JPH04106736A - Laser driving circuit for optical recording and reproducing device - Google Patents

Laser driving circuit for optical recording and reproducing device

Info

Publication number
JPH04106736A
JPH04106736A JP2225701A JP22570190A JPH04106736A JP H04106736 A JPH04106736 A JP H04106736A JP 2225701 A JP2225701 A JP 2225701A JP 22570190 A JP22570190 A JP 22570190A JP H04106736 A JPH04106736 A JP H04106736A
Authority
JP
Japan
Prior art keywords
current
power
recording
value
laser
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
JP2225701A
Other languages
Japanese (ja)
Inventor
Akira Inoue
明 井上
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson 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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP2225701A priority Critical patent/JPH04106736A/en
Publication of JPH04106736A publication Critical patent/JPH04106736A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain laser power equivalent to a set value by correcting a current value upon a variation of the current value due to a changeover of high frequency superimposing and a change of recording and reproducing power in using a memory recorded with a set power as an address and a correction value as a data. CONSTITUTION:When the high frequency superimposing (HF) is off, since a digital memory 104 is not selected by an HF on/off switch 103, an output of the memory 104 is zero. Recording power (Pw) is inputted also to a recording current setting circuit 105 to decide a current. Thus current is switched by a current circuit 107 in accordance with the recorded data 108, and a laser 109 is emitted. Then, when the HF is on, reproducing power (Pr) and the Pw are inputted to an address in the memory 104. Data of the memory 104 in contents is a difference between Iwon 204 when the HF is off and Iwoff 203 when the HF is off. When the HF is on, a value of a current to flow is increased, and this is added to the current of the circuit 107 after converting a correction data from the memory 104 at the address of the set Pr and Pw by a D/A converter 106. By this method, light power equivalent to the set value is obtained.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、光記録再生装置のレーザ駆動回路に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a laser drive circuit for an optical recording/reproducing device.

[従来の技術] 従来の光記録再生装置のレーザ駆動回路を第3図に示さ
れたブロック図に基づいて説明する。再生パワーは、再
生パワー設定部101で また記録パワーは、記録パワ
ー設定部102で各々設定される。記録パワーを発光す
るために必要な記録電流Iw  301は、記録電流設
定回路105に入力された記録設定パワーをレーザの発
光効1pLL(単位電流あたりのレーザパワー)によっ
て割った値となる。
[Prior Art] A laser drive circuit of a conventional optical recording/reproducing device will be explained based on the block diagram shown in FIG. The reproduction power is set by a reproduction power setting section 101 and the recording power is set by a recording power setting section 102. The recording current Iw 301 required to emit the recording power is the value obtained by dividing the recording setting power input to the recording current setting circuit 105 by the luminous efficiency of the laser 1 pLL (laser power per unit current).

記録電流Iwは、電流回路107で記録データ108に
応してスイッチされレーザ109に供給される。レーザ
106の出射光は、モニターフォトダイオード302で
モニターされ電流−電圧変換されたのち自動パワー制御
回路304(以後A20回路と略す)に入力され温度変
動などによって生じるレーザ出力の変動をバイアス電流
 Ib305を制御することによって調整していた。
The recording current Iw is switched by a current circuit 107 according to recording data 108 and is supplied to a laser 109. The emitted light from the laser 106 is monitored by a monitor photodiode 302 and subjected to current-to-voltage conversion, and then input to an automatic power control circuit 304 (hereinafter referred to as the A20 circuit), which uses a bias current Ib 305 to compensate for fluctuations in laser output caused by temperature fluctuations, etc. It was regulated by controlling.

[発明が解決しようとする課題] しかし従来の光記録再生装置のレーザ駆動回路では、高
周波重畳を行った場合の半導体レーザの発光効率の変化
を補正していないため出射される記録パワーが設定した
記録パワーの値より低くなり記録媒体に信号が最適に記
録できなかったり消去時にデータの消し残りが生じると
いう欠点を有していた。
[Problem to be solved by the invention] However, in the laser drive circuit of the conventional optical recording and reproducing device, the change in the luminous efficiency of the semiconductor laser when high frequency superimposition is performed is not corrected, so the emitted recording power is set. This has disadvantages in that the recording power is lower than the value of the recording power, and signals cannot be optimally recorded on the recording medium, and data remains unerased during erasing.

