TW504675B - Laser energy compensation method of CD-ROM drive - Google Patents
Laser energy compensation method of CD-ROM drive Download PDFInfo
- Publication number
- TW504675B TW504675B TW90106858A TW90106858A TW504675B TW 504675 B TW504675 B TW 504675B TW 90106858 A TW90106858 A TW 90106858A TW 90106858 A TW90106858 A TW 90106858A TW 504675 B TW504675 B TW 504675B
- Authority
- TW
- Taiwan
- Prior art keywords
- optical disc
- laser
- disc drive
- light source
- parameters
- Prior art date
Links
Landscapes
- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
Abstract
Description
五、發明説明( <發明領域> 本發明係有關於-種光碟機雷射能量之補償方法,尤 ----------装-- (讀先閱讀背面之注意事項再填頁) 指-種用於光碟機雷射光源能量調校及具最佳化的光源能 量補償控制的方法。 <發明背景及先前技藝> 按’光碟機廣泛使用於日常生活中之影音、視聽設備 及電腦資訊設備之中,以作為光碟片之影音播放資料及電 腦資料讀取之主要設備,然而厂在光碟機中用來讀取或寫 入= 貝料的元件,當為該用以發光的雷射元件,諸如習知的 可讀寫(CDR/W)光碟機,該雷射元件所發出的光源強弱將 決定光碟機進行資料讀或寫之品質,故有關於雷射元件的 發光參數及其光源能量的調校,相對之下,顯得格外的重 要0 線 經濟部智慧財產局員工消費合作社印製 然而’在習知光碟機的雷射元件發光的直接電力關係 值是以毫瓦(mw)來表示其值的大小,也就是用功率單位來 表不其輸出冗度或輸出參數’而整個雷射元件的發光參 數,則是以毫瓦/安培(MW/A)來表示其輸出對輸入的相對 關係,其值通常可視為一電壓值,在正常的狀態下,電射 光源能量(亮度),是恒與發光參數值的大小成正比的,也 就是在沒有任何擾動(RUN-OUT)的情況下,發光參數值愈 大,其所發出的雷射光源能量愈大。 但事實上,在光碟機中的電射元件在運作上,並非是 如上面所說的理想,如在第七圖中所示’即為習知的光碟 機雷射光源的能量分佈情形,由於雷射元件X與光碟機的 ______ 2 __ 本紙張尺度適用中國國家標準(CNS ) A视格(210x297公釐〉 A7 ^-----B7 五、發明説明() 鏡頭y間的組合關係,並非是毫無干_素之存在,例如: 鏡頭y的級裝偏移所造成的聚焦偏移之擾動問題,或者是 因為光碟機的主軸馬達及光碟片間組裝的後動因素,將直 接影響雷射元件x所發出的光源強度,而其中又以鏡頭γ 的偏移因素佔絕大多數,如在第六圖中則顯示反射點A1、 A2及A3所形成造的光源能量偏移之狀態,其中可看出反 射點A2的光源強度要較反射點A1及A3來得大,如以函 數幵乂釔來表示之,則發光參數Pw=f(p,offset),也就 是含鏡頭Y組裝偏移擾動因素的函數。 而第八圖更進一步地揭示該雷射光源受鏡頭γ組裝偏 移所造成的相對能量損失的曲線圖,其中,可明顯看出, 無論由鏡頭曲線ΡΗΟ、發光參數曲線RRF、光源回饋曲線 BHO及電力輪入曲線pLT各曲線中可明顯看出,該第六圖 中的反射點A2的能量損失為最小,而反射點A1及A3的 旎ϊ抽失為相對最大,易言之,即是反射點A2的光源能 里(焭度)為大,但並非表示其所輸入的發光參數pw為最 大,而在第九圖、第十圖、第十一圖及第十二圖中則分別 顯不光源回饋曲線BH0、電力輸入曲線PLT、發光參數曲 線RRF及雷射元件X的輸入電力FPDO的波形圖,可得到 相對的印證,也就是該反射點Al、A2及A3的光源能量 強度會觉到鏡頭γ的組裝偏移之擾動因素,造成電力參數 PW與光源能量關係產生擾動變化,而無法直接找出最佳 光源能量點的電力參數PW,造成光碟機在進行資料寫入 或讀取時的誤差或光源能量不足,造成資料寫入失敗或挑 ^i?TcNS)7^iTJ^^- J* m nn f --,*=I- I................... - ------ 11-------- III ml am I (請先閲讀背面之注意事項再填m頁) 訂 線 經濟部智慧財產局員工消費合作社印製 經濟部智慧財產局員工消費合作社印製 k發明説明( 片等問題。 此外,在習知光碟機業界, 則是在作祕切大量的人工來_=處理方法, 的檢測調校,不但耗費工時、人力太如乂 ’而以人工 產的經濟效益,對,㈣符產品生 人……, 之調校全憑專業人員之個 並不=相Γί每部光碟機的鏡頭〜裝偏移的情形 ^:“姻,根本無法使所有的產品皆能精確地調整 至f圭㈣総量輪出之狀態,、致產品岐之品質㈣ 不齊,嚴重影響光碟機產品的敎性及品質。 〈發明目的〉 月之主要目的即是在於提供_種光碟機雷射能量 之補侦方A T精確4出排除鏡頭組裝擾動因素的雷射光 源能量極大值及其相對的發光參數,使雷射元件於寫入或 讀取資料時,可發揮最佳的發光能量。 本發明之再一目的,即是在於提供一種光碟機雷射能 里之補你方法,可在於任何不同的鏡頭組裝偏移擾動因素 下,均能自動找出最佳的發光能量的發光參數,而適用於 所有的光碟機產品。 本發明之又一目的’即是在提供一種光碟機雷射能量 之補償方法,可自動及精確找出佳化的雷射發光能量之發 光參數’可大幅節省生產線上調校及測試之人力及成本。 以下為使貴審查委員對本發明之詳細技術内容及應用 狀態有進一步之目瞭解,以下茲列一個較佳之實施例,並 配合佐以各圖式作說明,其中: 請 先- I· 背 之 1意 事 項 再 填 m 頁 裝 訂 本紙張尺度適用中國國家榡準(CNS ) A4規格(210X297公釐) 67 04 5 % 經濟部智慧財產局員工消費合作社印製 A7 _......一_B7 ___五、發明説明() 圖式簡早說明: 第一圖為本發明的方法流程圖; 第二圖為本發明中的多種寫入之雷射光源之光源能量 及發光參數間之關係圖; 第三圖為本發明中進行底部曲線定位(bottom curve fit) 的初始取樣圖; 第四圖為本發明進行最小方塊定位處理的曲線圖; 第五圖為本發明底部曲定也(bottom curve fit)最終處 理結果的曲線圖; 第六圖為本發明方法之較佳應用例; 第七圖為習知的雷射元件與光碟機的鏡頭間的雷射光 源能量與發光參數之關係; 第八圖習知光碟機雷射元件因鏡頭組裝偏移擾動的各 項光源能量參數的曲線圖; 第九圖係習知的光碟機雷射元件之光源回饋曲線 BHO的波形圖; 第十圖係習知的光碟機雷射元件寫入曲線PLT的波形 圖; 第十一圖係習知的光碟機雷射元件發光參數曲線R R F 的波形圖; 第十二圖係習知的光碟機雷射元件輸入電力FPDO的 波形圖; 圖號說明: 一、創作部份 -----------裝— (請先閲讀背面之注意事項再填m頁)V. Description of the invention (< Invention field >) The present invention relates to a method for compensating the laser energy of an optical disc drive, especially ---------- install-(read the precautions on the back before filling (Page) Refers to a method for adjusting the laser light source energy of an optical disc drive and optimizing the compensation control of the light