JPS58211370A - Tracking servo signal generator of information reader - Google Patents

Tracking servo signal generator of information reader

Info

Publication number
JPS58211370A
JPS58211370A JP9328582A JP9328582A JPS58211370A JP S58211370 A JPS58211370 A JP S58211370A JP 9328582 A JP9328582 A JP 9328582A JP 9328582 A JP9328582 A JP 9328582A JP S58211370 A JPS58211370 A JP S58211370A
Authority
JP
Japan
Prior art keywords
detection
light
output
stage
phase
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
Application number
JP9328582A
Other languages
Japanese (ja)
Other versions
JPH0154780B2 (en
Inventor
Seiichi Osawa
誠一 大沢
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.)
Pioneer Corp
Original Assignee
Pioneer Corp
Pioneer Electronic 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 Pioneer Corp, Pioneer Electronic Corp filed Critical Pioneer Corp
Priority to JP9328582A priority Critical patent/JPS58211370A/en
Publication of JPS58211370A publication Critical patent/JPS58211370A/en
Publication of JPH0154780B2 publication Critical patent/JPH0154780B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/08Disposition or mounting of heads or light sources relatively to record carriers
    • G11B7/09Disposition or mounting of heads or light sources relatively to record carriers with provision for moving the light beam or focus plane for the purpose of maintaining alignment of the light beam relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following
    • G11B7/0901Disposition or mounting of heads or light sources relatively to record carriers with provision for moving the light beam or focus plane for the purpose of maintaining alignment of the light beam relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following for track following only

Landscapes

  • Moving Of The Head To Find And Align With The Track (AREA)
  • Optical Recording Or Reproduction (AREA)
  • Control Of Position Or Direction (AREA)

Abstract

PURPOSE:To eliminate completely noise components due to the shift of an optical axis, etc., by using only the high band component of a tracking information signal to perform so-called in-phase wave detection and then generating a tracking servo signal. CONSTITUTION:The outputs of amplifiers 10a and 10b which amplify the outputs of photoelectric transducers 9a and 9b are applied to an adder 17 and a subtractor 18. These addition and subtraction outputs are turned into the output of a multiplier 20 via an HPF19a and HPF19b respectively. This output of multiplication is applied to an equalizer 13 via an HPF21 and then amplified by a driving amplifier 14 to be used to a driving signal of a coil 8.

Description

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

本発明は情報読取り装置にJハノるトノッ1ングリーボ
イ8月発住装置に関づる(ンの−(・ある。 例えば光学式情報読取り装置にJj GJるl・ソツ4
−ングリーボ制御I装置とし−(第1図(2−小り如さ
構成のものがある1、すなわら、レーリ゛光源1J、り
の照射光栄は、レンズ2.ビームスノリツタ3.1 ′
4波長根4BCび対物レンズ5)を経−(6(1録ノイ
スク6の記録面へ入射する。対物レンズりk: J、リ
レーリ゛光は収東uしめられ(iiL!録面1縁面微小
<(情報検出点とし−(のビック7/ツ/光スボツl’
 ニー’ %る、。 この1゛イスクロによる反射光(×は透過光)は、ビー
ムスプリッタ3により分離され(組の尤−を変換系r9
a、9bの各受光向lに照射される3゜両尤電変換素i
’−9a、9bの出力は増幅ムlOa。 10b及びLPt<++−パスノCルタ) 1 ’l 
il 。 1’lbを人々経て差動アン112へ印加される。1こ
のit出力がイー1ライリ゛13を介しく駆動ノ′ンノ
1/Iへ入力され、対物レンズ5を1へノックII′I
父ノ°ノ向に移動さけるための駆動」イル8の駆動11
1号とな−J Tいる。 絹の光本変換木了9a、9bは、第2図(−小づように
 本の分割線9c1.こよりイの受光向か分割されたご
とく取付(〕られて、+3す、この分割線9Cは記録l
〜ノック接線り向(−矢印Yに−(示し−(いる。)に
・Illとされ、かつ光スポットの反射光の光軸7−に
関し
The present invention relates to an information reading device that has an optical information reading device.
- As a green control I device - (Figure 1 (2) There is a small configuration 1, that is, a ray light source 1J, the irradiation light is a lens 2, a beam snoritter 3.1'
The 4-wavelength root 4BC and the objective lens 5) are incident on the recording surface of the optical disk 6 (6). Minute <(Information detection point-(big 7/tsu/optical tube l'
Knee'%ru,. The reflected light (X is transmitted light) by this 1" iscro is separated by a beam splitter 3 (the combination of the beams is converted into a conversion system r9
3° double-likelihood electric conversion element i irradiated in each light receiving direction l of a and 9b
The outputs of '-9a and 9b are amplified by 10a. 10b and LPt<++-Pasno Cruta) 1 'l
il. 1' lb is applied to the differential amplifier 112 via the signal line. 1 This IT output is input to the drive knob 1/I via the E1 relay 13, and knocks the objective lens 5 to 1 II'I.
Drive 11 of Ile 8 to avoid moving in the father's direction
No. 1-JT is here. The silk light conversion wood 9a, 9b is attached as shown in Fig. 2 (-small book dividing line 9c1. is a record
~ knock tangent direction (- arrow Y - (indicated) - (is) Ill, and with respect to the optical axis 7- of the reflected light of the light spot

