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JPH04934B2 - - Google Patents
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JPH04934B2 - - Google Patents

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Publication number
JPH04934B2
JPH04934B2 JP19948590A JP19948590A JPH04934B2 JP H04934 B2 JPH04934 B2 JP H04934B2 JP 19948590 A JP19948590 A JP 19948590A JP 19948590 A JP19948590 A JP 19948590A JP H04934 B2 JPH04934 B2 JP H04934B2
Authority
JP
Japan
Prior art keywords
lens
photoreceptor
optical
weight
spectral
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
Application number
JP19948590A
Other languages
Japanese (ja)
Other versions
JPH0375236A (en
Inventor
Susumu Seto
Akihiko Chokai
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.)
Canon Inc
Ohara Inc
Original Assignee
Canon Inc
Ohara Inc
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
Priority claimed from JP56124210A external-priority patent/JPS5825607A/en
Application filed by Canon Inc, Ohara Inc filed Critical Canon Inc
Priority to JP19948590A priority Critical patent/JPH0375236A/en
Publication of JPH0375236A publication Critical patent/JPH0375236A/en
Publication of JPH04934B2 publication Critical patent/JPH04934B2/ja
Granted legal-status Critical Current

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  • Exposure Or Original Feeding In Electrophotography (AREA)
  • Glass Compositions (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は照明光源によつて照明された物体の像
を感光体上に結像する光学系を含む投影装置であ
つて、照明光源から感光体の間の光路中に配置さ
れるレンズ系の少なくとも一枚のレンズが感光体
の分光感度特性を補償する分光透過率特性を有す
るレンズである投影装置に関する。 なお、本明細書でレンズとは、多層干渉薄膜等
を設けたものを含まず、純粋なレンズをいい、ま
た感光体とは、感光ドラム又は感光シート、
CCD等の固体撮像素子、ビジコン等の撮像管そ
の他を含むものである。 このレンズを有する投影装置は、複写機、フア
クシミリ、テレビカメラ等として用いられるが、
以下、複写機として用いる場合を例にとつて説明
する。 一般に複写機に用いられる感光体の分光感度特
性は比視感度特性と異なり、又、原稿を照明する
光源の分光波長特性と掛け合わせた分光特性も比
視感度特性と異なつているため原稿と異なつた濃
淡のコピーが得られてしまう。 例えば光源としてハロゲンランプを、また感光
体としてCdS系のものを用いると、ハロゲンラン
プでは通常使用されるフイラメント温度3000°K
前後で、その発光エネルギーは800乃至900nmの
赤外域に最大値を持ち、短波長側へ行くに従つて
一様に減少し、一方CdS感光体の分光感度は、近
赤外域で高いため、赤色域から近赤外域での露光
量が、青色、緑色等の他色域に比べ過多となる。
これにより複写画像において、原稿に書かれた赤
色の文字や図形が薄くなつたり、全く写らなくな
つたりする現象が生ずる。 一方セレン(Se)系の感光体と、短波長域で
の発光エネルギーの高い光源を用いると、CdS系
感光体とハロゲンランプを用いる場合とは逆に青
色の文字や図形が写り難くなる。 ところCdS系感光体と、短波長域での発光エネ
ルギーの高い光源を用いる場合又は、セレン系の
感光体と、ハロゲンランプを用いる場合にも如上
の問題が解決されないのが現状である。 このような比視感度特性と異なる分光特性(以
下、感色性という)は補償されて原稿と同様の濃
淡のコピーを得ることが望ましい。 これを解決する手段として従来、平板色フイル
タを用いるものと、特開昭52−60142号広報、実
開昭52−99331号公報等に知られる多層干渉薄膜
を用いるものがある。 これらは、所定波長域例えば前述のCdS系感光
体及びハロゲンランプの組合わせの系では近赤外
域の光を減衰させ、この領域での露光過多を防ぐ
ものである。 しかし、平板色フイルタを用いると、平行平面
の収差があり、またフイルタの部品を一点追加す
る構成によりコスト高となり、表面反射による光
量損失が大きくなるという欠点がある。 一方、多層干渉薄膜を用いると、一般に膜数が
多く蒸着工程でコスト高となり、各光学系の諸元
とりわけ入射角度によつて分光特性が変動し、更
に熱・湿度等に対して性能変化があり耐久性に乏
しいといつた欠点がある。 ところで従来、近赤外域の光を減衰させる熱線
吸収フイルタをスライドプロジエクタ用のコンデ
ンサレンズとして用いられることが知られている
が、これは単に昇温防止のためのもので以下に詳
述する本発明のような感光体の分光感度特性に合
わせた広い波長域での波長選択という点を何等、
示唆していない。更には所定の光学性能をもつた
結像レンズとして用いられているものではない。 本発明の第1の目的は、感光体の分光感度特性
を補償するレンズを有する投影装置を提供するこ
とにある。 また本発明の第2の目的は、色収差補正等、光
学設計上、都合の良い高屈折、高分散乃至低分散
性であり所定の分光透過率特性を有する波長選択
性のレンズ系を提供することにある。 更に本発明の第3の目的は、耐失透性に優れ、
高屈折、高分散乃至低分散性であり所定の分光透
過率特性を有する新規な光学ガラスを提供するこ
とにある。 本発明を用いれば従来に比べ安価でかつ安定し
た感色性の補償がなされる。 上述した本発明の目的は以下に述べる本発明の
投影装置により実現できる。 照明光源によつて照明された物体の像を感光体
上に結像する光学系を含む投影装置において、前
記照明光源と感光体の間の光路中に配置されるレ
ンズ系の少なくとも一枚のレンズが前記感光体の
分光感度特性を補償する分光透過率特性を有する
レンズであり、該レンズは重量%で、B2O325〜
40%、SiO20〜12%、ZrO20〜10%、La2O325〜
50%、Gd2O30〜5%、CaO0〜12%、BaO0〜10
%、ZnO0〜7%、Ta2O50〜5%、および、
WO30〜3%を含有するガラス100重量部に対し、
重量で、CeO2を0.1〜1%加えてなり、且つ屈折
率(nd)1.65〜1.85、アツベ数(νd)57〜45の範
囲の光学恒数を有する光学ガラスである投影装
置。 重量%で、B2O325〜40%、SiO20〜12%、
ZrO20〜10%、La2O325〜50%、Gd2O30〜5%、
CaO0〜12%、BaO0〜10%、ZnO0〜7%、
Ta2O50〜5%、および、WO30〜3%を含有す
るガラス100重量部に対し、重量%で、CeO2
