JPH0625801B2 - Light splitting prism - Google Patents
Light splitting prismInfo
- Publication number
- JPH0625801B2 JPH0625801B2 JP57193066A JP19306682A JPH0625801B2 JP H0625801 B2 JPH0625801 B2 JP H0625801B2 JP 57193066 A JP57193066 A JP 57193066A JP 19306682 A JP19306682 A JP 19306682A JP H0625801 B2 JPH0625801 B2 JP H0625801B2
- Authority
- JP
- Japan
- Prior art keywords
- prism
- light splitting
- light
- incident
- splitting surface
- 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.)
- Expired - Lifetime
Links
- 230000004907 flux Effects 0.000 claims description 10
- 238000001514 detection method Methods 0.000 claims description 6
- 230000003287 optical effect Effects 0.000 description 6
- 230000006399 behavior Effects 0.000 description 4
- 230000011514 reflex Effects 0.000 description 3
- 125000006850 spacer group Chemical group 0.000 description 3
- 230000002411 adverse Effects 0.000 description 1
- 230000004075 alteration Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000011888 foil Substances 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 230000009191 jumping Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 210000001747 pupil Anatomy 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/04—Prisms
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Elements Other Than Lenses (AREA)
- Cameras In General (AREA)
Description
【発明の詳細な説明】 本発明は、一眼レフカメラ等に用いられる光分割用プリ
ズムに関するものである。The present invention relates to a light splitting prism used in a single-lens reflex camera or the like.
最近一眼レフカメラ等においては、結像光束から合焦検
出光束を分割するために、例えば第1図に示した如く写
真対物レンズ1と跳上げミラー2(第1図では跳上がつ
た状態を示している)との間に、ハーフミラーコートを
蒸着した光分割面3aを有する第一プリズム3と該光分
割面3aに対向し且つ接合された面4aを有する第二プ
リズム4とから成る光分割用プリズム5を配置し、写真
対物レンズ1の射出瞳1aを発した結像光束の大部分は
光分割面3aを透過して感光面6に入射し、該結像光束
の一部は第2図に示した如く光分割面3aで反射されて
合焦検出光束として第一プリズム3内で反射を繰返しな
がら合焦検出素子7へと導かれるようにしていた。とこ
ろが、第3図に示した如く、光分割面3aを透過した場
合には感光面6の外の位置P′に入射するはずの光束の
一部(ゴースト光束)が光分割面3aで反射された後第
一プリズム3の前面3bで全反射され、続いて光分割面
3aを透過した後第二プリズム4の後面4bで全反射さ
れ、更に光分割面3aで反射されて感光面6上の位置
P″に入射するため、ゴースト線が形成されるという問
題があつた。In recent single-lens reflex cameras and the like, in order to split the focus detection light beam from the image formation light beam, for example, as shown in FIG. 1, the photographic objective lens 1 and the jumping mirror 2 (in FIG. (Shown) between the first prism 3 having a light splitting surface 3a and a second prism 4 having a surface 4a facing the light splitting surface 3a and joined to the light splitting surface 3a. With the splitting prism 5 arranged, most of the image-forming light flux emitted from the exit pupil 1a of the photographic objective lens 1 passes through the light-splitting surface 3a and is incident on the photosensitive surface 6, and a part of the image-forming light flux is As shown in FIG. 2, the light is reflected by the light splitting surface 3a and is guided to the focus detection element 7 as a focus detection light beam while repeatedly reflected in the first prism 3. However, as shown in FIG. 3, a part of the light beam (ghost light beam) that should be incident on the position P ′ outside the photosensitive surface 6 when it passes through the light splitting surface 3a is reflected by the light splitting surface 3a. Then, the light is totally reflected by the front surface 3b of the first prism 3, then transmitted through the light splitting surface 3a, then totally reflected by the rear surface 4b of the second prism 4, further reflected by the light splitting surface 3a, and then on the photosensitive surface 6. Since the light enters the position P ″, there is a problem that a ghost line is formed.
