TW200822088A - Optical drive and integrated calibration method - Google Patents
Optical drive and integrated calibration method Download PDFInfo
- Publication number
- TW200822088A TW200822088A TW96130849A TW96130849A TW200822088A TW 200822088 A TW200822088 A TW 200822088A TW 96130849 A TW96130849 A TW 96130849A TW 96130849 A TW96130849 A TW 96130849A TW 200822088 A TW200822088 A TW 200822088A
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- TW
- Taiwan
- Prior art keywords
- offset
- tilt
- focus
- correction
- record carrier
- Prior art date
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 62
- 238000000034 method Methods 0.000 title claims abstract description 53
- 238000012937 correction Methods 0.000 claims description 111
- 238000004590 computer program Methods 0.000 claims description 2
- 238000005259 measurement Methods 0.000 description 11
- 239000011159 matrix material Substances 0.000 description 6
- 239000000463 material Substances 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 230000009467 reduction Effects 0.000 description 3
- 230000004044 response Effects 0.000 description 3
- 230000003044 adaptive effect Effects 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 206010033864 Paranoia Diseases 0.000 description 1
- 208000027099 Paranoid disease Diseases 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 230000004075 alteration Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 238000009987 spinning Methods 0.000 description 1
- 230000006641 stabilisation Effects 0.000 description 1
- 238000011105 stabilization Methods 0.000 description 1
- 238000003860 storage Methods 0.000 description 1
Classifications
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/08—Disposition or mounting of heads or light sources relatively to record carriers
- G11B7/09—Disposition 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
- G11B7/0945—Methods for initialising servos, start-up sequences
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/08—Disposition or mounting of heads or light sources relatively to record carriers
- G11B7/09—Disposition 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
- G11B7/095—Disposition 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 specially adapted for discs, e.g. for compensation of eccentricity or wobble
- G11B7/0956—Disposition 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 specially adapted for discs, e.g. for compensation of eccentricity or wobble to compensate for tilt, skew, warp or inclination of the disc, i.e. maintain the optical axis at right angles to the disc
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/08—Disposition or mounting of heads or light sources relatively to record carriers
- G11B7/09—Disposition 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
- G11B7/0943—Methods and circuits for performing mathematical operations on individual detector segment outputs
Landscapes
- Optical Recording Or Reproduction (AREA)
Abstract
Description
200822088 九、發明說明: 【發明所屬之技術領域】 本發㈣關於光碟機’ ^更特定言之,係㈣ 機之聚焦偏移及傾斜偏移校正方法。 、尤碟 【先前技術】 美國20_31060揭示一種校正光碟機裝置 移、聚焦偏移及徑向偏移的方法,其中獨立地進行聚= Ο200822088 IX. Description of the invention: [Technical field to which the invention pertains] The present invention (4) relates to an optical disk drive'. More specifically, it relates to a focus offset and tilt offset correction method of the (four) machine. [Prior Art] US 20_31060 discloses a method of correcting the movement, focus shift and radial offset of an optical disc device, wherein the poly = Ο is performed independently.
G m… 糟“疋不同傾斜校正點且量測 抖削,唬來進行傾斜偏移校正。相似 正。此方法並不產生最佳校正結果,且校正持二移权 秒。此通常增加光碟機之啟動時間及最= 大於1 其接著影響光碟機對使用者命令之回應時間。X日、間, 具有減小校正光碟機之聚焦偏移及傾斜偏移所需之時門 的校正方法係有利的。罝古 而之夺間 所需之時間的光销㈣_的。 減料偏移 【發明内容】 此處描述-種校正-光碟機之方法。財 記錄載體插入於該光碟機中 在將 -傾斜偏移之校正。中之相時執行對—聚焦偏移及 在-種此處描述之光碟機中, 統,該光學系統用於掃描— 先予糸 T2、…、τη)。該光學系…°己錄載體之磁軌(Tl、 -光束…接物鏡,发用:將…光束產生器’其產生 上。該光碟機進-步包含於_將該光束聚焦於該記錄載體 光學偵測器,其用於偵測一 123904.doc 200822088 反射光束;一可控制聚焦致動器,其用於使該接物鏡相對 , ⑥該記錄載體之—記錄參考平面而柄向移位;及一可控制 傾斜致動器’其用於使該接物鏡相對於該記錄載體而轉 動。該光碟機進一步包含一第一記憶體,該第一記憶體經 配置以儲存校正資料點。該光學機進一步包含一第二記憶 體,該第二記憶體經配置以儲存—最佳聚焦偏移值 佳傾斜偏移值。該光學機進一步包含:一控制電路,其具 Γ彳用於接收來自料學㈣11之信號的輸人端且具有麵接 至該聚焦致動器之-控制輸入端及該傾斜致動器之一控制 輸入端的輸出端。該控制電路進一步包含一整合校正單 元,該整合校正單元經配置以在將該記錄載體插入於該光 碟機中之後同時執行對一聚焦偏移及一傾斜偏移之校正。 此外’可利用—電腦程式實施校正該光碟機之該方法。 【實施方式】 圖1不思性地說明一光碟機1(例如,dvd機)之一實例, ^ 其適於對—記錄載體2(通常為DVD)寫人資訊且/或自一記 錄載體2讀取資訊。為旋轉記錄载體2,光碟機以含一馬 達4。通常將馬達4固定至界定一旋轉軸5之框 =固持記錄載體2,光碟⑴可包含—可轉或夾持轴套/, 在主軸馬達4之情況下安裝於馬達4之主軸7上。G m... 疋 “疋 Different tilt correction points and measurement of jitter, 进行 to perform tilt offset correction. Similar to positive. This method does not produce the best correction result, and the correction holds the second shift weight. This usually increases the disc player. The startup time and the most = greater than 1 then affect the response time of the CD player to the user command. On the X-day, the correction method for the time gate required to reduce the focus offset and tilt offset of the optical disk drive is advantageous. The light-spinning time required for the time between the old and the new (four) _. The material reduction offset [invention] The method of the correction-disc drive is described here. The financial record carrier is inserted in the optical disk drive. - Correction of the tilt offset. The phase in the middle performs a pair-focus shift and in the optical disc drive described herein, the optical system is used for scanning - first T2, ..., τη). The magnetic track (Tl, -beam...the objective lens is used to generate the beam generator). The optical disk drive is included in the optical fiber to focus on the record carrier. Detector for detecting a 123904.doc 200822088 reflected light a controllable focusing actuator for aligning the objective lens, 6 the record carrier, recording the reference plane and shifting the handle; and a controllable tilt actuator for making the objective lens Rotating on the record carrier. The optical disk drive further includes a first memory, the first memory is configured to store a corrected data point. The optical machine further includes a second memory, the second memory is configured to Storing—the best focus offset value is a good tilt offset value. The optical machine further includes: a control circuit for receiving the input end of the signal from the material (four) 11 and having a facet to the focus actuation The control input and one of the tilt actuators control the output of the input. The control circuit further includes an integrated correction unit configured to simultaneously insert the record carrier into the optical disk drive Correction of a focus offset and a tilt offset is performed. Further, the method of correcting the optical disc drive can be implemented by using a computer program. [Embodiment] FIG. 1 succinctly illustrates one An example of a disc drive 1 (for example, a dvd machine), which is suitable for writing information to a record carrier 2 (usually a DVD) and/or reading information from a record carrier 2. For rotating the record carrier 2, a disc The machine comprises a motor 4. The motor 4 is usually fixed to a frame defining a rotating shaft 5 = the holding record carrier 2, the optical disc (1) may comprise - a rotating or clamping bushing /, in the case of the spindle motor 4, mounted to the motor 4 on the spindle 7.