source energy. ≪ Background of the Invention and Previous Techniques > Press' Optical disc drive is widely used in daily life audio-visual, audio-visual Among the equipment and computer information equipment, it is used as the main equipment for reading and playing data on the disc and computer data. However, the components used by the factory to read or write = shell materials should be used to emit light. Laser components, such as the conventional readable / writable (CDR / W) optical disc drive, the intensity of the light source emitted by the laser element will determine the quality of the data read or write by the optical disc drive, so there are parameters about the light emission of the laser element The adjustment of the energy of the light source is relatively important. In contrast, it is printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs. However, the direct electric power value of the laser light emission of the conventional optical disc drive is in milliwatts ( mw) to represent its value The size, that is, the output redundancy or output parameter is expressed in terms of power units, and the luminous parameters of the entire laser element are expressed in milliwatts / amps (MW / A) as the relative relationship between the output and the input. The value is usually regarded as a voltage value. Under normal conditions, the energy (brightness) of the radioactive light source is constant and proportional to the value of the light emission parameter value, that is, the light is emitted without any disturbance (RUN-OUT). The larger the parameter value, the greater the energy of the laser light source it emits. But in fact, the operation of the electro-optical components in the optical disc drive is not as ideal as mentioned above, as shown in the seventh figure ' It is the energy distribution of the conventional laser light source of the optical disc drive. Since the laser element X and the optical disc drive are ______ 2 __ This paper size is applicable to the Chinese National Standard (CNS) A viewing grid (210x297 mm> A7 ^ --- --B7 V. Explanation of the invention () The combination relationship between the lens y is not completely non-existent, for example: the disturbance of the focus shift caused by the gradation shift of the lens y, or because of the optical disc drive Assembled between the spindle motor and the optical disc The back-moving factor will directly affect the intensity of the light source emitted by the laser element x, and the shift factor of the lens γ will account for the vast majority. As shown in the sixth figure, the reflection points A1, A2, and A3 are formed. The state of the energy source energy deviation of the light source, it can be seen that the light source intensity of the reflection point A2 is greater than the reflection points A1 and A3. If it is expressed by the function yttrium, the light emission parameter Pw = f (p, offset), It is also a function containing the disturbance factors of the lens Y assembly offset. And the eighth figure further reveals the graph of the relative energy loss of the laser light source caused by the lens γ assembly offset. Among them, it can be clearly seen that regardless of It can be clearly seen from the curves of the lens curve PΗ0, the luminous parameter curve RRF, the light source feedback curve BHO, and the power turn-in curve pLT that the energy loss at the reflection point A2 in the sixth figure is the smallest, and the reflection points