感に依存し、最適な値は、使用
するレンズの焦点距離やタブプリズム組立体の配列間隔
などによっても変わるため、実験あるいはコンピュータ
シュミレーション等を活用して[数1]の値よりやや小
さくするのがよい。
Further, the ratio a / b of the length b in the width direction of the tab prism to the length a of the base in the axial direction satisfies [Equation 1], so that the vicinity of the optical axis where the aberration of the lens is small is the most. It is preferable in terms of brightening, but the overall image brightness is a
It becomes brighter when / b is slightly smaller than [Equation 1]. Also,
Image uniformity is sensitive to a / b, and the optimum value varies depending on the focal length of the lens used and the arrangement interval of the tab prism assembly, so experiments or computer simulations should be used to It is better to make it slightly smaller than the value of 1].

【数1】 [Equation 1]

【0008】図4は本発明で用いるタブプリズム組立体
の斜視図であり、同図中8は2つのタブプリズムを接合
する黒色接着剤による接合面である。
FIG. 4 is a perspective view of a tab prism assembly used in the present invention. In FIG. 4, reference numeral 8 is a joint surface formed by a black adhesive for joining two tab prisms.

【0009】レンズアレイを使った面分割型投影素子で
は、レンズアレイを構成する結像素子自体が正立像を、
いずれかの方向で結ぶことがライン結像素子を面分割投
影素子として使うための必要条件であるが、この正立像
を結ぶ要件は結像素子をライン状に並べる方向のみで成
立すればよく、このライン方向と垂直方向では倒立像を
結像するものであっても十分に用い得る。
In a surface-division type projection element using a lens array, the image-forming element itself constituting the lens array produces an erect image.
Connecting in any direction is a necessary condition for using the line image forming element as a plane division projection element, but the requirement for forming an erect image may be satisfied only in the direction in which the image forming elements are arranged in a line, Even an inverted image can be sufficiently used in the direction perpendicular to the line direction.

【0010】図1は本発明の面分割投影素子のxz面と
その結像機構を示す平面図であり、図2はそのyz面の
平面図と結像機構を示す図であり、図3は本発明の面分
割投影素子を用いた縮小型画像読取りセンサの斜視図で
ある。これら図中の符号のうち、1はタブプリズム組立
体の光入射端に設けた凸レンズを、2はその光出射端に
設けた凸レンズを、3はタブプリズムであり、4は遮光
部材、5は物体面、6は結像を示す。物体面5、像面6
はそれぞれの凸レンズからの焦点距離だけ離れた位置に
あり、y方向には図3に示すごとく倒立像が結像し、x
方向ではタブプリズム3の働きで図3に示すごとく正立
像が結像する。
FIG. 1 is a plan view showing an xz plane and an image forming mechanism of the surface-division projection element of the present invention, FIG. 2 is a plan view of the yz plane and an image forming mechanism, and FIG. 3 is shown. It is a perspective view of a reduction type image reading sensor using the plane division projection element of the present invention. Among the reference numerals in these figures, 1 is a convex lens provided at the light incident end of the tab prism assembly, 2 is a convex lens provided at the light emitting end of the tab prism assembly, 3 is a tab prism, 4 is a light blocking member, and 5 is a light shielding member. The object plane, 6 shows the image formation. Object plane 5, image plane 6
Are at positions separated by the focal lengths from the respective convex lenses, and an inverted image is formed in the y direction as shown in FIG.
In the direction, the tab prism 3 serves to form an erect image as shown in FIG.