T 光碟機1進—步包含―用於掃描記錄載體2之磁執(Tl、 人一····..、Τη)之光學系統30。更特定言之,光學系統30包 光束32a之光產生器31(例如,雷射二極體)。光 a穿過-光束分光器33及—接物鏡34。接物鏡34將光 123904.doc 200822088 束32b(於一焦點F上)聚焦於記錄載體2上。光束32b自記錄 載體2反射(反射光束32c)且穿過接物鏡34及光束分光器 3 3(光束32d)以到達光學偵測器35。 使用直角座標系統XYZ。旋轉軸5為Z軸。徑向方向為χ 軸(垂直於Z軸,使得焦點F位於XZ平面中)。正切方向為γ 軸(垂直於X軸及Z軸)。極座標系統(r、φ)亦用於界定記錄 載體2之座標。 為達成且維持光束32b在所要位置上(在記錄載體2上)之 準確聚焦,接物鏡34經安裝以可軸向(Z方向)移位。此 外’光碟機1之致動器系統40包含一聚焦致動器42,該聚 焦致動器42經配置以使接物鏡34相對於記錄載體2之記錄 參考平面軸向移位。由於球體偏差(基板之折射率)之故, 光束在記錄載體2上之焦點F改變一偏移值。為消除此等影 響,進行聚焦偏移校正以將聚焦偏移恢復為合適情況。 纪錄載體2亦可經受傾斜。將記錄載體2之傾斜定義為記 錄載體2之記錄參考平面不垂直於旋轉軸之情況。作為整 體相對於雷射光束傾斜之記錄載體2(例如,因為馬達軸相 對於框架傾斜且因此傾斜量視記錄載體之位置而定)可導 致傾斜。尤其是具有相對較大數值孔徑(NA)之DVD系統易 經文碟片傾斜。通常,在一具有傾斜校正之光碟機1中, 接物鏡34可轉動,且光碟機1包含控制接物鏡34之傾斜位 置的傾斜致動器。為此,接物鏡34經安裝以可圍繞平行於 γ轴而定向之轉動軸轉動,使得一接物鏡34之光軸36位於 XZ平面内。較佳地,轉動軸係與接物鏡34之光學中心一 123904.doc 200822088 致。將轉動角Φ定義為在Z軸與接物鏡34之光軸%之間的 角。此外,光碟機1之致動器系統40包含一傾斜致動器 43,該傾斜致動器43經配置以使接物鏡34相對於記錄載體 2轉動。大體上,角度Φ應為零、然而,由於製造製程改變 之故,記錄載體2通常不平坦。記錄載體2在徑向方向及環 形方向上彎曲。因此,光學系統3〇在其光軸刊垂直於記 錄載體2之記錄表面的情況下無法掃描記錄磁軌。轉動角 Φ與接物鏡34之光軸36的偏差被稱為傾斜偏移。為消除 此等影響,進行傾斜偏移校正以將傾斜偏移恢復為合適 情況。 光碟機1另外包含一控制電路90,其具有一連接至一馬 達4之控制輸入端的第一輸出端92、一耦接至一徑向致動 器41之控制輸入端的第二輸出端93、一耦接至一聚焦致動 器42之控制輸入端的第三輸出端94及一耦帛至一傾斜致動 器43之控制輸入端的第四輸出端%。控制電路卯經設計以 產生: 在其第一輸出端92處,產生用於控制馬達4之控制信號 ScM, 在其第二輸出端93處,產生用於控制徑向致動器41之控 制信號SCR, 在八第一輸出端94處,產生用於控制聚焦致動器之控 制信號SCF,及 在其第四輸出端95處,產生用於控制傾斜致動器43之控 制信號SCT。 123904.doc 200822088 控制電路90另外且右一冷 來自光學伯測器々讀取號輸入端91,其用於接收 至==錄载體2(參看圖”讀取資料或將資料寫人 能。為達成此圖Ο之同時達成良好的聚焦及循軌效 評:取I ,進行聚焦偏移校正及傾斜偏移校正。 ==偏移校正及傾斜偏移校正通常基於抖動。 學差 1偏移校正及傾斜偏移校正通常基於徑向循 國膽_31_揭示—種校正程序,其中 獨立地進行聚焦偏移校正及傾斜偏移校正。藉由設 2斜Γ正點且量測抖動信號來進行傾斜偏移校正。相似 -數:Π焦偏移校正。因傾斜偏移及聚焦偏移並非獨立 故此方法佔用較多時間且通常不準確。傾斜偏移校 U將影響聚焦偏移校正結果,且反之亦然。 圖^及圖2b示意性地說明藉由在dvd機(參看圖^中獨 立執行聚焦偏移校正及傾斜偏移校正而獲得之校正社果。 首先執行傾斜偏移校正’且接著執行聚焦偏移校正。口由圖 2a及圖2b可見’使用此方法而獲得之最佳聚焦偏移及最佳 傾斜偏移並非實際最佳聚焦偏移及實際最佳傾斜偏移。此 外’此方法通常佔用賴少。該方法通常需要更多時間來 啟動及執行用於記錄之最佳功率校正(〇pc)程序。此通常 影響光碟機對用戶命令之回應時間。舉例而言,在㈣程 序期間,執行基於徑向循軌誤差信號之聚焦偏移校正及= 斜偏移校正以在記錄期間獲得最佳循規效能。在記錄之 後,為改良在OPC區域上之回讀效能,執行基於抖動:聚 123904.doc 200822088 ==傾斜偏移校正。聚焦偏移校正及傾斜 通吊總叶佔用多於2秒,其增加用於 咖時間。此通常影響播放及記錄之連續性广之總體 ^處料—種減小執行聚线移校正及傾斜偏移校 二::的方法。該方法同時執行聚焦偏移及傾斜偏移之校 。该方法在3維空間内同時皆執行聚焦偏移校正及 偏移校正。分別在第一維及第二維上設定聚隹偏… 及傾斜偏移校正點,而在第r唯上量 又點 你矛一雒上里測杈正信號。哕 =行^合校正來替代兩個分離校正,且因此減^正時 而言,對0PC而言,替代在〇pc期間執行4個校 ,所揭不方法僅執行2個校正(一個用於讀取且—個用於 且^總校正時間減小為約小㈣少。大體改良光碟機 之整體讀取及記錄效能。此外, ” 者命令之重放及記錄回應時間/ 良光碟機對使用 圖3示意性地展示經選擇以在例示性卿機(參看中 同時執行聚焦偏移校正及傾斜偏移校正之校正點 U參看剛常具有致動器以移動接物鏡且調整聚焦偏 移、傾斜偏移及徑向偏移。基於致動器之最大可允許移位 來選擇校正點。此等校正點儲存於光碟機之記憶體中。圖 3展示17個校正點,但诵當豐亚具丨 逋吊而要最少6個穩定點以能夠進行 表面擬合且計算所要參數。若穩定量測點之數目低於6, 則無法進行該校正方法。為得到良好且準確之校正姓果, 通常使用多於6個點’且此為選擇17個校正點之依據中之 一者。若所有17個點均穩定’則所有17個點均用於表面擬 123904.doc 10- 200822088 合以獲得拋物線表面。 後,對校正信號(抖動, 此處意謂在設定偏移值之 的。6個穩定點可為在 里測係穩疋 • 點。釋定點、雨〆 展不之17個點中之任何ό個 ^田闽 周圍。但此等穩定點可在確定相 位周圍且視光學拾取單元及 ^ ^ ^ ., . •、動機制而疋。進行對穩定點 =擇,使付在對抖動或徑向猶軌誤差信號量測期間不存 f μ點過遠,則此將焦偏移及傾斜偏移設定成距 Γ、" 職將導致不良循規效能,且因此導致讀取 ^ 貝或二白碟片之不良擺動信號品 貝。此導致HF鎖相迴路鎖定 叙# M ^ ^。待考慮之另—因素為抖 染^ 早過河(亦即,南於16%(其為當前解碼 ^ ^、之可罪置測限制h,貝,J校正點將被視為不穩定點。 2工:碟片之情況T ’在將聚焦偏移及傾斜偏移設定為距 被視^之最佳點過遠時存在捏向偏軌之可能性。 ^個可能實施例中,獲得在聚焦偏移、傾斜偏移與抖 > A之間的3維關係。在抖動信號大體上最小處得到最 佳頃取聚焦偏移值及最佳讀取傾斜偏移值。得到在聚焦偏 移:傾斜偏移與抖動信號之間的3維關係之步驟包含以下 内谷·獲侍聚焦偏移步長、傾斜偏移步長、最大可允許聚 焦偏移值及最小可允許聚焦偏移值。對聚焦偏移可調整範 圍及傾斜偏移可調整範圍之選擇視光學拾取單元而定。由 聚焦S曲線(聚焦偏移可調整範圍)確定聚焦偏移校正範 圍^員斜偏移权正範圍視光學拾取單元之可調整傾斜角度 (通币為d:12至15 mrad)而^。用於校正之最大步長接著藉 123904.doc 200822088 調整範圍除如圖3中所描述之點(亦即,6個點)而計 ”《不存在足以執行表面擬合之有效穩定點時,使用較 J步長。(亦即,在有效穩^點之數目小於6之情況下)。此 程序亦被稱為適應性校正步長。在此處所揭示之實例中, 2用先前丄交正步長之十其原因為’對—些碟片及/或 、:碟機*舌,肖斜偏移及聚焦㉟移穩定可調整範圍與光學 拾取單元所允許之範圍相比係非常小的。在—些情ς下, r 先學拾取單元之可調整傾斜範圍係在下限處,且光碟播放 或循軌之印貝較差。最小抖動非常高,例如咖。在該情 况下’聚焦偏移及/或傾斜偏移之較大偏移將導致抖動高 達16%。為達成有效校正點之最小值,使用較小之偏移步 長。換言之,減小校正覆蓋度。根據產品實體可調整範圍 規選擇開始17個校正以覆蓋典型傾斜及聚焦偏移可調 整耗圍。為獲得6個有效穩定點且得_ 之最佳聚焦偏移及最佳傾斜偏移,校正步長通常不= 大。因此,若校正點之數目低於6,則藉由使步長減小一 半(或一半以上)來引入適應性步長。 確定在不同聚焦偏移值及傾斜偏移值上之抖動信號。下 文描述用於執行讀取校正及獲得最佳讀取聚焦偏移值及最 佳讀取傾斜偏移值之程序。此程序之可能結果在圖4中示 意性地說明且涉及以下步驟: 1·開始,其中相位Ν=ι。 2·將聚焦偏移模式及傾斜偏移模式預設定為斜坡上 模式。 123904.doc -12- 200822088 3·對相位N設定斜坡模式。 4·將聚焦偏移及傾斜偏移設定為預設值。 5.設定聚焦偏移=聚焦偏移+焦點_步長; ± 傾斜偏移=傾斜偏移+傾斜-步長; 6 ·頃取抖動信號。 7.仏查在相位]^中之所有校正點是否完整。若該等校正 點完整,則轉至步驟8,否則重複步驟5至7。The T-disc machine 1 includes an optical system 30 for scanning the magnetic carrier (T1, human one, ..., Τη) of the record carrier 2. More specifically, the optical system 30 encloses a light generator 31 (e.g., a laser diode) of the beam 32a. The light a passes through the beam splitter 33 and the objective lens 34. The objective lens 34 focuses the light 123904.doc 200822088 bundle 32b (on a focus F) onto the record carrier 2. The light beam 32b is reflected from the recording medium 2 (reflected light beam 32c) and passes through the objective lens 34 and the beam splitter 3 3 (light beam 32d) to reach the optical detector 35. Use the Cartesian coordinate system XYZ. The rotating shaft 5 is a Z axis. The radial direction is the χ axis (perpendicular to the Z axis such that the focus F lies in the XZ plane). The tangent direction is the γ axis (perpendicular to the X and Z axes). The polar coordinate system (r, φ) is also used to define the coordinates of the record carrier 2. To achieve and maintain accurate focus of the beam 32b at the desired location (on the record carrier 2), the objective lens 34 is mounted for axial (Z-direction) displacement. Further, the actuator system 40 of the optical disk drive 1 includes a focus actuator 42 that is configured to axially displace the objective lens 34 relative to the recording reference plane of the record carrier 2. Due to the spherical aberration (refractive index of the substrate), the focus F of the light beam on the record carrier 2 changes by an offset value. To eliminate these effects, focus offset correction is performed to restore the focus offset to the appropriate condition. The record carrier 2 can also be subjected to tilting. The inclination of