JPS58113909A - Optical scanner - Google Patents

Optical scanner

Info

Publication number
JPS58113909A
JPS58113909A JP56211976A JP21197681A JPS58113909A JP S58113909 A JPS58113909 A JP S58113909A JP 56211976 A JP56211976 A JP 56211976A JP 21197681 A JP21197681 A JP 21197681A JP S58113909 A JPS58113909 A JP S58113909A
Authority
JP
Japan
Prior art keywords
scanning
hologram
hologram disk
disk
point
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.)
Pending
Application number
JP56211976A
Other languages
Japanese (ja)
Inventor
Kazuo Nishi
西 和郎
Shinji Yamato
大和 真二
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 Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56211976A priority Critical patent/JPS58113909A/en
Publication of JPS58113909A publication Critical patent/JPS58113909A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B26/00Optical devices or arrangements for the control of light using movable or deformable optical elements
    • G02B26/08Optical devices or arrangements for the control of light using movable or deformable optical elements for controlling the direction of light
    • G02B26/10Scanning systems
    • G02B26/106Scanning systems having diffraction gratings as scanning elements, e.g. holographic scanners

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Diffracting Gratings Or Hologram Optical Elements (AREA)
  • Facsimile Scanning Arrangements (AREA)
  • Mechanical Optical Scanning Systems (AREA)

Abstract

PURPOSE:To form easily a scanning pattern having a scanning line of the multi- direction by one hologram disk, by providing plural light sources at each different angle position against the hologram disk. CONSTITUTION:A light beam emitted from the first semiconductor laser 20 which is a light source is converted to the first incident beam 22, is diffracted and condensed, and is condensed to a point P on a scanning surface 8. When a hologram disk 1 is rotated, a scanning beam generated in order is deflected in the direction being parallel to a tangent of the hologram disk 1. As a result, a scanning pattern 25 of the number which is equal to that of the hologram lens is generated. Subsequently, optical beams emitted by the second and the third light sources 30, 40 also generate the second and the third scanning patterns 35, 45 having a direction being parallel to a tangent in points Q', Q'' on the disk 1 in the same way. In this way, it is possible to easily form a scanning pattern of a scanning line of the multi-direction by one hologram disk.

Description

【発明の詳細な説明】 この発明け、ホログラムスキャナにより霞ビームを偏向
かつ集光して、走査向上を光スポットが走査する光走査
装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical scanning device in which a hologram scanner deflects and focuses a haze beam so that a light spot scans the scanning area.

従来この唾の装置4としてオ1図に示すものがあった。Conventionally, there has been a saliva device 4 shown in Fig. 1.

図において、…はホログラムディスク、(21はホログ
ラムディスクfil上に記録された任意の1つのホログ
ラムレンズである。ホログラムレンズは、その個数が発
生すべき走査線数と汁しく、また、各・rその中心が走
査線ピッチに肘おした所だけホログラムディスク(1)
の半径方向に変位されて記録されている。(3)け入射
ビーム、141 。
In the figure, ... is a hologram disk, (21 is an arbitrary hologram lens recorded on the hologram disk fil.The number of hologram lenses corresponds to the number of scanning lines to be generated, and each r Hologram disk (1) only where its center touches the scanning line pitch
is recorded as being displaced in the radial direction. (3) Incident beam, 141.

(6)はそれぞれ空間的に分離した位置に回折されたオ
l、オ8の走査ビーム+ 1611 (7’はそれぞれ
走査ビーム141 、151を反射する平面鏡、+81
#−i走査面* [91、nuは・それぞれ走査ビーム
41 、 fIIllにより発生される走査線、 (u
) Hホログラムディスク・11を同転させるモータで
ある。
(6) are the scanning beams of O1 and O8 +1611 which are diffracted to spatially separated positions, respectively (7' is a plane mirror that reflects the scanning beams 141 and 151, respectively;
#−i scanning plane * [91, nu is the scanning line generated by the scanning beam 41, fIIll, respectively, (u
) This is a motor that simultaneously rotates the H hologram disk 11.

次に動作について説明する。Next, the operation will be explained.

ホログラムレンズ(21上の屯Qに1.+4Qを点光源
とする入射ビーム131を入射点せ、ホログラムディス
ク+11をモータ(It)により駆動回転させる。
An incident beam 131 with 1.+4Q as a point light source is set at the point Q on the hologram lens (21), and the hologram disk +11 is driven and rotated by a motor (It).