0.1〜1%加えてなり、且つ屈折率(nd)1.65〜
1.85、アツベ数(νd)57〜45の範囲の光学恒数を
有する光学ガラス。 以下図面を用いて本発明の実施例を説明する。
第1図は本発明を用いた複写機の概略図である。
原稿面1は照明用の光源2によつて照射され、そ
のスリツト領域からの光が原稿面1に平行に2対
1の速度比で移動する走査ミラー3,4によつて
固定された結像レンズ5に入射され、この結像レ
ンズ5によつて固定ミラー6,7を介し、矢印方
向に移動する感光体8上にスリツト状に投影され
ていく。 本実施例において波長選択性の光学ガラスは、
結像レンズ5に用いられている。 第2図は光源の分光波長特性、感光体の分光感
度特性、結像レンズの分光透過率特性を示す。こ
こで光源としてハロゲンランプ、感光体として
Seを用いる系を示す。 これら3つの特性を掛け合わせた、いわゆる相
乗効果として図中、破線で示される如く、比視感
度特性に近い分光特性が得られる。言い換えれ
ば、この比視感度特性に近い特性となるようレン
ズ系の分光透過率特性が定められる。 感光体としてSe系を、また照明光源としてハ
ロゲンランプを用いる場合レンズとして第2図に
示されるような分光透過率特性が必要とされる。
これによつて、総合分光感度特性として比視感度
特性に近いものが得られる。そこで、上記目的の
レンズに対し、比較的高屈折低分散性を有し、
400nm附近に吸収端があつて400〜500nmの波長
域において急激に光線吸収性が減少し、500〜
700nmの波長域において優れた光線透過性を示
し、かつ、耐失透性に優れたガラスが要望され
る。本発明において、上記の要望に対し極めて好
適であり、しかも新規である光学ガラスを提案す
る。すなわち、このガラスは、酸化性雰囲気下で
溶融され安定なCe4+イオンを成形しており、重
量%でB2O325〜40%、SiO20〜12%、ZrO20〜10
%、La2O325〜50%、Gd2O30〜5%、CaO0〜12
%、BaO0〜10%、ZnO0〜7%、Ta2O50〜5%、
およびWO30〜3%を含有するガラス100重量部
に対し、重量%で、CeO2を0.1〜1%を加えてな
り、かつ、屈折率(nd)1.65〜1.85、アツベ数
(νd)57〜45の範囲の光学恒数を有するものであ
る。 上記本発明の光学ガラスの実施組成例(No.1お
よびNo.2)をそれらのガラスの光学恒数(nd,
νd)とともに表−1に掲げる。また、これらの
実施組成例の光学ガラス試料(いずれも厚さ10
m/m)の分光透過率曲線を第3図に示す。
The present invention is a projection device including an optical system that forms an image of an object illuminated by an illumination light source on a photoreceptor, the projection device including at least one lens system disposed in an optical path between the illumination light source and the photoreceptor. The present invention relates to a projection device in which one lens is a lens having spectral transmittance characteristics that compensate for the spectral sensitivity characteristics of a photoreceptor. Note that in this specification, the lens refers to a pure lens, excluding those provided with a multilayer interference thin film, and the photoreceptor refers to a photosensitive drum, a photosensitive sheet,
This includes solid-state imaging devices such as CCDs, image pickup tubes such as vidicon, and others. Projection devices with this lens are used as copying machines, facsimiles, television cameras, etc.
Hereinafter, the case where it is used as a copying machine will be explained as an example. Generally, the spectral sensitivity characteristics of photoreceptors used in copying machines are different from the relative luminous efficiency characteristics, and the spectral characteristics multiplied by the spectral wavelength characteristics of the light source that illuminates the original are also different from the relative luminous efficiency characteristics, so the spectral sensitivity characteristics are different from the original. A copy with ivy shading is obtained. For example, if a halogen lamp is used as the light source and a CdS type photoreceptor is used, the filament temperature of 3000°K, which is normally used with halogen lamps, will be reduced.
The emission energy has a maximum value in the infrared region of 800 to 900 nm, and decreases uniformly as it goes to the shorter wavelength side.On the other hand, the spectral sensitivity of the CdS photoreceptor is high in the near infrared region, so it The amount of exposure in the near-infrared range becomes excessive compared to other color ranges such as blue and green.
