TW200837733A - Optical disc and recording power determination method - Google Patents

Optical disc and recording power determination method Download PDF

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Publication number
TW200837733A
TW200837733A TW96137946A TW96137946A TW200837733A TW 200837733 A TW200837733 A TW 200837733A TW 96137946 A TW96137946 A TW 96137946A TW 96137946 A TW96137946 A TW 96137946A TW 200837733 A TW200837733 A TW 200837733A
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Taiwan
Prior art keywords
recording power
power
radiation beam
recording
record
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TW96137946A
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Chinese (zh)
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Yu Zhou
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Koninkl Philips Electronics Nv
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Publication of TW200837733A publication Critical patent/TW200837733A/en

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    • 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
    • G11B7/004Recording, reproducing or erasing methods; Read, write or erase circuits therefor
    • G11B7/0045Recording
    • 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
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/125Optical beam sources therefor, e.g. laser control circuitry specially adapted for optical storage devices; Modulators, e.g. means for controlling the size or intensity of optical spots or optical traces
    • G11B7/126Circuits, methods or arrangements for laser control or stabilisation
    • G11B7/1267Power calibration

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  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Recording Or Reproduction (AREA)
  • Optical Head (AREA)

Abstract

A method (300) of determining an optimum recording power of a radiation beam for recording data onto a record carrier is disclosed. The method comprises determining a first recording power of the radiation beam based on Jitter and a second recording power of the radiation beam based on block error rate (BLER). The method further comprises determining the optimum recording power of the radiation beam based on a difference between the first recording power of the radiation beam and the second recording power of the radiation beam. The technique is useful for all optical disc recording devices.

Description

200837733 九、發明說明: 【發明所屬之技術領域】 本發明主旨係關於一種光碟記錄 關於用於在一光碟上記錄資料的_輻1且更明確地說係 ^ 射束之記錄功率之決 疋0 ^ 【先前技術】 US2003/0053386揭示一光碟梦署 、罝,其中用於在一 上寫入資料的雷射光功率係最佳化。一“ •冑料同時改變雷射光功率,並基於_=碟上寫入測試 口所卡柯乂土&amp;斗 、、J忒貝料之重播信號的 口口貝來敢仫化該雷射光功率。藉由 不精確。 万法獲侍的雷射功率 較有利的係具有精轉地決定適人 疋週口於在一記錄載體上記錄 貝枓的輻射束之一最佳記錄功率 ^ ^ . ^ 法亦杈有利的係具 有精確地決定適合於在該記錄 一县杜巧议上古 ㈣體上錢錢的輻射束之 最“ δ己錄功率的驅動器。 【發明内容】 ^ «錢用於在—記錄載體上記錄資料的—賴射束 之最佳記錄功率的方法。兮 * 一外 該方法決定基於抖動的輻射束之 二一記錄功率與基於區塊錯誤率的輻射束之-第二記錄 1血:財法進—步包含決定基於該輻射束之第-記錄功 午2輻射束之第二記錄功率之間的差的輻射束之最佳記 録功率。 島示之驅動器中,該驅動器包含一光學拾取單 70其係配置成用以產生一輻射束並將該輜射束聚焦於一 125644.doc -5- 200837733 記錄載體上。該驅動器進—步包含—控制單元,其係配置 成=以控制該光學拾取單元,其中該控制單元進-步包含 -第-記錄功率決定單元,其係置成用以決定基於抖動 的輻射束之一第一記錄功率。該控制單元進一步包含—第 二記錄功率決定單元’其係配置成用以決定基於區塊錯誤 率的輻射束之一第二記錄功率。該控制單元進一步包含一 最佳記錄功率決定單元,其係配置成用以決定絲該輕射 束之第-記錄功率與該輻射束之第二記錄功率之間的差的 輻射束之最佳記錄功率。 此外,精確決定用於在一記錄載體上記錄資料之一輻射 束之-最纟呑己錄X力率的彳法可使用—電腦冑式加以實施。 【實施方式】 圖3顯示決定用於在一記錄載體上記錄資料之一輻射束 的最佳記錄功率的方法3〇〇。在步驟3〇2中,決定基於抖動 的輪射束之一第—記錄功率。在步驟304中,&amp;定基於區 塊錯誤率(BLER)的輻射束之一第二記錄功率。在步驟3〇6 中决定基於该輻射束之第一記錄功率與該輻射束之第二 記錄功率之間的差的輻射束之最佳記錄功率。 抖動係HF彳a號品質之一極低位準/實體指示。通常,若 該HF信號抖動較低,則該信號品質受到保障並因而導致更 佳的資料精確性。BLER係區塊或訊框每秒具有至少一不 正確位兀的速率。BLER表示需欲進行讀取之資料的實際 。。質。通常假定低抖動意味著低BLER,其係大多數記錄 器或播放器使用抖動作為針對幾乎所有校準之一指數的原 125644.doc 200837733200837733 IX. INSTRUCTIONS OF THE INVENTION: TECHNICAL FIELD OF THE INVENTION The subject of the present invention relates to a disc recording of the recording power of the ray 1 for recording data on a disc and more specifically the beam. ^ [Prior Art] US 2003/0053386 discloses a CD-ROM, in which the laser light power for writing data on one is optimized. "" The material changes the laser light power at the same time, and based on the _= written on the disc, the mouth of the test port, the 重 & & 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 By means of inaccuracy, the laser power that is favored by the law is more favorable to determine the optimum recording power of one of the radiation beams of the Bayer on a record carrier. The Fa is also advantageous in that it has the ability to accurately determine the most "δ-recorded power" of the radiation beam that is suitable for the money spent on recording the ancient (4) body in the county. SUMMARY OF THE INVENTION ^The method of "money for recording the best recording power of the beam on the record carrier".兮* The method determines the two-dimensional recording power of the dither-based radiation beam and the radiation beam based on the block error rate - the second record 1 blood: the financial method further comprises determining the first-recording work based on the radiation beam The optimum recording power of the radiation beam of the difference between the second recording power of the beam of radiation. In the island display driver, the driver includes an optical pickup unit 70 configured to generate a beam of radiation and focus the beam onto a record carrier of 125644.doc -5 - 200837733. The driver further includes a control unit configured to control the optical pickup unit, wherein the control unit further includes a -th recording power determining unit configured to determine the jitter-based radiation beam One of the first recording powers. The control unit further includes a second recording power decision unit </ RTI> configured to determine a second recording power of one of the radiation beams based on the block error rate. The control unit further includes an optimum recording power determining unit configured to determine an optimum recording of the radiation beam of the difference between the first recording power of the light beam and the second recording power of the radiation beam power. In addition, the precise determination of the radiation beam used to record a beam of data on a record carrier can be carried out using a computer-based method. [Embodiment] Fig. 3 shows a method of determining the optimum recording power for a radiation beam for recording data on a record carrier. In step 3〇2, the first-recording power of one of the dither-based round beams is determined. In step 304, &amp; one of the radiation beams based on the block error rate (BLER) is the second recording power. The optimum recording power of the radiation beam based on the difference between the first recording power of the radiation beam and the second recording power of the radiation beam is determined in step 3〇6. Jitter is one of the very low level/physical indications of HF彳a quality. Generally, if the HF signal has low jitter, the signal quality is guaranteed and thus leads to better data accuracy. The BLER block or frame has a rate of at least one incorrect bit per second. BLER indicates the actual information that needs to be read. . quality. It is generally assumed that low jitter means low BLER, which is the original for most recorders or players to use jitter as an index for almost any calibration. 125644.doc 200837733

