JP2004163249A - Method for measuring quantity of light of led - Google Patents
Method for measuring quantity of light of led Download PDFInfo
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- JP2004163249A JP2004163249A JP2002329039A JP2002329039A JP2004163249A JP 2004163249 A JP2004163249 A JP 2004163249A JP 2002329039 A JP2002329039 A JP 2002329039A JP 2002329039 A JP2002329039 A JP 2002329039A JP 2004163249 A JP2004163249 A JP 2004163249A
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- led
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- Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Facsimile Heads (AREA)
- Led Devices (AREA)
Abstract
Description
【0001】
【発明の属する技術分野】
本発明は、複写機、ファクシミリ、プリンタといった電子写真方式の画像形成装置に搭載される感光体露光用としてのLEDの光量を測定するLEDの光量測定方法に関し、特に、多数のLEDが配列されてなるLEDプリントヘッドにおけるLED個々に対しての光量測定方法に関する。
【0002】
【従来の技術】
一般に画像形成装置は、軸回転可能なドラム状の感光体と、この感光体の表面に所定間隔をあけて対向し軸方向に延在するLEDプリントヘッドと、を搭載しており、入力画像の各画素の階調に対応する光量の光を、LEDプリントヘッド上に規則的に配列された多数のLED各々から感光体に向けて照射し、これにより感光体表面を所望の明電位に露光させて、入力画像に対応する静電潜像を形成するようになっている。各LEDとしては、例えばAl−Ga−As系のものが一般に用いられ、これは発光効率が高い反面、主たる発光ピークが存する主発光帯域(波長780nm付近)と、これとは別に副発光ピークが存する副発光帯域(波長870nm付近)とを有する。
【0003】
ところで、画像形成装置の製造段階においては、取り付けられたLEDプリントヘッドにおけるLED間の単位時間あたりの光量を均一にする目的から、LED毎に設定電流値を微調整することが通常なされる。そのため、LED個々の光量を事前に把握しておく必要があり、その光量把握に際し、LED各々に対する光量測定方法が極めて重要となる。
【0004】
従来の光量測定方法は、波長域を問わず感度が一定なPINフォトダイオード等のセンサでLEDからの光を受光し、その光量を出力するようになっており、出力される光量(測定値)には、上記した主発光帯域のみならず副発光帯域のものも含まれる。しかし、副発光帯域の光量は、LED間でその量にばらつきがあるだけでなく、感光体の露光にほとんど寄与しないことから、この光量が測定値に含まれると、適正な設定電流値にLEDを調整できず、測定値が活用できないという不都合が生じる。このような不都合に対し、副発光帯域の光量を測定値から積極的に排除する目的で、副発光帯域の光を遮断し主発光帯域の光を高効率に透過させるようなバンドパスフィルタを介して、センサで受光する方法が提案されている(例えば、特許文献1参照)。
【0005】
【特許文献1】
特開2001−158129号公報(第4−5頁、第1−4図)
【0006】
【発明が解決しようとする課題】
しかし、LED(LEDプリントヘッド)は、実質、画像形成装置内で感光体と対をなすものであるが、半導体レーザーとは異なり、半値幅が約40nmと広い波長分布を示すため、その感光体の分光感度特性、すなわち感光体の材質の違いによっては、例え上記の光量測定方法により得られた各LED光量の測定値にそのまま従って、各LEDの設定電流値が調整されたとしても、感光体表面の露光量、すなわち明電位がばらつき、ひいては画像形成の品位に支障を来たすという問題がある。その理由について、図2を参照しながら以下に述べる。
【0007】
図2は感光体の分光感度特性を材質別に示す図である。ここでは、感光体の材質として、OPC(有機感光体)、a−Si(アモルファス−シリコン)、Se(セレン)系であるSe−Te(セレン−テルル)を代表的に挙げる。なお、図中斜線部は、一例としてのAl−Ga−As系のLEDにおける主発光帯域である。従来最も一般的であるOPCの場合、図中破線で示すように、波長広範に亘って感度がほぼ一定で、特に主発光帯域では感度は一定である。他方a−Siの場合、図中実線で示すように、波長広範に亘って感度が高い反面、波長に従って感度の変化が著しく、特に主発光帯域ではその変化が大きい。またSe−Teの場合は、図中一点鎖線で示すように、主発光帯域の感度が最も低くその変化も大きい。
【0008】
従って、感光体がa−SiやSe−Teの場合は、主発光帯域における感光体感度の変化が大きいことから、これに全く配慮がなされていない上記の光量測定方法による測定値を以って、そのまま設定電流値が調整されたLEDからの光では、感光体表面の露光量がばらつき、上記の問題が生じるわけである。一方、感光体がOPCの場合は、主発光帯域における感光体感度が一定であることから、感光体表面の露光量はばらつくことはなく、上記の問題は生じない。
【0009】
そこで、本発明は、上記の問題に鑑みてなされたものであり、画像形成装置に搭載される感光体露光用としてのLEDプリントヘッドのLEDについて、得られた各LED光量の測定値にそのまま従って、各LEDの設定電流値が調整されたとしても、感光体表面の露光量のばらつきの低減が可能な光量測定方法を提供することを目的とするものである。