【これら糸r≦)a、gbが対称となる様に設【ノ
られくいる。1尚、7Cよ入射光光軸ぐあり、15はノ
′イスク回転用スピン1−ルし一タを示している。。 第3図はノ“イスクロ1の記録1〜ノツクを構成づるピ
ッ1へ16−1.16−2.16−3と情報検di )
Illとしての光スポットS(lとの関係を小り図ぐあ
る9、この先スポットStJの中心がピッI・列りなわ
ら記録トラックの中心線10の1に沿って、助劾t[)
から順次図面の右1ノ向へ所定相対達磨をもつ(移動し
た場合にお(〕るアンプ10a、10bの各出ツノ波形
(イ)、(+1)が第4図(A)。 (B )に大々示されている。これら両波形(イ)。 ([])のiPF 11a 、1 lbを経た出力は夫
々第4図(Δ>、(B)の(ハ)、  (−)の如くな
る。よって、この時の差#1IJ7ンノ12の出力は第
7図の(ホ)に示づように零レベルとなりトラン1ング
エラーが存在t!ヂ正確なトソッ4−ングがなされCい
ることを示しくいる。 次に、記録トラックの偏心によるトノッ1シグヂれ秀の
原因にJ、り光スポット中心が1へノック、−++交り
向(X>へす゛れ(4J3図の六線S1の5」、)(、
゛なり、これが点線11にd>−>て図面のイi /J
向l\移動した場合、7/ン−プ10a 、 10bの
各出力波形〈イ)、(1’l)は第5図(△)、N()
i、−人々小づ(イ)、(II>の如<’(Nる。1こ
れら両波形〈イ)、([1)のI−、pH1a 、1 
lbをR1、出ノJ(,1人々第5)図(A)、(]3
)の(ハ) 、  (−) k:(1)、1、うになる
から、差vJ/ンプ12の出力には第1図の(へ)に承
りように(−′l極↑11のf−)−イ?1S2か1ノ
られる。−乃、光スポツト中心が第3図の 点鎖線S−
のようにX方向にり′れて 点鎖線1−に冶・りて図面
の右り向−へ移動した場合、/ジノ10a。 10F+の各出力波形が第0図(△)、(+3)の(イ
)、(I])!ご人々丙、され−(’ J>す、両波形
のIPFlla、iqbを経た出カバ人々’Ji 6図
< A )、(B)の(ハ)、()のようになる2、3
J、)−(差動)Iシブ12の出力には第7図の(1〜
)の如く1]極竹の1ノーイ昌シJが得られる。 以1のことから判るように、X−動ノ/シ112の出力
には、ピックアップ光スボツ1へ中心が記録i〜ソノツ
ク中14\線10tご対しトノツク+[!1交/J向×
のい(rれに偏イ、コしたかによりit負極竹をとり、
まIJイの11Ii仙量に二応じた大きさをとる(i’
; ;’rが1けられるからこれがトノツlングリ〜ホ
信Bとなるの(゛ある。 かかるトラツA−ングリーボIS舅発生装置では以1の
ように41ii成され−(いるの(゛、2−)の光重°
塵換木f’9a 、≦)bの受光面を光軸7 ’−L二
対し1F確に対称に配置し′C段【」る必要がある1、
し、かじ、1■確に対称に設りることは極め(困難−(
・・ありまた−J’イスクロの而触れによる光軸7−の
り゛れによつ(もイの対称性が悪くなり、この時たとえ
ピックツ1ツブ光スボッ1−がi[確にトノツクを追跡
しくいでも、[−1つ「11a、11bの出力は等しく
ならづ゛、結果とし【1〜>ツーlングリーボ系に小人
な[−1椋碩ずれを生ずるという欠点がある。 本発明の目的は、受光面の対称づ゛れや光軸d゛れ等に
起因するト・ラフ1−ングリーボ15号への悪影響を防
II シ’C11確な1〜ノツ−1ングゐり御がI】J
能なトノッ1ングリー小4i、舅発1装置を提供t16
(−とぐある。 A発明による1−フッ1−ング1) 小lit Sj介
11装置は、ピック7ツl情報検出点のトノツクll’
4交lJ向にJjりる偏倚量に対応しく検出用ツノ相り
間にΔが生じる。J、うに設()られた−組の検出手段
と、この−紺の検出1段の検出出力の高域成分の差17
1号4得る1段と、この 組の検出1段の検出出力の高
域成分の和信号ど当該差(ii号どの位相Δに対応17
た極付を右しか′つclの差信号レベルに対応〔、た1
ノベルを石りる1シ一信号を光11!lる手段とを含む
ことを特徴としている3゜ 以トに図面により本発明を説明づる3゜第E3図は本発
明の実施例の回路図(・あり、第1図とJrij等部分
はII′I〕−0月にJ、り示♂れ(Jjりでの説明は
省略づる。各光電変換素子9a、911の出力を増幅4
る77ンブ10a、10bの各出力は加算器17及び減
紳器18へ人々111加される。加篩出力は111) 
l’ (バイパスノイルタ)19aを介し、また減算出
力はII+)+19bを介し人/イ東0器20の各人力
とへつ(いる。(二の東q出ツノは11]121を介し
くイ1ノイザ1ご3へ印加され、これが駆動ノ′ン/’
1/lにより増幅され゛(’lイルε3の駆動イ、)シ
」と4cるの(・ある。 第0図及び第10図は第8図の回路装置の各部動作波形
図(・あり、第9図(△)は′:)S3図に小すよ)l
、:尤スポットS oが記録トノツク中心線10に治っ
て図面右り向l\移e?る。&i合の加算器17の出力
波形を示しくいる。この7111 Ell器17の出力
は受光1「1已)a 、9bの非対称t!1名しくは光
軸7′のずれの影響を【よとんと受iJないし、まIご
光スポットが1〜ノック中心線1−0に対し直交り向X
に偏倚して第3図の点線[Iや1−4を移動した場合の
加算器17の出力の波形変化は無視りるものといる。 第9図(13)は光軸7−の4“れがイ1い場合のJ[
書簡の減紳器18の出力波形(・あり、点線及び一点鎖
線の各波形が人々第3図にJ31〕る光スポットS十及
びS−が点線1−骨及び 点鎖線し−1を移動じ!、二
場合を小しくいる1、尚、光スポット光コS儀・が]・
ノック中心線;0を移動しくいる11規の場合の減粋器
18の出力は当然に有レベルとな)(いる。 第9図(0)は光軸7″か光電変換素子931゜9bの
分割線9Cの略自交IJ向にづ゛れl、場合の減粋器1
8の出力波形であり、点線及び +:、1鎖線の各波形
が大々第3図にお()る光スポットSL及びS−が点線
[−1及び一点鎖線]−1を移動し/J−合を小しくい