This causes a phenomenon in which red characters and figures written on the original become faint or disappear completely in the copied image. On the other hand, when a selenium (Se) based photoreceptor and a light source with high emission energy in a short wavelength range are used, it becomes difficult to see blue letters and figures, contrary to when a CdS based photoreceptor and a halogen lamp are used. However, the current situation is that the above problems cannot be solved even when using a CdS-based photoreceptor and a light source with high emission energy in a short wavelength range, or when using a selenium-based photoreceptor and a halogen lamp. It is desirable to compensate for such spectral characteristics (hereinafter referred to as color sensitivity) that differ from the relative luminous sensitivity characteristics to obtain a copy with the same shading as the original. Conventional means for solving this problem include those that use a flat color filter and those that use a multilayer interference thin film known from Japanese Patent Application Laid-open No. 52-60142 and Japanese Utility Model Application No. 52-99331. These are intended to attenuate light in a predetermined wavelength range, for example, in the near-infrared region in the case of the above-described combination of a CdS photoreceptor and a halogen lamp, thereby preventing overexposure in this region. However, when using a flat color filter, there are drawbacks such as parallel plane aberration, high cost due to the addition of one filter component, and large loss of light amount due to surface reflection. On the other hand, when using a multilayer interference thin film, the number of films is generally large, which increases the cost of the vapor deposition process, the spectral characteristics vary depending on the specifications of each optical system, especially the angle of incidence, and the performance changes due to heat, humidity, etc. However, it has the disadvantage of being lacking in durability. By the way, it has been known that a heat absorption filter that attenuates light in the near-infrared region is used as a condenser lens for a slide projector, but this is simply to prevent temperature rise and is described in detail in the following book. What is the point of wavelength selection in a wide wavelength range that matches the spectral sensitivity characteristics of the photoreceptor as in the invention?
Not suggested. Furthermore, it is not used as an imaging lens with predetermined optical performance. A first object of the present invention is to provide a projection device having a lens that compensates for the spectral sensitivity characteristics of a photoreceptor. A second object of the present invention is to provide a wavelength-selective lens system that has high refraction, high dispersion or low dispersion, and has predetermined spectral transmittance characteristics, which are convenient for optical design such as correction of chromatic aberration. It is in. Furthermore, the third object of the present invention is to have excellent devitrification resistance,
The object of the present invention is to provide a novel optical glass that has high refraction, high to low dispersion, and has predetermined spectral transmittance characteristics. By using the present invention, color sensitivity can be compensated more cheaply and stably than in the past. The above-mentioned objects of the present invention can be achieved by the projection apparatus of the present invention described below. In a projection device including an optical system that forms an image of an object illuminated by an illumination light source on a photoreceptor, at least one lens of the lens system is arranged in an optical path between the illumination light source and the photoreceptor. is a lens having spectral transmittance characteristics that compensate for the spectral sensitivity characteristics of the photoreceptor, and the lens has B 2 O 3 25 to 25% by weight.