そこで本発明はこのような問題点を解決するためのもの
で、その目的とするところは、設定する光パワーの変更
や高周波重畳の切り替えを行なっても、レーザから出射
される記録、消去パワーが設定した光パワーに等しい光
記録再生装置のレーザ駆動回路を提供することにある。
The present invention is intended to solve these problems, and its purpose is to maintain the recording and erasing power emitted from the laser even if the set optical power is changed or the high frequency superimposition is switched. It is an object of the present invention to provide a laser drive circuit for an optical recording/reproducing device that has an optical power equal to a set optical power.

[課題を解決するための手段] 本発明の光記録再生装置のレーザ駆動回路は、光学ピッ
クアップを用い光ディスク、光カードなどの光記録媒体
に情報を記録再生する光記録再生装置のレーザ駆動回路
において 高周波重畳を行った時に生じるレーザ駆動電流の変動を
補正するために再生レーザパワーと記録レーザパワーの
値をアドレスとし補正値をデータとして記録したデジタ
ルメモリーと 前記補正値をアナログ値に変換するD/Aコンバーター
と 前記補正値を高周波重畳を行わない場合の電流値に加算
し駆動電流とする電流回路からなることを特徴とする。
[Means for Solving the Problems] A laser drive circuit for an optical recording and reproducing apparatus of the present invention is a laser driving circuit for an optical recording and reproducing apparatus that uses an optical pickup to record and reproduce information on an optical recording medium such as an optical disk or an optical card. In order to correct fluctuations in laser drive current that occur when performing high frequency superimposition, there is a digital memory that uses the values of the reproduction laser power and recording laser power as addresses and records correction values as data, and a digital memory that converts the correction values into analog values. It is characterized by comprising an A converter and a current circuit that adds the correction value to the current value when high frequency superimposition is not performed to obtain a drive current.

[実施例] 以下本発明の実施例について図面に基づいて詳細に説明
する。まず 半導体レーザの電流−光パワー特性〔以後
 I−P特性と略記する)について第2図を用いて説明
する。第2図において横軸は、電流を示し 縦軸は、レ
ーザの発光パワーを示している。201は、高周波重畳
を行っていない場合、また202は、高周波重畳を行っ
ている場合のI−P特性である。高周波重畳を行ってい
ない場合のr−P特性201は、ダイオードと同じ非線
形特性を有しており、電流がしきい値電流I th20
5を越えると一定の傾きで直線的に光パワーが増加する
[Example] Hereinafter, an example of the present invention will be described in detail based on the drawings. First, the current-optical power characteristics (hereinafter abbreviated as IP characteristics) of a semiconductor laser will be explained using FIG. 2. In FIG. 2, the horizontal axis represents current, and the vertical axis represents laser emission power. 201 is the I-P characteristic when high frequency superimposition is not performed, and 202 is the I-P characteristic when high frequency superimposition is performed. The r-P characteristic 201 when high frequency superimposition is not performed has the same nonlinear characteristic as a diode, and the current is the threshold current I th20
When the value exceeds 5, the optical power increases linearly with a constant slope.

つぎに高周波重畳を行っている場合のI−P特性は、駆
動電流を高周波で変調しているため202のI−P特性
のように201に比べ低い電流値から発光が始まり パ
ワーが増加するにしたがい201に漸近していく。した
がって高周波重畳を行う場合の発光効率は、高周波重畳
を行わない場合と異なり一定値ではなく、記録再生パワ
ーの値によって変化する。
Next, the I-P characteristic when high frequency superimposition is performed is that the drive current is modulated with high frequency, so as in the I-P characteristic of 202, light emission starts from a lower current value compared to 201, and as the power increases. Therefore, it gradually approaches 201. Therefore, unlike the case where high frequency superimposition is not performed, the luminous efficiency when high frequency superimposition is performed is not a constant value, but changes depending on the value of recording and reproducing power.