【0011】まず、底辺長20mm、底辺巾5mm、高さ10m
m、斜辺角θ=45°の2つのポリメチルメタクリレート
製タブプリズムを上底面が合うように黒色接着剤にて接
合し、タブプリズム組立体4個を用意する。凸レンズと
して、焦点距離F=40mmの凸レンズ(A) 3個と、焦点距
離f=45mmの凸レンズ(B) 4個を用意した。タブプリズ
ム組立体4個を、図1に示すごとく厚さ6.6mm の遮光部
材4をタブプリズム組立体間に配して組立てた。上記タ
ブプリズム組立体の配列体上面に、図1に示すごとく、
凸レンズ(A) のうち2個を光軸中心になるように10mm×
20mmの長方形に切断し、残りの2個は光軸中心に10mm×
10mmに切断し、図1に示すごとく、入射側の凸レンズ
(A) の軸間隔D=20mmとして配設し、さらに凸レンズ
(B) を10mm×15mmの長方形に切断し、出射側に光軸間隔
d=15mmで配設し、本発明の面分割投影素子とした。
First, the bottom length is 20 mm, the bottom width is 5 mm, and the height is 10 m.
Two tab prisms made of polymethylmethacrylate with m and hypotenuse angle θ = 45 ° are joined with a black adhesive so that the top and bottom surfaces are aligned, and four tab prism assemblies are prepared. As convex lenses, three convex lenses (A) having a focal length F = 40 mm and four convex lenses (B) having a focal length f = 45 mm were prepared. As shown in FIG. 1, four tab prism assemblies were assembled by placing a light shielding member 4 having a thickness of 6.6 mm between the tab prism assemblies. On the upper surface of the array of the tab prism assembly, as shown in FIG.
10 mm × 2 of the convex lenses (A) so that they are centered on the optical axis
Cut it into a rectangle of 20mm, and the other 2 pieces are 10mm at the center of the optical axis.
Cut into 10mm, as shown in Fig. 1, convex lens on the incident side
(A) Axial distance D = 20 mm is arranged, and a convex lens
(B) was cut into a rectangle of 10 mm × 15 mm and arranged on the emitting side with an optical axis interval d = 15 mm to obtain a plane division projection element of the present invention.

【0012】図1により本発明の面分割投影素子のxz
面内の結像機構について説明する。まず、凸レンズ(A)
アレイの要素内に含まれる単レンズ(A) の光軸と物体面
5との交点を0とし、レンズ(B) アレイの要素内に含ま
れる単レンズ(B) の光軸と像面6との交点を0'とする。
物体面5上の点0よりx1の距離離れた点x1より発した光
は凸レンズ(A) に入り、凸レンズ(A) の作用で光軸(z
軸)と角度−tan-1(x1/F) をなす平行光に変換される
(ただし、Fは凸レンズ(A) の焦点距離を示す)。次い
でタブプリズムの作用により、この光は光軸とのなす角
度tan-1(x1/F) をなす平行光に変換され、凸レンズ(B)
の作用によって、像面6上の点0'からx1'=x1×f/F だ
け離れた距離に結像する(ただし、fは凸レンズ(B) の
焦点距離を示す)。
Referring to FIG. 1, xz of the plane division projection element of the present invention.
The in-plane image forming mechanism will be described. First, convex lens (A)
The intersection of the optical axis of the single lens (A) included in the array element and the object plane 5 is set to 0, and the optical axis of the single lens (B) included in the element of the lens (B) array and the image plane 6 The intersection of is 0 '.
Light emitted from the distance apart points x 1 of x 1 from the point 0 on the object surface 5 enters the convex lens (A), the optical axis by the action of the convex lens (A) (z
It is converted into parallel light that forms an angle −tan −1 (x 1 / F) with the axis) (where F is the focal length of the convex lens (A)). Then, by the action of the tab prism, this light is converted into parallel light that forms an angle tan -1 (x 1 / F) with the optical axis, and the convex lens (B)
By the action of, the image is formed at a distance of x 1 '= x 1 × f / F from the point 0'on the image plane 6 (where f is the focal length of the convex lens (B)).

【0013】すなわち、像面上の像は、像面上の原点0
が結像面の原点0'に移ったf/F 倍の縮小像として結像す
る。隣り合う凸レンズ間の距離は物体面側でD(=20m
m)であるのに対し、像面側ではd(=15mm)となって
おり、d/D =f/F (3/4 倍)であるから、隣り合う凸レ
ンズの投影する縮小像はずれを生ずることなく、図3に
示すごとき連続像として結像する。
That is, the image on the image plane is the origin 0 on the image plane.
Is moved to the origin 0'of the image plane and is formed as a reduced image of f / F times. The distance between adjacent convex lenses is D (= 20 m on the object side).
m) whereas d (= 15 mm) on the image side, and d / D = f / F (3/4 times), the reduced image projected by the adjacent convex lens is displaced. Instead, it forms a continuous image as shown in FIG.