各ホログラムレンズにより用1次走斤ビームか争生され
るが、これらの内代表的なものがオ鳳。
The primary traveling beam is generated by each hologram lens, but the most representative one is the Oho beam.

第2の走査ビーム+41 、 t51である。これらの
圭介ビームは、各ホログラムレンズの中心がf位してい
るため、ホログラムディスク+11の点Qにおける接線
方向と垂直な方向にシフトして偏向され、ホログラムレ
ンズの個数と等しい数の暇に平行な走査線を発生する。
The second scanning beam is +41, t51. Since the center of each hologram lens is at position f, these Keisuke beams are shifted and deflected in a direction perpendicular to the tangential direction at point Q of the hologram disk +11, and are deflected in parallel to a number of holes equal to the number of hologram lenses. generates a scan line.

ここで、上記走査線の方向をy化させるための平面鏡の
9定を容易1でするため、全走斤ビームは2つのグルー
プに分け、空間的に分帷した位1直に発生する。
Here, in order to easily reduce the 9 constant of the plane mirror for changing the direction of the scanning line to y, the entire scanning beam is divided into two groups, and each group is spatially divided to generate one direct beam.

次に、オlの走査ビーム(41で代表される走査ビーム
は所定の角斥9位置に、設定されたオlの平面鏡(6)
によ、り反射され、走査面(8)上で走査パターン(9
)を形成する。また同様に、オ8.の走査ビーム(6)
で代表される走査ビームは第2の乎面槻(71により反
射され、走査パターンttci、を発生する。以上の結
果、2つの走査方向を有する走査パターンが形成される
Next, the scanning beam (represented by 41) is placed at a predetermined angle angle 9 position by the plane mirror (6) of
is reflected by the scanning pattern (9) on the scanning surface (8).
) to form. Similarly, O8. scanning beam (6)
The scanning beam, represented by , is reflected by the second mirror 71 to generate a scanning pattern ttci. As a result of the above, a scanning pattern having two scanning directions is formed.

従来の光走査装置は以上のように構成されているので、
多方向の走査方向を有する走査パターンを発生する場合
、少なくとも必要とする方向数だけの平面鏡を設定する
春型があり、溝・戊が々鰯となり、走査方向の増加に限
界がある等の欠点があった。
Since the conventional optical scanning device is configured as described above,
When generating a scanning pattern with multiple scanning directions, there is a spring type in which plane mirrors are set up in at least as many directions as required, and there are drawbacks such as grooves and sardines, and a limit to the increase in the number of scanning directions. was there.

一定数の走査線を必要とする走査方向数−分割しなけれ
ばならず、各走査方向の走査線数が減少する欠点があっ
た。
A certain number of scanning lines must be divided in the number of scanning directions, which has the disadvantage that the number of scanning lines in each scanning direction is reduced.

この発明は上記のような従来のものの欠点を除去するた
めになされたもので、複数の光源を用いて、同一のホロ
グラムディスクより多方向の走査方向を有する走査パタ
ーンを容易に形成できる光走査装置を堤供することを目
的とする。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and provides an optical scanning device that can easily form a scanning pattern having multiple scanning directions from the same hologram disk using a plurality of light sources. The purpose is to provide.

以下、この発明の一実施例を図によって説明する。・ オ8図において、en 1m、 sに)は、それぞれオ
l。
Hereinafter, one embodiment of the present invention will be described with reference to the drawings.・In Figure 8, en 1m and s) are respectively Ol.

オ8.オ8の光源である半導体レーデ光源、211゜6
υ、(財)は、それぞれオ1.オ8.オ8の集光光学系
、暢、(至)、四は、それぞれ点0*aO’、点O“を
点光゛源とするオ1.第2.オ8の入射ビーム。
E8. Semiconductor radar light source, which is the light source of O8, 211°6
υ and (goods) are respectively O1. E8. The condensing optical system of O8, and 4 are the incident beams of O1, 2nd, and O8, with point 0*aO' and point O'' as point light sources, respectively.