【0010】
【課題を解決するための手段】
上記目的を達成するため、本発明によるLEDの光量測定方法は、感光体を露光させるための多数のLEDが配列されたLEDプリントヘッドにおける前記LED個々の光量を測定するLEDの光量測定方法において、前記感光体の分光感度特性に合わせたフィルタを介して、前記LEDからの光を感度が一定なセンサで受光し、その光量を出力することを特徴とする。これにより、得られた各LED光量の測定値が感光体の分光感度特性に応じたものとなるため、これら各測定値にそのまま従って、各LEDの設定電流値が調整されたとしても、感光体表面の露光量のばらつきが抑えられる。
【0011】
例えば、前記フィルタは所定の波長毎に透過率が異なるものであることが好ましい。また、LEDの主発光帯域で感度が高いが感度変化の大きい感光体に好適であり、特に前記感光体がアモルファス−シリコンであるとよい。
【0012】
【発明の実施の形態】
以下に、本発明の実施形態について図面を参照しながら詳述する。図1は、本発明のLEDの光量測定方法を採用した光量測定装置の要部構成を示すブロック図である。図中、1はLEDプリントヘッドであって、規則的に一直線上に配列された多数のLED2と、これら各LED2に電流を供給するための端子(不図示)と、を備えている。なお実際には、各LED2は、所定の数毎にチップ状のLEDヘッド3に収納されている。
【0013】
このようなLEDプリントヘッド1のLED2各々の光量を測定する光量測定装置は、大きくは、LEDプリントヘッド1の端子に接続されて各LED2に発光信号を与える発光信号発信部11、LEDプリントヘッド1を保持し各LED2の配列方向に移動(両矢印の実線で図示)が可能な保持部12、LED2が発光した光を集光するレンズ等の集光部13、この集光部13からの光を受光してその光量を検出し電気信号に変換するセンサ14、このセンサ14の受光面に配設されたフィルタ15、センサ14からの電気信号を受け所定の処理を施す検出信号処理部16から構成される。なお全体の測定動作は、入力操作に基づいてCPU等の制御部(不図示)で制御される。
【0014】
ここでセンサ14は、波長域を問わず感度が一定なものであって、例えばPINフォトダイオードが好適である。またフィルタ15は、本実施形態に特徴的なものであり、画像形成装置内でLEDプリントヘッド1と対になる感光体の材質に特有の分光感度特性に合わせた光透過性を有する。具体的には、感光体が、波長に従って特にLED2の主発光帯域で感度の変化する分光感度特性を有する材質、例えばa−Siの場合、フィルタ15は所定の波長毎に透過率が異なるようになっている。
【0015】
このような構成の光量測定装置による光量測定方法について、以下に述べる。制御部からの指令により、保持部12が駆動し、1つのLED2が集光部13、フィルタ15及びセンサ14の光軸上に位置決めされる。次いで、そのLED2に対して発光信号発信部11から発光信号が与えられ、LED2を発光させる。LED2からの光は、集光部13を通じて集光し、フィルタ15を経てセンサ14で受光される。このセンサ14は、受光の光量を検出してアナログ信号の電気信号に変換し検出信号処理部16に出力する。そして、検出信号処理部16は、その電気信号に基づく光量値を測定値として、画面に表示させたり、用紙に印字させたり、或いは、その電気信号をAD変換器でデジタル信号に変換してメモリに記憶させたりする。引き続き、全てのLED2に対して上記の動作が繰り返され、光量測定が完了する。
【0016】
このようにして得られた各LED2の光量の測定値は、フィルタ15を介して検出されたものであるため、感光体の分光感度特性に応じたものとなる。そうすると、これら各測定値にそのまま従って、各LED2の設定電流値が調整されたとしても、感光体表面の露光量のばらつきが効果的に抑えられ、ひいては画像形成の品位向上につながる。
【0017】
なお本実施形態では、感光体の材質として、感度が高い点で優れるa−Siを例に挙げて説明したが、フィルタ15が感光体の分光感度特性に合わせたものである限り、これ以外のSe系のものにも適用可能である。勿論、OPCでも構わない。
【0018】
その他本発明は上記の実施形態に限定されず、本発明の趣旨を逸脱しない範囲で、種々の変更が可能である。
【0019】
【発明の効果】
以上説明した通り、本発明のLEDの光量測定方法によれば、得られた各LED光量の測定値が感光体の分光感度特性に応じたものとなるため、これら各測定値にそのまま従って、各LEDの設定電流値が調整されたとしても、感光体表面の露光量のばらつきが抑えられ、ひいては画像形成の品位が向上する。
【図面の簡単な説明】
【図1】本発明のLEDの光量測定方法を採用した光量測定装置の要部構成を示すブロック図である。
【図2】感光体の分光感度特性を材質別に示す図である。
【符号の説明】
1 LEDプリントヘッド
2 LED
3 LEDヘッド
11 発光信号発信部
12 保持部
13 集光部
14 センサ
15 フィルタ
16 検出信号処理部[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a method for measuring the light amount of an LED used for exposing a photosensitive member mounted on an electrophotographic image forming apparatus such as a copying machine, a facsimile, and a printer. The present invention relates to a method for measuring the amount of light for each LED in an LED print head.
