JPS63214922A - Semiconductor laser driving circuit - Google Patents
Semiconductor laser driving circuitInfo
- Publication number
- JPS63214922A JPS63214922A JP62048265A JP4826587A JPS63214922A JP S63214922 A JPS63214922 A JP S63214922A JP 62048265 A JP62048265 A JP 62048265A JP 4826587 A JP4826587 A JP 4826587A JP S63214922 A JPS63214922 A JP S63214922A
- Authority
- JP
- Japan
- Prior art keywords
- write data
- signal
- semiconductor laser
- circuit
- pit
- 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.)
- Granted
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 23
- 230000010355 oscillation Effects 0.000 claims abstract description 11
- 230000007274 generation of a signal involved in cell-cell signaling Effects 0.000 claims abstract description 7
- 230000003287 optical effect Effects 0.000 claims description 8
- 230000000630 rising effect Effects 0.000 claims description 3
- 230000007704 transition Effects 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 7
- 230000000694 effects Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 2
- 230000002123 temporal effect Effects 0.000 description 2
- 239000003990 capacitor Substances 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
Landscapes
- Optical Head (AREA)
- Optical Recording Or Reproduction (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、半導体レーザを光源として用い情報の記録再
生を行う光学式記録再生装置の半導体レーザ駆動回路に
関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a semiconductor laser drive circuit for an optical recording/reproducing device that records and reproduces information using a semiconductor laser as a light source.
従来半導体レーザを用いた光学式記録再生装置では、情
報記録時においてはバイアス電流に加算する形で、外部
から与えられるライトデータでパルス電流を印加して半
導体レーザを駆動する。記録方式としては、ピットの打
無に情報を持ちピットの間隔を変えて記録を行うピット
位置記録と、ピットの両端に情報をもたせるeット長変
調記録がある。ピット位置記録の場合は各々のピットの
時間的長さは、常に一定であるが、ピット長変調記録の
場合においては、それぞれのピットの時間的長さがデー
タにより変調を受けて変化する。In a conventional optical recording/reproducing device using a semiconductor laser, when recording information, the semiconductor laser is driven by applying a pulse current based on external write data in addition to a bias current. There are two types of recording methods: pit position recording, in which information is recorded in the presence or absence of pits, and recording is performed by changing the interval between pits, and e-t length modulation recording, in which information is recorded in both ends of pits. In the case of pit position recording, the temporal length of each pit is always constant, but in the case of pit length modulation recording, the temporal length of each pit is modulated by data and changes.
しかし、前述の従来技術では、記録しようするピットと
実際に記録されたピットを1丁生したり−ドデータの波
形の間にずれが生じてしまう。この様子を第2図に示す
、この原因は記録媒体上へのピット形成は熱的エネルギ
ーで行うためであり、すなわちビット部分は高パワーの
レーザ照射をすることにより記録をする。しかし、記録
レーザ光の移動方向に熱が偏るために、ピッ)終端では
温度が上がり過ぎて、リードデータ24と、ライトデー
タ12には、Lr、Lmのずれができてしまう。この現
象はピット長の長いピットにおいて顕著である。従って
ピットを再生したリードデータは、ジッタを多く含み信
頼性の低いものとなりエラーレートが悪化する。However, in the above-mentioned prior art, a gap occurs between the pits to be recorded and the pits actually recorded, or the waveform of the recorded data. This situation is shown in FIG. 2. The reason for this is that pits are formed on the recording medium using thermal energy, that is, the bit portions are recorded by irradiating a high-power laser. However, since the heat is biased in the moving direction of the recording laser beam, the temperature rises too much at the end, resulting in a deviation of Lr and Lm between the read data 24 and the write data 12. This phenomenon is remarkable in pits with long pit lengths. Therefore, the read data obtained by reproducing the pits contains a lot of jitter and has low reliability, resulting in a worsening of the error rate.
そこで本発明は従来のこのような問題点を解決するもの
で、その目的とするところはジッタが少な(信頼性の高
いリードデータが得られるようなピットを記録すること
のできる、半導体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 conventional problems, and its purpose is to provide a semiconductor laser drive circuit that can record pits with low jitter (reliable read data can be obtained). Our goal is to provide the following.