the record carrier 2 is defined as the case where the recording reference plane of the record carrier 2 is not perpendicular to the rotation axis. The record carrier 2, which is tilted as a whole with respect to the laser beam (e.g., because the motor shaft is tilted relative to the frame and therefore the amount of tilt depends on the position of the record carrier) can cause tilting. In particular, DVD systems with relatively large numerical apertures (NA) are easy to tilt. Generally, in a disc player 1 having tilt correction, the objective lens 34 is rotatable, and the optical disc drive 1 includes a tilt actuator that controls the tilt position of the objective lens 34. To this end, the objective lens 34 is mounted for rotation about a rotational axis oriented parallel to the gamma axis such that the optical axis 36 of an objective lens 34 lies in the XZ plane. Preferably, the rotational axis is coupled to the optical center of the objective lens 34 by 123904.doc 200822088. The angle of rotation Φ is defined as the angle between the Z-axis and the optical axis % of the objective lens 34. Furthermore, the actuator system 40 of the optical disk drive 1 includes a tilt actuator 43, which is configured to rotate the objective lens 34 relative to the record carrier 2. In general, the angle Φ should be zero, however, the record carrier 2 is generally not flat due to manufacturing process changes. The record carrier 2 is curved in the radial direction and the ring direction. Therefore, the optical system 3 cannot scan the recording track with its optical axis perpendicular to the recording surface of the recording carrier 2. The deviation of the rotational angle Φ from the optical axis 36 of the objective lens 34 is referred to as a tilt offset. To eliminate these effects, tilt offset correction is performed to restore the tilt offset to the appropriate condition. The optical disc drive 1 further includes a control circuit 90 having a first output end 92 coupled to a control input of a motor 4, a second output end 93 coupled to a control input of a radial actuator 41, and a A third output terminal 94 coupled to the control input of a focus actuator 42 and a fourth output terminal coupled to the control input of a tilt actuator 43 are coupled. The control circuit is designed to produce: at its first output 92, a control signal ScM for controlling the motor 4 is generated, and at its second output 93, a control signal for controlling the radial actuator 41 is generated The SCR, at the eight first output 94, generates a control signal SCF for controlling the focus actuator, and at its fourth output 95, generates a control signal SCT for controlling the tilt actuator 43. 123904.doc 200822088 The control circuit 90 is additionally and rightly cooled from the optical detector 々 reading input 91, which is used to receive the == record carrier 2 (see figure) to read the data or to write the data. In order to achieve this figure, a good focus and tracking effectiveness is achieved: take I, focus offset correction and tilt offset correction. == Offset correction and tilt offset correction are usually based on jitter. The correction and tilt offset correction is usually based on a radial calibration method in which focus offset correction and tilt offset correction are performed independently. By setting the slope punctuality and measuring the jitter signal Tilt offset correction. Similar-number: Π focus offset correction. Since the tilt offset and focus offset are not independent, this method takes more time and is usually inaccurate. The tilt offset correction U will affect the focus offset correction result, and Fig. 2 and Fig. 2b schematically illustrate the correction result obtained by performing the focus offset correction and the tilt offset correction independently in the dvd machine (refer to Fig. 2 first. Perform tilt offset correction first) and then Perform focus offset Correction. The port is shown in Figure 2a and Figure 2b. 'The best focus offset and optimal tilt offset obtained using this method are not the actual best focus offset and the actual optimal tilt offset. In addition, this method usually occupies Less. This method usually requires more time to start and execute the best power correction (〇pc) program for recording. This usually affects the response time of the CD player to user commands. For example, during the (4) program, execution is based on Focus offset correction of the radial tracking error signal and = skew offset correction to obtain the best compliance performance during recording. After recording, to improve the readback performance on the OPC area, perform jitter-based: Poly123904. Doc 200822088 == tilt offset correction. Focus offset correction and tilt-over-hanging total leaves take more than 2 seconds, which increases the time spent on coffee. This usually affects the overall continuity of playback and recording. The method of performing small line shift correction and tilt offset correction:: This method simultaneously performs focus offset and tilt offset correction. This method performs focus offset correction and offset simultaneously in 3D space. Positive. Set the convergence offset and the tilt offset correction point in the first dimension and the second dimension, respectively, and measure the positive signal in the r-th only quantity and point you on the glitch. To replace the two separation corrections, and thus the reduction of the positive timing, for the 0PC, instead of performing 4 calibrations during the 〇pc, the unexamined method performs only 2 corrections (one for reading and one for