、21 、01 、 IIG 、 #−!、それぞれオ
1.第2.オ8のホログラムレンズI 1241[有]
、(44け、キれぞれオl、オ8.オ8の走査ビーム、
919缶、に)は、それぞれオ1.第2.オ8の走憂パ
ターンである。
, 21 , 01 , IIG , #-! , respectively. Second. O8 hologram lens I 1241 [available]
, (44 digits, respectively O1, O8, and O8 scanning beams,
919 cans, 2) are each O1. Second. This is a running pattern for O8.

各走査パターン澱、(至)、(ハ)は走査面(8)上で
交差している。
Each of the scanning patterns lats, (to) and (c) intersect on the scanning plane (8).

次に仙作について説明す、る。光源である第1の半導体
レーザ(以後LDとよぶ)四から出射された光ビームは
集光光学系(211により点0を点光源とする第1の入
射ビーム(社)に変換される。
Next, I will explain about Sensaku. A light beam emitted from a first semiconductor laser (hereinafter referred to as LD) 4 serving as a light source is converted by a condensing optical system (211) into a first incident beam with point 0 as a point light source.

次に、入射ビーム器はホログラムレンズ1231の屯Q
に入射する。入射ビーム■は同折かつ集光されてオlの
走査ビーム、24となυ、走査面(8)上の点PK集光
される。ホログラムディスク+11を回転すると、各ホ
ログラムレンズにより順次発生される走査ビームは、Q
点におけるホログラムディスクfi+の接線と平行な方
向に偏向される。
Next, the incident beam device is the tun Q of the hologram lens 1231
incident on . The incident beam (2) is refracted and condensed into a scanning beam (24) and condensed at a point PK on the scanning surface (8). When the hologram disk +11 is rotated, the scanning beams sequentially generated by each hologram lens are Q
It is deflected in a direction parallel to the tangent to the hologram disk fi+ at the point.

この実施例に用いられる各ホログラムレンズの中心は、
ホログラムディスク+11の半径方向に変位させて記録
しであるので、その変位′@に対応して、各走査ビーム
は上記接線方向と垂直な方向にシフ)して偏向される。
The center of each hologram lens used in this example is
Since recording is performed by displacing the hologram disk +11 in the radial direction, each scanning beam is shifted and deflected in a direction perpendicular to the tangential direction, corresponding to the displacement '@.

以上の結果、ホログラムディスク+11上のホログラム
レンズの個Vと等しい数の互に平行な走査線を何する十
作、<ターフ12119が発生される。
As a result of the above, ten pieces of parallel scanning lines, <Turf 12119, having a number equal to the number of hologram lenses V on the hologram disk +11 are generated.

次に、第2.オ8の光源であるLD関、船により出射さ
れた光ビームも、上記と同様に、そ、れぞれ、点′1点
“を点光源する第2.第3の入射ビーム(ホ)、に)に
変換され、ホログラムディスクIl+の点Q、′9点“
に同時に入射する。第3.オ8の走査ビーム(2)、H
ld、ホログラムディスクill上の点Q′1点Q“に
おける接線と平行な方向を有する第2.オ8の走査パタ
ーン(イ)、(ハ)を発生する。
Next, the second. Similarly to the above, the light beams emitted by the LD and the ship, which are the light sources of E8, are the second and third incident beams (E), respectively, which are point light sources at point '1'. ), and the points Q and '9' of the hologram disk Il+
are simultaneously incident on the Third. Scanning beam (2) of O8, H
ld, point Q'1 on the hologram disk ill generate scanning patterns (a) and (c) of 2.o8 having a direction parallel to the tangent at point Q''.

以上のようにして、8方向の走1Kを何する十食パター
ンが形成される。例えば、ホログラムディスク上の点Q
1点Ql1点Q/rが正三角形の頂点の関係にあるとす
れば、走査泉の交角60°で3方向を有する走査パター
ンが?Uられる。
In the manner described above, a ten-eclipse pattern is formed in which the number of 1K runs in eight directions is determined. For example, point Q on the hologram disk
If 1 point Ql 1 point Q/r is in the relationship of the vertices of an equilateral triangle, what is the scanning pattern that has 3 directions with an intersection angle of 60° of scanning springs? U gets hit.

なお、上記実施例では、8方向の走査線をイ1する走査
パターンを発生する場合について示したが、8方向以上
の場合も、方向数だけの光源を用いることにより容易に
発生できることば明らかである。
In the above embodiment, a case was shown in which a scanning pattern with scanning lines in eight directions was generated, but it is clear that a scanning pattern in eight or more directions can be easily generated by using light sources as many as the number of directions. be.