40%, SiO2 0~12%, ZrO2 0 ~10%, La2O3 25 ~
50%, Gd2O3 0 ~5%, CaO0~12%, BaO0~10
%, ZnO 0-7%, Ta 2 O 5 0-5%, and
For 100 parts by weight of glass containing 0-3% WO3 ,
A projection device which is an optical glass to which 0.1 to 1% by weight of CeO 2 is added and which has optical constants in the range of a refractive index (nd) of 1.65 to 1.85 and an Abbe number (νd) of 57 to 45. In weight%, B2O3 25-40% , SiO2 0-12%,
ZrO 2 0-10%, La 2 O 3 25-50%, Gd 2 O 3 0-5%,
CaO0~12%, BaO0~10%, ZnO0~7%,
CeO 2 was added in weight% to 100 parts by weight of glass containing 0 to 5% Ta 2 O 5 and 0 to 3 % WO 3 .
0.1~1% added, and refractive index (nd) 1.65~
1.85, an optical glass with an optical constant in the range of Atsube number (νd) 57-45. Embodiments of the present invention will be described below with reference to the drawings.
FIG. 1 is a schematic diagram of a copying machine using the present invention.
The document surface 1 is illuminated by a light source 2 for illumination, and the light from the slit area forms an image fixed by scanning mirrors 3 and 4 that move parallel to the document surface 1 at a speed ratio of 2:1. The light enters a lens 5, and is projected by the imaging lens 5 into a slit shape onto a photoreceptor 8 moving in the direction of the arrow via fixed mirrors 6 and 7. In this example, the wavelength selective optical glass is
It is used for the imaging lens 5. FIG. 2 shows the spectral wavelength characteristics of the light source, the spectral sensitivity characteristics of the photoreceptor, and the spectral transmittance characteristics of the imaging lens. Here, a halogen lamp is used as a light source, and a photoreceptor is used as a
A system using Se is shown. As a so-called synergistic effect obtained by multiplying these three characteristics, a spectral characteristic close to the relative luminous efficiency characteristic can be obtained, as shown by the broken line in the figure. In other words, the spectral transmittance characteristic of the lens system is determined so as to have a characteristic close to this specific luminous efficiency characteristic. When a Se-based photoreceptor is used and a halogen lamp is used as an illumination light source, the lens is required to have spectral transmittance characteristics as shown in FIG.
As a result, a comprehensive spectral sensitivity characteristic close to a specific luminous efficiency characteristic can be obtained. Therefore, for the lens for the above purpose, it has a relatively high refractive index and low dispersion.
There is an absorption edge near 400 nm, and the light absorption property decreases rapidly in the wavelength range of 400 to 500 nm, and
There is a need for a glass that exhibits excellent light transmittance in the 700 nm wavelength range and has excellent devitrification resistance. In the present invention, we propose a novel optical glass that is extremely suitable for meeting the above requirements. That is, this glass is melted in an oxidizing atmosphere to form stable Ce4 + ions, and contains 25-40% B2O3 , 0-12% SiO2 , 0-10% ZrO2 by weight.
%, La 2 O 3 25-50%, Gd 2 O 3 0-5%, CaO 0-12
%, BaO0~10%, ZnO0~7%, Ta 2 O 5 0~5%,
and 0.1 to 1% by weight of CeO 2 is added to 100 parts by weight of glass containing 0 to 3% of WO 3 , and has a refractive index (nd) of 1.65 to 1.85 and an Atsube number (νd) of 57. It has optical constants in the range of ~45. The optical constants (nd,
νd) are listed in Table-1. In addition, optical glass samples of these practical composition examples (each with a thickness of 10
The spectral transmittance curve of (m/m) is shown in FIG.

