JPH04188434A - Current-voltage conversion circuit for optical recording reproducer - Google Patents
Current-voltage conversion circuit for optical recording reproducerInfo
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- JPH04188434A JPH04188434A JP31990790A JP31990790A JPH04188434A JP H04188434 A JPH04188434 A JP H04188434A JP 31990790 A JP31990790 A JP 31990790A JP 31990790 A JP31990790 A JP 31990790A JP H04188434 A JPH04188434 A JP H04188434A
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- 230000003287 optical effect Effects 0.000 title claims abstract description 30
- 230000003321 amplification Effects 0.000 claims 1
- 238000003199 nucleic acid amplification method Methods 0.000 claims 1
- 239000003990 capacitor Substances 0.000 abstract description 24
- 230000006866 deterioration Effects 0.000 abstract description 5
- 238000010586 diagram Methods 0.000 description 7
- 239000002131 composite material Substances 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
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Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、光学式記録媒体からの光情報を光電変換し電
圧情報を得ることのできる光学式記録再生装置の電流電
圧変換回路に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a current-voltage conversion circuit for an optical recording/reproducing device that can photoelectrically convert optical information from an optical recording medium to obtain voltage information.
[従来の技術]
近年、レーザを利用して光学式記録媒体にビットを形成
して情報を記録し、また、光学式記録媒体に形成したビ
ットに基づいて情報を再生して読み出す光学式記録再生
装置が開発されている。光学式記録媒体はディスク状、
または、カード状の形状であり、記録面は複数のトラッ
クに分割されている。さらに、トラックは、リードライ
ト制御に於ける記録単位であるセクタに分割されている
。[Prior Art] In recent years, optical recording and reproducing technology has been developed, in which information is recorded by forming bits on an optical recording medium using a laser, and information is reproduced and read out based on the bits formed on the optical recording medium. A device is being developed. Optical recording media are disc-shaped,
Alternatively, it has a card-like shape, and the recording surface is divided into a plurality of tracks. Furthermore, the track is divided into sectors, which are recording units in read/write control.
光学式記録媒体に情報を記録する場合、効率的に記録す
るために、記録データをは変調符号に変換してから記録
を行う必要がある。When recording information on an optical recording medium, in order to record efficiently, it is necessary to convert the recording data into a modulation code before recording.
この変調符号の中で、信号の極性が反転した場合だけ記
録を行うマーク間記録方法が知られている。この方法で
は、信号の極性が頻繁に反転する区間と、頻繁には反転
しない区間とを比較するとマークの密度に差が生じる。Among these modulation codes, an inter-mark recording method is known in which recording is performed only when the polarity of the signal is reversed. In this method, when a section where the polarity of the signal is frequently reversed is compared with a section where the polarity of the signal is not frequently reversed, a difference occurs in the density of marks.
そのため密度差を一定範囲に制限するための変調符号と
して、RLL変調(Run Length Lim
1ted(:□rding)が知られている。Therefore, RLL modulation (Run Length Lim
1ted (:□rding) is known.
−例として、ISO規格の130mmディスクの連続サ
ーボ方法に採用された(2.7)RLL変調符号に於い
て、最短マーク間隔と最長マーク間隔が隣接した場合の
タイミング図を第3図に示す。 (a)は(2,7)R
LL変調符号を示し、(b)はこの(2,7)RLL変
調符号により記録された記録媒体上のマークを示し、
(C)は光学式ピックアップ(以下、ピックアップと略
記する)により再生された再生信号を示す。- As an example, FIG. 3 shows a timing diagram when the shortest mark interval and the longest mark interval are adjacent to each other in the (2.7) RLL modulation code adopted in the continuous servo method for a 130 mm disc according to the ISO standard. (a) is (2,7)R
LL modulation code is shown, (b) shows a mark on the recording medium recorded by this (2,7) RLL modulation code,
(C) shows a reproduction signal reproduced by an optical pickup (hereinafter abbreviated as pickup).
変調符号により記録されたマークをピックアップで再生
した場合の再生信号は、ピックアップの光学的な周波数
特性が(光源の波長)/(対物レンズのNA)に比例す
るため、マークの区切りを明確に識別することができな
い。そのためマークの再生信号は、マークの前後のマー
クの密度により影響を受ける。この影響は符号量干渉と
呼ばれる。When a mark recorded using a modulation code is reproduced by a pickup, the reproduced signal can clearly identify the mark boundaries because the optical frequency characteristics of the pickup are proportional to (wavelength of light source)/(NA of objective lens). Can not do it. Therefore, the reproduction signal of a mark is affected by the density of marks before and after the mark. This effect is called code amount interference.