る。図(C)の実線は光スポットSOが中心線101を
移動し/cvA合(・あり、減C>器18の出力には光
軸7′のり“れに対応しtごl) CAノセットαが重
畳されており、このAルットαが光軸7′のずれによる
雑品成分とな)(いるのである。 次に第10図を参照りれは、図(A)は加Q器17の加
締出力の11P)=19.3を紅だ(ir +−;波形
(・ある。1図(13)は減紳器1E3の減0出力の1
11)+19bを経た信号波形(パあり、It P l
” 19 bの作用にJ、る雑音成分【・あるD CA
)しツ1〜αか除ノ、されIこbのとなってJjすr:
、<線、  J:、を鎖線及び実線(11,+f間軸に
 致〉が第9図(O)の点線2 点鎖線及び実線の各波
形に人々対応しくいる1、第10図(C)は東粋器20
に、」、る東弾出力波形(・あり、同様に白線、一点鎖
線及び実線が同図(13)の各線の波形と人々対応して
いる。、この乗Q出力の(1)I−21を経/Jイi月
波形が第10図(1)〉の如くなり、夫々第7図の例と
11+1様に1F確tJ、 l・ノッ(レグ1ノー化月
と4つ(いることが判る。 換d7れば、第10図(A)に小づ加ζ) 70力の高
域成分と同図()3)に示づ減粋出ツノの高域成分とは
、トラック自交プノ向×にaハノる光スポットの偏倚り
向に応じて同相又G、L逆相の関係にあり、減算出力の
高域成分レベルは当該光スポラI・の偏(6+量に比例
しくいることから、乗幹器20及び1F)F−21によ
りいわゆる同相検波を行″)−Cいるのである。すなわ
ら、この同相検波にょっ−(、乗眸器20の2人力が同
相にあれば11つ1−21の出力は11極竹(点鎖線)
ぐあり、逆相にあれば負極性く点線〉となり、ぞの絶対
値レベル(よ偏倚φに比例づるの(ある3゜ 従・) (,1ll)l’ 10;iの出力を第′(0
図(1)のJ、うに矩形波に波形整形しくレベルを A
I化17、この9J1形波によりI−I P r 19
 bの出力をX(ツJングし−ct)同様に乗韓結末が
得られ【いtlゆる同相検波が可能である。狛に、この
矩形波を用いねば、−ぞのレベルは 電化されCいるの
て゛、光軸づ”れLによる加斡器17の加静出力のLノ
ベル変動があ−)ても常に正確なトノッ1ング1ノー1
,1号が1!Iられるし、東p器20の構成り 、1.
、rツJング回路を用いれば良く命中化される1゜ まl、:、他の/j ?Aとしくは、tlt)119a
の+1弦波出力の1及び負ピーク時人ノイ1c11期し
くIll’119bの出力をリンゾルホールドしこの両
車−ルト出力の差をとようにしCム全く同様(ご同相検
波/lX川能用なる。 尚、1ilj!例−(−44情報検出点の一伺手段とじ
(対物レンズbを用い(いるが、いわゆるトノッ1ング
ミーノー等の仙の手段を用い(も1Ωく、3Lだ光学式
に限らず他の例えは静電方式等であ−)−(シまい。 史に(よ記録媒体は〕゛イスク状に限定されるしの“(
・番よ イ鉱 い 1゜ 叙1の如く、本発明によればトノッ1ング情報伝りの^
酸成分のみを用い(いわゆる1【J1相検波をなづよう
tこしくl・フッ1ングリー小(ii >’jを光′1
げるようにシノー(いるから、光軸ずれ等に起因する低
域の雑?1成分を完全に除去でさI[確な1〜ノッ−1
ングリーボa+制御がi+J能となる1゜
[These threads r≦] a and gb are set so that they are symmetrical. 1. 7C is the optical axis of the incident light, and 15 is the spin wheel for rotating the disk. . Figure 3 shows "Iscro 1 record 1 to 16-1.16-2.16-3 and information detection di)
The relationship between the light spot S (Ill) and the light spot S (I) is shown below.Then, the center of the spot StJ is aligned with the pitch I, and along the center line 10 of the recording track, the center line 10 of the recording track is t[).
Figure 4 (A) shows the output horn waveforms (A) and (+1) of the amplifiers 10a and 10b, which have a predetermined relative darism (when they are moved sequentially from 1 to the right in the drawing). (B) These two waveforms (A) are shown in Figure 4 (Δ>, (C) and (-) in (B)). Therefore, at this time, the output of the difference #1 IJ7 and 12 becomes zero level as shown in (e) of Fig. 7, indicating that there is a running error and that accurate switching has been carried out. Next, the cause of the tonnage shift due to the eccentricity of the recording track is J, the center of the light spot knocks to 1, -++ cross direction (X > 5) ”,)(,
゛, this is d>-> on the dotted line 11, i/J in the drawing.