因。研究已顯示BLER與抖動之間的清楚相關性。當抖動 並不那麼高時,一較低的抖動可導致一高BLER,反之亦 然。此可以係由於媒體之性質及/或光碟裝置系統之特性 所致。依據媒體與系統特性使用BLER或抖動將保障對應 媒體與系統達到最佳性能。依據該媒體與該系統特性選擇 一對應功率校準指數提供適合於該些媒體的最佳記錄功率 (即實現隶佳媒體記錄品質)。隨著環境的改變(如溫度與濕 度),媒體穩定性與DVD土R/RW之特性會改變,而該bler 將比抖動提供更佳的此改變及與不可校正誤差之相關性的 指示。因此,在所揭示方法中使用bler。 在一具體實施例中,決定基於該輻射束之第一記錄功率 與孩輻射束之第二記錄功率之間的差的輻射束之最佳記錄 功率包括決定基於校準段差的輻射束之光學記錄功率。此 條件有助於決定要使用何校準功率。 在另一具體實施例中,基於用於在該記錄載體上記錄資 料的輻射束之功率的解析度來決定該等校準段差。校準段 差的數目取決於校準功率解析度。例如,該校準段差可對 應於每一段差0.75 mW。解釋此點的另一方式係使用〇75 mW的校準功率差而非該等校準功率段差之一詳細表示。 在另—具體實施例中,決定基於該等校準段差的輻射束 之最佳記錄功率包括決定該輻射束之第—記錄功率與該輻 射束之第二記錄功率之間的差是否實質上大於2個校準段 :。若該差大於2個校準段差’則決定處於該輻射束之; 一記錄功率的BLER計數是否比處於該輻射束之第二記錄 125644.doc 200837733 功率的BLER計數大-預定的計數數目且若係如此則 選擇該輻射束之第二記錄功率作為該輻射束之最佳記錄功 率。該預定的計數數目可以係大約〗5。 若(第一記錄功率〜第二記錄功率)&gt;2個校準段差,則{若 (處於第-記錄功率的BLER計數—處於第二記錄功率的 BLER計數)&gt;15)則{最佳記錄功率=第二記錄功率}。 在另-具體實施例中,使用該輻射束之決定的最佳記錄 功率來在該記錄載體上記錄資料。此確保較佳的記錄品質 並改良總體記錄性能。 在另-具體實施例中’基於抖動的輻射束之第一記錄功 率與基於BLER的輻射束之第二記錄功率的衫包括以下 步驟且在圖4中顯示此程序之一可能結果, 1·將該輻射束之記錄功率設定為最大允許功率,其係計 算為 Pwp+25%。 2·以一段差大小來減小測試功率值; 3 ·在該記錄載體上記錄測試資料。 4. U買取遠5己錄的測試資料並測量抖動與bler。 5. 重複步驟2至4直至該測試功率值達到一最小測試功 率’其對應於Pwp-25%。 6·曲線擬合該等測試功率值與對應的抖動與BLER值。 7·找到該抖動實質上最小的輻射束之第一記錄功率。 8·找到該BLER實質上最小的輻射束之第二記錄功率。 基於抖動的功率校準係在β之功率校準結果的基礎上加 乂執行。其意味著,該系統首先執行該β-OPC並獲得該校 125644.doc 200837733 準光功率Pwp,其對應於該媒體所要求的目標β值。針對 基於抖動的微調校準的開始功率將係PwP - 25%。針對抖 動的最大校準功率將係Ρ\νβ + 25%。在此校準功率範圍 内,如圖5所示,選擇15個段差的功率。 如圖5所示,針對每一功率Pi pregroove ;預刻溝槽内位址)訊框(即2個ECC (error correction code ;誤差校正碼)區塊=4個ADIP訊框而1個 ADIP訊框=4個實體磁區)。當實施抖動與bLER之測量時,because. Studies have shown a clear correlation between BLER and jitter. When jitter is not as high, a lower jitter can result in a higher BLER and vice versa. This may be due to the nature of the media and/or the characteristics of the disc device system. Using BLER or jitter based on media and system characteristics will ensure optimal performance for the media and system. Selecting a corresponding power calibration index based on the media and the system characteristics provides an optimum recording power suitable for the media (i.e., achieving superior media recording quality). As the environment changes (such as temperature and humidity), the stability of the media and the characteristics of the DVD soil R/RW will change, and the bler will provide better indication of this change and the correlation with the uncorrectable error than jitter. Therefore, bler is used in the disclosed method. In a specific embodiment, determining an optimum recording power of the radiation beam based on a difference between the first recording power of the radiation beam and the second recording power of the radiation beam comprises determining an optical recording power of the radiation beam based on the calibration step difference . This condition helps determine which calibration power to use. In another embodiment, the calibration step differences are determined based on the resolution of the power of the radiation beam used to record the data on the record carrier. The number of calibration step differences depends on the calibration power resolution. For example, the calibration step can correspond to a difference of 0.75 mW per segment. Another way to interpret this is to use a calibrated power difference of 〇75 mW instead of one of the calibrated power step differences. In another embodiment, determining an optimum recording power of the radiation beam based on the calibration step includes determining whether a difference between the first recording power of the radiation beam and the second recording power of the radiation beam is substantially greater than 2 Calibration segments: If the difference is greater than 2 calibration step differences, then it is determined to be in the radiation beam; whether the BLER count of a recording power is greater than the BLER count of the power of the second record of the radiation beam 125644.doc 200837733 - the predetermined number of counts and if The second recording power of the radiation beam is then selected as the optimum recording power of the radiation beam. The predetermined number of counts can be about 7.5. If (first recording power to second recording power) &gt; 2 calibration step differences, then {if (BLER count at the first recording power - BLER count at the second recording power) &gt; 15) then {best record Power = second recording power}. In another embodiment, the determined recording power of the radiation beam is used to record data on the record carrier. This ensures better recording quality and improves overall recording performance. In another embodiment, the first recording power of the jitter-based radiation beam and the second recording power of the BLER-based radiation beam comprise the following steps and one of the possible outcomes of the procedure is shown in FIG. The recording power of the radiation beam is set to the maximum allowable power, which is calculated as Pwp + 25%. 2. Reduce the test power value by a difference in length; 3. Record the test data on the record carrier. 4. U buy test data from far 5 and measure jitter and bler. 5. Repeat steps 2 through 4 until the test power value reaches a minimum test power' which corresponds to Pwp-25%. 6. Curve fitting the test power values and corresponding jitter and BLER values. 7. Find the first recorded power of the radiation beam that is substantially the smallest. 8. Find the second recording power of the substantially minimum beam of radiation of the BLER. The jitter-based power calibration is performed on the basis of the beta power calibration result. It means that the system first executes the β-OPC and obtains the school 125644.doc 200837733 quasi-optical power Pwp, which corresponds to the target beta value required by the medium. The starting power for the jitter-based trimming calibration will be PwP - 25%. The maximum calibration power for jitter will be Ρ\νβ + 25%. Within this calibrated power range, as shown in Figure 5, 15 steps of power are selected. As shown in FIG. 5, for each power Pi pregroove; pre-groove intra-site address frame (ie, 2 ECC (error correction code) blocks = 4 ADIP frames and 1 ADIP signal Box = 4 physical magnetic regions). When performing jitter and bLER measurements,

