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JPH0330843B2 - - Google Patents
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JPH0330843B2 - - Google Patents

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Publication number
JPH0330843B2
JPH0330843B2 JP56141222A JP14122281A JPH0330843B2 JP H0330843 B2 JPH0330843 B2 JP H0330843B2 JP 56141222 A JP56141222 A JP 56141222A JP 14122281 A JP14122281 A JP 14122281A JP H0330843 B2 JPH0330843 B2 JP H0330843B2
Authority
JP
Japan
Prior art keywords
scanning
laser beam
laser diode
scanning direction
plane
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
Application number
JP56141222A
Other languages
Japanese (ja)
Other versions
JPS5842025A (en
Inventor
Iwao Hamaguchi
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP56141222A priority Critical patent/JPS5842025A/en
Publication of JPS5842025A publication Critical patent/JPS5842025A/en
Publication of JPH0330843B2 publication Critical patent/JPH0330843B2/ja
Granted legal-status Critical Current

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  • Dot-Matrix Printers And Others (AREA)
  • Laser Beam Printer (AREA)
  • Mechanical Optical Scanning Systems (AREA)
  • Exposure Or Original Feeding In Electrophotography (AREA)
  • Facsimile Scanning Arrangements (AREA)
  • Fax Reproducing Arrangements (AREA)

Description

【発明の詳細な説明】 本発明は画像記録装置に関するものである。[Detailed description of the invention] The present invention relates to an image recording device.

光源としてレーザーダイオードを使用している
画像記録装置において、従来、第1図に示すよう
にレーザーダイオード1の接合面の方向S−Sを
走査面2上の主走査方向xに対し平行若しくは垂
直(副走査方向yと同方向)になる様対応させて
配置する技術が知られている。具体的には、例え
ば、 第2図に示す如く、レーザーダイオード1から
のレーザー光束は、結合レンズ3、プリズム7、
スリツト4、回転ミラー5、f・θレンズ6等の
光学系を介して走査面2上に副走査方向yに長軸
を合致させた楕円スポツトとして結像される(第
3図d参照)。
In an image recording apparatus that uses a laser diode as a light source, conventionally, as shown in FIG. A technique for arranging them in correspondence with each other in the same direction as the sub-scanning direction y is known. Specifically, for example, as shown in FIG. 2, the laser beam from the laser diode 1 is transmitted through a coupling lens 3, a prism 7,
An image is formed on the scanning surface 2 as an elliptical spot whose major axis coincides with the sub-scanning direction y through an optical system including a slit 4, a rotating mirror 5, an f/θ lens 6, etc. (see FIG. 3d).

なお、第2図において、レーザー光束の光軸L
上であつて、、、で示す各部位で
のレーザー光束の、光軸直交方向における切断面
での概形は各々第3図におけるa,b,c,dに
対応し、この例におけるレーザーダイオード1の
接合面の方向S−Sは主走査方向xに対応させて
配置されている。
In addition, in FIG. 2, the optical axis L of the laser beam
Above, the general shape of the laser beam at each location indicated by , , on the cut plane in the direction perpendicular to the optical axis corresponds to a, b, c, and d in FIG. 3, respectively, and the laser diode in this example The direction S-S of the joint surface of No. 1 is arranged to correspond to the main scanning direction x.

レーザーダイオード1の配置形態としては、上
記例の他に、前記した如く、接合面の方向S−S
を副走査方向yに合わせて配置する場合もある
が、この場合においても、プリズム7を光学的性
能の異なる他のプリズムと交換すること等によ
り、最終的に走査面2に結像されるレーザー光束
は、第3図dに示す如く、副走査方向yに長軸を
合致させた楕円スポツトに整えられる。
In addition to the above example, the laser diode 1 may be arranged in the direction S-S of the junction surface, as described above.
In some cases, the prism 7 is arranged in alignment with the sub-scanning direction y, but even in this case, by replacing the prism 7 with another prism with different optical performance, etc., the laser image finally formed on the scanning surface 2 can be adjusted. The light beam is arranged into an elliptical spot whose long axis coincides with the sub-scanning direction y, as shown in FIG. 3d.

このように、楕円スポツトの長軸を副走査方向
yに合致させているのは、ガルバノミラーや回転
ミラー5等の機械式走査装置におけるミラー軸
の、回動時の倒れ傾向の変動に伴なう走査ライン
のピツチむらへの影響を極力少なくするための配
慮である。
In this way, the reason why the long axis of the elliptical spot is aligned with the sub-scanning direction y is due to the fluctuation in the tendency of the mirror axis of mechanical scanning devices such as the galvanometer mirror and rotating mirror 5 to fall when rotated. This is a consideration to minimize the influence on pitch unevenness of scanning lines.