When moving in the direction l\, the output waveforms of 7/amps 10a and 10b (a) and (1'l) are shown in Fig. 5 (△) and N ().
i, - people's small (a), (II> like <' (Nru. 1) Both of these waveforms (a), ([1) I-, pH1a, 1
lb to R1, Deno J (,1 people 5th) Figure (A), (]3
) of (c), (-) k: (1), 1, so the difference vJ/amplifier 12 output has (-'l pole ↑ f of 11) −)−I? 1S2 or 1 no. -No, the center of the light spot is the dotted chain line S- in Figure 3.
If you turn to the X direction, follow the dotted chain line 1, and move to the right in the drawing, /Jino 10a. Each output waveform of 10F+ is (A), (I]) in Fig. 0 (△), (+3)! The output of both waveforms through IPFlla and iqb is as shown in Figure 6 (A), (B) (c), () 2, 3
J, )-(differential) The output of the I-sib 12 is as shown in FIG.
), 1] Gokutake's 1 Noi Masashi J is obtained. As can be seen from the above, the output of the X-movement/shaft 112 shows that the center of the optical pickup slot 1 is recorded i~sonok 14\line 10t and the center + [! 1/J direction
Depending on whether it is biased or not, take the negative electrode bamboo,
It takes a size that corresponds to the amount of 11Ii of IJi (i'
;;'r is digitized by 1, so this becomes Tonotsungri~hoshinB (゛). In such a TRATSU A~nguribo IS 舅 generator, 41ii is created as shown in 1 below. −) light weight °
It is necessary to arrange the light-receiving surface of the dust replacement tree f'9a, ≦)b exactly 1F symmetrically with respect to the optical axis 7'-L2, and to
However, it is very difficult to install it exactly symmetrically.
... due to the displacement of the optical axis 7 due to the touch of J'iscro (the symmetry of the beam becomes worse, and at this time even if the pick 1 tube 1- optic axis 7- Even if it is done correctly, the outputs of 11a and 11b are not equal, and as a result, there is a drawback that a small deviation occurs in the Gribo system. The purpose is to prevent adverse effects on the TRAF 1-GREEBO No. 15 caused by the symmetrical deviation of the light-receiving surface or the deviation of the optical axis. ]J
Providing capable Tonok1 Green Elementary School 4I, Father-in-law 1 device T16
(-Toguru. 1-Function 1 by A invention) The small lit Sj-11 device is the pick 7 l information detection point tip ll'
Δ is generated between the detection horns corresponding to the amount of deviation Jj in the 4-cross lJ direction. Difference between the high-frequency components of the detection output of the - set of detection means installed in J.
The difference between the sum signal of the high-frequency components of the detection output of the first stage of No. 1 and the detection output of the first stage of detection of this set (corresponding to the phase Δ of No. ii)