本発明は、上記問題点に鑑み、光分割面とこれに対向し
且つ接合された面との間に薄い空気層を形成して、ゴー
スト光束を全反射により光路外へ取り出すようにした光
分割用プリズムを提供せんとするものであるが、以下第
4図乃至第6図に示した一実施例に基づきこれを説明す
れば、光分割面3aとこれに対向し且つ接合された面4
aとの間に十分薄い空気層8が形成されている。この空
気層8を形成するには、例えば第5図(a)に示した如
く、光分割面3aと面4aとの間に箔又は薄い蒸着膜か
ら成るスペーサー9を介在せしめれば良い。この場合、
第5図(b)に示した如く、スペーサー9を光分割面3a
上において有効光束の境界線Aの外側に位置する斜線部
Bに配置すれば、結像光学系の特性に悪影響を及ぼすこ
とはない。In view of the above problems, the present invention forms a thin air layer between a light splitting surface and a surface that faces the light splitting surface and is joined to the light splitting surface so that the ghost light flux is extracted out of the optical path by total reflection. A prism for use in the present invention will be described below. According to an embodiment shown in FIGS. 4 to 6, the light splitting surface 3a and the surface 4 facing and joined to the light splitting surface 3a will be described.
A sufficiently thin air layer 8 is formed between a and a. To form the air layer 8, for example, as shown in FIG. 5A, a spacer 9 made of foil or a thin vapor deposition film may be interposed between the light splitting surfaces 3a and 4a. in this case,
As shown in FIG. 5 (b), the spacer 9 is attached to the light splitting surface 3a.
By arranging it in the shaded portion B located outside the boundary line A of the effective light flux, the characteristics of the imaging optical system are not adversely affected.
本発明による光分割用プリズムは上述の如く構成されて
おり、空気層8が十分に薄いから光分割面3aを透過し
た光束の振舞いは上記従来例の場合(第1図)と変らな
い。又、光分割面3aで反射されて合焦検出光束となる
光束の振舞いも上記従来例の場合(第2図)と全く同じ
である。しかし、光分割面3aで反射されたゴースト光
束は、第一プリズム3の前面3bで全反射されて再び光
分割面3aに入射した時、この面3aの射出側が空気層
8であるため、第4図に示した如く全反射されて光路外
へ取り出される。取り出されたゴースト光束は、感光面
6へも入射しないし、又合焦検出素子へも入射しない。
これについて詳しく説明すれば、第6図は第一プリズム
3の要部拡大断面図であつて、光分割面3aを透過した
際に感光面6の外へ向うはずの光線lが第一プリズム3
に入射した時の屈折角をi′とすると、光分割面3aで
の反射角φは第一プリズム3の頂角をαとして、φ=α
-i′となる。そして、前面3bでの反射角ωは、ω=
2α-i′となり、更に光分割面3aでの再反射角δ
は、δ=3α-i′となる。従つて、この時、光が光分
割面3aを透過しないためには、全反射の条件 nsinδ≧n0……(a) を満足すれば良い。ここで、nは第一プリズム3の屈折
率、n0は空気の屈折率である。即ち、式(a)を満足する
ように第一プリズム3の頂角及び位置を決めれば良い。
尚、通常は収差の発生を防ぐ意味などから、プリズムの
入射面は光軸と垂直にするのが多い。この場合、光線l
の入射角iは画角そのものになる。The light splitting prism according to the present invention is constructed as described above, and since the air layer 8 is sufficiently thin, the behavior of the light beam transmitted through the light splitting surface 3a is the same as in the case of the conventional example (FIG. 1). Further, the behavior of the light flux which is reflected by the light splitting surface 3a and becomes the focus detection light flux is exactly the same as in the case of the conventional example (FIG. 2). However, when the ghost light flux reflected by the light splitting surface 3a is totally reflected by the front surface 3b of the first prism 3 and enters the light splitting surface 3a again, since the exit side of this surface 3a is the air layer 8, As shown in FIG. 4, the light is totally reflected and taken out of the optical path. The extracted ghost light flux does not enter the photosensitive surface 6 nor the focus detection element.
This will be described in detail. FIG. 6 is an enlarged cross-sectional view of an essential part of the first prism 3, in which a light ray 1 that should go to the outside of the photosensitive surface 6 when passing through the light splitting surface 3a.
Let i ′ be the refraction angle upon incidence on the optical axis, the reflection angle φ at the light splitting surface 3a is φ = α, where α is the apex angle of the first prism 3.
-i '. The reflection angle ω on the front surface 3b is ω =
2α-i ′, and the re-reflection angle δ at the light splitting surface 3a
Is δ = 3α-i ′. Therefore, at this time, in order that light does not pass through the light splitting surface 3a, it is sufficient to satisfy the condition of total reflection nsin δ ≧ n 0 (a). Here, n is the refractive index of the first prism 3, and n 0 is the refractive index of air. That is, the apex angle and the position of the first prism 3 may be determined so as to satisfy the expression (a).