また′、各走査線の交角が等しい場合を示したが、ホロ
グラムディスク照明点すなわち点Qを任意に、9定する
ことKより、任意の交角の゛走査線が発生できることは
言うまでもない。
Although the case where the intersecting angles of the scanning lines are equal has been shown, it goes without saying that scanning lines with arbitrary intersecting angles can be generated by arbitrarily setting the hologram disk illumination point, that is, the point Q.

以上Oように、この発明によればホログラムディスクに
対して互いに異なる角度位置に配設された複数の光源を
備え、各々の光源からの光ビームがホログラムディスク
の回転に伴ない互に嚇なった方向で走査・面を走査する
ので、1つのホログラムディスクによって多方向の走査
線を有する走査パターンが容易に形成で°きる。また、
走査系の構成が簡略化できる。
As described above, according to the present invention, a plurality of light sources are provided at different angular positions with respect to the hologram disk, and the light beams from each light source threaten each other as the hologram disk rotates. Since the surface is scanned in the direction, a scanning pattern having scanning lines in multiple directions can be easily formed using one hologram disk. Also,
The configuration of the scanning system can be simplified.

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

第1図は、従来の光走査装置を示す斜視図、第2図はこ
の発明の一実施例による光°走査装置を示す斜視図であ
る。 図において、111けホログラムディスク、(8)は走
査面、帷翰顛けそれぞれ光源−I(財)はホログラムレ
ンズを示す。 なお、図中、同一符号は同一、又は相当部分を示す。 代理人  葛 野  信 − 第1図 3 第2図
FIG. 1 is a perspective view showing a conventional optical scanning device, and FIG. 2 is a perspective view showing an optical scanning device according to an embodiment of the present invention. In the figure, number 111 is a hologram disk, (8) is a scanning surface, and the light source (I) is a hologram lens. In addition, in the figures, the same reference numerals indicate the same or equivalent parts. Agent Shin Kuzuno - Figure 1 3 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 光ビームを走査向上“に集光させかつ走査させるための
少なくとも1つのホログラムレンズを何し回転駆動され
るホログラムディスク、およびこのホログラムディスク
に対して斤いに異なる角度位置に配役された複数の光源
を備え、各々ρ光源からの光ビームが上記ホログラムデ
ィスクのto1転に伴ない斤いに異なった方向で上記走
査面を走査する光走査装置。
a hologram disc rotatably driven by at least one hologram lens for focusing and scanning a light beam; and a plurality of light sources disposed at different angular positions with respect to the hologram disc. An optical scanning device comprising: a light beam from each of the ρ light sources scans the scanning surface in different directions as the hologram disk rotates from one to the other.
JP56211976A 1981-12-26 1981-12-26 Optical scanner Pending JPS58113909A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56211976A JPS58113909A (en) 1981-12-26 1981-12-26 Optical scanner

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56211976A JPS58113909A (en) 1981-12-26 1981-12-26 Optical scanner

Publications (1)

Publication Number Publication Date
JPS58113909A true JPS58113909A (en) 1983-07-07

Family

ID=16614819

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56211976A Pending JPS58113909A (en) 1981-12-26 1981-12-26 Optical scanner

Country Status (1)

Country Link
JP (1) JPS58113909A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0206454A2 (en) * 1985-06-12 1986-12-30 Mitsubishi Denki Kabushiki Kaisha Stationary hologram scanner
JP2007214948A (en) * 2006-02-10 2007-08-23 Canon Inc Image reader

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52146523A (en) * 1976-05-31 1977-12-06 Fujitsu Ltd Light scanner
JPS5444552A (en) * 1977-09-14 1979-04-09 Fujitsu Ltd Information reader

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS52146523A (en) * 1976-05-31 1977-12-06 Fujitsu Ltd Light scanner
JPS5444552A (en) * 1977-09-14 1979-04-09 Fujitsu Ltd Information reader

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0206454A2 (en) * 1985-06-12 1986-12-30 Mitsubishi Denki Kabushiki Kaisha Stationary hologram scanner
JP2007214948A (en) * 2006-02-10 2007-08-23 Canon Inc Image reader

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