8個ADIP訊框的記錄補償諸如離心率之類的可能誤差,使 得該抖動與BLER讀出測量在一碟片旋轉期間發生。該記 錄係從該記錄載體之外部邊緣至其内部邊緣而執行。該開 始功率係由β OPC之Pwp的功率導出,如圖5所示。該雷射 功率將以15個功率位準(30個ECC區塊)從pwp + 25%行進 直至Ρχνβ _ 25%。於每一功率位準,在一旋轉期間測量抖 動與BLER並計算平均值。”校正指向前感測校正。 圖6示意性解說針對一範例性〇¥;〇+以汛碟片的與碟片半 徑成函數關係的完整最佳功率控制程序。該程序包括執 行:i) β-OPC ; ii)抖動&amp; BLER_OPC ; m)向前感測校正; 乂及IV)寫入檢查。實際上’引入一 β之校正來補償雷射中 :光學回授。為找出應使用何校正,將讀取該向前感測同 柃寫入该碟片上之一空白區域。因此,使用實際決定的光 學㈣個ECC區塊寫入内部碟片職區域。針對 此等1.5個ECCI1塊讀取向前感測值。基於此等值,一校正 的β值係基於該測量的降而計算。校正㈣值與測量㈣值 125644.doc 200837733 之間的Δ差應在一特定視窗(例如1〇%)内,否則執行重試直 至該得爾塔差處於該允許視窗内。 圖4係一曲線圖,其示意性解說使用上面列舉的步驟針 對一較佳TDK R8x DVD+R碟片獲得之結果的範例。該抖 動、區塊錯誤率(垂直軸)係針對該等測試功率值(水平轴) 繪製。該等方塊指示測量結果。熟習此項技術者應清楚, 具有針對X=Xm之最小值的任何函數γ(χ),在此最小值 周圍之一小範圍内,可藉由依據以下等式之二次函數合理 地近似 Y(X)=c〇+c1(X-Xm)+c2(X.Xm)2 其中C0、4及4係常數。找到針對測量 效於找到針對X▲…知的最佳值。通t,此係2 熟知的最小平方方法完成,其無需在此解釋。在任何情況 下,熟習此項技術者應清楚,可基於在此一函數之最小值 周圍的數個測量來計算一最佳拋物線擬合,並因此可計算 、與丫以义。。圖4所示曲線解說此一拋物線擬合。使用 x(抖動/BLER)與Y(測試功率值)之校正資料,可計算係數 Co、Mc2。在計算該等係數c。、〇1及。2之後,計算該點4 並將該輻射束之第一記錄功率設定為對應於該最小抖動值 之一最佳值。在相同線上,將該輻射束之第二記錄功率設 定為對應於該最小區塊錯誤率(BLER)之一最佳值。此外, 如具體實施例所說明,該最佳記錄功率係使用該輻射束之 第一記錄功率與第二記錄功率加以決定。該最小抖動或區 塊錯誤率(BLER)之決定係基於多項式回冑,而因此所獲得 125644.doc -10- 200837733 的最佳記錄功率係精確與可靠的。 在另-具財施財,㈣決定該輻射束 率與該輻射束之第二記錄功率。 ^力 應庄思,在一碟片旋轉期 間該BLER測量應與該抖動 率之類的誤差。同時執起發生以補償諸如離心 &gt; +動”BLER 〇pc以減低總體 Ο P C 間。在—韓 66 SL· X人 1. ^ 句可濾出隨機測量雜訊並且亦 可濾出藉由碟片偏差與轉盤馬達擺動引人的週期性干擾。 在另一具體實關巾,針對該測試功率值之每—變更在 該記錄載體上記錄測試資料 匕祜以具有從該記錄載體之中 心至該記錄載體之一外部邊 吋次抓丄 緣S加之半徑的同心圓記錄測 试負料。由於媒體中的變更 料厚度、製造變更)”二(=塵、指紋、刮痕、染 、_ 文广、衣境改變所致’需要動態功率校準 以補你記錄時所發現的德莫 良好記錄品質。 。此確保橫跨整個記錄載體的 在另一具體實施例中,針對該測試功率值之每-變更在 ==载體上記錄測試資料包括以具有從該記錄載體之外 二ΓίΓ錄載體之中心減小之半徑的同心圓記錄測試 =更此確保橫跨整個記錄載體的良好記錄品質並補償媒 如兮望θ㈣動111GG可以係調適成用以執行決定用於 =具體實施例所揭示在該記錄载體i。上記錄資料的一 人佳記錄功率的方法。為此目的,該控制單元24 基於料=°己錄功率決定單元24A,其係配置成用以決定 土、 &amp;輻射束之-第-記錄功率。該控制單元24進一 125644.doc 200837733 步包含一第二記錄功率決定單元24B,其係配置成用以決 定基於區塊錯誤率(BLER)的輻射束之一第二記錄功率。該 控制單元24進一步包含一最佳記錄功率決定單元,其 係配置成用以決定基於該輻射束之第一記錄功率與該輻射 束之弟一 §己錄功率之間的差的輻射束之最佳記錄功率。 具有該驅動器100之一記錄器可執行最佳功率校準並如 該等具體實施例所揭示來決定該輻射束之最佳記錄功率, 從而改良該記錄器的總體記錄性能。 雖然已藉由使用DVD碟片的具體實施例來說明本發明主 曰’但本發明主旨可應用於所有類型的記錄載體,例如, 一-人寫入媒體與多次寫入可記錄類型(Dvd-RW、 DVD+RW、藍光碟片)。其不限於單面兩層記錄載體(即雙 層記錄載體)或雙面兩層記錄載體(即雙面雙層記錄載體)。 熟習此項技術者可在軟體中或在硬體與軟體兩者中實施決 定用於記錄資料的一輻射束之最佳記錄功率之方法的所述 具體實施例。熟習實施所主張主旨之技術者由研究圖式、 揭示内容及隨附申請專利範圍可瞭解並實現所揭示具體實 施例之其他變更。動詞”包含”的使用並不排除申請專利範 圍或說明中未提及之元件的存在。在元件或步驟前使用不 定冠詞”一”或”一個”並不排除複數個此類元件或步驟之存 在。該等圖式與說明應僅視為解說性而並不限制本發明主 旨。 【圖式簡單說明】 已參考附圖僅以範例方式藉由以上說明進一步說明此等 125644.doc •12- 200837733 2其他態樣、特徵及優點,附圖中相同參考數字指The recording of the eight ADIP frames compensates for possible errors such as eccentricity such that the jitter and BLER readout measurements occur during a disc rotation. The recording is performed from the outer edge of the record carrier to its inner edge. The starting power is derived from the power of Pwp of β OPC, as shown in Figure 5. The laser power will travel from pwp + 25% to Ρχνβ _ 25% at 15 power levels (30 ECC blocks). At each power level, the jitter and BLER are measured during a rotation and the average is calculated. "Correction Pointing Pre-Sense Correction. Figure 6 is a schematic illustration of a complete optimal power control procedure for a parametric disc as a function of disc radius. The program includes: i) β - OPC; ii) Jitter &BLER_OPC; m) Forward Sensing Correction; 乂 and IV) Write Check. Actually 'Introducing a beta correction to compensate for the laser: optical feedback. To find out what should be used Correction, the reading of the forward sensing peer is written to a blank area on the disc. Therefore, the actually determined optical (four) ECC blocks are written to the internal disc job area. For these 1.5 ECCI1 blocks Reading forward sensed values. Based on this value, a corrected beta value is calculated based on the measured drop. The delta difference between the corrected (four) value and the measured (iv) value 125644.doc 200837733 should be in a particular window (eg Within 1%), otherwise a retry is performed until the delta difference is within the allowable window. Figure 4 is a graph illustrating the use of the steps outlined above for a preferred TDK R8x DVD+R disc. An example of the result of this jitter, block error rate (vertical axis) pin These test power values (horizontal axes) are plotted. These squares indicate the measurement results. It should be clear to those skilled in the art that any function γ(χ) with a minimum value for X=Xm is small around this minimum. Within the range, Y(X)=c〇+c1(X-Xm)+c2(X.Xm)2 can be reasonably approximated by the quadratic function of the following equation, where C0, 4 and 4 are constants. The measurement is effective to find the best value for X ▲. It is done by the well-known least squares method, which is not required to be explained here. In any case, those skilled in the art should be aware that it can be based on Several measurements around the minimum of a function are used to calculate an optimal parabolic fit, and thus can be calculated and approximated. The curve shown in Figure 