Incidentally, in order to prevent the occurrence of aberrations, the incident surface of the prism is usually perpendicular to the optical axis. In this case ray l
The incident angle i of is the angle of view itself.
上述の如く、本発明による光分割用プリズムは、その光
学的特性を何ら変えることなく、ゴースト光束を取り除
き得るという極めて重要な利点を有している。As described above, the light splitting prism according to the present invention has a very important advantage that the ghost light flux can be removed without changing its optical characteristics.
第1図は一眼レフカメラ内に配置した従来の光分割用プ
リズムにおける透過光束の振舞いを示す断面図、第2及
び第3図は夫々上記従来例における反射光束及びゴース
ト光束の振舞いを夫々示す断面図、第4図は本発明によ
る光分割用プリズムの一実施例の断面図、第5図は上記
実施例における空気層の形成方法を示す図、第6図は上
記実施例の第一プリズムの要部拡大断面図である。 3……第一プリズム、3a……光分割面、4……第二プ
リズム、8……空気層、9……スペーサー。FIG. 1 is a sectional view showing the behavior of a transmitted light beam in a conventional light splitting prism arranged in a single-lens reflex camera, and FIGS. 2 and 3 are sectional views showing the behaviors of a reflected light beam and a ghost light beam in the conventional example, respectively. 4 and 5 are sectional views of an embodiment of a light splitting prism according to the present invention, FIG. 5 is a view showing a method for forming an air layer in the above embodiment, and FIG. 6 is a view of the first prism of the above embodiment. It is a principal part expanded sectional view. 3 ... First prism, 3a ... Light splitting surface, 4 ... Second prism, 8 ... Air layer, 9 ... Spacer.
Claims (1)
フミラーコートを蒸着した光分割面を有する第一プリズ
ムと、 前記光分割面に微小空気間隙を隔てて対向させた面を有
する第二プリズムとで構成され、 前記第一プリズムから入射した結像光束のうちで、前記
光分割面で反射した成分を前記第一プリズムの入射面で
全反射して合焦検出素子へ導くと共に、前記光分割面を
透過した成分を前記第二プリズムを介して感光面に入射
する光分割用プリズムであって、 前記第一プリズムの入射面から前記感光面外に入射する
光線のうちで、前記光分割面で反射した成分が前記第一
プリズムの入射面で全反射して、再度前記光分割面に入
射する際の入射角をδとするとき、以下の条件式を満た
すように前記第一プリズムを選定したことを特徴とする
光分割用プリズム。 n sinδ≧n0 ここで、nは第一プリズムの屈折率、 n0は空気の屈折率である。1. A first prism having an incident surface and a light splitting surface inclined with respect to the incident surface and having a half mirror coat deposited thereon, and a first prism having a surface facing the light splitting surface with a minute air gap therebetween. It is composed of two prisms, and in the image forming light flux incident from the first prism, the component reflected by the light splitting surface is totally reflected by the incident surface of the first prism and guided to the focus detection element, A light splitting prism that allows a component that has passed through the light splitting surface to enter the photosensitive surface via the second prism, wherein among the light rays that are incident from the incident surface of the first prism to the outside of the photosensitive surface, When the component reflected by the light splitting surface is totally reflected by the incident surface of the first prism and the incident angle when entering the light splitting surface again is δ, the first condition is satisfied so that the following conditional expression is satisfied. Characterized by selecting a prism Light splitting prism. n sin δ ≧ n 0 Here, n is the refractive index of the first prism, and n 0 is the refractive index of air.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57193066A JPH0625801B2 (en) | 1982-11-02 | 1982-11-02 | Light splitting prism |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57193066A JPH0625801B2 (en) | 1982-11-02 | 1982-11-02 | Light splitting prism |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5983103A JPS5983103A (en) | 1984-05-14 |
| JPH0625801B2 true JPH0625801B2 (en) | 1994-04-06 |
Family
ID=16301632
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57193066A Expired - Lifetime JPH0625801B2 (en) | 1982-11-02 | 1982-11-02 | Light splitting prism |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0625801B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6945657B2 (en) * | 2000-10-19 | 2005-09-20 | Pentax Corporation | Surveying instrument |
-
1982
- 1982-11-02 JP JP57193066A patent/JPH0625801B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5983103A (en) | 1984-05-14 |
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