第3図(C)に於いて、符号量干渉を起こした再生信号
の最短マーク間隔での振幅をaとし、最長マーク間隔で
の振幅をbとして次のような量を定義する。In FIG. 3C, the following quantities are defined, where a is the amplitude at the shortest mark interval of the reproduced signal that caused code amount interference, and b is the amplitude at the longest mark interval.
MTF= (a/b)* 100 [%]=11)この
MTFの値が小さくなりすぎると、最短マーク間隔の識
別が不可能となる。MTFの下限値は、通常30%程度
である。MTF=(a/b)*100 [%]=11) If the value of this MTF becomes too small, it becomes impossible to identify the shortest mark interval. The lower limit of MTF is usually about 30%.
一方、第47に示すように、再生信号を増幅するため初
段の増幅回路として光学式記録再生装置のt流電正変換
回路30がよく知られている。このt流電正変換回路3
0はバイアス電源31に接続されたディテクタ32で発
生した光電流を電圧に変換する。On the other hand, as shown in No. 47, a t-current current positive conversion circuit 30 of an optical recording/reproducing apparatus is well known as a first-stage amplifying circuit for amplifying a reproduced signal. This t current positive conversion circuit 3
0 converts the photocurrent generated in the detector 32 connected to the bias power supply 31 into a voltage.
ここで増幅器33の帰還抵抗34の抵抗値をRとし、こ
の帰還抵抗34のキャパシタ成分をCとすると、この電
流電圧変換回路30の伝達関数G(S)は
G (s) =E (s)/I (s)=R* (1+
5CR) ・ (2)となり、周波数特性G (f
)は、5=j2πf(j”=−1)として
G(f)=R/ 1+(2πfCR)2 (3)とな
る。Here, if the resistance value of the feedback resistor 34 of the amplifier 33 is R, and the capacitor component of this feedback resistor 34 is C, then the transfer function G(S) of this current-voltage conversion circuit 30 is G (s) = E (s) /I (s)=R* (1+
5CR) ・(2), and the frequency characteristic G (f
) becomes G(f)=R/1+(2πfCR)2 (3) with 5=j2πf(j''=-1).
[発明が解決しようとする課題]
ところで、実際の光学式記録再生装置に於いて、(3)
式がどのような値になるか調べてみる。[Problem to be solved by the invention] By the way, in an actual optical recording/reproducing device, (3)
Let's check what value the expression gives.
IO5規格の13’Ommディスクを3600rpmで
回転させて再生して場合、最短マーク間隔の同期周波数
f、=7.4 [MHz]となり、最長マーク間隔の同
期周波数f、=2.775 [MHz]となる。When playing a IO5 standard 13'Omm disc by rotating it at 3600 rpm, the synchronization frequency f for the shortest mark interval is 7.4 [MHz], and the synchronization frequency f for the longest mark interval is 2.775 [MHz]. becomes.
ココテ、R=20[KΩ]、C=0.3 [pF]とす
ると、それぞれの振幅特性G (f)はG (f、)
=G (7,4’MHz)=0. 963*20[KΩ
コ
G (f、)=G (2,775MHz)=0. 99
5*20[KΩコ
となり、 (4)式及び(5)式より最長マークの振幅
を1としたときのMTFは
MTP= (G (f、) /G (f、) )本10
0= (0,96310,995)*100=96.8
[%]
となる。このことは、電流電圧変換回路でMTFが3.
2%(=100−96.8)低下することを意味する。If R = 20 [KΩ] and C = 0.3 [pF], each amplitude characteristic G (f) is G (f, )
=G (7,4'MHz)=0. 963*20[KΩ
G (f,)=G (2,775MHz)=0. 99
5 * 20 [KΩ], and from equations (4) and (5), when the amplitude of the longest mark is set to 1, the MTF is MTP = (G (f,) /G (f,)) 10
0= (0,96310,995)*100=96.8
[%]. This means that the MTF in the current-voltage conversion circuit is 3.
This means a decrease of 2% (=100-96.8).
MTFの実際の下限値が30%程度であるので、3.2
%の低下は下限値の約107%の劣化に相当する。Since the actual lower limit of MTF is about 30%, 3.2
% decrease corresponds to a deterioration of about 107% of the lower limit.