【表】【table】

【表】 以上、Se系感光体の分光感度特性を補償する
本発明の実施例について述べたが、更に有機半導
体(opc)よりなる感光体に対しても同様に補償
できる。すなわちopcは、種類により分光感度特
性が広汎にばらつくものであるが、その分光感度
特性に合わせて少なくとも長波長域又は短波長域
で更に場合によつては両波長域で急峻に低下する
分光透過率特性をもつ光学ガラスより成るレンズ
を用いれば良い。 さて次に如上の波長選択性の光学ガラスを用い
た本発明に係るレンズ系の実施例について説明す
る。 本発明においてはレンズ系は光源から感光体の
間の光路中いかなる所に配置しても良いものであ
るが第1図にも示されるように原稿から感光体の
間の光路中に配置する場合を例にとつて、特に該
レンズ系が結像レンズとして構成される場合につ
いて説明する。ここで第4図以降、如上の波長選
択性の光学ガラスを用いた単レンズは斜線部をも
つて示す。 なお、このレンズ系は、如上のSe系、opcその
他の感光体に適用できるものである。 第4図は本発明に係る結像レンズの第1実施例
である。 これは透過型レンズであつて両凸レンズ,
′、両凹の負レンズ,′が絞りAに対し対称
的に設けられる。正レンズ,′に用いられる
光学ガラスの分散は小さく、他方、負レンズ,
′に用いられる光学ガラスの分散は大きくこれ
らが結合されて色収差が抑えられ、他の諸収差が
補正された結像レンズを構成している。正レンズ
,′は例えば通常のクラウン系の光学ガラス
が用いられ、負レンズ′には通常のフリント系
の光学ガラスが、また、負レンズには本発明に
係わる波長選択性の光学ガラスが用いられる。 ここで本実施例のレンズデータを示せば以下の
通りとなる。曲率半径r、間隔dの単位はmmで
ある。
[Table] The embodiments of the present invention that compensate for the spectral sensitivity characteristics of Se-based photoreceptors have been described above, but it is also possible to similarly compensate for photoreceptors made of organic semiconductors (OPC). In other words, the spectral sensitivity characteristics of OPCs vary widely depending on the type, but depending on the spectral sensitivity characteristics, the spectral transmission decreases sharply at least in the long wavelength region or short wavelength region, and in some cases, in both wavelength regions. It is sufficient to use a lens made of optical glass that has optical properties. Next, an embodiment of a lens system according to the present invention using the wavelength-selective optical glass described above will be described. In the present invention, the lens system may be placed anywhere in the optical path between the light source and the photoreceptor, but as shown in FIG. 1, the lens system may be placed in the optical path between the original and the photoreceptor. Taking as an example, the case where the lens system is configured as an imaging lens will be explained. Here, from FIG. 4 onwards, the single lens using the above-mentioned wavelength-selective optical glass is shown with diagonal lines. Note that this lens system can be applied to the above-mentioned Se-based, OPC, and other photoreceptors. FIG. 4 shows a first embodiment of the imaging lens according to the present invention. This is a transmission type lens, which is a biconvex lens.
', a biconcave negative lens, and ' are provided symmetrically with respect to the aperture A. The dispersion of the optical glass used for the positive lens, ′, is small, while the negative lens,
The optical glass used in ' has a large dispersion and is combined to form an imaging lens in which chromatic aberration is suppressed and other aberrations are corrected. For the positive lens, for example, normal crown-type optical glass is used, for the negative lens ', normal flint-type optical glass is used, and for the negative lens, wavelength-selective optical glass according to the present invention is used. . Here, the lens data of this example is as follows. The units of the radius of curvature r and the interval d are mm.