Corresponds to the difference signal level of cl if the polarization is on the right side.
Light 11 signal to read the novel! The present invention will now be described with reference to the drawings. Figure E3 is a circuit diagram of an embodiment of the present invention. 'I]-0 month J, shown ♂ (Explanation for Jj is omitted. The output of each photoelectric conversion element 9a, 911 is amplified 4
The respective outputs of the 77 modules 10a and 10b are added to an adder 17 and a reducer 18. The sieving output is 111)
l' (bypass noise filter) 19a, and the subtracted output is II + It is applied to noisers 1 and 3, and this is the driving noise /'
4c is amplified by 1/l. Figure 9 (△) is smaller in Figure S3)
, :The spot So is fixed to the recording center line 10 and moved to the right of the drawing l\e? Ru. The output waveform of the adder 17 for &i is shown below. The output of this 7111 Ell device 17 is determined by the influence of the asymmetrical t!1 of the light receiving 1 (1) a, 9b or the deviation of the optical axis 7'. Direction X perpendicular to center line 1-0
The change in the waveform of the output of the adder 17 when the dotted line [I or 1-4 in FIG. 3 is shifted is ignored. Figure 9 (13) shows J [
The light spots S0 and S- of the output waveform of the letter reducer 18 (the waveforms of the dotted line and the dashed-dotted line are shown in FIG. !, 2 cases are small 1. In addition, the light spot light source is]
The output of the attenuator 18 in the case of 11 scales when the knock center line is moved from 0 is naturally at a certain level. Subtractor 1 in the case where the dividing line 9C deviates in the substantially orthogonal IJ direction.
8, and the waveforms of the dotted line, +:, and one-dot chain line are approximately the same as those shown in Figure 3 () where the light spots SL and S- move along the dotted line [-1 and one-dot chain line]-1. - Keep the amount small. The solid line in Figure (C) indicates that the optical spot SO moves along the center line 101 and the /cvA combination (with, the output of the reducer 18 corresponds to the displacement of the optical axis 7') CA noset α are superimposed, and this A route α is a miscellaneous component due to the deviation of the optical axis 7'. Next, refer to FIG. 10. 11P of the tightening force) = 19.3 is red (ir +-; waveform (・There is. Figure 1 (13) is 1 of the reducing output of the reducing device 1E3.
11) Signal waveform after +19b (with P, It P l
”19 Due to the action of b, there is a noise component [・some D CA