すなわち、電流電圧変換回路の帰還抵抗に03pFのキ
ャパシタ成分があるだけで、MTFは約10%劣化する
。That is, the presence of a capacitor component of 0.3 pF in the feedback resistance of the current-voltage conversion circuit degrades the MTF by about 10%.
このことを防止するために、抵抗のキャパシタ成分の値
の小さな抵抗を選ぶという方法が考えられるが、このキ
ャパシタ成分は抵抗の構造によりきまるので、キャパシ
タ成分の減少には抵抗の構造上の制限がある。また、抵
抗値を下げるという方法も考えられるが、キャパシタ成
分を半分にした場合と同じ効果を得るためには、抵抗値
を半分に下げる必要があり、抵抗値を半分にすると(3
)式かられかるように、出力も半分に低下してしまいノ
イズに対して弱くなるという問題点がある。One way to prevent this is to choose a resistor with a small value for the capacitor component, but since this capacitor component is determined by the structure of the resistor, there are restrictions on reducing the capacitor component due to the structure of the resistor. be. Another option is to lower the resistance value, but in order to obtain the same effect as when the capacitor component is halved, it is necessary to reduce the resistance value by half, and if the resistance value is halved (3
) As can be seen from the equation, there is a problem that the output is also reduced by half, making it vulnerable to noise.
本発明は、上記事情に鑑みてなされたものであり、抵抗
のキャパシタ成分の値は抵抗値に関係なく抵抗の構造に
より決まることを利用して、抵抗を直列に接続しキャパ
シタ成分だけを減少させ抵抗値を変化させないで、MT
Fの劣化を防止する光学式記録再生装置の電流電圧変換
回路を提供することを目的としている。The present invention was made in view of the above circumstances, and utilizes the fact that the value of the capacitor component of a resistor is determined by the structure of the resistor regardless of the resistance value, and connects resistors in series to reduce only the capacitor component. MT without changing the resistance value
It is an object of the present invention to provide a current-voltage conversion circuit for an optical recording/reproducing device that prevents F deterioration.
[課題を解決するための手段]
本発明の光学式記録再生装置の電流電圧変換回路は、光
学式記録媒体からの戻り光を受光し光電変換できる光電
変換手段と、前記光電変換手段より得られた電流を電圧
に変換しゲインを決める帰還抵抗を備えた増幅手段とか
ら構成される電流電圧変換回路に於いて、前記帰還抵抗
が少なくとも直列に接続された複数の抵抗より構成され
ている。[Means for Solving the Problems] A current-voltage conversion circuit of an optical recording/reproducing device of the present invention includes a photoelectric conversion means capable of receiving and photoelectrically converting returned light from an optical recording medium, and a current-voltage conversion circuit obtained from the photoelectric conversion means. In the current-voltage conversion circuit, the feedback resistor is composed of at least a plurality of resistors connected in series.
[作 用]
本発明では、帰還抵抗が直列に接続された複数の抵抗よ
り構成されているので、所望の抵抗値を得ると共に帰還
抵抗のもつキャパシタ成分を減少させる。[Function] In the present invention, since the feedback resistor is composed of a plurality of resistors connected in series, a desired resistance value can be obtained and the capacitor component of the feedback resistor can be reduced.
[実施例]
以下、図面を参照しながら本発明の実施例について述べ
る。[Example] Hereinafter, an example of the present invention will be described with reference to the drawings.
第1図は本発明の第1実施例に係わり、電流電圧変換回
路の構成を示す構成図である。FIG. 1 is a configuration diagram showing the configuration of a current-voltage conversion circuit according to a first embodiment of the present invention.
第1実施例の(光学式記録再生装置の)電流電圧変換回
路1は、図示しない光学式記録媒体からの光を光電変換
できるディテクタ2と、このディテクタ2より生成され
た光電流を電圧に変換する増幅器3より構成されていて
、前記増幅器3は、キャパシタ4を成分として有する抵
抗5と、キャパシタ6を成分として有する抵抗7とを直
列に接続した帰還抵抗8を介して帰還されている。尚、
前記ディテクタ2にはバイアス電源9が接続されている
。また、前記帰還抵抗8の前記キャパシタ4及び6の値
は共にc [pF]、前記抵抗5及び7の抵抗値は共に
r [KΩ]である。A current-voltage conversion circuit 1 (of an optical recording/reproducing device) of the first embodiment includes a detector 2 that can photoelectrically convert light from an optical recording medium (not shown), and a photocurrent generated by this detector 2 that converts it into a voltage. The amplifier 3 is fed back via a feedback resistor 8 in which a resistor 5 having a capacitor 4 as a component and a resistor 7 having a capacitor 6 as a component are connected in series. still,
A bias power supply 9 is connected to the detector 2 . Further, the values of the capacitors 4 and 6 of the feedback resistor 8 are both c [pF], and the resistance values of the resistors 5 and 7 are both r [KΩ].