高周波重畳を行わない場合には、記録時に必要な電流は
、再生パワーがどのような値であってもPwの光パワー
を発光効率(単位レーザパワーを出力するために必要な
電流、 すなわち直線の傾き)で割った値に一義的に決
定できる。例えばPw=5mW、発光効率50 u W
 / m Aとすると駆動電流は、 10mAが必要に
なる。しかし高周波重畳を行った場合には、発光効率が
一定でないためPWの値が同じてあっても 記録時に必
要な電流値は、再生パワーの値により変化する。光ディ
スクなどの記録媒体の記録感度やD適な再生パワー光学
ピックアップの特性を求める場合には、再生パワーを変
化させたり高周波重畳を○N/○FFする必要が生じて
くる。この課題を解決する一実施例を第1図を用いて詳
細に説明する。
When high-frequency superimposition is not performed, the current required during recording is determined by dividing the optical power of Pw by the luminous efficiency (current required to output unit laser power, i.e., linear It can be uniquely determined by the value divided by the slope). For example, Pw=5mW, luminous efficiency 50 uW
/mA, the drive current will be 10mA. However, when high frequency superimposition is performed, the luminous efficiency is not constant, so even if the PW value is the same, the current value required during recording changes depending on the value of the reproducing power. When determining the recording sensitivity of a recording medium such as an optical disk or the characteristics of an optical pickup with an appropriate reproduction power, it becomes necessary to change the reproduction power or change the high frequency superimposition to N/FF. An embodiment for solving this problem will be explained in detail using FIG. 1.

第1図において再生パワーPrと記録パワーPwは、再
生パワー設定部101、記録パワー設定部102でデジ
タル的に設定される。例えば 1ビツトあたり0.1m
Wとして光パワーを設定する。
In FIG. 1, the reproduction power Pr and the recording power Pw are digitally set by a reproduction power setting section 101 and a recording power setting section 102. For example, 0.1m per 1 bit
Set the optical power as W.

高周波重畳を行わない場合には、HF ON10 FF
スイッチ103がデジタルメモリ104をセレクトしな
いためデジタルメモリー104の出力は常にOである。
If high frequency superposition is not performed, HF ON10 FF
Since the switch 103 does not select the digital memory 104, the output of the digital memory 104 is always O.

記録パワーは、記録電流設定回路105にも入力され電
流が一義的に決定される。
The recording power is also input to a recording current setting circuit 105 to uniquely determine the current.

この電流が電流回路107で記録データ108に応じて
スイッチされ、 レーザ109が発光する。
This current is switched in a current circuit 107 according to recorded data 108, and a laser 109 emits light.

次に高周波重畳がONの場合には、再生パワーと記録パ
ワーがデジタルメモリー104のアドレスに入力される
。    デジタルメモリ104のデータの内容は、第
2図に示す高周波重畳ON時のIwon204と高周波
重畳OFF時のIwoff203の差である。前述した
ように高周波重畳ON時の場合、流すべき電流値が増加
する。設定された再生パワー、記録パワーをアドレスと
してデジタルメモリ104から補正データが出力される
。このデータをD/Aコンバータ106によりアナログ
値として電流回路107の電流値に加算され、設定値に
等しい光パワーが得られる。
Next, when high frequency superimposition is ON, the reproduction power and recording power are input to the address of the digital memory 104. The content of the data in the digital memory 104 is the difference between Iwon 204 when high frequency superimposition is ON and Iwoff 203 when high frequency superimposition is OFF, as shown in FIG. As described above, when high frequency superimposition is ON, the current value to be passed increases. Correction data is output from the digital memory 104 using the set reproduction power and recording power as addresses. This data is added as an analog value to the current value of the current circuit 107 by the D/A converter 106, and optical power equal to the set value is obtained.