[0002]
[Prior art]
Generally, an image forming apparatus is equipped with a drum-shaped photoreceptor rotatable about an axis, and an LED print head that is opposed to the surface of the photoreceptor at a predetermined interval and extends in the axial direction. A large amount of light corresponding to the gradation of each pixel is irradiated from each of a large number of LEDs regularly arranged on the LED print head toward the photoconductor, thereby exposing the photoconductor surface to a desired bright potential. Thus, an electrostatic latent image corresponding to the input image is formed. As each LED, for example, an Al-Ga-As-based LED is generally used, which has high luminous efficiency, but has a main luminous band (at a wavelength of about 780 nm) where a main luminous peak exists, and a sub-luminous peak separately from this. Sub-emission band (wavelength around 870 nm).
[0003]
By the way, in the manufacturing stage of the image forming apparatus, it is usual to finely adjust the set current value for each LED in order to equalize the amount of light per unit time between the LEDs in the attached LED print head. Therefore, it is necessary to grasp the light amount of each LED in advance, and in grasping the light amount, the method of measuring the light amount for each LED is extremely important.
[0004]
In the conventional light quantity measuring method, a sensor such as a PIN photodiode having a constant sensitivity regardless of the wavelength range receives light from the LED and outputs the light quantity, and the output light quantity (measured value) Includes not only the main light emission band described above but also the sub light emission band. However, since the amount of light in the sub-emission band varies not only between the LEDs but also hardly contributes to the exposure of the photoconductor, if the amount of light is included in the measured value, the LED will reach an appropriate set current value. Cannot be adjusted, and the measured value cannot be used. For such inconvenience, in order to positively exclude the light amount in the sub-emission band from the measured value, a band-pass filter that blocks light in the sub-emission band and transmits light in the main emission band with high efficiency is used. Thus, a method of receiving light with a sensor has been proposed (for example, see Patent Document 1).
[0005]
[Patent Document 1]
JP 2001-158129 A (Page 4-5, FIG. 1-4)
[0006]
[Problems to be solved by the invention]
However, although an LED (LED print head) substantially forms a pair with a photoconductor in an image forming apparatus, unlike a semiconductor laser, the half-width shows a wide wavelength distribution of about 40 nm. Depending on the spectral sensitivity characteristics of the photoreceptor, that is, the difference in the material of the photoreceptor, even if the set current value of each LED is adjusted in accordance with the measurement value of each LED light amount obtained by the above light amount measurement method, There is a problem that the exposure amount on the surface, that is, the light potential varies, and the quality of image formation is hindered. The reason will be described below with reference to FIG.
[0007]
FIG. 2 is a diagram showing the spectral sensitivity characteristics of the photoconductor for each material. Here, as the material of the photoconductor, OPC (organic photoconductor), a-Si (amorphous silicon), and Se (Se) -based Se-Te (selenium-tellurium) are representatively mentioned. The hatched portions in the drawing are the main light emission bands in an Al-Ga-As-based LED as an example. Conventionally, in the case of OPC, which is the most common, the sensitivity is almost constant over a wide wavelength range, as shown by the broken line in the figure, and particularly the sensitivity is constant in the main light emission band. On the other hand, in the case of a-Si, as shown by the solid line in the figure, the sensitivity is high over a wide range of wavelengths, but the change in sensitivity is remarkable according to the wavelength, especially in the main emission band. In the case of Se-Te, the sensitivity in the main emission band is the lowest and the change is large, as indicated by the dashed line in the figure.
[0008]
Therefore, when the photoreceptor is a-Si or Se-Te, the change in the photoreceptor sensitivity in the main emission band is large. With the light from the LED whose set current value is adjusted as it is, the exposure amount on the surface of the photoreceptor varies, and the above problem occurs. On the other hand, when the photoconductor is OPC, since the photoconductor sensitivity in the main light emission band is constant, the exposure amount on the photoconductor surface does not vary, and the above problem does not occur.