このように構成された電流電圧変換回路1の動作は、デ
ィテクタ2で生成された光電流は増幅器3と帰還抵抗8
で電圧に変換される。抵抗5及び7は直列に接続されて
いるので、合成抵抗の値は2倍になり、合成キャパシタ
の値は1/2倍になる。 ここで、 r=10[KΩ]
、 c=o、、3[pF]とすると、合成抵抗値Rおよ
び合成キャパシタ値Cは、
R=2*r=20 [KΩ]
C= (1/2)本c=0.15[pF]となる。また
、振幅特性G (f)は
G(f)=R/、/”璽]丁口了R)2 ・(4)と
なる。The operation of the current-voltage conversion circuit 1 configured in this way is such that the photocurrent generated by the detector 2 is transferred to the amplifier 3 and the feedback resistor 8.
is converted to voltage. Since resistors 5 and 7 are connected in series, the value of the combined resistance is doubled and the value of the combined capacitor is 1/2. Here, r=10 [KΩ]
, c=o,, 3 [pF], then the combined resistance value R and combined capacitor value C are R=2*r=20 [KΩ] C= (1/2) c=0.15 [pF] becomes. Further, the amplitude characteristic G (f) is G(f)=R/, /”〽〇〇〇〇゜゜(4).
図示しない光学式媒体からの光信号、例えば、IO5規
格の130mmディスクを3600rpmで回転させて
再生された光信号による最短マーク間隔及び最長マーク
間隔に対応する同期周波数f0及びflは
f、=7.4 [MHz]
f、=2. 775 [MHzコ
であるので、最短マーク間隔の振幅特性G (f、)及
び最長マーク間隔の振幅特性G(fl)は(4)式より
G (f、) =G (7,4[MHz コ )
=o、 990*20[KΩコ
G (f、) =G (2,775[MHz
コ )=0. 999*20[KΩコ
となり、MTFは
MTF= (G (fo)/G (f、)) *10
0=99.1[%]
となる。すなわち、電流電圧変化回路1のMTFの低下
は09%になる。The synchronization frequencies f0 and fl corresponding to the shortest mark interval and longest mark interval by an optical signal from an optical medium (not shown), for example, an optical signal reproduced by rotating a 130 mm disk of IO5 standard at 3600 rpm, are f, = 7. 4 [MHz] f,=2. 775 [MHz], the amplitude characteristic G (f,) of the shortest mark interval and the amplitude characteristic G (fl) of the longest mark interval are calculated from equation (4) as follows: G (f,) = G (7,4 [MHz )
=o, 990*20[KΩkoG (f,) =G (2,775[MHz
) = 0. 999*20[KΩ, MTF is MTF= (G (fo)/G (f,)) *10
0=99.1[%]. That is, the decrease in MTF of the current-voltage changing circuit 1 is 09%.
このように第1実施例の電流電圧変換回路lは、前述し
た従来例の電流電圧変換回路に比べ、MTFの低下は、
3、 2−0. 9=2. 3 [%]の改善となり、
MTFの下限値に対する相対的な改善量は
(2,3/30)*100=7.7 [%]となる。As described above, the current-voltage conversion circuit l of the first embodiment has a decrease in MTF of 3.2-0. compared to the conventional current-voltage conversion circuit described above. 9=2. It was an improvement of 3 [%],
The amount of improvement relative to the lower limit of MTF is (2,3/30)*100=7.7 [%].
従って、帰還抵抗8を単に分割し直列に接続することに
より所望の合成抵抗を構成するという極めて簡単な回路
構成でMTFの改善ができるので光学式記録再生装置で
容易に実現できる。Therefore, the MTF can be improved with an extremely simple circuit configuration in which a desired combined resistance is constructed by simply dividing the feedback resistor 8 and connecting them in series, so that it can be easily realized with an optical recording/reproducing device.