4 illustrates this parabolic fit. Using x (jitter/BLER) and For the correction data of Y (test power value), the coefficients Co, Mc2 can be calculated. After calculating the coefficients c, 〇1 and .2, the point 4 is calculated and the first recording power of the radiation beam is set to correspond to One of the minimum jitter values is the best value. On the same line, the second recording power of the radiation beam is set. The optimum value corresponding to the minimum block error rate (BLER) is determined. Further, as explained in the specific embodiment, the optimal recording power is determined by using the first recording power and the second recording power of the radiation beam. The decision of the minimum jitter or block error rate (BLER) is based on a polynomial response, and thus the best recording power of 125644.doc -10- 200837733 is accurate and reliable. (4) Determining the radiation beam rate and the second recording power of the radiation beam. ^力应思思, the BLER measurement should be compared with the jitter rate during a disc rotation. At the same time, the occurrence occurs to compensate for such things as centrifugation &gt; + move "BLER 〇 pc to reduce the overall Ο PC. In - Korea 66 SL · X people 1. ^ sentence can filter out random measurement noise and can also filter out the disk The disc deviation and the periodic disturbance of the turntable motor swing. In another specific real towel, the test data is recorded on the record carrier for each change of the test power value to have from the center of the record carrier to the One of the record carriers, the outer edge, the edge of the picking edge, and the concentric circle of the radius, the test negative material. Due to the change in the thickness of the material, the manufacturing change) "two (= dust, fingerprint, scratch, dye, _ text) Due to changes in clothing environment, dynamic power calibration is required to compensate for the good recording quality of Demo found in your records. This ensures that in another embodiment, across the entire record carrier, for each of the test power values - The change to record the test data on the == carrier includes a concentric circle recording test having a radius reduced from the center of the record carrier other than the record carrier = more ensuring good recording quality across the entire record carrier and complementing The media, such as the θ(4) move 111GG, may be adapted to perform a method for determining a good recording power for a person recorded on the record carrier i as disclosed in the specific embodiment. For this purpose, the control unit 24 is based on The material=° recorded power determining unit 24A is configured to determine the first-recording power of the soil, &amp; radiation beam. The control unit 24 further comprises a second recording power determining unit 24B, step 125644.doc 200837733, The system is configured to determine a second recording power of a radiation beam based on a block error rate (BLER). The control unit 24 further includes an optimal recording power determining unit configured to determine the radiation beam based on the radiation beam The optimum recording power of the radiation beam of the difference between the first recorded power and the radiant power of the radiation beam. One of the recorders 100 can perform optimal power calibration and, as such specific embodiments The disclosed method determines the optimum recording power of the radiation beam, thereby improving the overall recording performance of the recorder. Although the present invention has been described by using a specific embodiment of a DVD disc. However, the subject matter of the present invention is applicable to all types of record carriers, for example, one-person write media and multiple-write recordable types (Dvd-RW, DVD+RW, Blu-ray disc). It is not limited to one-sided and two-layer. Record carrier (ie double-layer record carrier) or double-sided record carrier (ie double-sided double-layer record carrier). Those skilled in the art can implement the decision to record data in software or in both hardware and software. The specific embodiments of the method for optimally recording the power of a radiation beam. Those skilled in the art to implement the claimed subject matter will be able to understand and practice other embodiments of the disclosed embodiments. The use of the verb "comprise" does not exclude the existence of a component that is not mentioned in the scope of the patent application or the description. The use of the indefinite article "a" or "an" The drawings and description are to be considered as illustrative only and not limiting. BRIEF DESCRIPTION OF THE DRAWINGS Other aspects, features, and advantages of the present invention are further described by way of example only with reference to the accompanying drawings.