each). And the total correction time is reduced to be less than (four) less. The overall read and record performance of the CD player is substantially improved. In addition, the playback and recording response time of the commander/good CD player is schematically shown using FIG. Selected to perform the focus correction and tilt offset correction correction points U at the same time (see also the actuators to move the objective lens and adjust the focus offset, tilt offset and radial offset) shift. The correction point is selected based on the maximum allowable shift of the actuator. These correction points are stored in the memory of the CD player. Figure 3 shows 17 correction points, but when the feng ya 丨 逋 而 要 要 要 要 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少 最少If the number of stable measurement points is less than 6, the correction method cannot be performed. In order to obtain a good and accurate correction of the surname, usually more than 6 points are used' and this is one of the basis for selecting 17 correction points. If all 17 points are stable, then all 17 points are used for surface pseudo-123904.doc 10-200822088 to obtain a parabolic surface. After that, the correction signal (jitter, here means that the offset value is set. The 6 stable points can be stabilized in the measurement system. Point. Any of the 17 points of the release point and the rain show. Between the fields and the fields, but these stable points can be determined around the phase and the optical pickup unit and the ^ ^ ^ , . . . , moving mechanism 进行 进行 进行 进行 进行 进行 进行 进行 进行 进行 进行 进行 = = = = = = If there is no f μ point too far during the measurement of the error signal, then setting the focus offset and tilt offset to a distance of Γ, " will result in poor compliance, and thus result in reading ^ 贝 or 二白The bad sway signal of the disc is the same. This causes the HF phase-locked loop to lock the # M ^ ^. The other factor to be considered is the dithering ^ early crossing the river (that is, south of 16% (which is the current decoding ^ ^ The guilty detection limit h, shell, J correction point will be regarded as unstable point. 2 work: the case of the disc T 'set the focus offset and tilt offset to the best point from the view There is a possibility of pinching off the track at a long time. In one possible embodiment, a 3-dimensional relationship between focus offset, tilt offset and jitter > A is obtained. The jitter signal is substantially minimized to obtain the optimum focus offset value and the optimal read tilt offset value. The step of obtaining a 3-dimensional relationship between the focus offset: the tilt offset and the jitter signal includes the following inner valley. The focus shift step size, the tilt offset step size, the maximum allowable focus offset value, and the minimum allowable focus offset value are selected. The optical pickup unit is selected for the focus offset adjustable range and the tilt offset adjustable range. The focus S-curve (the focus offset adjustable range) is determined by the focus offset correction range. The oblique offset weight range is the adjustable tilt angle of the optical pickup unit (the currency is d: 12 to 15 mrad). ^. The maximum step size for correction is then borrowed from 123904.doc 200822088. The adjustment range is calculated by the point (ie, 6 points) as described in Figure 3. "There is no effective stable point sufficient to perform surface fitting." , using a J step. (ie, in the case where the number of effective stabilization points is less than 6.) This procedure is also referred to as the adaptive correction step size. In the example disclosed herein, 2 is used previously. The reason for the ten step is '' - some discs and / or,: disc player * tongue, oblique offset and focus 35 shift stable adjustable range is very small compared to the range allowed by the optical pickup unit. In some cases, r first The adjustable tilt range of the pickup unit is at the lower limit, and the disc playing or tracking is poor. The minimum jitter is very high, such as coffee. In this case, the 'focus offset and/or tilt offset are larger. Shift will result in jitter up to 16%. To achieve the minimum of the effective correction point, use a smaller offset step size. In other words, reduce the correction coverage. Select 17 corrections to cover the typical tilt according to the product entity adjustable range gauge And the focus offset can adjust the cost. In order to obtain 6 effective stable points and obtain the best focus offset and the optimal tilt offset, the correction step size is usually not = large. Therefore, if the number of correction points is less than 6, the adaptive step size is introduced by reducing the step size by half (or more than half). Determine the jitter signal at different focus offset values and tilt offset values. The procedure for performing read correction and obtaining the best read focus offset value and the best read tilt offset value is described below. The possible results of this procedure are illustratively illustrated in Figure 4 and involve the following steps: 1. Start with phase Ν = ι. 2. Set the focus shift mode and tilt offset mode to the on-slope mode. 123904.doc -12- 200822088 3. Set the ramp mode for phase N. 4. Set the focus offset and tilt offset to the preset values. 5. Set focus offset = focus offset + focus _ step size; ± tilt offset = tilt offset + tilt - step size; 6 · take the jitter signal. 7. Check that all calibration points in phase ^^ are complete. If the correction points are complete, go to step 8, otherwise repeat steps 5 through 7.