) Shitsu 1 ~ α or excluding, it is I this b and Jjsr:
, <Line, J: , on the dashed line and solid line (11, +f axis) are the dotted line 2 in Figure 9 (O). is Tokiki 20
``,'', the output waveform of the Tohoku bomb (・Similarly, the white line, dashed-dotted line, and solid line correspond to the waveforms of each line in the same figure (13). , (1) I-21 of this multiplied Q output The waveform of the /Ji month becomes as shown in Fig. 10 (1)〉, and the 1F definite tJ, l-not (leg 1 no change month and 4) are respectively similar to the example of Fig. 7 and 11+1 If we convert d7, we can add a small amount to Figure 10 (A). Depending on the direction of deviation of the light spot in the direction x, there is an in-phase or G, L anti-phase relationship, and the high frequency component level of the subtracted output should be proportional to the polarization (6+ amount) of the optical spora I. Therefore, so-called in-phase detection is performed by the multiplier 20 and 1F) F-21.In other words, if the two multipliers 20 are in the same phase, The output of 11 1-21 is 11 pole bamboo (dotted chain line)
If the phase is in the opposite phase, the polarity becomes negative (dotted line), and the absolute value level (proportional to the deviation φ (a certain 3°) (,1ll) l'10; 0
J in Figure (1), A to shape the waveform into a square wave.
I conversion 17, due to this 9J1 type wave I-I P r 19
Similarly, the multiplication result can be obtained by converting the output of b to If this square wave is used as a guide, the level of the beam will be electrified, so even if there is a fluctuation in the L-novel of the excitation output of the adjuster 17 due to the deviation of the optical axis L, it will always be possible to obtain an accurate tone. 1 ng 1 no 1
, No. 1 is 1! The structure of the Toppu device 20, 1.
, 1゜ which can be easily hit by using the r-jing circuit, :, other /j? A is tlt) 119a
1 and the negative peak of the +1 sinusoidal output of 1c11 and the output of Ill'119b are held in place, and the difference between the two vehicle and rut outputs is determined to be exactly the same. In addition, 1ilj!Example-(-44 Information detection point one-way closing means (using objective lens b) (but using other means such as so-called 1 ohms and 3L optical type) Other examples include the electrostatic method.
・According to the present invention, as described in 1.
Using only the acid component (so-called 1 [J1 phase detection)
It is possible to completely remove the low frequency miscellaneous components caused by optical axis misalignment etc.
1゜ when Green Bore a+ control becomes i+J function