或類似部分,且其中: J 圖1不意性解說一範例性驅動器; 圖2示意性解說針對一範例性TDK-R8X DVD+R碟片之 動與區塊錯誤率(BLER)繪製的雷射功率; ’、' 圖3顯示解說依據本發明主旨的決定一輻射束之最佳記 錄功率的方法之步驟的範例性流程圖; °Or a similar part, and wherein: Figure 1 is a schematic representation of an exemplary driver; Figure 2 is a schematic illustration of the laser power plotted against the motion and block error rate (BLER) of an exemplary TDK-R8X DVD+R disc. ',' Figure 3 shows an exemplary flow chart illustrating the steps of a method for determining the optimum recording power of a radiation beam in accordance with the teachings of the present invention;

圖4不意性解說依據本發明主旨的針對一範例性 R8X DVD+R碟片獲得之結果; 圍意性解說依據本發明主旨的-範例性功率校準範 圍之選擇;以及 广圖6不意性解說針對一範例性dvd+r/_r碟片的與碟片半 裣成函數關係的完整最佳功率控制程序。 7記錄載體(例如DVD)包含依—連續螺旋形式或多個同 :圓形式之至少一磁軌’其中可以一資料圖案之形式儲存 貧料。該記錄載體可以係一可儲存或記錄資訊之可記錄 ⑻或可重寫(RW)類型’例如DVD+RW、dvd rw、 DVD+R、BD_RE(單層與多層)。一般使用輻射束(例如雷射 光束)來記錄資訊。 圖1係顯示-範例性驅動器1〇〇之結構的方塊圖。一記錄 载體10係藉由一韓麵^ j 9 &amp; 士 得釉馬達12而恆疋角速度(CAV)控制或恆 定線速度(CLV)控制。 一光學拾取單元14藉由使用從—t射二極體發射之雷射 光(於一記錄功率值)在該記錄載體1〇上記錄資料。當欲記 125644.doc -13- 200837733 錄資料時,將欲進行記錄之資料供應至一編碼器單元18並 將藉由該編碼器單元1S編碼之資料供應至一雷射二極體驅 動單元16。該雷射二極體驅動單元16基於該編碼的資料產 生一驅動信號並將該驅動信號供應至該光學拾取單元〗4之 雷射二極體。此外,將來自一控制單元24之一控制信號供 應至該雷射二極體驅動單元16以便藉由該控制信號來決定 記錄策略與記錄功率。 另一方面,當讀取資料時,該光學拾取單元14之雷射二 ⑩極體發射一讀取功率(讀取功率〈記錄功率)之雷射光,並 收反射光所接收的反射光係轉換成一電信號而獲得 一碩取RF (radio frequency ;射頻)信號。該讀取尺?信號係 供應至一 RF信號處理單元2〇。 該RF信號處理單元20包含—等化器、一二進制化單元、 一鎖相迴路(PLL)單元,並二進制化該讀取RF信號,產生 。同步時脈及將此等信號供應至—解碼器單元22。該解碼 φ 1單元22基於此等供應的信號來解碼資料並作為讀取資料 輸出解碼的資料。 亦將來自該RF信號處理單元2〇之讀取RF信號供應至該 控制單元24用於評估讀取信號品質。該驅動器1〇〇還包括 電路(用於貝料項出),其用於藉由分別產生一循軌誤差 信號或一聚焦誤差信號與形成於該記錄載體1〇上之一擺動 信號來控制該聚焦伺服赤俯# h m , ^叫版次循轨伺服(例如,用於位址解調 變或用於控制旋轉之數目)。然而,㈣控縣構與傳统 驅動系統中的該些伺服控制結構相同,因此不詳細說明。 125644.doc -14- 200837733 當欲在該記錄載體1 〇上兮产铃二欠 執股上屺錄貝科時,將測試資料反復記 錄於該記錄載體10之-預定區域(即功率校準區域)中同時 改變該記錄功率。重播該測試資料並將該重播信號之品質 係最大化處的記錄功率選擇為最佳記錄功率。使用該最佳 、彔力率來„己錄資料(一般稱為最佳功率控制(OPC)之一程 序該控制早70 24藉由驅動該雷射二極體驅動單元16、 評估記錄的測試資料之品質並決定該最佳記錄功率來執行 該最佳功率控制(〇PC)程序。 S 2003/0053386中揭不的方法使用錯誤率來判斷基於 抖動的校準寫人功率是否異常。若使用該校準寫入功率,、 該錯誤率高於預定位準,則即使該抖動較小,該校準點仍 係異常的而不用於決定該最佳寫入功率。換言之,使用該 錯誤率來決定該抖動功率校準點的有效性。最佳寫入雷射 功率之此蚊導致—較佳的抖%HF記錄品質 '然而,一較 佳/較低抖動HF信號仍會具有一回讀問題,由於一極高的 區鬼錯誤率(BLER)所致,其可藉由該記錄载體4 is a non-intentional illustration of the results obtained for an exemplary R8X DVD+R disc in accordance with the teachings of the present invention; a deliberate interpretation of the selection of an exemplary power calibration range in accordance with the teachings of the present invention; and a broad view of FIG. A complete optimal power control program for an exemplary dvd+r/_r disc that is functionally related to the disc. 7 A record carrier (e.g., a DVD) comprises a continuous spiral form or a plurality of at least one magnetic track of the same circular shape, wherein the poor material can be stored in the form of a data pattern. The record carrier can be a recordable (8) or rewritable (RW) type that can store or record information such as DVD+RW, dvd rw, DVD+R, BD_RE (single layer and multi-layer). A beam of radiation, such as a laser beam, is typically used to record information. Figure 1 is a block diagram showing the structure of an exemplary driver. A record carrier 10 is controlled by a constant yaw rate (CAV) control or a constant linear velocity (CLV) by a glaze motor 12. An optical pickup unit 14 records data on the record carrier 1 by using laser light (at a recording power value) emitted from the -t diode. When the information is recorded, the data to be recorded is supplied to an encoder unit 18 and the data encoded by the encoder unit 1S is supplied to a laser diode driving unit 16. . The laser diode driving unit 16 generates a driving signal based on the encoded data and supplies the driving signal to the laser diode of the optical pickup unit. Further, a control signal from a control unit 24 is supplied to the laser diode driving unit 16 to determine the recording strategy and recording power by the control signal. On the other hand, when reading data, the laser diode 10 of the optical pickup unit 14 emits a laser beam of read power (reading power <recording power), and receives reflected light converted by the reflected light. An electrical signal is obtained to obtain a radio frequency (radio frequency) signal. The reading ruler? The signal system is supplied to an RF signal processing unit 2A. The RF signal processing unit 20 includes an equalizer, a binarization unit, a phase locked loop (PLL) unit, and binarizes the read RF signal to generate. The clock is synchronized and the signals are supplied to the decoder unit 22. The decoding φ 1 unit 22 decodes the data based on the signals supplied and outputs the decoded data as read data. A read RF signal from the RF signal processing unit 2 is also supplied to the control unit 24 for evaluating the read signal quality. The driver 1A further includes a circuit (for a billing item) for controlling the tracking signal or a focus error signal and a wobble signal formed on the record carrier 1 to generate the tracking signal Focus servo red tilt # hm , ^ is called version tracking servo (for example, for address demodulation or for controlling the number of rotations). However, (4) The control structure of the county is the same as that of the conventional drive system, and therefore will not be described in detail. 125644.doc -14- 200837733 When the record carrier 1 is to be recorded on the record carrier, the test data is repeatedly recorded in the predetermined area (ie, the power calibration area) of the record carrier 10. The recording power is also changed at the same time. The test data is replayed and the recording power at which the quality of the reproduced signal is maximized is selected as the optimum recording power. Use the best, the force rate to record the data (generally called one of the best power control (OPC) program. The control is early 70 24 by driving the laser diode drive unit 16, evaluating the recorded test data. The quality and determines the optimal recording power to perform the optimal power control (〇PC) procedure. The method disclosed in S 2003/0053386 uses the error rate to determine whether the jitter-based calibration write power is abnormal. Write power, which is higher than the predetermined level, even if the jitter is small, the calibration point is abnormal and is not used to determine the optimal write power. In other words, the error rate is used to determine the jitter power. The effectiveness of the calibration point. This mosquito with the best write laser power results in a better jitter %HF recording quality. However, a better/lower jitter HF signal will still have a readback problem due to a very high Due to the regional ghost error rate (BLER), which can be obtained by the record carrier