【表】 第5図は本発明に係る結像レンズの第2実施例
である。 ここで波長選択性の光学ガラスは単レンズに
用いられている。 波長選択性レンズは通過する有効光束の軸上光
路長、軸外光路長がほぼ等しいことが光吸収によ
る光路損失のバランスの点で望ましく、本実施例
のようなメニスカスレンズはこれに適合する。な
おメニスカスレンズに限らず曲率差の小さいレン
ズであれば適合するものである。 ところで単レンズだけでこの光路長のバランス
がとれない系にあつては複数枚の単レンズに波長
選択性ガラスを用い、通過する全光路長でバラン
スをとることができる。 本実施例のレンズデータを示せば以下の通りで
ある。
[Table] FIG. 5 shows a second embodiment of the imaging lens according to the present invention. Here, wavelength-selective optical glass is used for a single lens. In the wavelength selective lens, it is desirable that the on-axis optical path length and the off-axis optical path length of the effective light beam passing through the lens be approximately equal in terms of the balance of optical path loss due to light absorption, and the meniscus lens as in this embodiment is suitable for this. Note that not only meniscus lenses but also lenses with a small difference in curvature are suitable. By the way, in a system in which the optical path length cannot be balanced using only a single lens, it is possible to use wavelength selective glass for a plurality of single lenses and to balance the total optical path length. The lens data of this example is as follows.

【表】 第6図は本発明に係る結像レンズの第3実施例
の図で波長選択性の光学ガラスを反射型レンズに
用いたものである。 ミラーレンズの第2面はミラー面となつてお
り有効光束はミラーレンズを2度通過する。 第7図は本発明に係る結像レンズの第4実施例
の図である。 これは物像間距離を変えることなく倍率変換可
能なズームレンズに波長選択性の光学ガラスを用
いたものである。ここで波長選択性の光学ガラス
は単レンズL5に用いられている。変倍時、ズー
ムレンズはレンズ全体移動、内部移動を行なつて
結像関係を保つ光学位置、焦点距離に設定される
ためミラーによる光路長補正等を必要としない。 ここで単レンズL5は移動群に属し変倍時、内
部移動される。 本実施例の構成はL1よりL10の10枚の単レンズ
より成り絞りAに対し対称的に設けられる。 ここで本実施例のレンズデータは次のとおりで
ある。
[Table] FIG. 6 is a diagram of a third embodiment of the imaging lens according to the present invention, in which a wavelength-selective optical glass is used as a reflective lens. The second surface of the mirror lens is a mirror surface, and the effective light flux passes through the mirror lens twice. FIG. 7 is a diagram of a fourth embodiment of the imaging lens according to the present invention. This uses wavelength-selective optical glass in a zoom lens that can change the magnification without changing the distance between objects and images. Here, wavelength-selective optical glass is used for the single lens L5. When changing the magnification, the zoom lens moves the entire lens and moves internally to set the optical position and focal length to maintain the imaging relationship, so there is no need for optical path length correction using a mirror. Here, the single lens L5 belongs to the moving group and is internally moved during zooming. The configuration of this embodiment consists of 10 single lenses L1 to L10 , which are arranged symmetrically with respect to the aperture A. Here, the lens data of this example is as follows.

【表】【table】

【表】 以上、本発明によれば複写機における感色性を
安価に且つ安定して補償できる。なお本発明は冒
頭述べたように、複写機に限らずフアクシミリ、
テレビカメラ等、広汎な分野に適用されるもので
あり、非常に有用である。
[Table] As described above, according to the present invention, color sensitivity in a copying machine can be compensated for inexpensively and stably. As mentioned at the beginning, the present invention is applicable not only to copying machines but also to facsimile machines,
It is applicable to a wide range of fields such as television cameras, and is extremely useful.

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

第1図は本発明を用いた複写機の概略図、第2
図は光源の分光波長特性、Se系感光体の分光感
度特性、レンズ系の分光透過率特性を示す図、第
3図はSe系感光体に適する本発明に係わる波長
選択性の光学ガラスの分光透過率特性の図、第4
図乃至第7図は本発明のレンズ系の実施例の図で
ある。 1……原稿、2……照明光源、3,4……走査
ミラー、5……結像レンズ、6,7……固定ミラ
ー、8……感光体、A……絞り。
Figure 1 is a schematic diagram of a copying machine using the present invention, Figure 2 is a schematic diagram of a copying machine using the present invention;
The figure shows the spectral wavelength characteristics of the light source, the spectral sensitivity characteristics of the Se-based photoreceptor, and the spectral transmittance characteristics of the lens system. Figure 3 shows the spectral spectrum of the wavelength-selective optical glass according to the present invention, which is suitable for the Se-based photoreceptor. Diagram of transmittance characteristics, 4th
7 to 7 are diagrams of embodiments of the lens system of the present invention. 1... Original document, 2... Illumination light source, 3, 4... Scanning mirror, 5... Image forming lens, 6, 7... Fixed mirror, 8... Photoreceptor, A... Aperture.

