JPS583201B2 - Hikari Bun Katsuki - Google Patents
Hikari Bun KatsukiInfo
- Publication number
- JPS583201B2 JPS583201B2 JP50068766A JP6876675A JPS583201B2 JP S583201 B2 JPS583201 B2 JP S583201B2 JP 50068766 A JP50068766 A JP 50068766A JP 6876675 A JP6876675 A JP 6876675A JP S583201 B2 JPS583201 B2 JP S583201B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- diffraction grating
- splitter
- diffraction
- diffracted light
- 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
Links
Landscapes
- Exposure Control For Cameras (AREA)
- Optical Elements Other Than Lenses (AREA)
Description
【発明の詳細な説明】
本発明は回折格子により光束を分割する光分割器の改良
に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a light splitter that splits a light beam using a diffraction grating.
回折格子を使用した光分割器は、昭和47年12月11
日昭和47年特許出願第124196号として、又昭和
48年11月29日、昭和48年特許出願第13478
2号として本件出願人によって出願されている。A light splitter using a diffraction grating was introduced on December 11, 1971.
Japan as Patent Application No. 124196, dated November 29, 1972, and Patent Application No. 13478, filed on November 29, 1972.
This application has been filed by the applicant as No. 2.
本発明はこの様な光分割器の改良に係るもので、その特
徴として回折格子がこの回折格子とほぼ同一の屈折率を
有する光学部材の2つの境界面の藺に配されている。The present invention relates to an improvement of such a light splitter, and its feature is that a diffraction grating is arranged at the interface between two optical members having substantially the same refractive index as the diffraction grating.
ここで、境界面とは屈折率が互に異なる2つの物質の境
界面で、通常ガラスと空気の境界面である。Here, the boundary surface is the boundary surface between two substances having different refractive indexes, and is usually the boundary surface between glass and air.
この様な構成上の特徴によって、本発明の光分割器は大
きな回折格子を使用することが可能となる、及び、回折
格子が品質の劣化が防止されるという効果を有している
。These structural features have the advantage that the light splitter of the present invention allows the use of a large diffraction grating and prevents the quality of the diffraction grating from deteriorating.
以下本発明の実施例を本発明の構成を採らなかった光分
割器と比較して説明する。Examples of the present invention will be described below in comparison with a light splitter that does not have the configuration of the present invention.
第1図は先に述べた出願に示された光分割器である。FIG. 1 is the light splitter shown in the above-mentioned application.
この光分割器1は平行平面ガラス板2の面に回折格子3
が接着剤等によって接着されている。This light splitter 1 has a diffraction grating 3 on the surface of a parallel plane glass plate 2.
are attached with adhesive or the like.
そして、この平行平面ガラス板2、回折格子3、接着剤
はほぼ等しい屈折率を有することが望ましい。It is desirable that the parallel plane glass plate 2, the diffraction grating 3, and the adhesive have substantially the same refractive index.
又、回折格子は立体的な格子構造を有する体積型回折格
子が望ましい。Further, the diffraction grating is preferably a volume type diffraction grating having a three-dimensional grating structure.
4,5は夫々空気と接する境界面である。4 and 5 are boundary surfaces in contact with air, respectively.
6は出射面である。7は受光素子である。6 is an exit surface. 7 is a light receiving element.
一方の境界面5から入射光8は回折格子3によって非回
折光9と回折光10に分割される。Incoming light 8 from one boundary surface 5 is split by the diffraction grating 3 into undiffracted light 9 and diffracted light 10.
非回折光は境界面5を透過するが、回折光10は回折体
3が回折光10を他の境界面4に対して全反射の条件を
満す角度に回折される様に構成されているため、境界面
4によって全反射される。The undiffracted light passes through the boundary surface 5, but the diffracted light 10 is configured so that the diffraction body 3 diffracts the diffracted light 10 to another boundary surface 4 at an angle that satisfies the condition for total reflection. Therefore, it is totally reflected by the boundary surface 4.