ところで、上記の要請からレーザーダイオード
1の接合面の方向S−Sの主走査方向yと平行若
しくは、垂直になる様にレーザーダイオード1を
配置する場合、いずれの配置形態においても回転
ミラー5の反射率には入射角依存性が認められ、
回転ミラー5の回転に伴なう入射角の変動に応じ
て露光むらを生ずるという欠点がある。
By the way, in view of the above requirements, when the laser diode 1 is arranged parallel to or perpendicular to the main scanning direction y in the direction S-S of the junction surface of the laser diode 1, the reflection of the rotating mirror 5 is The incidence angle dependence is recognized in the rate,
There is a drawback that exposure unevenness occurs in response to fluctuations in the angle of incidence as the rotating mirror 5 rotates.

例えば、アルミニウムの複素屈折率をn−ik
(n=1.9、k=7.0)とするとき入射面と平行成
分の反射率Rpと、垂直な成分の反射率Rsは、次
式(1)、(2)で表わすことができる。
For example, the complex refractive index of aluminum is n-ik
(n=1.9, k=7.0), the reflectance R p of the component parallel to the incident plane and the reflectance R s of the component perpendicular to the plane of incidence can be expressed by the following equations (1) and (2).

Rp=(n2+k2)cos2θ−2ncosθ+1/(n2+k2)cos
2θ+2ncosθ+1……(1) Rs=(n2+k2)−2ncosθ+cos2/(n2+k2)+2ncos
θ+cos2θ……(2) (但し、θは入射角とする) 上記各式(1)、(2)を計算した結果が第5図のグラ
フであり、通常機械式走査装置の反射面はアルミ
ニウム蒸着面であるので、第5図に示す反射率に
従う。そして、レーザーダイオードからのレーザ
ー光束は、その接合面の方向に直線偏光している
ので、レーザーダイオードの配置形態、例えば接
合面の方向を主走査方向に合わせるか又は副走査
方向に合わせることにより、第5図に示すRs
Rpかのいずれか一方のみの反射率特性に従うこ
とになる。例えば、光学レイアウト上、第4図に
示す如く、回転ミラー5へのレーザー光束の平均
入射角δは45°前後を使用する場合が多く、この
為レーザー光束の入射角は45°±15°程度の範囲内
で変動し、反射率も変動するので走査面2上で露
光むらを生じる。
R p = (n 2 + k 2 ) cos 2 θ−2n cos θ + 1/(n 2 + k 2 ) cos
2 θ + 2 n cos θ + 1……(1) R s = (n 2 + k 2 ) − 2 n cos θ + cos 2 / (n 2 + k 2 ) + 2 n cos
θ+cos 2 θ……(2) (However, θ is the angle of incidence) The result of calculating each formula (1) and (2) above is the graph in Figure 5, and the reflective surface of a mechanical scanning device is usually Since it is an aluminum vapor-deposited surface, the reflectance shown in FIG. 5 is followed. Since the laser beam from the laser diode is linearly polarized in the direction of its junction surface, by adjusting the arrangement of the laser diode, for example, by aligning the direction of the junction surface with the main scanning direction or the sub-scanning direction, R s shown in Figure 5?
It follows the reflectance characteristics of only one of R p . For example, due to the optical layout, as shown in Fig. 4, the average incident angle δ of the laser beam onto the rotating mirror 5 is often around 45°, so the incident angle of the laser beam is about 45°±15°. Since the reflectance varies within the range of , and the reflectance also varies, exposure unevenness occurs on the scanning surface 2.

このことは、反射面としてアルミニユウム蒸着
面を有する回転ミラー5に限らず、他の反射面、
例えばAl蒸着膜+保護膜とか、Al蒸着膜+SiO2
+TiO2或いは、誘電体多層膜による反射面を有
する機械式走査装置等においても同様な傾向を示
す。
This is true not only for the rotating mirror 5 having an aluminum vapor-deposited surface as a reflective surface, but also for other reflective surfaces,
For example, Al vapor deposited film + protective film, Al vapor deposited film + SiO 2
A similar tendency is shown in mechanical scanning devices having a reflective surface made of +TiO 2 or a dielectric multilayer film.

ところで、このような、入射角依存性の強い機
械式走査装置であつても、レーザーダイオードの
接合面の方向が、主走査方向に45°となる様に配
置すれば、その反射率特性は第5図に破線で示す
如く入射角依存性がなくなり、露光むらは解消さ
れる。
By the way, even with such a mechanical scanning device that is highly dependent on the incident angle, if the direction of the junction surface of the laser diode is arranged at 45 degrees to the main scanning direction, its reflectance characteristics will be as follows. As shown by the broken line in FIG. 5, the dependence on the incident angle is eliminated and the exposure unevenness is eliminated.