[発明の効果コ 以上、説明したように本発明の光記録再生装置のレーザ
駆動回路を用いると高周波重畳の切り替えや記録再生パ
ワーの変更により生じる電流値の変動を設定パワーをア
ドレスとし、補正値をデータとして記録したデジタルメ
モリを用いて電流値を補正することにより、設定値に等
しいレーザパワーを得ることが可能となるため、信頼性
の高いデータの記録消去が行える。
[Effects of the Invention] As explained above, when the laser drive circuit of the optical recording/reproducing apparatus of the present invention is used, the fluctuation of the current value caused by switching the high frequency superimposition or changing the recording/reproducing power can be adjusted by using the set power as an address and adjusting the correction value. By correcting the current value using a digital memory that records the data as data, it becomes possible to obtain a laser power equal to the set value, so data can be recorded and erased with high reliability.

またレーザの個体差の補正もデジタルメモリーのデータ
を変更することにより、容易に可能である。
Furthermore, individual differences in lasers can be easily corrected by changing the data in the digital memory.

さらに光ディスクの記録再生特性や光学ピックアップの
性能を評価するうλで、高周波重畳の切り替え、記録再
生パワーの変更が調整なしに行えるため有用なデータを
提供するという効果を有する。
Furthermore, when evaluating the recording/reproducing characteristics of an optical disk or the performance of an optical pickup, it is possible to switch high frequency superimposition and change the recording/reproducing power without adjustment, thereby providing useful data.

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

第1図は、本発明の光記録再生装置のレーザ駆動回路を
示すブロック図。 第2図は、本発明を説明するためのレーザの光パワー−
電流特性を示す図。 第3図は、従来の光記録再生装置のレーザ駆動回路のブ
ロック図。 ot 再生パワー設定部 記録パワー設定部 HF0N10FFスイツチ デジタルメモリ 記録電流設定回路 D/Aコンバータ 電流回路 記録データ レーザ 比願人 セイコーエプソン株式会社 代理人 弁理士 鈴木 喜三部(他1名)以上 Iwon:204
FIG. 1 is a block diagram showing a laser drive circuit of an optical recording/reproducing apparatus according to the present invention. Figure 2 shows the optical power of the laser for explaining the present invention.
A diagram showing current characteristics. FIG. 3 is a block diagram of a laser drive circuit of a conventional optical recording/reproducing device. ot Reproduction power setting section Recording power setting section HF0N10FF switch Digital memory recording current setting circuit D/A converter current circuit Recording data laser Higento Seiko Epson Co., Ltd. Agent Patent attorney Kizobe Suzuki (and 1 other person) Iwon: 204

Claims (1)

【特許請求の範囲】[Claims] 光学ピックアップを用い光ディスク、光カードなどの光
記録媒体に情報を記録再生する光記録再生装置のレーザ
駆動回路において、高周波重畳を行った時に生じるレー
ザ駆動電流の変動を補正するために再生レーザパワーと
記録レーザパワーの値をアドレスとし補正値をデータと
して記録したデジタルメモリーと前記補正値をアナログ
値に変換するD/Aコンバーターと前記補正値を高周波
重畳を行わない場合の電流値に加算し駆動電流とする電
流回路からなることを特徴とする光記録再生装置のレー
ザ駆動回路
In the laser drive circuit of an optical recording and reproducing device that uses an optical pickup to record and reproduce information on optical recording media such as optical disks and optical cards, the reproduction laser power and the A digital memory that uses the recording laser power value as an address and records the correction value as data, a D/A converter that converts the correction value into an analog value, and a drive current that adds the correction value to the current value when high frequency superimposition is not performed. A laser drive circuit for an optical recording/reproducing device, characterized by comprising a current circuit having the following characteristics:
JP2225701A 1990-08-28 1990-08-28 Laser driving circuit for optical recording and reproducing device Pending JPH04106736A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2225701A JPH04106736A (en) 1990-08-28 1990-08-28 Laser driving circuit for optical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2225701A JPH04106736A (en) 1990-08-28 1990-08-28 Laser driving circuit for optical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPH04106736A true JPH04106736A (en) 1992-04-08

Family

ID=16833447

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2225701A Pending JPH04106736A (en) 1990-08-28 1990-08-28 Laser driving circuit for optical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPH04106736A (en)

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