8·檢查N疋否>4。若N>4,則轉至步驟1〇,$則轉至步 疋相位N N+1 ,檢查N是否>4,若N>4,則轉至步 10 ’否則重複步驟3至8。 夕 1〇·形成讀取抖動信號之向量。 11 ·计异一階表面模型係數。 12·曲線擬合聚焦偏移值 獲得3維關係。 傾斜偏移值及抖動信號值且8. Check N疋No>4. If N>4, go to step 1〇, then go to step phase N N+1 and check if N is > 4, if N>4, go to step 10' otherwise repeat steps 3 to 8.夕 〇· Form a vector for reading the jitter signal. 11 · Calculate the first-order surface model coefficients. 12. Curve fitting focus offset value Obtain a 3-dimensional relationship. Tilt offset value and jitter signal value and
、 —忍謂聚焦偏移及傾斜偏移均為斜坡上 移=坡焦偏移為斜坡下降模式且傾斜偏 意謂聚焦偏移及傾斜偏移均 傾斜偏:::式’且N=4意謂聚焦偏移為斜坡上升模式且 方tr坡下降模式。相何視待校正之參數及斜坡 向之疋義而合適地改變。 時:主二,量測時間大體上等於執行—次碟片旋轉需要之 :使仔抖動信號值之量測結果為在一次碟片旋轉令之 -值。圖W意性地㈣使用以上料獲得之讀取户正 123904.doc -13- 200822088 結果之一實例。對0¥0機1(參看圖丨)執行該程序。使用之 DVD機為DVD記錄器,其具有±86〇 nm聚焦偏移可調整範 圍及±9 mrad之傾斜角。編碼聚焦偏移值及編碼傾斜偏移 值相對於抖動信號值成曲線。使用編碼值之原因為使實施 更具一般性(使得可將實施應用於不同類型之光學記錄設 備)。 由於應對熟習此項技術者顯得清晰之故,可將二階模型 表示為, z = ax+ a2x + a3y + a4x2 + a5y2 + a6xy.......⑴ 使用編碼變數,基於抖動之校正之矩陣X及向量Z應為 (參看表1) x = 123904.doc -2.6 0 6.76 0 (Γ "22.87" 0 一 3 0 9 0 12.1 -2 0 4 0 0 17.14 0 - 2 0 4 0 10.72 2 - 2 4 4 一 4 10.78 -2 - 2 4 4 4 18.50 1 -1 1 1 -1 9.94 一1 ~1 1 1 1 11.07 0 0 0 0 0 ζ = 9.50 一 1 1 1 1 一 1 10.02 1 1 1 1 1 9.21 〜2 2 4 4 一 4 15.59 2 2 4 4 4 10.00 0 2 0 4 0 9.35 2 0 4 0 0 9.76 0 3 0 9 0 11.42 2.6 0 6.76 0 0 _ 9.72 _ 可將估計/預測係數計算為 Αζζ{Χτχγλχτζ.............(2) -14- 200822088 其中χΤ為矩陣χ之轉置矩陣 (X X)為(χτχ)之逆矩陣,且 A=[aj a2 a3 a4 a5 a6] 〇 在實際實施中,分量(乃作由預定義校正點確定且被 稱為矩陣Β。此矩陣值儲存於光碟機i之記憶體中。ζ為經 量測抖動值。在完成所有量測之後,執行5χζ之簡單相乘 以計算二階表面模型係數。- Forbearance of focus offset and tilt offset are slope upshift = slope focus offset is ramp down mode and tilt bias means focus offset and tilt offset are both skewed:::式' and N=4 The focus offset is the ramp-up mode and the square tr-slope down mode. The parameters and slopes to be corrected are changed as appropriate. Time: Master 2, the measurement time is roughly equal to the execution - the rotation of the disc is required: the measurement result of the jitter signal value is the value of the rotation of the disc. Figure W is intended to (iv) an example of the results obtained by using the above materials to read the household 123904.doc -13- 200822088. This program is executed for 0¥0 machine 1 (see Fig. 。). The DVD player used is a DVD recorder with a ±86〇 nm focus shift adjustable range and a tilt angle of ±9 mrad. The coded focus offset value and the coded tilt offset value are plotted against the jitter signal value. The reason for using the encoded values is to make the implementation more general (so that the implementation can be applied to different types of optical recording devices). Since it should be clear to those skilled in the art, the second-order model can be expressed as z = ax + a2x + a3y + a4x2 + a5y2 + a6xy.... (1) Using the coding variable, matrix based on jitter correction And the vector Z should be (see Table 1) x = 123904.doc -2.6 0 6.76 0 (Γ "22.87" 0 a 3 0 9 0 12.1 -2 0 4 0 0 17.14 0 - 2 0 4 0 10.72 2 - 2 4 4 - 4 10.78 -2 - 2 4 4 4 18.50 1 -1 1 1 -1 9.94 1 1 ~ 1 1 1 1 11.07 0 0 0 0 0 ζ = 9.50 1 1 1 1 1 1 10.02 1 1 1 1 1 9.21 ~ 2 2 4 4 - 4 15.59 2 2 4 4 4 10.00 0 2 0 4 0 9.35 2 0 4 0 0 9.76 0 3 0 9 0 11.42 2.6 0 6.76 0 0 _ 9.72 _ The estimated/predicted coefficient can be calculated as Αζζ{Χτχγλχτζ.............(2) -14- 200822088 where χΤ is the inverse matrix of the matrix χ transposed matrix (XX) is (χτχ), and A=[aj a2 a3 A4 a5 a6] 实际 In actual implementation, the component is determined by a predefined correction point and is called matrix Β. This matrix value is stored in the memory of the CD player i. The measured jitter value is completed. After all measurements, perform 5 Multiplying the surface model to calculate a single coefficient of second order.
圖4說明二階表面關係之一實例。利用校正資料χ(編碼 聚焦偏移值)、Υ(編碼傾斜偏移值)及2:(量測抖動信號),計 算係數幻、心、心、〜、幻及〜。接著將最佳讀取聚焦偏移 值及最佳讀取傾斜偏移值計算為: ^ opt {i.e.optimumreadfocusoffset) = (2α2α5 -α3α6)/(α62 -4α4α5)...........(3) Y〇pt(J.e.optimumreadtiltoffset、- - /^^4^5 )...........(4) 最佳讀取聚焦偏移值及最佳讀取傾斜偏移值為編碼值, 且將在用於自DVD讀取資料之前被解碼。 表1 A -------------— ________1 _ Β 聚焦偏移 傾斜 (mrad) X Υ —--- ζ 1 -743 0.0 22 87 2 0 -4.922 - ^^0 9%J i 一 1? 1 3 -572 0.0 -2 一__ 丄 i _ 17 14 4 0 -3.281 0 ___^ 10 72 5 572 -3.281 2 ------ ΊΓ —一 _ -2 10.78 6 572 -3.281 -2 -----— 18 5 7 286 -1.640 1 1 丄 ^ _ 9 94 8 -286 -1.640 7\ ^ y-y^__ 11 07 9 0 0.0 ____ 〇 丄丄刀’-- 〇 5 10 -286 1.640 -1 y,J__ 10.02」 123904.doc -15- 200822088Figure 4 illustrates an example of a second order surface relationship. Using the correction data 编码 (coded focus offset value), Υ (coded skew offset value) and 2: (measurement jitter signal), calculate the coefficients illusion, heart, heart, ~, illusion and ~. The best read focus offset value and the best read tilt offset value are then calculated as: ^ opt {ieoptimumreadfocusoffset) = (2α2α5 -α3α6)/(α62 -4α4α5).......... (3) Y〇pt(Jeoptimumreadtiltoffset, - - /^^4^5 )...........(4) Optimal reading focus offset value and optimal read tilt offset The value is the encoded value and will be decoded before being used to read data from the DVD. Table 1 A -------------—— ________1 _ 聚焦 Focus offset tilt (mrad) X Υ —--- ζ 1 -743 0.0 22 87 2 0 -4.922 - ^^0 9% J i -1? 1 3 -572 0.0 -2 a __ 丄i _ 17 14 4 0 -3.281 0 ___^ 10 72 5 572 -3.281 2 ------ ΊΓ —一 _ -2 10.78 6 572 - 3.281 -2 ----- 18 5 7 286 -1.640 1 1 丄^ _ 9 94 8 -286 -1.640 7\ ^ yy^__ 11 07 9 0 0.0 ____ Scythe '-- 〇5 10 - 286 1.640 -1 y, J__ 10.02" 123904.doc -15- 200822088