【0014】図2は本発明の面分割投影素子のyz面の
結像機構を説明する図である。凸レンズ(A) および凸レ
ンズ(B) はタンデムに使われていることより、その倍率
はf/F (3/4倍)の倒立像となる(図3参照)。
FIG. 2 is a view for explaining the image forming mechanism of the yz plane of the plane division projection element of the present invention. Since the convex lens (A) and the convex lens (B) are used in tandem, the magnification is an inverted image of f / F (3/4 times) (see Fig. 3).

【0015】すなわち各投影要素については、(イ) レン
ズ(A) による位置−角度変換、(ロ)タブプリズムによる
xz面内の角度の反転、(ハ) 凸レンズ(B) による角度−
位置変換、によってy方向のみ倒立したf/F 倍像が得ら
れ、これらの像の間隔f/F (d/D)倍に縮小されるため、
全体として倒立したf/F 倍の連続した倒立像が得られ
る。物体面と結像面とを逆にすることにより、F/f 倍の
倒立像の拡大像を結像することもできる。
That is, for each projection element, (a) position-angle conversion by the lens (A), (b) angle inversion in the xz plane by the tab prism, (c) angle by the convex lens (B)-
By position conversion, an inverted f / F magnified image is obtained only in the y direction, and the distance between these images is reduced by f / F (d / D) times.
As a whole, an inverted image of f / F times inverted is obtained. By inverting the object plane and the image plane, it is possible to form a magnified image of an inverted image of F / f times.

【0016】図1の面分割投影素子の縮小(拡大)倍率
は、3/4(4/3)であることがわかる。すなわち、この縮小
倍率はf/F =d/D =3/4 である。このように1組の凸レ
ンズアレイとタブプリズム組立体の配列体とを組合せた
本発明の面分割投影素子の投影像の縮小長さは投影側の
レンズアレイのピッチが限界である。従って、凸レンズ
アレイのタブプリズム組立体の配列数が多いほど、その
投影素子の縮小倍率の限界も大きくなる。タブプリズム
組立体の使用数をできるだけ多く使う投影素子とするこ
とにより、装置の小型化を図ることができる。このよう
な観点よりすると、本発明の面分割投影素子の縮小、拡
大倍率の範囲は0.75〜1.3 倍の範囲のものとするのが装
置上も好ましい。
It can be seen that the reduction (enlargement) magnification of the plane division projection element of FIG. 1 is 3/4 (4/3). That is, this reduction ratio is f / F = d / D = 3/4. As described above, the reduction length of the projected image of the plane-division projection element of the present invention in which one set of the convex lens array and the array of the tab prism assembly are combined is limited by the pitch of the lens array on the projection side. Therefore, the larger the number of tab prism assemblies arranged in the convex lens array, the larger the limit of reduction magnification of the projection element. The size of the apparatus can be reduced by using a projection element that uses as many tab prism assemblies as possible. From this point of view, it is preferable for the apparatus that the reduction and enlargement ratios of the surface-division projection element of the present invention are in the range of 0.75 to 1.3 times.

【0017】図6は本発明の面分割投影素子の他の一例
のxz面の平面図である。この例においては投影素子の
結像の明るさを向上させるため、図1で用いたものと同
じタブプリズム組立体の配列間隔をなくし、薄い遮光板
7を挿入した型とし、凸レンズアレイ9、10としては単
純な凸レンズの配列体とはせず、単レンズの一部を少し
ずつ位置を変えながら切り取った形の凸レンズを用い
た。凸レンズ9の焦点距離Fは60mm、凸レンズ10の焦点
距離fは40mmのものを用い、凸レンズアレイ9の凸レン
ズ(A) の光軸間距離Dを12mm、凸レンズアレイ10の凸レ
ンズ(B) の光軸間距離dを8mmとした。この投影素子に
よる投影像の縮小倍率は2/3 、拡大倍率は3/2 となって
いる。
FIG. 6 is a plan view of the xz plane of another example of the plane division projection element of the present invention. In this example, in order to improve the image forming brightness of the projection element, the same tab prism assembly arrangement as that used in FIG. 1 is eliminated, and a thin light shielding plate 7 is inserted in the convex lens arrays 9 and 10. As for the above, a simple convex lens array was not used, but a convex lens of a shape obtained by cutting out a part of a single lens while gradually changing the position was used. The convex lens 9 has a focal length F of 60 mm, and the convex lens 10 has a focal length f of 40 mm. The convex lens array 9 has a convex lens (A) with an inter-optical axis distance D of 12 mm, and the convex lens array 10 has a convex lens (B) with an optical axis. The distance d was set to 8 mm. The reduction ratio of the projected image by this projection element is 2/3, and the enlargement ratio is 3/2.