Claims (1)

【特許請求の範囲】 1 照明光源によつて照明された物体の像を感光
体上に結像する光学系を含む投影装置において、
前記照明光源と感光体の間の光路中に配置される
レンズ系の少なくとも一枚のレンズが前記感光体
の分光感度特性を補償する分光透過率特性を有す
るレンズであり、該レンズは重量%で、B2O325
〜40%、SiO20〜12%、Zr02O〜10%、La2O325
〜50%、Gd2O30〜5%、CaO0〜12%、BaO0〜
10%、ZnO0〜7%、Ta2O50〜5%、および、
WO30〜3%を含有するガラス100重量部に対し、
重量%で、CeO2を0.1〜1%加えてなり、且つ屈
折率(nd)1.65〜1.85、アツベ数(νd)57〜45の
範囲の光学恒数を有する光学ガラスであることを
特徴とする投影装置。 2 重量%で、B2O325〜40%、SiO20〜12%、
ZrO20〜10%、La2O325〜50%、Gd2O30〜5%、
CaO0〜12%、BaO0〜10%、ZnO0〜7%、
Ta2O50〜5%、および、WO30〜3%を含有す
るガラス100重量部に対し、重量%で、CeO2
0.1〜1%加えてなり、且つ屈折率(nd)1.65〜
1.85、アツベ数(νd)57〜45の範囲の光学恒数を
有することを特徴とする光学ガラス。
[Claims] 1. A projection device including an optical system that forms an image of an object illuminated by an illumination light source on a photoreceptor,
At least one lens of the lens system disposed in the optical path between the illumination light source and the photoreceptor is a lens having spectral transmittance characteristics that compensate for the spectral sensitivity characteristics of the photoreceptor, and the lens is , B 2 O 3 25
~40%, SiO2 0 ~12%, Zr02O ~10%, La2O3 25
~50%, Gd2O30 ~ 5%, CaO0~12%, BaO0~
10%, ZnO 0-7%, Ta 2 O 5 0-5%, and
For 100 parts by weight of glass containing 0-3% WO3 ,
It is characterized by being an optical glass containing 0.1 to 1% of CeO 2 by weight, and having optical constants in the range of a refractive index (nd) of 1.65 to 1.85 and an Atsube number (νd) of 57 to 45. Projection device. 2% by weight, B 2 O 3 25-40%, SiO 2 0-12%,
ZrO 2 0-10%, La 2 O 3 25-50%, Gd 2 O 3 0-5%,
CaO0~12%, BaO0~10%, ZnO0~7%,
CeO 2 was added in weight% to 100 parts by weight of glass containing 0 to 5% Ta 2 O 5 and 0 to 3 % WO 3 .
0.1~1% added, and refractive index (nd) 1.65~
1.85, an optical constant having an Atsbe number (νd) in the range of 57 to 45.
JP19948590A 1981-08-08 1990-07-26 projection device Granted JPH0375236A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19948590A JPH0375236A (en) 1981-08-08 1990-07-26 projection device

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP56124210A JPS5825607A (en) 1981-08-08 1981-08-08 projection device
JP19948590A JPH0375236A (en) 1981-08-08 1990-07-26 projection device

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP56124210A Division JPS5825607A (en) 1981-08-08 1981-08-08 projection device

Publications (2)

Publication Number Publication Date
JPH0375236A JPH0375236A (en) 1991-03-29
JPH04934B2 true JPH04934B2 (en) 1992-01-09

Family

ID=26460929

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19948590A Granted JPH0375236A (en) 1981-08-08 1990-07-26 projection device

Country Status (1)

Country Link
JP (1) JPH0375236A (en)

Also Published As

Publication number Publication date
JPH0375236A (en) 1991-03-29

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