引起。 、又I 一般而言’最小抖動點對應於最小區塊錯誤率(BLER)。 但是’對於通常對記錄功率敏感的特定記錄載體(例如且 有二碟以數的碟片,如BLERb、意味著記錄 之^的區塊錯决率並表示記錄之前的預刻凹坑信號中的誤 差量’而Rb意味著記錄之前的溝槽反射率))’該最動 點可遠離最小BLEU。圖示針對該抖動與 料 革(BLER)繪製的雷射功率。垂直軸顯示該抖動與該则汉 125644.doc -15- 200837733 值而水平軸顯示該等雷射功率值。此處考量的記錄載體係 一較差的TDK-R8x DVD+R碟片。由圖2可清楚,最小抖動 不對應於最小BLER值。將對應於低抖動的雷射功率用於 記錄資料將導致記錄與重製問題。 【主要元件符號說明】cause. And I generally say that the minimum jitter point corresponds to the minimum block error rate (BLER). But 'for a particular record carrier that is usually sensitive to recording power (for example, and there are two discs, such as BLERb, meaning the block error rate of the record and indicates the pre-pit signal in the record before recording The amount of error 'and Rb means the groove reflectivity before recording)) 'The most moving point can be far from the minimum BLEU. The laser power plotted for this jitter and material (BLER) is shown. The vertical axis shows the jitter and the value of the horizontal axis shows the laser power values. The record carrier considered here is a poor TDK-R8x DVD+R disc. As can be seen from Figure 2, the minimum jitter does not correspond to the minimum BLER value. Using laser power corresponding to low jitter for recording data will result in recording and reproduction problems. [Main component symbol description]

10 記錄載體 12 轉軸馬達 14 光學拾取單元 16 雷射二極體驅動單元 18 編碼器單元 20 RF信號處理單元 22 解碼器單元 24 控制單元 24A 第一記錄功率決定單元 24B 第二記錄功率決定單元 24C 最佳記錄功率決定單元 100 驅動器 I25644.doc •16-10 Record carrier 12 Spindle motor 14 Optical pickup unit 16 Laser diode drive unit 18 Encoder unit 20 RF signal processing unit 22 Decoder unit 24 Control unit 24A First recording power decision unit 24B Second recording power decision unit 24C Good recording power decision unit 100 driver I25644.doc •16-

Claims (1)