【0018】図7はタブプリズム組立体を7個用いた本
発明の面分割投影素子の他の実施例を示す平面図であ
り、この投影素子の縮小倍率は87.5%(拡大倍率では11
4 %)である。
FIG. 7 is a plan view showing another embodiment of the surface-splitting projection element of the present invention using seven tab prism assemblies, the projection element having a reduction ratio of 87.5% (enlargement ratio of 11).
4%).

【0019】図1および図6に示した投影素子において
は、レンズアレイ1、2、9、10の各単レンズの光軸間
隔を一定に並べたものを用いたが、これは本発明の面分
割投影素子の必要条件ではなく、物体面側と結像面側に
対応する凸レンズの光軸間隔が、それぞれの凸レンズの
焦点距離の比、すなわち縮小、拡大倍率に等しければ、
場所によってその間隔が異なってもよい。
In the projection elements shown in FIGS. 1 and 6, the single lenses of the lens arrays 1, 2, 9 and 10 are arranged with a constant optical axis interval. This is an aspect of the present invention. If the optical axis spacing of the convex lenses corresponding to the object plane side and the image plane side is not the requirement of the split projection element but is equal to the ratio of the focal lengths of the respective convex lenses, that is, reduction and enlargement magnification,
The interval may be different depending on the place.

【0020】本発明の面分割投影素子は、従来用いられ
ていたロッドレンズアレイ、三層レンズアレイを用いた
投影素子では不可能であった、縮小、拡大像を結像しう
る投影素子となし得た点、および色収差の少ない結像が
できるという点に大きな特徴を有するものである。
The plane-division projection element of the present invention is a projection element capable of forming a reduced or enlarged image, which is impossible with the projection element using a rod lens array or a three-layer lens array which has been conventionally used. It has a great feature in that it can obtain an image with little chromatic aberration.

【0021】[0021]

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の面分割投影素子のxz面の結像機構を
示す平面図である。
FIG. 1 is a plan view showing an image forming mechanism of an xz plane of a plane division projection element of the present invention.

【図2】図1の投影素子のyz面の結像機構を示す平面
図である。
2 is a plan view showing an image forming mechanism on a yz plane of the projection element in FIG. 1. FIG.

【図3】図1の投影素子をセンサとした例を示す斜視図
である。
FIG. 3 is a perspective view showing an example in which the projection element of FIG. 1 is used as a sensor.

【図4】タブプリズムの光伝送機構を示す平面図であ
る。
FIG. 4 is a plan view showing an optical transmission mechanism of a tab prism.

【図5】タブプリズム組立体の斜視図である。FIG. 5 is a perspective view of a tab prism assembly.

【図6】本発明の面分割投影素子の他の例のxz面の平
面図である。
FIG. 6 is a plan view of the xz plane of another example of the surface-division projection element of the present invention.

【図7】本発明の面分割投影素子の他の例のxz面の平
面図である。
FIG. 7 is a plan view of the xz plane of another example of the plane-division projection element of the present invention.

【符号の説明】[Explanation of symbols]

1,2,9,10 … 凸レンズアレイ 3 ………………… タブプリズム 4 ………………… 遮光体部 5 ………………… 物体面 6 ………………… 結像面 7 ………………… 遮光板 8 ………………… タブプリズム接合面 11,12 …………… 凸レンズの光軸 Tc ………………… 共役長 1, 2, 9, 10… Convex lens array 3 ………………… Tab prism 4 ………………… Light-shielding body 5 ………………… Object surface 6 ………………… Image plane 7 ……………… Light-shielding plate 8 …………………… Tab prism junction surface 11, 12, …………… Optical axis of convex lens Tc ………………… Conjugate length

─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───

【手続補正書】[Procedure amendment]

【提出日】平成5年2月18日[Submission date] February 18, 1993

【手続補正1】[Procedure Amendment 1]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】特許請求の範囲[Name of item to be amended] Claims

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【特許請求の範囲】[Claims]

【手続補正2】[Procedure Amendment 2]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0004[Correction target item name] 0004

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0004】[0004]