本発明の半導体レーザ駆動回路は、
(a)半導体レーザを光源として用いて情報の記録再生
を行う光学式記録再生装置の半導体レーザ駆動回路にお
いて、
(b)記録信号1(以下ライトデータ1と呼ぶ)の立ち
上がりにより、一定時間幅Tのゲート信号を生成するゲ
ート信号生成回路と、
(e)前記ライトデータlの打する周波数帯域よりも十
分高い周波数のパルス波を発生ずる発振回路と、
(d)前記ライトデータ1と前記ゲート信号生成回路と
前記発振回路の出力から、ライトデータ1の中でゲート
信号長Tより長い部分が前記/A振回路よりのパルス波
でチロフプされたライトデータ2を生成する論理回路と
、
(e)前記ライトデータ2により、情報記録時に半導体
レーザをパルス駆動するパルス電流駆動回路からなるこ
とを特徴とする。The semiconductor laser drive circuit of the present invention includes: (a) a semiconductor laser drive circuit for an optical recording and reproducing device that records and reproduces information using a semiconductor laser as a light source; (b) recording signal 1 (hereinafter referred to as write data 1); ); (e) an oscillation circuit that generates a pulse wave with a frequency sufficiently higher than the frequency band of the write data l; (d) ) From the write data 1 and the outputs of the gate signal generation circuit and the oscillation circuit, write data 2 is generated in which the portion of the write data 1 that is longer than the gate signal length T is tilofupped by the pulse wave from the /A oscillation circuit. and (e) a pulse current drive circuit that pulse-drives a semiconductor laser when recording information using the write data 2.
本発明の上記の構成によれば、ライトデータ2はライト
データ1に比べ、一定時間幅Tより長いデータに対し、
その後半が高周波でチーツブされているため、この信号
で半導体レーザを駆動すれば、ピット終端で記録媒体の
温度が上昇しすぎることなく、本来のライトデータで記
録しようとするピット長と同じ長さのリードデータが再
生される。According to the above configuration of the present invention, compared to write data 1, write data 2 is longer than a certain time width T,
Since the latter half is cheated with high frequency, if you drive the semiconductor laser with this signal, the temperature of the recording medium will not rise too much at the end of the pit, and the pit length will be the same as the original write data. The read data is played back.
第1図は本発明の半導体レーザ駆動回路のブロック図、
第3図は本発明の一実施例における主要部分の回路図で
ある。以下図面に基づいて詳細に説明する。FIG. 1 is a block diagram of a semiconductor laser drive circuit of the present invention,
FIG. 3 is a circuit diagram of the main parts in one embodiment of the present invention. A detailed explanation will be given below based on the drawings.
まずm1図において、半導体レーザ1の光出力はモニホ
トダイオード2でモニタされ、l−V変換増幅回路3に
より電流信号から電圧信号に変換増幅され、光出力が電
圧値として得られる。この値と基準電圧4とを差動増幅
回路5で差をとり、設定した光出力との差かえられる。First, in FIG. m1, the optical output of the semiconductor laser 1 is monitored by the monophotodiode 2, and converted and amplified from a current signal to a voltage signal by the l-V conversion amplifier circuit 3, and the optical output is obtained as a voltage value. The difference between this value and the reference voltage 4 is taken by a differential amplifier circuit 5, and the difference is then changed from the set optical output.
この差信号により、バイアス電流駆動回路0は半導体レ
ーザ1に流すバイアス電流を制御して、半導体レーザの
光出力が温度変化等によらずに一定となるように、いわ
ゆるAI)C(Δu L o a L i c I’
o wcr ConLrol)が行われる。Based on this difference signal, the bias current drive circuit 0 controls the bias current flowing through the semiconductor laser 1, so that the optical output of the semiconductor laser remains constant regardless of temperature changes, etc. a L i c I'
o wcr ConLrol) is performed.