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

第1図は従来のトノツー1ングリーボ装置のll1lツ
ク図、第2図は情報検出貞【゛ある光スポッ1−の記録
面反銅光と受光素子どの関係を承り図、第3図は記録1
−″)ツクを構成りるピッI・列と光スポットどの関係
を承り図、第4図乃金第7図(よ第1図のブ[1ツクの
各部動伯波形を承り図、第8図は本発明の実施例のブ[
−1ツク図、′;:A9図及び第10図は第8図の10
ツクの動性を説明りる波形図(゛ある。 一1要部分の符月の説明 5・・・・・・対物レンズ 6・・・・・・記録〕“r
スク7・・・・・・記録ノーrスク 9・・・・・・光電変換糸f ]7・・・・・・加Q器   133・・・・・減粋器
19・・・・・・1ll)+    20・・・・・・
東0器21・・・・・・11)1 出願人   バイA−ノ′株+(会、?、I代理人  
 ブr理1  砂利)し1′↓382
Fig. 1 is a diagram of a conventional Tono21 Gribo device, Fig. 2 is a diagram showing the relationship between the recording surface of a light spot 1 for information detection and the light-receiving element, and Fig. 3 is a diagram of the recording
-") A diagram showing the relationship between the pitch I/rows and the light spot that make up the block, and Figure 4, Figure 7, and Figure 1. The figure shows a block diagram of an embodiment of the present invention.
-1 tsuk figure, ';: A9 figure and figure 10 are 10 of figure 8.
Waveform diagram explaining the dynamics of Tsuku (there is.
Screen 7...Record no r Screen 9...Photoelectric conversion thread f]7...Adder Q unit 133...Reducer 19... 1ll) + 20...
Toki 21...11) 1 Applicant Bai A-no' stock + (Kai, ?, I agent)
Burri 1 Gravel) Shi 1'↓382

Claims (1)