しかし、その反面、走査面2上での走査スポツ
トも、主走査方向xに対して45°傾いた楕円とな
つてしまい、この為、機械式走査装置におけるミ
ラー軸の回動時の倒れ傾向の変動に伴なう走査ラ
インのピツチむらの影響を受け易くなり印字品質
が低下してしまう。
However, on the other hand, the scanning spot on the scanning surface 2 also becomes an ellipse inclined at 45 degrees with respect to the main scanning direction This makes it susceptible to the unevenness of the pitch of the scanning line due to fluctuations, resulting in a decrease in print quality.

本発明は上記の事情に着目してなされたもの
で、光源としてレーザーダイオードを使用し、走
査面上での露光スポツト形状を副走査方向に長軸
を有する楕円スポツトとし、且つ、露光むらの少
ない画像記録装置を提供することを目的とする。
The present invention has been made in view of the above circumstances, and uses a laser diode as a light source, makes the exposure spot shape on the scanning surface an elliptical spot having a long axis in the sub-scanning direction, and has less uneven exposure. The purpose is to provide an image recording device.

以下、本発明を詳細に説明する。 The present invention will be explained in detail below.

本発明に係る画像記録装置は、反射面を回転若
しくは揺動させて走査する機械式走査装置とレー
ザーダイオードとの間に、レーザー光束の偏光方
向が、前記機械式走査装置の走査方向に対し、略
45°になるように偏光面を回転させて前記機械式
走査装置に入射させる光学素子又はレーザー光束
の直接偏光を円若しくは楕円偏光に変換して前記
機械式走査装置に入射させる光学素子を配置した
ことを特徴とする。
The image recording device according to the present invention is provided between a laser diode and a mechanical scanning device that scans by rotating or swinging a reflective surface, such that the polarization direction of the laser beam is relative to the scanning direction of the mechanical scanning device. omitted
An optical element is arranged that rotates the plane of polarization to 45° and causes it to enter the mechanical scanning device, or an optical element that converts the direct polarization of the laser beam into circular or elliptical polarization and makes it enter the mechanical scanning device. It is characterized by

第6図に、本発明の一実施例としての画像記録
装置を示す。
FIG. 6 shows an image recording apparatus as an embodiment of the present invention.

図において、符号1はレーザーダイオードを、
符号2は走査面を示し、上記両者間には、レーザ
ーダイオード1に近い順から、結合レンズ3、ビ
ーム整形光学形8、光学素子9、回転ミラー5、
f・θ光学系10等が配置されている。
In the figure, numeral 1 indicates a laser diode,
Reference numeral 2 indicates a scanning plane, and between the two, in order of proximity to the laser diode 1, a coupling lens 3, a beam shaping optical shape 8, an optical element 9, a rotating mirror 5,
An f/θ optical system 10 and the like are arranged.

図の例では、レーザーダイオード1の接合面の
方向S−Sは走査面2上で、主走査方向xに対応
して配置され、レーザー光束はプリズムやシリン
ドリカルレンズ等により構成されたビーム整形光
学系8によつて走査面2上で副走査方向yに長軸
を有する楕円のスポツトとして結像される。仮に
レーザーダイオード1の接合面の方向S−Sが走
査面2上で、副走査方向yに対応して配置されて
いる場合でもレーザー光束は走査面2上で副走査
方向yに長軸を有する楕円のスポツトとして結像
される。
In the example shown in the figure, the direction S-S of the junction surface of the laser diode 1 is arranged on the scanning surface 2, corresponding to the main scanning direction 8, the spot is imaged on the scanning plane 2 as an elliptical spot having its major axis in the sub-scanning direction y. Even if the junction surface direction S-S of the laser diode 1 is arranged on the scanning surface 2 and corresponds to the sub-scanning direction y, the laser beam has a long axis on the scanning surface 2 in the sub-scanning direction y. The image is formed as an elliptical spot.

第6図において、レーザー光束は、回転ミラー
5に入射される以前に、位相差をλ/2とするよう
な結晶板である光学素子9を通過することによ
り、該レーザー光束の偏光方向が主走査方向に対
してほぼ45°の傾きを有する様に回転するので、
その反射率特性は第5図に破線で示す如き特性と
なり、入射角の変動に伴なう反射率の変動は解消
される。
In FIG. 6, before the laser beam is incident on the rotating mirror 5, it passes through an optical element 9, which is a crystal plate with a phase difference of λ/2, so that the main polarization direction of the laser beam is changed. Since it rotates at an angle of approximately 45° to the scanning direction,
The reflectance characteristics are as shown by the broken line in FIG. 5, and variations in reflectance due to variations in the angle of incidence are eliminated.

なお、光学素子9としては、前記、位相差を
λ/2とする結晶に代えてレーザー光束の直線偏光
を円若しくは楕円偏光に変換させるところの位相
差をλ/4とする結晶板を使用してもよく、同等の
効果を得ることができる。
As the optical element 9, a crystal plate having a phase difference of λ/4 for converting the linearly polarized light of the laser beam into circular or elliptically polarized light may be used instead of the above-mentioned crystal having a phase difference of λ/2. You can also obtain the same effect.