200837733 申請專利範圍: 1· 一種決定用於在-記錄載體⑽上記錄f料的―轄射束 之一最佳記錄功率的方法(300),該方法(300)包含: 決定基於抖動的該輻射束之-第-記錄功率(302); 決定基於區塊錯誤率(bler)的該輻射束之—第二記 率(304);以及 ^決疋基於該輻射束之該第一記錄功率與該輻射束之誃 第二記錄功率之間之—差的該輻射束之該最佳記: (306) 〇 千 2·如請求項1之方法,其中決定基於該輕射束之該第-記 錄力率與該輻射束之該第二記錄功率之間之該差的該輕 射束之該最佳記錄功率包含·· 決定基於;k準段差的該輻射束之該最佳記錄功率。 3·如口月求項2之方法,其中基於用於在該記錄載體(⑺)上記 錄資料的該_束之該功率的解析度來決定該等校準段 差。 4 · 如睛求項2之方法,甘山 法其中決定基於該等校準段差的該輻 射束之該最佳記錄功率包含·· 、定°亥&amp;射束之該第一記錄功率與該輻射束之該第二 記=率之間之該差是否實w兩個㈣段差; 右:貝定處於該輕射束之該第—記錄功率的該區 塊錯誤率(bler)計數是否比處於該輕射束之該第二記錄功 率區塊錯誤率(BLER)計數大—預定的計數數目;以及 右疋則選擇該輻射束之該第二記錄功率作為該輻射 125644.doc 200837733 束之該最佳記錄功率。 5.如請求項4之方法,其進一步包含: 使用該輻射束之該決定的 體⑽上記錄資料。 ^錄功率來在該記錄載 6·如請求項1之方法,直由A &amp;廿 該第—記錄功率包含^ 、該抖動的該轄射束之 功ί允許測試功率值之—範圍内改變該輻射束之該記錄 針對該測試功率值之每—較來在 測試資料; )私版上尤錄 讀取該記錄的測試資料並測量該抖動; 2線擬合該等職功率值與對應的測量抖動值;以及 率。到该抖動實質上最小的該輻射束之該第一記錄功 7·如请求項6之方法,其中針對該測試功率值之每一變更 在該記錄載體上記錄該測試資料包含: 以具有從該記錄載體之中心至該記錄載體之一外部邊 緣增加之半徑的同心圓記錄該測試資料。 :求項1之方法,其中決定基於該區塊錯誤率^⑻的 该輻射束之該第二記錄功率包含: ^許測試功率值之圍内改變該輻射束之該記錄 功率; 針,該測試功率值之每—變更來在該記㈣體上記錄 測武資料; 125644.doc 200837733 區塊錯誤率(bier); 胃應的測量區塊錯誤 讀取該記錄的測試資料並測量該 曲線擬合該等測試功率值與該等 率(Mer)值;以及 找到該區塊錯誤率(b】er)實 '^ ►錄功率。 質上最小的該輻射束之該第 9.如請求項8之方法’其中針對該測試功率值之每一變更 在該記錄載體上記錄該測試資料包含·· 以具有從該記錄載體之該外部邊 ,^ ^ Γ 1瓊緣至该記錄載體之該 〜/小之半徑的同心圓記錄該測試資料。 10·如请求項1之方法,1中 八中同%决疋该輻射束之該第一記 錄功率與該輻射束之該第二記錄功率。 11·如句求項7或9之方法,其中針對該測試功率值之每一變 更在該記錄載體上記錄該測試資料包含: 在DVD上g己錄該測試資料。 12.如請求項6或8之方法,i 八T項取该C錄的測試資料包 含· 口貝取在一 DVD上記錄之該測試資料。 13· 一種驅動器(100),其包含: ::學拾取單元(14)’其係配置成用以產生一輻射束 並:該輕射束聚焦於一記錄載體⑽上; _ 1單元(24) ’其係g&amp;置成用以控制該光學拾取單 70,其中該控制單元進一步包含·· — &gt;己錄功率決定單元(24A),其係配置成用以決 疋基於抖動的該轄射束之-第-記錄功率; 125644.doc 200837733 —第二記錄功率決定單元(24B),其係配置成用以決定 基於區塊錯誤率(bler)的該輻射束之一第二記錄功率;以及 一最佳記錄功率決定單元(24C),其係配置成用以決定 ;“輕射束之該弟一 έ己錄功率與該輻射束之該第二記 錄功率之間之一差的該輻射束之該最佳記錄功率。 如明求項13之驅動器(1 〇〇),其中該最佳記錄功率決定單 疋(24C)係進一步配置成用以決定基於校準段差的該輻射 束之該最佳記錄功率。 15·如請求項14之驅動器(1〇〇),其中基於用於在該記錄載體 (10)上記錄資料的該輻射束之該解析度來決定該等校準 段差。 16. 如明求項14之驅動器(100),其中該最佳記錄功率決定單 元(24C)係進一步配置成用以: 決定該輻射束之該第一記錄功率與該輻射束之該第二 δ己錄功率之間之該差是否實質上大於兩個校準段差; 若是,則決定處於該輻射束之該第一記錄功率的該區 塊錯誤率(bier)計數是否比處於該輻射束之該第二記錄功 率的該區塊錯誤率(BLER)計數大一預定的計數數目;以及 若是,則選擇該輻射束之該第二記錄功率作為該輻射 束之該最佳記錄功率。 17. 如請求項13之驅動器(100),其中用以決定基於抖動的該 輻射束之該第一記錄功率的該第一記錄功率決定單元 (24A)係進一步配置成用以: 在允許測試功率值之一範圍内改變該輻射束之該記錄 125644.doc 200837733 功率; 针對該測試功率值之每 測試資料; t更來在該兄錄冑體上記錄 讀取該記錄的測試資料並測量該抖動; 以及 2線擬合該等測試功率值與該等對應的測量抖動值; 率找到該抖動實質上最小的該輻射束之該第一記錄功200837733 Patent Application Range: 1. A method (300) for determining an optimum recording power of a "beam" for recording a material on a record carrier (10), the method (300) comprising: determining the radiation based on jitter a beam-first-recording power (302); determining a second rate (304) of the radiation beam based on a block error rate (bler); and determining a first recording power based on the radiation beam and the The method of claim 1, wherein the first recording power of the light beam is based on the difference between the second recording power of the radiation beam: (306) The method of claim 1, wherein the first recording force based on the light beam is determined The optimum recording power of the light beam of the difference between the rate and the second recording power of the radiation beam comprises determining the optimum recording power of the radiation beam based on the k-segment difference. 3. The method of claim 2, wherein the calibration step is determined based on a resolution of the power of the bundle for recording data on the record carrier ((7)). 4) The method of claim 2, wherein the optimal recording power of the radiation beam based on the calibration step comprises: the first recording power and the radiation of the beam Whether the difference between the second = rate of the bundle is true w (four) step difference; right: whether the block error rate (bler) count of the first recording power of the light beam is higher than The second recording power block error rate (BLER) count of the light beam is large - a predetermined number of counts; and the right side selects the second recording power of the radiation beam as the best of the radiation 125644.doc 200837733 Record the power. 5. The method of claim 4, further comprising: recording the data on the determined body (10) of the radiation beam. ^ Recording power is recorded in the record. 6. The method of claim 1 is directly changed by A &amp; 第 the first recording power contains ^, the jitter of the ray of the ray allows the test power value to be changed within the range The record of the radiation beam is for each of the test power values - compared to the test data;) the private version of the test data is read and measured; and the line is fitted with the corresponding power values and corresponding Measure the jitter value; and rate. The first recorded work of the radiation beam to the jitter is substantially the same as the method of claim 6, wherein the recording of the test data on the record carrier for each change of the test power value comprises: The test data is recorded by concentric circles of the center of the record carrier to the increased radius of the outer edge of one of the record carriers. The method of claim 1, wherein the determining the second recording power of the radiation beam based on the block error rate ^(8) comprises: changing the recording power of the radiation beam within a test power value; Each of the power values—changes to record the test data on the record (IV); 125644.doc 200837733 Block error rate (bier); The test block of the stomach should read the test data of the record and measure the curve fit The test power value and the rate (Mer) value; and finding the block error rate (b) er). 