そしてこの面4によって反射された回折光10は更に境
界面5によって、全反射され射出面6より射出され受光
素子7によって受けられる。The diffracted light 10 reflected by this surface 4 is further totally reflected by the boundary surface 5, emitted from the exit surface 6, and received by the light receiving element 7.
この図から明らかな様に光分割器1の大きさが犬の場合
回折光10は更に回折格子3に11.12の位置で再入
射してしまう。As is clear from this figure, when the size of the light splitter 1 is a dog, the diffracted light 10 further enters the diffraction grating 3 at a position of 11.12.
従って、この11,12の位置で回折光は再び回折され
1部は迷光となる。Therefore, the diffracted light is diffracted again at these positions 11 and 12, and part of it becomes stray light.
回哲格子が狭い角度特性を有するものであれば、11の
位置で生じ葛再回折光の回折率はよい。If the diffraction grating has narrow angular characteristics, the diffraction index of the re-diffracted light generated at position 11 will be good.
しかしながら、12の位置で生じる再回折光は入射光8
の入射角に近いため再回折光の回折率は太きい。However, the re-diffracted light generated at position 12 is the incident light 8
The diffraction index of the re-diffracted light is large because the angle of incidence is close to that of .
従ってこの12の位置の再回折光を取り除く必要が有る
。Therefore, it is necessary to remove the re-diffracted light at these 12 positions.
又更に、第1図の如き構成では回折格子が、直接外気に
接しているため、この回折格子がダイクロメーテイドゼ
ラチンの如き湿度に対して影響を受けやすいものであっ
た場合、品質の劣化を生じさせる恐れが有った。Furthermore, in the configuration shown in Figure 1, the diffraction grating is in direct contact with the outside air, so if the diffraction grating is made of dichromated gelatin, which is easily affected by humidity, quality deterioration may occur. There was a risk that it would occur.
本発明はこの様な点を考慮して発明されたもので、第2
回に示す様に、回折体3はガラス板によって挾持されて
いる。The present invention was invented taking these points into consideration, and the second
As shown in Figure 3, the diffractive body 3 is held between glass plates.
すなわち、回折体3の境界面5に先述の如き接着剤によ
り平行平面ガラス板13は接着されている。That is, the parallel plane glass plate 13 is bonded to the boundary surface 5 of the diffractive body 3 using the adhesive as described above.
このガラス板13は回折格子5とほぼ同一の屈折率のガ
ラスを使用することが望ほしい。It is desirable to use glass having almost the same refractive index as the diffraction grating 5 for the glass plate 13.
又、ガラス板2,13は面に於いては平行平面ガラス板
が示されているが、これに限らず曲面を有するものであ
っても良い。Further, although the glass plates 2 and 13 are shown as parallel plane glass plates, the present invention is not limited to this, and may have curved surfaces.
図から明らかな様に12の位置は遠く離れ再回折は生じ
ない、従って迷光は生じない。As is clear from the figure, the position 12 is far away and no re-diffraction occurs, so no stray light occurs.
又、回折格子3は直接空気に晒されないため、品質の劣
化を生ぜさせる恐れはない。Furthermore, since the diffraction grating 3 is not directly exposed to air, there is no risk of quality deterioration.
尚、本実施例において、、回折格子3を2枚の平行平面
ガラス板で挾持した場合を説明したが、回折格子3とほ
ぼ同一のガラス板中に封入しても同様の効果を有するも
のである。In this embodiment, the case where the diffraction grating 3 is sandwiched between two parallel plane glass plates has been described, but the same effect can be obtained even if the diffraction grating 3 is enclosed in almost the same glass plate as the diffraction grating 3. be.
又更に本実施例に於いて、回折光10が出射側の境界面
4の方向に進行する様に説明したが、入射面側の境界面
5′の方向に進行する様にしても良い。Further, in this embodiment, the diffracted light 10 is described as traveling in the direction of the boundary surface 4 on the exit side, but it may be made to travel in the direction of the boundary surface 5' on the incident surface side.