尚、分割した抵抗5及び7の抵抗値は互いに等しいもの
から構成したが、第1実施例はこれに限らず、所望の合
成抵抗値が得られれば良い。Although the divided resistors 5 and 7 have the same resistance value, the first embodiment is not limited to this, as long as a desired combined resistance value can be obtained.
第2図は本発明の第2実施例に係わり、電流電圧変化回
路の構成を示す構成図である。FIG. 2 is a configuration diagram showing the configuration of a current-voltage changing circuit according to a second embodiment of the present invention.
増幅器3はキャパシタlOを成分として有する抵抗13
と、キャパシタ11を成分として有する抵抗14と、キ
ャパシタ12を成分として有する抵抗15とを直列に接
続した帰還抵抗15を介して帰還されていて、前記帰還
抵抗15のキャパシタ10ないし12の値は共にc=0
.3 [pF]、抵抗13ないし14の値は共にr=2
0/3[KΩ]である。The amplifier 3 includes a resistor 13 having a capacitor lO as a component.
is fed back through a feedback resistor 15 which is a series connection of a resistor 14 having the capacitor 11 as a component and a resistor 15 having the capacitor 12 as a component, and the values of the capacitors 10 to 12 of the feedback resistor 15 are both c=0
.. 3 [pF], the values of resistors 13 and 14 are both r = 2
It is 0/3 [KΩ].
その他の構成及び作用は第1実施例と同じである。Other configurations and operations are the same as in the first embodiment.
このように構成された第2実施例の電流電圧変換回路1
の合成抵抗R及び合成キャパシタCはR=3 本r=2
0[KΩコ
C= (1/3) *C=0. 1 [pFコ
である。Current-voltage conversion circuit 1 of the second embodiment configured in this way
The combined resistance R and combined capacitor C are R=3 pieces r=2
0 [KΩ C= (1/3) *C=0. 1 [pF].
図示しない光学式媒体からの光信号、例えば、IO5規
格の130mmディスクを360Orpmで回転させて
再生された光信号の最短マーク間隔の振幅特性G(fO
)及び最長マーク間隔の振幅特性G (f、)は、前述
の(4)式よりG (f、) =G (7,4[MHz
])=0.997本20[KΩ]
G (f、)=G (2,775[MHz] )=
0. 999*20[KΩ]
となり、MTFは
MTF= (G (f、)/G (f、))* 100
=99.8[%]
となる。すなわち、電流電圧変換回路1のMTFの低下
は02%になる。An optical signal from an optical medium (not shown), for example, the amplitude characteristic G (fO
) and the amplitude characteristic of the longest mark interval G (f,) can be calculated from the above equation (4) as G (f,) = G (7,4[MHz
]) = 0.997 lines 20 [KΩ] G (f,) = G (2,775 [MHz] ) =
0. 999*20[KΩ], and the MTF is MTF= (G (f,)/G (f,))*100
=99.8[%]. That is, the decrease in MTF of the current-voltage conversion circuit 1 is 02%.
このように第2実施例のt流電圧変検回路1は、前述の
従来例の電流電圧変換回路に比べ、MTFの低下は、
3、 2−0. 2=3. 0[%]
の改善となり、さらにMTFの下限値に対する相対的な
改善量は
(3,O/30) 本 100=10 0 [%コ
となり、第1実施例に比較してもさらにMTFは改善さ
れる。As described above, the t-current voltage conversion circuit 1 of the second embodiment has a decrease in MTF of 3.2-0. compared to the conventional current-voltage conversion circuit described above. 2=3. The improvement is 0 [%], and the relative improvement amount to the lower limit of MTF is (3, O/30) 100 = 10 0 [%], and the MTF is further improved compared to the first example. be done.
尚、合成抵抗は2分割或いは3分割した抵抗より構成さ
れた合成抵抗であるが、本実施例はこれに限らず、4分
割以上の任意の数に分割された抵抗より構成された合成
抵抗でも良い。また、合成抵抗は直列接続により構成さ
れているが、抵抗のキャパシタ成分を減少させることが
できるならば、直列及びへいれつ接続により構成される
合成抵抗でも良い。Note that the composite resistance is a composite resistance made up of resistors divided into two or three parts, but this embodiment is not limited to this, and may also be a composite resistance made up of resistors divided into any number of parts, such as four or more. good. Furthermore, although the composite resistor is configured by series connections, it may also be a composite resistor configured by series and interconnect connections as long as the capacitor component of the resistance can be reduced.