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

第1図は走査方向とレーザーダイオードの接合
面の方向との関係を説明した図、第2図は画像記
録装置の光学系の構成を説明した図、第3図は第
2図中の光軸上でのビーム断面形状及び大きさを
説明した図、第4図は回転ミラーの回転に伴なう
入射角の変動について説明した図、第5図はアル
ミニユウム反射面における入射角と反射率との関
係を説明した図、第6図は本発明の一実施例とし
ての画像記録装置の主要構成を示す斜視図であ
る。 5……(機械式走査装置の一例としての)回転
ミラー、9……光学素子。
Figure 1 is a diagram explaining the relationship between the scanning direction and the direction of the junction surface of the laser diode, Figure 2 is a diagram explaining the configuration of the optical system of the image recording device, and Figure 3 is the optical axis in Figure 2. Figure 4 is a diagram explaining the cross-sectional shape and size of the beam mentioned above, Figure 4 is a diagram explaining the variation of the incident angle due to the rotation of the rotating mirror, and Figure 5 is a diagram explaining the relationship between the incidence angle and the reflectance on the aluminum reflecting surface. FIG. 6, which is a diagram explaining the relationship, is a perspective view showing the main structure of an image recording apparatus as an embodiment of the present invention. 5... Rotating mirror (as an example of a mechanical scanning device), 9... Optical element.

Claims (1)

【特許請求の範囲】 1 光源にレーザーダイオードを使用していて、
このレーザーダイオードを、その接合面の方向が
走査面上の主走査方向に平行若しくは垂直になる
様に対応させて配置し、前記接合面の方向が走査
面上の主走査方向に平行若しくは垂直の何れの場
合でも、前記レーザーダイオードから前記走査面
までの間に設けた光学系の性質により、最終的に
前記走査面に結像されるレーザー光束を副走査方
向に長軸を合致させた楕円スポツトとなしている
画像記録装置において、 反射面を回転若しくは揺動させて走査する機械
式走査装置とレーザーダイオードとの間に、レー
ザー光束の偏光方向が、前記機械式走査装置の走
査方向に対し、略45°になるように偏光面を回転
させて前記機械式走査装置に入射させる光学素子
又はレーザー光束の直線偏光を円若しくは楕円偏
光に変換して前記機械式走査装置に入射させる光
学素子を配置したことを特徴とする画像記録装
置。
[Claims] 1. A laser diode is used as a light source,
The laser diodes are arranged so that the direction of the bonded surface is parallel or perpendicular to the main scanning direction on the scanning surface, and the direction of the bonded surface is parallel or perpendicular to the main scanning direction on the scanning surface. In either case, due to the properties of the optical system provided between the laser diode and the scanning surface, the laser beam that is finally imaged on the scanning surface is formed into an elliptical spot whose long axis coincides with the sub-scanning direction. In an image recording device, between a laser diode and a mechanical scanning device that scans by rotating or swinging a reflective surface, the polarization direction of the laser beam is such that the direction of polarization of the laser beam is different from the scanning direction of the mechanical scanning device. Arrangement of an optical element that rotates the plane of polarization to approximately 45° and causes the plane to enter the mechanical scanning device, or an optical element that converts linearly polarized light of the laser beam into circular or elliptically polarized light and causes the plane to enter the mechanical scanning device. An image recording device characterized by:
JP56141222A 1981-09-08 1981-09-08 image recording device Granted JPS5842025A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56141222A JPS5842025A (en) 1981-09-08 1981-09-08 image recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56141222A JPS5842025A (en) 1981-09-08 1981-09-08 image recording device

Publications (2)

Publication Number Publication Date
JPS5842025A JPS5842025A (en) 1983-03-11
JPH0330843B2 true JPH0330843B2 (en) 1991-05-01

Family

ID=15286958

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56141222A Granted JPS5842025A (en) 1981-09-08 1981-09-08 image recording device

Country Status (1)

Country Link
JP (1) JPS5842025A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE8331822U1 (en) * 1983-11-07 1984-02-09 Werner H.K. Peters Maschinenfabrik Gmbh, 2000 Hamburg SINGLE-SIDED CARDBOARD MACHINE
JPH0612383B2 (en) * 1984-09-27 1994-02-16 富士ゼロックス株式会社 Optical beam recorder
JPH0611521B2 (en) * 1985-05-27 1994-02-16 アイキ工業株式会社 Method and apparatus for producing single-sided corrugated paper
DE69232124T2 (en) 1991-05-14 2002-03-14 Seiko Epson Corp., Tokio/Tokyo Image forming apparatus

Also Published As

Publication number Publication date
JPS5842025A (en) 1983-03-11

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