次にライト時の動作について説明する。第1図中で、本
発明の主要部分であるゲート信号生成回路7と、発振回
路8と論理回路1)の具体的な回路図を第3図に、各部
信号波形を第4図にそれぞれ示す。端子11からはライ
トデータ1が人力される。第4図中位号12がそれであ
る。ゲート信号生成回路7は、ワンショットマルチバイ
ブレータで構成されており、ゲート時間Tは抵抗Rとコ
ンデンサCで定められる。ライトデータ1がクロック入
力端子へ人力され、立ち上がりでトリガがかかり、時間
幅Tの信号が出力端子Qより出力される。(信号13)
一方、発振回路8はこの場合水晶振動子を用いて実現し
ている。(信号14)図中点線で囲った部分9が論理回
路で、イ/バータと2人カアンドゲートで構成されてい
る。論理回路9の出力信号15は第4図に示すように、
ゲート時間Tよりも短い信号はそのまま、長いものは立
ち上がりからTの後の部分が信号14でチjツブされて
いて、これがライトデータ2である。ライトデータ2に
より半3D体レーザ1をパルス電流駆動回路10でパル
ス駆動してライトデータの記録を行う。なお他の方法と
してゲート信号生成回路は遅延素子(例えばディレィラ
イン等)を用いて簡単に実現できる。Next, the operation during writing will be explained. In Fig. 1, a specific circuit diagram of the gate signal generation circuit 7, oscillation circuit 8, and logic circuit 1) which are the main parts of the present invention is shown in Fig. 3, and signal waveforms of each part are shown in Fig. 4. . Write data 1 is input manually from the terminal 11. This is the middle number 12 in Figure 4. The gate signal generation circuit 7 is composed of a one-shot multivibrator, and the gate time T is determined by a resistor R and a capacitor C. Write data 1 is input to the clock input terminal, a trigger is activated at the rising edge, and a signal with a time width T is output from the output terminal Q. (Signal 13)
On the other hand, the oscillation circuit 8 is realized using a crystal resonator in this case. (Signal 14) A portion 9 surrounded by a dotted line in the figure is a logic circuit, which is composed of an in/verter and a two-man AND gate. The output signal 15 of the logic circuit 9 is as shown in FIG.
Signals shorter than the gate time T are left as they are, and signals longer than the gate time T are ticked by the signal 14 from the rising edge, and this is write data 2. Based on the write data 2, the semi-3D body laser 1 is pulse-driven by the pulse current drive circuit 10 to record the write data. Alternatively, the gate signal generation circuit can be easily realized using a delay element (for example, a delay line).
以上述べたように本発明によれば、次の様な効果がもた
らされる。第4図において、信号12のライトデータ1
に対して、半導体レーザを駆動するのは信号!5のライ
トデータ2であり、記録されたビットは、25.2G、
27の様になる。本来記録しようとしていたビット長と
同じ長さに、ずなわちライトデータ1での時間と等しく
なっている。この結果、再生されたリードデータ28は
、リードデータ24と比ベピットによる時間ずれが無く
、シックが少なく信頼性の高いものとなる。また本発明
は特にピットの両端に情報を持たせたピット長変調方式
の場合に効果が大きいのは言うまでもない。As described above, according to the present invention, the following effects are brought about. In FIG. 4, write data 1 of signal 12
On the other hand, it is the signal that drives the semiconductor laser! 5 write data 2, the recorded bits are 25.2G,
It will look like 27. The length is the same as the bit length that was originally intended to be recorded, that is, it is equal to the time for write data 1. As a result, the reproduced read data 28 has no time lag with respect to the read data 24 due to pitting, and is highly reliable with fewer sicks. It goes without saying that the present invention is particularly effective in the case of a pit length modulation method in which information is provided at both ends of a pit.