表1展示DVD機1(參看圖1}獲得之讀取校正結果的一實 例。將總校正點(在DVD機中)設定為如圖3中所示之共17 個點。以使系統在整個校正過程中大體上穩定之方式確定 Γ 校正點、聚焦偏移步長及傾斜偏移步長。此經執行以保證 抖動對聚焦偏移表面及傾斜偏移表面之準確表面擬合及預 測,使得可準確得到最佳設定。由於聚焦偏移及傾斜偏移 對光碟機系統之影響的敏感性(影響循軌效能),使用小於 可允許聚焦偏移可調整範圍及傾斜偏移可調整範圍之範 圍。當將聚焦偏移及/或傾斜偏移設定成距最佳點過遠時 可到達不穩定狀態,在該情況下可不良地影響徑向循執或 ^^#號(例如,當碟片品質非常差時,諸如在碟片基板層 c 厚度與碟片標準實質上不同之情況下)。為排除此情況: 若 i· 量測之HF抖動位準>13% i i ·存在由於較差HF信號品質之故的一些鎖相迴路鎖定故 卩早’則將聚焦偏移步長減少一半(甚至若半個步長仍無法 收集足夠穩定校正點’則仍可重複減小步長之行為)。鎖 相迴路故障通常在系統時脈無法鎖定不良HF信號時發生。 此通常在HF信號不良時發生(不良眼圖、不良hf信號不對 123904.doc •16- 200822088 私性、調變或當聚焦偏移值及傾斜偏移值遠離最佳聚焦偏 移值及傾斜偏移值時)。 :在表1中展示之資料而言’最佳聚焦偏移為255 18 _ 且最佳傾斜偏移為丨.21 mrad。最小抖動為8 2%。在相似條 件下,當使用分離之校正方法時,獲得以下值:277 73 nm之最佳聚焦偏移’ _9〇4職^最佳傾斜偏移。最小抖 動為9.2%。可觀察到,使用所揭示之3維讀取校正方法, HF ^號抖動效能增加1 %。 〃在製造光碟機1(參看圖⑽間’視碟片類型及轉速而執 行聚焦偏移校正及傾斜偏移校正且將校正值儲存於光碟機 1中。儲存於光碟機中之此等值被用作預設值。在隨後啟 動期間,,行3維讀取校正。所獲得之最佳讀取聚焦偏移 值及最佳讀取傾斜偏移值根據區域而儲存於在光碟機!中 之記憶體中。儲存值係用於讀取資料。 實質上’所揭示讀取校正程序係基於同時執行聚焦偏移 校正及傾斜偏移校正。獲得在聚焦偏移、傾斜偏移與抖動 信號之間的3維關係。由該3維關係獲得最佳讀取聚焦偏移 值及最佳讀取傾斜偏移值。該3維讀取校正方法通常改良 、,準確(·生且知到系統讀取傾斜偏移及讀取聚焦偏移。可 通常改良光碟機之整體讀取效能。 :又:實施例中’獲得在聚焦偏移、傾斜偏移與徑向循 軌&差k號之間的3維關係。在徑向循軌誤差信號大體上 =大處得到最佳寫人聚焦偏移值及最佳寫人傾斜偏移值。 " 聚“、、偏移、傾斜偏移與徑向循轨誤差信號之間的3 123904.doc •17- 200822088 維關係之步驟包含以下内容··獲得聚焦偏移步長、傾斜偏 移步長、最大可允許聚焦偏移值及最大可允許傾斜偏移 值’如前文所描述。此程序之可能結果在圖4中示意性地 說明且涉及以下步驟·· 開始,其中相位N=i。 2 模式 將聚焦偏移模式及傾斜偏移模式預設定為斜坡上升 對相位N設定斜坡模式。 4 將聚焦偏移及傾斜偏移設定為預設值。 设定聚焦偏移=聚焦偏移+焦點-步長 傾斜偏移=傾斜偏移+傾斜_步長 6·量測峰值至峰值徑向循執誤差信號。 若該等校正 7·檢查在相位N中之所有校正點是否完整 點元整,則轉至步驟8 ,否則重複步驟5至7。 否則轉至步 8.檢查N是否>4。若N>4,則轉至步驟1〇 驟9。 9·設定相位N=N+1 ;檢查N是否>4,若N>4,則轉至步 驟10,否則重複步驟3至8。 乂 10.形成量測徑向循執誤差信號之向量。 11 · ef ^—階表面模型係數。 12 ·曲線擬合聚焦偏移值、傾斜 阻頂斜偏移值及毪向循規誤差 信號值且獲得3維關係。 應注意,量測時間大體上等於執行—次碟片旋轉需要之 時間’使得徑向循軌誤差信號值之量測結果為在—次碟片 123904.doc 18 200822088 旋轉中之平均值。 亦可能量測擺動信號振幅而 著執行校正。 非徑向循執誤差信號,且接 圖5示意性地說明使用以上程序 々斤後侍之寫入校正結果之 一實例。對DVD機1(參看圖1)執杆兮妒广 ^ 丁该%序。編碼聚焦偏移 值及編碼傾斜偏移值相對於徑向循軌誤差信號值成曲線。 圖5說明二階表面關係之一實例。利用校正資衫(編碼Table 1 shows an example of the read correction result obtained by the DVD player 1 (refer to Fig. 1). The total correction point (in the DVD player) is set to a total of 17 points as shown in Fig. 3 so that the system is throughout The 稳定 correction point, the focus offset step size, and the tilt offset step size are determined in a substantially stable manner during the calibration process. This is performed to ensure accurate surface fitting and prediction of the jitter to the focus offset surface and the tilt offset surface, such that The optimum setting can be accurately obtained. Due to the sensitivity of the focus offset and tilt offset to the influence of the CD player system (affecting the tracking performance), the range of the allowable focus offset adjustable range and the tilt offset adjustable range is used. An unstable state can be reached when the focus offset and/or tilt offset are set too far from the optimal point, in which case the radial circumstance or ^^# can be adversely affected (eg, when the disc When the quality is very poor, such as in the case where the thickness of the disc substrate layer c is substantially different from the disc standard.) To eliminate this situation: If i·measured HF jitter level > 13% ii · Exist due to poor HF Some phase lockbacks due to signal quality Locking the early ones will reduce the focus offset step by half (even if half a step still cannot collect enough stable correction points), the step size can be repeated repeatedly. The phase-locked loop fault is usually at the system clock. This can only occur when a bad HF signal cannot be locked. This usually occurs when the HF signal is bad (bad eye diagram, bad hf signal is not correct for 123904.doc •16- 200822088 private, modulation or when the focus offset value and tilt offset value are far from the most Good focus offset value and tilt offset value) : In the data shown in Table 1, 'the best focus offset is 255 18 _ and the optimal tilt offset is 丨.21 mrad. The minimum jitter is 8 2 %. Under similar conditions, when using the separate calibration method, the following values are obtained: 277 73 nm best focus offset ' _9 〇 4 job ^ optimal tilt offset. Minimum jitter is 9.2%. Observe, Using the disclosed 3D read correction method, the HF^ jitter performance is increased by 1%. 聚焦In the manufacture of the optical disk drive 1 (see Figure (10), the focus offset correction and tilt offset correction are performed depending on the disc type and the rotational speed. The correction value is stored in the optical disk drive 1. Stored in the light This value in the disc drive is used as a preset value. During the subsequent start-up, the 3-dimensional read correction is performed. The best read focus offset value and the best read tilt offset value obtained are based on the area. Stored in the memory in the CD player! The stored value is used to read the data. Essentially, the disclosed read correction procedure is based on simultaneous execution of focus offset correction and tilt offset correction. The 3-dimensional relationship between the tilt offset and the jitter signal. The optimal read focus offset value and the optimal read tilt offset value are obtained from the 3-dimensional relationship. The 3-dimensional read correction method is usually improved, accurate ( • It is known that the system reads the tilt offset and reads the focus offset, which can generally improve the overall read performance of the optical disc drive. : Again: In the embodiment, a 3-dimensional relationship between the focus offset, the tilt offset, and the radial tracking & difference k is obtained. The optimum write focus offset value and the optimum write tilt offset value are obtained at a radial = substantially large error signal. " The convergence between the "," offset, tilt offset, and radial tracking error signals. 123 123.doc • 17- 200822088 The steps of the dimensional relationship include the following: · Obtain the focus offset step, tilt offset step The long, maximum allowable focus offset value and the maximum allowable tilt offset value are as described above. The possible results of this procedure are schematically illustrated in Figure 4 and relate to the following steps, where phase N = i. 2 Mode Presets the focus shift mode and tilt shift mode to ramp up Set the ramp mode to phase N. 4 Set the focus offset and tilt offset to the preset value. Set focus offset = focus offset + focus - Step tilt offset = tilt offset + tilt _ step length 6. Measure peak to peak radial tracking error signal. If the corrections 7 check whether all the correction points in phase N are complete points, Then go to step 8, otherwise repeat steps 5 to 7. Otherwise go to step 8. Check if N > 4. If N > 4, go to step 1 step 9. 9 · Set phase N = N + 1; Check if N is > 4, if N > 4, go to step 10, otherwise repeat steps 3 to 8. 