この様にするには、第3図に示す様に入射光8に対して
、回折格子3の格子構造の傾き角を大きくすれば良い。To achieve this, the inclination angle of the grating structure of the diffraction grating 3 with respect to the incident light 8 may be increased as shown in FIG.
第4図に示した第3実施例は、本発明の最も好ましい実
施例である。The third embodiment shown in FIG. 4 is the most preferred embodiment of the invention.
この実施例では、回折格子3の接着剤14によって、完
全に密封され、外気に晒されることが無い上、更にガラ
ス板2,3の結合状態を強固にしている。In this embodiment, the adhesive 14 of the diffraction grating 3 completely seals the diffraction grating 3 so that it is not exposed to the outside air, and further strengthens the bonding state between the glass plates 2 and 3.
第5図は、本発明の光分割器に使用する回折体の最も好
ましい作成方法を示す図である。FIG. 5 is a diagram showing the most preferable method for producing a diffraction material used in the light splitter of the present invention.
15はレーザーチューブ等のコヒーレント光源である。15 is a coherent light source such as a laser tube.
16はビームエキスパンダー、17はビームスプリッタ
ー、18.19は該ビームスプリッターによって2分割
されたコヒーレント光束、20は反射ミラーである。16 is a beam expander, 17 is a beam splitter, 18 and 19 are coherent light beams divided into two by the beam splitter, and 20 is a reflecting mirror.
21,22はほぼ等しい屈折率のプリズムである。21 and 22 are prisms having approximately the same refractive index.
このプリズム21,22の間にはガラス基板23に塗布
された感光剤24が挾まれている。A photosensitive agent 24 coated on a glass substrate 23 is sandwiched between the prisms 21 and 22.
尚、ガラス基板23は先に説明した平行平面ガラス板2
として使用出来るものが望ましく又、この屈折率はプリ
ズム21 .22とほぼ等しい。Note that the glass substrate 23 is the parallel plane glass plate 2 described earlier.
It is desirable that the prism can be used as the prism 21. Almost equal to 22.
又、感光材24は、体積型ホログラムが作成可能な様に
十分厚く塗布されていることが望ましく、又感光剤とし
てはダイクロメーテイドゼラチン又はホトポリマーの如
く位相型ホログラムが作成可能であるものが望ましい。The photosensitive material 24 is preferably coated sufficiently thickly so that a volume hologram can be created, and the photosensitive material is preferably one that can create a phase hologram, such as dichromated gelatin or a photopolymer. .
又、更に、プリズム21.22の間に空気層が形成され
ることを除くため、各光学ガラス等と等しい屈折率の液
体を2つのプリズム21,22の間に浸すことが望まれ
る。Furthermore, in order to eliminate the formation of an air layer between the prisms 21 and 22, it is desirable to immerse a liquid having the same refractive index as each optical glass or the like between the two prisms 21 and 22.
ビームスプリッター17によって分割された一方のコヒ
ーレント光束18はガラス基板23を透過する様に指向
され、もう一方のコヒーレント光束19はミラー20に
よってガラス基板23の上面に対して全反射角度で指向
される。One coherent light beam 18 split by the beam splitter 17 is directed so as to pass through the glass substrate 23, and the other coherent light beam 19 is directed by the mirror 20 at an angle of total reflection to the upper surface of the glass substrate 23.
この様にして、ホログラフィックに回折体一作成される
。In this way, a holographic diffractive material is created.
又、第6図には第5図と.異なる回折格子の作成方法が
示されている。Also, Figure 6 shows Figure 5 and . Different methods of making diffraction gratings are shown.
この方法の異なる点は第5図の方法に比べて、コヒーレ
ント光束19の光路中にシリンドリカルレンズ25が入
っている点である。This method differs from the method shown in FIG. 5 in that a cylindrical lens 25 is included in the optical path of the coherent light beam 19.