[0009]
In view of the above, the present invention has been made in view of the above-described problem, and the LED of a LED print head for exposing a photosensitive member mounted on an image forming apparatus is directly used in accordance with the measured value of each obtained LED light amount. It is another object of the present invention to provide a light amount measuring method capable of reducing the variation in the exposure amount on the photoreceptor surface even when the set current value of each LED is adjusted.
[0010]
[Means for Solving the Problems]
In order to achieve the above object, a method for measuring the light amount of an LED according to the present invention is a method for measuring the light amount of an LED in an LED print head in which a large number of LEDs for exposing a photoreceptor are arranged, Light from the LED is received by a sensor having a constant sensitivity via a filter adapted to the spectral sensitivity characteristic of the photoconductor, and the amount of light is output. As a result, the measured value of the amount of light of each LED obtained corresponds to the spectral sensitivity characteristic of the photoconductor. Therefore, even if the set current value of each LED is adjusted in accordance with these measured values, Variations in surface exposure can be suppressed.
[0011]
For example, the filter preferably has a different transmittance for each predetermined wavelength. Further, it is suitable for a photoreceptor having high sensitivity in the main light emission band of the LED but having a large change in sensitivity. In particular, the photoreceptor is preferably amorphous-silicon.
[0012]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. FIG. 1 is a block diagram showing a configuration of a main part of a light quantity measuring device adopting the LED light quantity measuring method of the present invention. In the figure,
[0013]
Such a light quantity measuring device for measuring the light quantity of each of the
[0014]
Here, the
[0015]
A method for measuring the light amount by the light amount measuring device having such a configuration will be described below. The holding
[0016]
Since the measured value of the light amount of each
[0017]
In the present embodiment, as a material of the photoconductor, a-Si, which is excellent in terms of high sensitivity, has been described as an example. It is also applicable to Se type. Of course, OPC may be used.
[0018]
In addition, the present invention is not limited to the above embodiment, and various modifications can be made without departing from the spirit of the present invention.
[0019]
【The invention's effect】
As described above, according to the method for measuring the light amount of the LED of the present invention, the obtained measured value of the light amount of each LED corresponds to the spectral sensitivity characteristic of the photoreceptor. Even if the set current value of the LED is adjusted, the variation in the exposure amount on the surface of the photoconductor is suppressed, and the quality of image formation is improved.
[Brief description of the drawings]
FIG. 1 is a block diagram showing a main configuration of a light quantity measuring device employing a method for measuring the light quantity of an LED according to the present invention.
FIG. 2 is a diagram illustrating spectral sensitivity characteristics of a photoconductor for each material.
[Explanation of symbols]
1
3
Claims (3)
前記感光体の分光感度特性に合わせたフィルタを介して、前記LEDからの光を感度が一定なセンサで受光し、その光量を出力することを特徴とするLEDの光量測定方法。In an LED light quantity measuring method for measuring the light quantity of each LED in an LED print head in which a large number of LEDs for exposing a photoconductor are arranged,
A light quantity measuring method for an LED, comprising: receiving light from the LED by a sensor having a constant sensitivity via a filter adapted to a spectral sensitivity characteristic of the photoconductor; and outputting the light quantity.
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Cited By (3)
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KR100925225B1 (en) * | 2008-12-31 | 2009-11-06 | 주식회사 대한전광 | Apparatus for measuring a group of light source |
JP2012503758A (en) * | 2008-09-27 | 2012-02-09 | 中茂電子(深▲ちぇん▼)有限公司 | Light-emitting element measuring device including solar module and measuring method thereof |
CN101726404B (en) * | 2008-10-15 | 2012-10-10 | 中茂电子(深圳)有限公司 | Detection platform for luminous component with a plurality of luminous elements and detection method thereof |
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JP2011085743A (en) | 2009-10-15 | 2011-04-28 | Seiko Epson Corp | Image forming apparatus, and image forming method |
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Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
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JP2012503758A (en) * | 2008-09-27 | 2012-02-09 | 中茂電子(深▲ちぇん▼)有限公司 | Light-emitting element measuring device including solar module and measuring method thereof |
KR101380700B1 (en) * | 2008-09-27 | 2014-04-03 | 크로마 일렉트로닉스 (센젠) 컴퍼니 리미티드 | A test table with solar cells for light-emitting components and a test method thereof |
CN101726404B (en) * | 2008-10-15 | 2012-10-10 | 中茂电子(深圳)有限公司 | Detection platform for luminous component with a plurality of luminous elements and detection method thereof |
KR100925225B1 (en) * | 2008-12-31 | 2009-11-06 | 주식회사 대한전광 | Apparatus for measuring a group of light source |
CN101769820A (en) * | 2008-12-31 | 2010-07-07 | 株式会社大韩电光 | Integrated light source measuring apparatus |
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