【課題を解決するための手段】そこで本発明者は、画像
の拡大、縮小機能を備えた面分割素子を開発することを
目的として検討した結果、本発明を完成したものであ
り、その要旨とするところは、タブプリズム2つを、そ
の光反射面が外側となるように、対称型に組立たタブプ
リズム組立体複数個を、その光反射面が対面するように
直線状に配列し、直線状に配列したタブプリズム組立体
の光入・出射端面に焦点距離の異なる2種の凸レンズ
を、光入射端側に配設する凸レンズの配列間隔Dと、光
出射端側に配設する凸レンズの配列間隔dとの比を、光
入射端側に配設する凸レンズの焦点距離と、光出射端側
に配設する凸レンズの焦点距離の比に等しくなるように
配設したことを特徴とする面分割投影素子にある。
Therefore, the present inventor has completed the present invention as a result of an examination for the purpose of developing a surface division element having an image enlarging / reducing function. Whereas, two tab prisms are symmetrically assembled so that their light reflecting surfaces are on the outside, and a plurality of tab prism assemblies are arranged linearly so that their light reflecting surfaces face each other. Of the two types of convex lenses having different focal lengths on the light input / output end faces of the tab prism assembly arranged in a circular pattern, and the arrangement interval D of the convex lenses arranged on the light incident end side and the convex lens arranged on the light emitting end side. A surface characterized by being arranged such that the ratio to the array interval d is equal to the ratio of the focal length of the convex lens arranged on the light incident end side to the focal length of the convex lens arranged on the light emitting end side. It is in a split projection element.

【手続補正3】[Procedure 3]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0005[Name of item to be corrected] 0005

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0005】本発明で用いるタブプリズム3の断面を図
5に示した。このタブプリズムの軸との角αをもって入
射した光はタブプリズムの斜辺で、その光反射面側へ屈
折され、光反射面で反射した光は、タブプリズムの光出
射面側の斜辺より、その軸とのなす角度αで反転方向に
出射する。
A cross section of the tab prism 3 used in the present invention is shown in FIG. The light incident at an angle α with the axis of the tab prism is refracted to the light reflecting surface side of the tab prism, and the light reflected on the light reflecting surface is The light is emitted in the inversion direction at an angle α with the axis.

【手続補正4】[Procedure amendment 4]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0006[Correction target item name] 0006

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0006】タブプリズムの斜辺と底面とのなす角度は
θであり、この角度θが大きくなると、物体面より発し
た光がタブプリズムの光反射面で反射せず、直接出射面
から出射する迷光を生ずるようになり、得られる像のコ
ントラストが低下する。このような観点より、角度θは
θ≦90゜−sin−1(1/n)、(ただし、nはタ
ブプリズムを構成する素材の屈折率)なる条件を満足さ
せておくことが好ましい。
The angle between the hypotenuse of the tab prism and the bottom surface is θ. When this angle θ becomes large, the light emitted from the object surface is not reflected by the light reflection surface of the tab prism, but is stray light directly emitted from the emission surface. And the contrast of the obtained image is reduced. From this point of view, it is preferable that the angle θ satisfies the condition of θ ≦ 90 ° -sin −1 (1 / n) (where n is the refractive index of the material forming the tab prism).

【手続補正5】[Procedure Amendment 5]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0007[Correction target item name] 0007

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0007】またタブプリズムの巾方向の長さbと、軸
方向の底辺の長さaとの比a/bは[数1]を満足せし
めることにより、レンズの収差の少ない光軸付近が最も
明るくなる意味で好ましいが、全体的な像の明るさはa
/bが[数1]よりやや小さい方が明るくなる。また、
像の均一さはa/bに敏感に依存し、最適な値は、使用
するレンズの焦点距離やタブプリズム組立体の配列間隔
などによっても変わるため、実験あるいはコンピュータ
シュミレーション等を活用して[数1]の値よりやや小
さい最適値を決めるのがよい。
Further, the ratio a / b of the length b in the width direction of the tab prism to the length a of the base in the axial direction satisfies [Equation 1], so that the vicinity of the optical axis where the aberration of the lens is small is the most. It is preferable in terms of brightening, but the overall image brightness is a
It becomes brighter when / b is slightly smaller than [Equation 1]. Also,
Image uniformity is sensitive to a / b, and the optimum value varies depending on the focal length of the lens used and the arrangement interval of the tab prism assembly, so experiments or computer simulations should be used to It is better to decide an optimum value that is slightly smaller than the value of 1].