このシリンドリカルレンズ25によって、第7図に示す
様に光束19は将来受光素子7が配される位置に集束さ
れ、その後発散する。As shown in FIG. 7, the cylindrical lens 25 focuses the light beam 19 on a position where the light receiving element 7 will be placed in the future, and then diverges.
従って、この様なシリンドリカルレンズを使用して作成
した回折格子を光分割器に使用した場合集光レンズなし
で、受光器上に回折光を集光出来るという利点を有して
いる。Therefore, when a diffraction grating made using such a cylindrical lens is used as a light splitter, it has the advantage that diffracted light can be focused on a light receiver without a focusing lens.
尚、26は光吸収物質である。Note that 26 is a light absorbing substance.
第1図は先行技術の光分割器を示す図、第2図は本発明
に係る光分割器の第1実施例を示す図、第3図は第2実
施例を示す図、第4図は第3実施例を示す図、第5図は
本発明に使用する回折体の最も良い作成方法を示す図、
第6,7図は第5図と異なる作成方法を示す図である。
図中、1は光分割器、2は平行平面ガラス板、3は回折
格子、4,5は境界面、6は出射面、7は受光素子、8
は光線、9は非回折光、10は回折光、11,12は再
回折が生じる位置、13は平行平面ガラスである。FIG. 1 shows a prior art light splitter, FIG. 2 shows a first embodiment of a light splitter according to the present invention, FIG. 3 shows a second embodiment, and FIG. A diagram showing the third embodiment, FIG. 5 is a diagram showing the best method for producing the diffraction material used in the present invention,
FIGS. 6 and 7 are diagrams showing a production method different from that in FIG. 5. In the figure, 1 is a light splitter, 2 is a parallel plane glass plate, 3 is a diffraction grating, 4 and 5 are boundary surfaces, 6 is an output surface, 7 is a light receiving element, 8
9 is a light beam, 9 is a undiffracted light, 10 is a diffracted light, 11 and 12 are positions where re-diffraction occurs, and 13 is a parallel plane glass.
Claims (1)
マッチング作用を有する屈折率の接着剤で光学的に密着
状態で挾持させ、一方の側を入射面、他方の側を出射面
とし、前記入射面から入射した光束を前記回折格子によ
って非回折光と回折光に分離し、非回折光を出射面から
射出させ、回折光を前記入射面若しくは出射面によって
全反射させ受光器に導びくことを特徴とする光分割器。1 A diffraction grating is sandwiched between two plate-shaped optical members in a state of optical close contact with an adhesive having a refractive index that has an index matching effect, one side is used as an incident surface, the other side is used as an output surface, and the above-mentioned Separating the light beam incident from the incident surface into undiffracted light and diffracted light by the diffraction grating, emitting the undiffracted light from the exit surface, and totally reflecting the diffracted light by the entrance surface or the exit surface and guiding it to the light receiver. A light splitter featuring:
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50068766A JPS583201B2 (en) | 1975-06-06 | 1975-06-06 | Hikari Bun Katsuki |
| US05/691,628 US4103153A (en) | 1975-06-06 | 1976-06-01 | Device for measuring light incident on an image forming optical system |
| US05/869,447 US4178084A (en) | 1975-06-06 | 1978-01-16 | Device for measuring light incident on an image forming optical system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50068766A JPS583201B2 (en) | 1975-06-06 | 1975-06-06 | Hikari Bun Katsuki |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS51144635A JPS51144635A (en) | 1976-12-11 |
| JPS583201B2 true JPS583201B2 (en) | 1983-01-20 |
Family
ID=13383174
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50068766A Expired JPS583201B2 (en) | 1975-06-06 | 1975-06-06 | Hikari Bun Katsuki |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS583201B2 (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5625652B2 (en) * | 1972-12-11 | 1981-06-13 |
-
1975
- 1975-06-06 JP JP50068766A patent/JPS583201B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS51144635A (en) | 1976-12-11 |
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