10. Form a vector for measuring the radial tracking error signal. 11 · ef ^ - order surface model coefficient. 12 · Curve fitting focus offset value, tilt resistance top offset value and heading error signal value and Obtain a 3-dimensional relationship. It should be noted that the measurement time is substantially equal to the time required to perform the rotation of the disc - so that the measurement result of the radial tracking error signal value is in the rotation of the disc 123904.doc 18 200822088 The average value can also be measured by the energy measurement of the amplitude of the wobble signal. The non-radial tracking error signal, and Figure 5 schematically illustrates an example of the result of the writing correction using the above procedure. 1 (See Fig. 1) The 聚焦 ^ ^ % % % 。 。 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码 编码Use correction shirt (code
t焦偏移值)、γ(編碼傾斜偏移值)及2(正規化徑向猶軌誤 差)’計鼻係數❼Β π # 5 4…及〜。接著將最佳寫入 聚焦偏移值及最佳寫入傾斜偏移值計算為, ^0PKi-e.optimumwritefocusoffset) = (2〇2^5 ~ ^3^)/— 4ί24α5) (5) Y〇pt (Le .optimumwritetiltoffset) =(2a3a4 - a2a6)/(a62 一 4a4a5)...........⑹ 最佳寫人聚焦偏移值及最佳寫人傾斜偏移值為編碼值, 且將在用於在DVD上記錄資料之前被解碼。 以使系統在整個校正過程中大多數情盯穩定之方式確 定校正點、聚线移步長及傾斜偏移步n經執行以保 證徑向循執誤差信號或擺動信號振幅對聚焦偏移表面及傾 斜^移表面之準確表面擬合及制,使得可準確得到理想 最佳设A。由力聚焦偏移及傾斜偏移對光碟機循規效能之 影響的敏感性,使用小於可允許聚焦偏移可調整範圍及傾 斜:移可調整範圍之範圍。當將聚焦偏移及/或傾斜偏移 »又定成距其最佳點過遠時,可發生狀態不穩定之徑向偏 軌。為排除此情況,若 用於記錄之有效校正點數目低於6,或 123904.doc -19- 200822088 i i ·偵測到一此彳⑤a # & 半 二向偏執,則將聚焦偏移步長減少一 在製造光碟機丨期間,禎 移校正及傾斜偏移校正且而執行聚焦偏 I將杈正值儲存於光碟機1中。德 Ο u =光碟機k此等值制作預設值。在隨後啟動期間, 订…、入才父正。所獲得之最佳寫入聚焦偏移值及最佳 -入傾斜偏移值根據區域而儲存於在光碟機中之記 中。儲存值係用於記錄資料。 〜一 :貝上所揭不寫入校正程序係基於同時執行聚焦偏移 X及傾斜偏移校正。獲得在聚焦偏移、傾斜偏移盘徑向 循軌誤差信號之間的3維關係。由該3維關係獲得最佳寫入 聚焦偏移值及最佳寫入傾斜偏移值。該3維寫入校正方法 通电改良校正準確性且得到系統寫入傾斜偏移及寫入聚隹 偏移。可通常改良光碟機之整體記錄效能。 …、 現參看圖1,光碟機1可經修改以執行如實施例中所揭示 之枝正方法。為此,光碟機1包括一第一記憶體加〇〇,咳 第一記憶體2_經配置以儲存校正資料點。此外,光碟機 1包括-第二記憶體編,該第二記憶體扇經配置以儲 =最佳讀取m移值、最佳讀取傾斜偏移值、最佳寫入 聚焦偏移值及最佳寫人傾斜偏移值。分量χτ係由 儲存校正資㈣計算且料於光碟機之第—記憶體編 中。控制電路90(參看圖υ包括一整合校正單元胸,該整 合校正單元1000經配置以在將記錄載體插入於光碟機中之 後同時執行對聚焦偏移及傾斜偏移之校正,如實施例中所 t〇^904.doc -20- 200822088 描述。 具有光碟機!之記錄器或播放機可 及傾斜偏移之校正,籍此改良該記錄器/播放機焦偏移 錄/讀取效能。光碟機丨能夠 、之整體記 可能的。此外,在铸記錄载體2亦係 至少一記錄操作。 。己錄益可執行 儘管已由使用DVD機及DVD碟片之實施T-focus offset value), γ (coded skew offset value), and 2 (normalized radial orbital error) count nasal coefficients π π # 5 4... and ~. Then calculate the best write focus offset value and the best write tilt offset value as ^0PKi-e.optimumwritefocusoffset) = (2〇2^5 ~ ^3^)/— 4ί24α5) (5) Y〇 Pt (Le .optimumwritetiltoffset) = (2a3a4 - a2a6) / (a62 - 4a4a5)...........(6) The best writer focus offset value and the best writer tilt offset value are the encoded values. And will be decoded before being used to record material on the DVD. The correction point, the gather shift step, and the tilt offset step n are determined in such a manner that the system is mostly stable throughout the calibration process to ensure that the radial trace error signal or the wobble signal amplitude is on the focus offset surface and The accurate surface fitting and system of the tilting surface makes it possible to accurately obtain the ideal optimum A. Sensitivity to the effect of force focus offset and tilt offset on the compliance performance of the disc drive, using a range that is less than the allowable focus offset adjustable range and the tilt: shift adjustable range. When the focus offset and/or tilt offset » is again set too far from its optimum point, a radially unstable rail with state instability can occur. To eliminate this, if the number of valid correction points for recording is less than 6, or 123904.doc -19- 200822088 ii · If a 彳5a # & semi-two-way paranoia is detected, the focus offset step will be The reduction correction and the tilt offset correction are performed during the manufacture of the optical disk drive, and the focus bias I is performed to store the positive value in the optical disk drive 1. De Ο u = CD player k this value to make a preset value. During the subsequent start-up, order... The optimum write focus offset value and the optimum-input tilt offset value obtained are stored in the recorder in the disc player according to the area. Stored values are used to record data. ~1: The correction procedure is not written on the shell, which is based on simultaneous execution of the focus offset X and tilt offset correction. A 3-dimensional relationship between the focus offset and the tilt offset disk radial tracking error signal is obtained. The optimum write focus offset value and the optimum write tilt offset value are obtained from the 3-dimensional relationship. The 3-dimensional write correction method energizes to improve the correction accuracy and obtains the system write tilt offset and write poly offset. The overall recording performance of the optical disk drive can usually be improved. ..., referring now to Figure 1, the optical disk drive 1 can be modified to perform the positive method as disclosed in the embodiments. To this end, the optical disk drive 1 includes a first memory plus, and the first memory 2_ is configured to store corrected data points. In addition, the optical disc drive 1 includes a second memory block configured to store an optimal read m shift value, an optimal read tilt offset value, an optimum write focus offset value, and The best write tilt offset value. The component χτ is calculated by the storage correction (4) and is included in the first memory of the CD player. The control circuit 90 (see FIG. υ includes an integrated correction unit chest configured to simultaneously perform correction of focus offset and tilt offset after inserting the record carrier into the optical disk drive, as in the embodiment T〇^904.doc -20- 200822088 Description A recorder or player with a CD player can correct the tilt offset, thereby improving the recorder/player focus offset/read performance. In addition, the cast record carrier 2 is also at least one recording operation. The self-recording executable can be implemented despite the use of DVD players and DVD discs.