【数1】[Equation 1]

【手続補正6】[Procedure correction 6]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0009[Correction target item name] 0009

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0009】レンズアレイにて構成されたライン結像素
子では、各ユニットが正立像を結ぶことが、つながりの
あるライン像を結像させるための必須条件となる。ただ
し、この正立像の条件はライン結像素子のライン方向で
のみ成り立てば十分であるため、本発明ではライン方向
にタブプリズムの像反転作用を使ってレンズの負担を低
減し、色収差の少ない、かつ、組立容易なライン結像素
子とすることに成功した。本発明ではライン方向と垂直
な方向には像は倒立するが、正立像が必要な場合は、鏡
を使って像を反転し、正立像に変えて用いればよい。
In a line image forming element composed of a lens array, each unit forms an erect image is an essential condition for forming a continuous line image. However, the condition of this erect image is sufficient if it is satisfied only in the line direction of the line image forming element, so in the present invention, the burden on the lens is reduced by using the image inverting action of the tab prism in the line direction, and the chromatic aberration is small. In addition, we succeeded in making a line imaging element that is easy to assemble. In the present invention, the image is inverted in the direction perpendicular to the line direction. However, if an erect image is required, the image may be inverted by using a mirror and used as an erect image.

【手続補正7】[Procedure Amendment 7]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0010[Correction target item name] 0010

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0010】図1は本発明の面分割投影素子のxz面と
その結像機構を示す平面図であり、図2はそのyz面の
平面図と結像機構を示す図であり、図3はその斜視図で
ある。これら図中の符号のうち、1はタブプリズム組立
体の光入射端に設けた凸レンズを、2はその光出射端に
設けた凸レンズを、3はタブプリズムであり、4は遮光
部材、5は物体面、6は像面を示す。物体面5、像面6
はそれぞれの凸レンズからの焦点距離だけ離れた位置に
あり、y方向には図3に示すごとく倒立像が結像し、x
方向ではタブプリズム3の働きで図3に示すごとく正立
像が結像する。
FIG. 1 is a plan view showing an xz plane and an image forming mechanism of the surface-division projection element of the present invention, FIG. 2 is a plan view of the yz plane and an image forming mechanism, and FIG. 3 is shown. It is the perspective view. Among the reference numerals in these figures, 1 is a convex lens provided at the light incident end of the tab prism assembly, 2 is a convex lens provided at the light emitting end of the tab prism assembly, 3 is a tab prism, 4 is a light blocking member, and 5 is a light shielding member. The object plane and 6 are image planes. Object plane 5, image plane 6
Are at positions separated by the focal lengths from the respective convex lenses, and an inverted image is formed in the y direction as shown in FIG.
In the direction, the tab prism 3 serves to form an erect image as shown in FIG.

【手続補正8】[Procedure Amendment 8]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0011[Correction target item name] 0011

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0011】説明を分かりやすくするために、具体的な
実施例を示す。底辺長20mm、底辺巾5mm、高さ1
0mm、斜辺角θ=45゜の2つのポリメチルメタクリ
レート製タブプリズムを上底面が合うように黒色接着剤
にて接合したタブプリズム組立体4個と、焦点距離F=
60mmの凸レンズ(A)4個と、焦点距離f=45m
mの凸レンズ(B)4個を用意し、タブプリズム組立体
4個を、図1に示すごとく厚さ6.6mmの遮光部材4
をタブプリズム組立体間に配して組立てた。次に凸レン
ズ(A)は2個を光軸が中心になるように10mm×2
0mmの長方形に切り、残りの2個はこの半分の10m
m×10mmに切って図1のように入射側に軸間隔D=
20mmで配設し、さらに凸レンズ(B)は10mm×
15mmの長方形に切って、出射側に軸間隔d=15m
mで配設して、本発明の面分割投影素子とする。
Specific examples will be shown for the sake of clarity. Base length 20 mm, base width 5 mm, height 1
Four tab prism assemblies made by joining two polymethylmethacrylate tab prisms with 0 mm and hypotenuse angle θ = 45 ° with a black adhesive so that the top and bottom surfaces match, and the focal length F =
Four 60 mm convex lenses (A) and focal length f = 45 m
4 convex lenses (B) having a thickness of 6.6 mm are provided as shown in FIG.
Were assembled between the tab prism assemblies. Next, place 2 convex lenses (A) so that the optical axis is at the center and 10 mm x 2
Cut it into a rectangle of 0mm, and the other two are 10m which is half of this
Cut into m × 10 mm and set the axial distance D = on the incident side as shown in Fig. 1.
20 mm, and the convex lens (B) is 10 mm ×
Cut into a rectangle of 15 mm, and have an axial distance d = 15 m on the exit side.
m to provide the plane-division projection element of the present invention.