抵抗の構造及び材質は本実施例の効果が得られるものな
らばよく、例えば、構造はリード抵抗、チップ抵抗等、
材質はカーボン、金属皮膜等でも良い。The structure and material of the resistor may be any material as long as the effects of this embodiment can be obtained.For example, the structure may be a lead resistor, a chip resistor, etc.
The material may be carbon, metal film, etc.
さらにディテクタは光電変換できるものならば良い。Further, the detector may be one that can perform photoelectric conversion.
[発明の効果]
以上説明したように本発明によれば、本発明の光学式記
録再生装置の電流電圧変換回路は、光学式記録媒体から
の戻り光を受光し光電変換できる光電変換手段と、前記
光電変換手段より得られた電流を電圧に変換しゲインを
決める帰還抵抗を備えた増幅手段とから構成される電流
電圧変換回路に於いて、前記帰還抵抗が少なくとも直列
に接続された複数の抵抗より構成されているので、キャ
パシタ成分だけを減少させ抵抗値を変化させないで、M
TFの劣化を防止することができる。また、構成が単純
なので容易に実現できる。[Effects of the Invention] As explained above, according to the present invention, the current-voltage conversion circuit of the optical recording/reproducing device of the present invention includes a photoelectric conversion means capable of receiving and photoelectrically converting returned light from an optical recording medium; and an amplifying means equipped with a feedback resistor that converts the current obtained from the photoelectric converter into a voltage and determines a gain, the current-voltage conversion circuit comprising at least a plurality of resistors in which the feedback resistor is connected in series. Since the structure is made up of M
Deterioration of TF can be prevented. Moreover, since the configuration is simple, it can be easily realized.
第1図は本発明の第1実施例に係わり、電流電圧変換回
路の構成を示す構成図、第2図は本発明の第2実施例に
係わり、電流電圧変化回路の構成を示す構成図、第3図
及び第4図は従来例に係わり、第3図は(2,7)RL
L変調符号に於けるMTFを説明するタイミング図、第
4図は電流電圧変化回路の構成を示す構成図である。
1・電流電圧変換回路 2・ディテクタ3 増幅器
8・・帰還抵抗、Z’ニー。
ど′
第1図
tuff″t1“1°02
第2図 /−・
第3図
Otoo too I 00 10000000
1 000000010fa)
第4図FIG. 1 is a block diagram showing the configuration of a current-voltage conversion circuit according to a first embodiment of the present invention, and FIG. 2 is a block diagram showing the configuration of a current-voltage changing circuit according to a second embodiment of the present invention. 3 and 4 relate to the conventional example, and FIG. 3 shows (2,7)RL
FIG. 4 is a timing diagram illustrating the MTF in the L modulation code. FIG. 4 is a configuration diagram showing the configuration of the current-voltage changing circuit. 1. Current-voltage conversion circuit 2. Detector 3 Amplifier
8. Return resistance, Z' knee. Do' Figure 1 tuff"t1"1°02 Figure 2 /-・ Figure 3 Otoo too I 00 10000000
1 000000010fa) Figure 4
Claims (1)
光電変換手段と、前記光電変換手段より得られた電流を
電圧に変換しゲインを決める帰還抵抗を備えた増幅手段
とから構成される電流電圧変換回路に於いて、前記帰還
抵抗が少なくとも直列に接続された複数の抵抗より構成
されることを特徴とする光学式記録再生装置の電流電圧
変換回路。A current/voltage device comprising a photoelectric conversion means capable of receiving and photoelectrically converting returned light from an optical recording medium, and an amplification means equipped with a feedback resistor that converts the current obtained from the photoelectric conversion means into voltage and determines a gain. 1. A current-voltage conversion circuit for an optical recording/reproducing device, wherein the feedback resistor is comprised of at least a plurality of resistors connected in series.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31990790A JPH04188434A (en) | 1990-11-22 | 1990-11-22 | Current-voltage conversion circuit for optical recording reproducer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31990790A JPH04188434A (en) | 1990-11-22 | 1990-11-22 | Current-voltage conversion circuit for optical recording reproducer |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04188434A true JPH04188434A (en) | 1992-07-07 |
Family
ID=18115561
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31990790A Pending JPH04188434A (en) | 1990-11-22 | 1990-11-22 | Current-voltage conversion circuit for optical recording reproducer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04188434A (en) |
-
1990
- 1990-11-22 JP JP31990790A patent/JPH04188434A/en active Pending
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