第1図は、本発明の半導体レーザ駆動回路のブロック図
。
第2図は、従来例の場合のライトデータとピット及びリ
ードデータの関係を示す図。
m3図は、本発明の一実施例における主要部分の具体的
な回路図。
第4図は、第3図の各部信号波形図。
1・・・半導体レーザ
2・・・ゲート信号生成回路
8・・・発振回路
0・・・論理回路
以 上
出願人 セイコーエプソン株式会社
代理人 弁理士 最 上 務 他1名躬4mFIG. 1 is a block diagram of a semiconductor laser drive circuit according to the present invention. FIG. 2 is a diagram showing the relationship between write data, pits, and read data in a conventional example. Figure m3 is a specific circuit diagram of main parts in an embodiment of the present invention. FIG. 4 is a signal waveform diagram of each part of FIG. 3. 1...Semiconductor laser 2...Gate signal generation circuit 8...Oscillation circuit 0...Logic circuit or above Applicant: Seiko Epson Co., Ltd. Agent Patent attorney Tsutomu Mogami and 1 other person 4m
Claims (1)
録再生を行う光学式記録再生装置の半導体レーザ駆動回
路において、 (b)記録信号1(以下ライトデータ1と呼ぶ)の立ち
上がりにより、一定時間幅Tゲート信号を生成するゲー
ト信号生成回路と、 (c)前記ライトデータ1の有する周波数帯域とりも十
分高い周波数のパルス波を発生する発振回路と、 (d)前記ライトデータ1と前記ゲート信号生成回路と
前記発振回路の出力から、ライトデータ1の中でゲート
信号長Tより長い部分が前記発振回路よりのパルス波で
チョップされたライトデータ2を生成する論理回路と、 (e)前記ライトデータ2により、情報記録時に半導体
レーザをパルス駆動するパルス電流駆動回路からなるこ
とを特徴とする、半導体レーザ駆動回路。(1) (a) In the semiconductor laser drive circuit of an optical recording and reproducing device that records and reproduces information using a semiconductor laser as a light source, (b) the rising edge of recording signal 1 (hereinafter referred to as write data 1) (c) an oscillation circuit that generates a pulse wave having a sufficiently high frequency in the frequency band of the write data 1; (d) the write data 1 and the gate; a logic circuit that generates write data 2 in which a portion of write data 1 that is longer than the gate signal length T is chopped by a pulse wave from the oscillation circuit from the output of the signal generation circuit and the oscillation circuit; A semiconductor laser drive circuit comprising a pulse current drive circuit that pulse-drives a semiconductor laser during information recording using write data 2.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62048265A JP2573832B2 (en) | 1987-03-03 | 1987-03-03 | Semiconductor laser drive circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62048265A JP2573832B2 (en) | 1987-03-03 | 1987-03-03 | Semiconductor laser drive circuit |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63214922A true JPS63214922A (en) | 1988-09-07 |
JP2573832B2 JP2573832B2 (en) | 1997-01-22 |
Family
ID=12798605
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62048265A Expired - Lifetime JP2573832B2 (en) | 1987-03-03 | 1987-03-03 | Semiconductor laser drive circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2573832B2 (en) |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02244430A (en) * | 1989-03-17 | 1990-09-28 | Nec Home Electron Ltd | Recorder |
JPH02304730A (en) * | 1989-05-19 | 1990-12-18 | Nikon Corp | Method and device for modulating laser power for recording |
JPH0431420U (en) * | 1990-06-29 | 1992-03-13 | ||
JPH04255914A (en) * | 1991-02-07 | 1992-09-10 | Taiyo Yuden Co Ltd | Optical information recording method |
JPH05143990A (en) * | 1991-11-15 | 1993-06-11 | Taiyo Yuden Co Ltd | Method and device for recording optical information |
JPH05143991A (en) * | 1991-11-15 | 1993-06-11 | Taiyo Yuden Co Ltd | Method and device for recording optical information |
JPH0660380A (en) * | 1992-08-14 | 1994-03-04 | Nec Corp | Optical disk device |
US5469422A (en) * | 1993-01-18 | 1995-11-21 | Nec Corporation | Writing and erasing information by varying the temperature of an optical recording medium |
-
1987
- 1987-03-03 JP JP62048265A patent/JP2573832B2/en not_active Expired - Lifetime
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02244430A (en) * | 1989-03-17 | 1990-09-28 | Nec Home Electron Ltd | Recorder |
JPH02304730A (en) * | 1989-05-19 | 1990-12-18 | Nikon Corp | Method and device for modulating laser power for recording |
JPH0431420U (en) * | 1990-06-29 | 1992-03-13 | ||
JPH04255914A (en) * | 1991-02-07 | 1992-09-10 | Taiyo Yuden Co Ltd | Optical information recording method |
JPH05143990A (en) * | 1991-11-15 | 1993-06-11 | Taiyo Yuden Co Ltd | Method and device for recording optical information |
JPH05143991A (en) * | 1991-11-15 | 1993-06-11 | Taiyo Yuden Co Ltd | Method and device for recording optical information |
JPH0660380A (en) * | 1992-08-14 | 1994-03-04 | Nec Corp | Optical disk device |
US5469422A (en) * | 1993-01-18 | 1995-11-21 | Nec Corporation | Writing and erasing information by varying the temperature of an optical recording medium |
Also Published As
Publication number | Publication date |
---|---|
JP2573832B2 (en) | 1997-01-22 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
EXPY | Cancellation because of completion of term |