【手続補正9】[Procedure Amendment 9]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0015[Name of item to be corrected] 0015

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0015】すなわち各投影要素については、(イ)レ
ンズ(A)による位置−角度変換、(ロ)タブプリズム
によるxz面内の角度反転、(ハ)凸レンズ(B)によ
る角度−位置変換、によってy方向のみ倒立したf/F
倍像が得られ、これら像間の間隔f/F(d/D)倍に
縮小されるため、全体として倒立したf/F倍の連続し
た倒立像が得られる。また、本面分割投影素子は物体面
と結像面とを逆にすることにより、F/f倍の拡大投影
素子として使うこともできる。
That is, for each projection element, (a) position-angle conversion by the lens (A), (b) angle inversion in the xz plane by the tab prism, and (c) angle-position conversion by the convex lens (B). Inverted f / F only in y direction
Since a doubled image is obtained and the distance between these images is reduced by a factor of f / F (d / D), a continuous inverted image of an inverted f / F is obtained as a whole. Further, the present plane division projection element can also be used as an F / f times magnifying projection element by reversing the object plane and the image plane.

【手続補正10】[Procedure Amendment 10]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0016[Correction target item name] 0016

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0016】図1の面分割投影素子では、像側の凸レン
ズの光軸が、物体側の凸レンズの光軸に比べて、両端の
レンズでd/2ずつ内側に移動し、縮小像を投影してい
る。このように1組の凸レンズアレイとタブプリズム組
立体の配列体とを組合せた本発明の面分割投影素子の投
影像の縮小長さは投影側のレンズアレイのピッチが限界
である。従って、凸レンズとタブプリズム組立体光学ユ
ニットの配列数が多いほど、その投影素子の縮小倍率の
限界も大きくなる。一方、光学ユニットの配列数を少な
くするほど、面分割して投影することによる装置の小型
化(投影距離の短縮)の効果が薄くなるため、あまり配
列数を少なくすることはできない。
In the plane-division projection element of FIG. 1, the optical axis of the convex lens on the image side is moved inward by d / 2 by the lenses at both ends compared to the optical axis of the convex lens on the object side, and a reduced image is projected. ing. As described above, the reduction length of the projected image of the plane-division projection element of the present invention in which one set of the convex lens array and the array of the tab prism assembly are combined is limited by the pitch of the lens array on the projection side. Therefore, the larger the number of the convex lenses and the tab prism assembly optical units arranged, the larger the limit of the reduction ratio of the projection element. On the other hand, the smaller the number of arrays of the optical units, the smaller the effect of downsizing the apparatus (shortening the projection distance) by performing the plane division and projecting, and thus the number of arrays cannot be reduced so much.

【手続補正11】[Procedure Amendment 11]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0017[Correction target item name] 0017

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0017】図6は本発明の面分割投影素子の他の一例
のxz面の平面図である。この例においては投影素子の
結像の明るさを向上させるため、図1で用いたものと同
じタブプリズム組立体の配列間隔をなくし、薄い遮光板
7を挿入した型とし、凸レンズアレイ9、10としては
単純な凸レンズの配列体とはせず、単レンズの一部を少
しずつ位置を変えながら切り取った形の凸レンズを用い
た。具体的には、凸レンズ9の焦点距離Fは60mm、
凸レンズ10の焦点距離fは40mmとし、凸レンズア
レイ9の凸レンズ(A)の光軸間距離Dを12mm、凸
レンズアレイ10の凸レンズ(B)の光軸間距離dを8
mmとすると、この投影素子による投影像の縮小倍率は
2/3、拡大倍率は3/2となる。
FIG. 6 is a plan view of the xz plane of another example of the plane division projection element of the present invention. In this example, in order to improve the image forming brightness of the projection element, the same tab prism assembly arrangement as that used in FIG. 1 is eliminated, a thin light shielding plate 7 is inserted, and the convex lens arrays 9 and 10 are used. As for the above, a simple convex lens array was not used, but a convex lens of a shape obtained by cutting out a part of a single lens while gradually changing the position was used. Specifically, the focal length F of the convex lens 9 is 60 mm,
The focal length f of the convex lens 10 is 40 mm, the inter-optical axis distance D of the convex lens (A) of the convex lens array 9 is 12 mm, and the inter-optical axis distance d of the convex lens (B) of the convex lens array 10 is 8 mm.
In mm, the reduction ratio of the projected image by this projection element is 2/3, and the enlargement ratio is 3/2.