【特許請求の範囲】 (1) ピックノノツ/情報検出)気か記録トノツクを
jl確に追跡Jるように前記情報検出点を記録トノツク
の略直交1ノ向に偏倚せしめるJ、゛)禍成された1〜
ノツ1ングリー小制御装置のり−ボf+ ;;光生装置
であって、前記情報検出点の前記/J向1,1お【ノる
偏倚吊を検出すへくこの偏倚−にλ・jl心(2(検出
出力相り間に差異が生じるJ= ’l +、’−設りら
れI、−絹の検出f段ど、前記−組の検出f段の検出用
〕)の高域成分の相伝y〕ど前記差イ、)シシとの(台
相;X(、二対応した極性をイjしか゛つ前6J差り月
しl\ルに対応したレベルをhする1〜ラツ■ングl−
ノー信号を発句づるrノーイー、局発/14丁段どを曾
むリーホイ4,8発/1装置。 (2) 前記1ノー(F1号発1丁段は前記相イL月ど
前記7 (ij杉とを1hる東わ器をイJし、この乗(
こ3) 前記1ノー(+j弓光り「段【よ前記相イJ、
号に基づ゛く矩形波(a ”5ど前、記A (!i 5
4とを乗0づる東錦器をわし、この東紳出力を前記1ノ
ーic+弓と1](イするトl、1品求の範囲第1項記
載のリーボイ91月発生装置、。 (4) 前記情報検出1.′、ζは光スポット(あり、
前記−組の検出−1段(よ、受光面が 木の分割線によ
り分割されこれら分割受光面がjlいに独立した2個の
光電弯換素Yよりなり、前記分割線は記録1−ラック接
線り向に中(Jに配置され、前記光スポットの記録面を
粁I、:光を前記受光面に照射づるようにしてなる特許
請求の範囲第1項、第2項又は第3項記載のり一小僧号
′g:、’:L装置。
[Scope of Claims] (1) Pick point/information detection) The information detection point is biased in one direction substantially orthogonal to the recording mark so as to accurately track the recording mark; Ta1~
Notes 1 Green small control device Noribo f + 2 (for detection of the above-mentioned - set of detection f stages, such as J = 'l +, '- installed I, - silk detection f stage, etc., where a difference occurs between the detection outputs)) y] The difference between A,) and (phase; −
No signal is emitted by Lee Hoi 4, 8 shots/1 device, which has a local/14th stage. (2) Said 1 no (1st stage from F1 is the said phase I L month and said 7
3) Said 1 no (+j bow light "dan [yo said phase i J,
A rectangular wave based on the number (a ”5 ago, written A (!i 5
Multiply 4 by 0 and remove the Azuma Nishikiki, and take this Toshin output as the 1 no IC + bow and 1] (I, 1 item range, the Riboi 91 month generator described in item 1. ) The information detection 1.', ζ are light spots (with,
Detection of the set - 1st stage Claims 1, 2, or 3 are arranged in the tangential direction (J), and the recording surface of the light spot is irradiated with light onto the light-receiving surface. Noriichi Kozogo'g:,':L device.
JP9328582A 1982-06-01 1982-06-01 Tracking servo signal generator of information reader Granted JPS58211370A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9328582A JPS58211370A (en) 1982-06-01 1982-06-01 Tracking servo signal generator of information reader

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9328582A JPS58211370A (en) 1982-06-01 1982-06-01 Tracking servo signal generator of information reader

Publications (2)

Publication Number Publication Date
JPS58211370A true JPS58211370A (en) 1983-12-08
JPH0154780B2 JPH0154780B2 (en) 1989-11-21

Family

ID=14078138

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9328582A Granted JPS58211370A (en) 1982-06-01 1982-06-01 Tracking servo signal generator of information reader

Country Status (1)

Country Link
JP (1) JPS58211370A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0246919A2 (en) * 1986-05-23 1987-11-25 Pioneer Electronic Corporation Tracking servo device for data reading device
JP2008545217A (en) * 2005-06-29 2008-12-11 コーニンクレッカ フィリップス エレクトロニクス エヌ ヴィ Single spot correlation tracking

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58125242A (en) * 1982-01-22 1983-07-26 Victor Co Of Japan Ltd Tracking error detecting system of optical information signal reproducing device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58125242A (en) * 1982-01-22 1983-07-26 Victor Co Of Japan Ltd Tracking error detecting system of optical information signal reproducing device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0246919A2 (en) * 1986-05-23 1987-11-25 Pioneer Electronic Corporation Tracking servo device for data reading device
JP2008545217A (en) * 2005-06-29 2008-12-11 コーニンクレッカ フィリップス エレクトロニクス エヌ ヴィ Single spot correlation tracking

Also Published As

Publication number Publication date
JPH0154780B2 (en) 1989-11-21

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