7但該校正方法可應用於所有類型之光碟媒體及光: 機,例如’單次寫入媒體及多次寫入可記錄先碟 RW、謂-RW、DVD+RW、藍光碟片)。熟習此項技|舒者 可以軟體或以硬體及軟體兩者實施校正方法之所描述實施 例。實踐所主張發明之熟習此項技術者經由學習圖式、揭 不内容及隨附申請專利範圍可理解且實現對所揭示實施例 之其他改變。動詞”包含”之使用並不排除存在除彼等陳述 於申請專利範圍或描述中之元件之外的元件。在元件或步 驟前之不定冠詞”一,,的使用並不排除存在複數個該等元件7 However, the calibration method can be applied to all types of optical disc media and optical: for example, 'single write media and multiple writes can record first disc RW, pre-RW, DVD+RW, Blu-ray disc). Those skilled in the art can implement the described embodiments of the method of correction either in software or in both hardware and software. Other variations to the disclosed embodiments can be understood and effected by the teachings of the invention. The use of the verb "comprise" or "comprising" does not exclude the claim The use of the indefinite article “a” before an element or step does not exclude the existence of the plural.
或步驟。應將圖及描述視為僅說明性的且並不限制本發 明。 X 總之,描述一種校正光碟機之方法。該方法包含在將記 錄載體插入於光碟機中之後同時執行對聚焦偏移及傾斜偏 移之校正。 【圖式簡單說明】 圖1示意性地說明例示性DVD機; 圖2a及圖2b示意性地說明藉由在例示性DVD機中獨立執 1 "H904.doc •21 - 200822088 行聚焦偏移校正及傾斜偏移校ιΜ 圖3示意性地展示經選擇 又結果; 丁、、擇以在例示性DVD機中π 士 聚焦偏移校正及傾斜偏移校正之校正點; °時執行 圖4示意性地說明藉由在例示性dvd機中同時執一 a 偏移校正及傾斜偏移校正而獲得之讀取校正結果·2聚焦Or steps. The drawings and the description are to be regarded as illustrative only and not limiting. X In summary, a method of calibrating an optical disk drive is described. The method includes performing corrections for focus offset and tilt offset simultaneously after inserting the record carrier into the optical disk drive. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 schematically illustrates an exemplary DVD player; FIGS. 2a and 2b schematically illustrate the focus shift by independently performing 1 "H904.doc •21 - 200822088 in an exemplary DVD player; Correction and tilt offset calibration Fig. 3 schematically shows the selected and the result; D, the correction point of the π-spot focus offset correction and the tilt offset correction in the exemplary DVD player; Explain the reading correction result obtained by simultaneously performing an offset correction and tilt offset correction in an exemplary dvd machine.
圖5不意性地說明藉由在例示性DVD機中同時執行$ 偏移校正及傾斜偏移校正而獲得之寫入校正結果。丁聚焦 【主要元件符號說明】 1 光碟機 2 記錄載體 4 馬達 5 旋轉軸 6 夾持軸套 7 主軸 30 光學系統 31 光產生器 32a 光束 32b 光束 32c 光束 32d 光束 33 光束分光器 34 接物鏡 35 光學偵測器 36 光軸 123904.doc -22· 200822088 ΓFig. 5 unintentionally illustrates a write correction result obtained by simultaneously performing $ offset correction and tilt offset correction in an exemplary DVD player. Ding Focus [Major component symbol description] 1 CD player 2 Record carrier 4 Motor 5 Rotary shaft 6 Clamping sleeve 7 Spindle 30 Optical system 31 Light generator 32a Beam 32b Beam 32c Beam 32d Beam 33 Beam splitter 34 Objective lens 35 Optics Detector 36 optical axis 123904.doc -22· 200822088 Γ
40 致動器系統 41 徑向致動器 42 聚焦致動器 43 傾斜致動器 90 控制電路 91 讀取信號輸入端 92 第一輸出端 93 第二輸出端 94 第三輸出端 95 第四輸出端 1000 整合校正單元 2000 記憶體 2100 記憶體 F 焦點 ScF 控制信號 ScM 控制信號 ScR 控制信號 Sct 控制信號 Sr 讀取信號 Ti、Tn 磁軌 123904.doc -23-40 Actuator system 41 Radial actuator 42 Focusing actuator 43 Tilting actuator 90 Control circuit 91 Read signal input 92 First output 93 Second output 94 Third output 95 Fourth output 1000 Integrated Correction Unit 2000 Memory 2100 Memory F Focus ScF Control Signal ScM Control Signal ScR Control Signal Sct Control Signal Sr Read Signal Ti, Tn Track 123904.doc -23-
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| Country | Link |
|---|---|
| TW (1) | TW200822088A (en) |
| WO (1) | WO2008023319A1 (en) |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5898654A (en) * | 1994-07-14 | 1999-04-27 | Matsushita Electric Industrial Co., Ltd. | Optical disk and optical disk apparatus having a predetermined pattern of marks on tracks such that a reproduced signal is caused to jitter |
| JP3702817B2 (en) * | 2000-09-13 | 2005-10-05 | ティアック株式会社 | Optical disk drive device |
| DE60318424T2 (en) * | 2002-04-02 | 2008-12-18 | Koninklijke Philips Electronics N.V. | METHOD AND DEVICE FOR TILTING CORRECTION BY MEANS OF A MULTI-DIMENSIONAL ACTUATOR |
| TWI260013B (en) * | 2003-12-04 | 2006-08-11 | Mediatek Inc | Optical incidence auto-adjusting system |
-
2007
- 2007-08-20 TW TW96130849A patent/TW200822088A/en unknown
- 2007-08-20 WO PCT/IB2007/053309 patent/WO2008023319A1/en not_active Ceased
Also Published As
| Publication number | Publication date |
|---|---|
| WO2008023319A1 (en) | 2008-02-28 |
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