【手続補正12】[Procedure Amendment 12]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0018[Correction target item name] 0018

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【0018】図7はタブプリズム組立体を8個用いた本
発明の面分割投影素子の他の実施例を示す平面図であ
り、この投影素子の縮小倍率は87.5%(拡大倍率で
は114%)である。
FIG. 7 is a plan view showing another embodiment of the plane-division projection element of the present invention using eight tab prism assemblies. The reduction magnification of this projection element is 87.5% (the enlargement magnification is 114%). %).

【手続補正13】[Procedure Amendment 13]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】符号の説明[Correction target item name] Explanation of code

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【符号の説明】 1,2,9,10 … 凸レンズアレイ 3 …………………… タブプリズム 4 …………………… 遮光体部 5 …………………… 物体面 6 …………………… 結像面 7 …………………… 遮光板 8 …………………… 黒色接着剤 11,12 ………… 凸レンズの光軸 Tc ………………… 共役長[Explanation of reference numerals] 1, 2, 9, 10 ... Convex lens array 3 …………………… Tab prism 4 …………………… Light-shielding body 5 …………………… Object plane 6 …………………… Image forming surface 7 …………………… Light-shielding plate 8 …………………… Black adhesive 11, 12 ………… Optical axis of convex lens Tc ………… ……… Conjugate length

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 断面対称台形のタブプリズム2つを、そ
の光反射面が外側となるように、対称型に組立たタブプ
リズム組立体複数個を、その光反射面が互いに対面する
ように直線状に配列し、この直線状に配列したタブプリ
ズム組立体の光入・出射端面に、焦点距離の異なる2種
の凸レンズを光入射端側に配設する凸レンズの配列間隔
D(レンズ軸間距離)と、光出射端側に配設する凸レン
ズの光軸の配列間隔d(レンズ軸間距離)との比を、光
入射端側に配設する凸レンズの焦点距離と、光出射端側
に配設する凸レンズの焦点距離の比に等しくなるように
配設したことを特徴とする面分割投影素子。
1. A plurality of tab prism assemblies which are symmetrically assembled such that two tab prisms having a symmetric trapezoidal cross section are arranged so that their light reflecting surfaces are on the outside, and straight tabs are arranged so that their light reflecting surfaces face each other. The convex-lens array interval D (distance between the lens axes), in which two kinds of convex lenses having different focal lengths are arranged on the light-incident end side, on the light-incident / outgoing end faces of the tab prism assembly arranged in a straight line ) And the array distance d (lens axis distance) of the optical axes of the convex lenses arranged on the light emitting end side, the focal length of the convex lenses arranged on the light incident end side and the A plane-division projection element characterized in that it is arranged so as to be equal to the ratio of the focal lengths of the convex lenses to be provided.
JP30590192A 1992-10-21 1992-10-21 Planar split projection element Expired - Fee Related JP3258097B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30590192A JP3258097B2 (en) 1992-10-21 1992-10-21 Planar split projection element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30590192A JP3258097B2 (en) 1992-10-21 1992-10-21 Planar split projection element

Publications (2)

Publication Number Publication Date
JPH06130325A true JPH06130325A (en) 1994-05-13
JP3258097B2 JP3258097B2 (en) 2002-02-18

Family

ID=17950665

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006292748A (en) * 2005-04-06 2006-10-26 Dr Johannes Heidenhain Gmbh Scanning unit for position-measuring apparatus for optically scanning measuring scale

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006292748A (en) * 2005-04-06 2006-10-26 Dr Johannes Heidenhain Gmbh Scanning unit for position-measuring apparatus for optically scanning measuring scale
DE102005015743B4 (en) 2005-04-06 2018-08-23 Dr. Johannes Heidenhain Gmbh Scanning unit for a position measuring device for optically scanning a material measure and position measuring device

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