9. The method of claim 8, wherein the method of claim 8 wherein the test data is recorded on the record carrier for each change of the test power value comprises: having the exterior from the record carrier The test data is recorded by the concentric circles of the radius of the ~/ Γ 1 to the record carrier. 10. The method of claim 1, wherein the first of the eight is equal to the first recording power of the radiation beam and the second recording power of the radiation beam. 11. The method of clause 7 or 9, wherein the recording of the test data on the record carrier for each change in the test power value comprises: recording the test data on a DVD. 12. The method of claim 6 or 8, wherein the test data of the C record is included in the test record of the C record, and the test data recorded on a DVD is taken. 13. A driver (100) comprising: a learning pick-up unit (14) configured to generate a radiation beam and focusing the light beam on a record carrier (10); _ 1 unit (24) 'The g& is configured to control the optical pickup unit 70, wherein the control unit further includes a recording power determining unit (24A) configured to determine the yaw based on the jitter a beam-first recording power; 125644.doc 200837733 - a second recording power decision unit (24B) configured to determine a second recording power of the one of the radiation beams based on a block error rate (bler); An optimum recording power decision unit (24C) configured to determine; "the beam of light of the difference between the recorded power of the light beam and the second recording power of the radiation beam" The optimum recording power, such as the driver (1 〇〇) of claim 13, wherein the optimum recording power decision unit (24C) is further configured to determine the optimum of the radiation beam based on the calibration step difference Record the power. 15. The driver of claim 14 ( 1)) wherein the calibration step is determined based on the resolution of the radiation beam used to record data on the record carrier (10). 16. The driver (100) of claim 14, wherein the Preferably, the recording power determining unit (24C) is further configured to: determine whether the difference between the first recording power of the radiation beam and the second delta recording power of the radiation beam is substantially greater than two calibration step differences And if so, determining whether the block error rate (bier) count at the first recording power of the radiation beam is greater than the block error rate (BLER) count at the second recording power of the radiation beam The number of counts; and if so, the second recording power of the radiation beam is selected as the optimum recording power of the radiation beam. 17. The driver (100) of claim 13, wherein the radiation is determined based on the jitter The first recording power determining unit (24A) of the first recording power of the bundle is further configured to: change the recording of the radiation beam within a range of allowable test power values 125644.doc 200837733 Each test data for the test power value; t further records the test data of the record on the brother record body and measures the jitter; and 2-line fitting the test power values corresponding to the Measuring the jitter value; finding the first recorded work of the radiation beam that is substantially minimized by the jitter 請求们3之驅動器_),其中用以決定基㈣塊錯誤 :的該輻射束之該第二記錄功率的該第二記錄功率 决定單元(24Β)係進一步配置成用以·· 在允許測4功率值之一範圍内改變該輕射束之該記錄 功率; 針對该測試功率值之每一變更來在該記錄載體上記錄 測試資料; 讀取該記錄的測試資料並測量該區塊錯誤率(Mer); 曲線擬合該等測試功率值與該等對應的測量區塊錯誤 率(bier)值;以及 找到該區塊錯誤率(bier)實質上最小的該輻射束之該第 —§己錄功率。 19·如請求項13之驅動器(100),其中該驅動器係一dvd驅動 器。 20· —種包含如請求項19之驅動器的記錄器。 21·如請求項20之記錄器,其中該記錄器係一 DVD記錄器。 125644.doc 200837733 22. —種電腦程式,其包含裎 一記錄載體上記錄資料的^構件用以執行決定用於在 一方法,該方法包含·· 射束之一最佳記錄功率的 一第一記錄功率; 該輕射束之一第二記錄功 決定基於抖動的該輻射束之 決定基於區塊錯誤率(bler)的 率;以及 決疋基於該輕射束之該第一 ^ ^ ^ °己錄功率與該輻射束之該The driver _) of the requester 3, wherein the second recording power determining unit (24Β) for determining the second recording power of the radiation beam of the base (four) block error is further configured to be used for Changing the recording power of the light beam within one of the power values; recording the test data on the record carrier for each change of the test power value; reading the recorded test data and measuring the block error rate ( Mer); curve fitting the test power values to the corresponding measurement block error rate (bier) values; and finding the radiation beam of the block having a substantially minimum error rate (bier) power. 19. The drive (100) of claim 13, wherein the drive is a dvd drive. 20. A recorder comprising a drive as claimed in claim 19. 21. The recorder of claim 20, wherein the recorder is a DVD recorder. 125644.doc 200837733 22. A computer program comprising: a component for recording data on a record carrier for performing a decision for use in a method comprising a first recording of an optimal recording power of a beam Recording power; a second recording power of the light beam determines a rate based on a block error rate (bler) based on the jitter of the radiation beam; and determining the first ^ ^ ^ ° based on the light beam Recording power and the radiation beam 第二記錄功率之間之一差的該輻射束之該最佳記錄功 率。The optimum recording power of the radiation beam, which is a difference between the second recording powers. 125644.doc125644.doc
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