A1 and A3 are 旎ϊ is relatively large, in other words, the light source energy (焭) of the reflection point A2 is large, but it does not mean that the input light parameter pw is the largest, and in the ninth, tenth, Figures 11 and 12 are divided The waveform of the light source feedback curve BH0, the power input curve PLT, the light emission parameter curve RRF, and the input power FPDO of the laser element X can be corroborated, that is, the energy intensity of the light source at the reflection points Al, A2 and A3 will be Perceived the perturbation factor of the assembly deviation of the lens γ, which caused the perturbation change of the power parameter PW and the energy of the light source, but could not directly find the power parameter PW of the optimal light source energy point, causing the optical disc drive to write or read data Time error or insufficient light source energy, causing data writing to fail or pick ^ i? TcNS) 7 ^ iTJ ^^-J * m nn f-, * = I- I ........... ........------- 11 -------- III ml am I (please read the precautions on the back before filling in page m) Cooperatives printed the Intellectual Property Bureau of the Ministry of Economic Affairs, the consumer co-operatives printed the invention description (films, etc.). In addition, in the conventional optical disc drive industry, a large number of manual methods are being used to detect and adjust, which not only consumes man-hours and manpower, but also uses the economic benefits of artificial production. Fu products are born…, the adjustment is entirely based on the professional not equal to the phase of the lens of each optical disc drive ~ installation situation ^: "Marriage, can not make all products can be accurately adjusted to The state of measuring the amount of rotation, the quality of the product is not uniform, which seriously affects the nature and quality of the optical disc drive product. 〈Objective of the invention〉 The main purpose of the month is to provide _ kinds of supplementary laser energy The detective AT accurately outputs the maximum energy value of the laser light source and its relative light emission parameters, which eliminates the lens assembly disturbance factors, so that the laser element can exert the best light emission energy when writing or reading data. One purpose is to provide a method for supplementing the laser energy of the optical disc drive, which can automatically find the best luminous parameters of the luminous energy under any different lens assembly offset disturbance factors, and it is applicable to all Another object of the present invention is to provide a method for compensating the laser energy of an optical disc drive, which can automatically and accurately find the optimized light emission parameters of the laser light emitting energy, which can greatly save the production line adjustment and Manpower and cost of testing. The following is to make your review members have a better understanding of the detailed technical content and application status of the present invention. Below is a preferred embodiment, which will be described with the accompanying drawings. Among them: Please first -I · Meaning of the first intention and refilling m pages. The paper size is applicable to China National Standard (CNS) A4 (210X297 mm) 67 04 5% Printed by A7 _... ... 一 _B7 ___ V. Description of the invention () Brief description of the drawings: The first diagram is a flowchart of the method of the invention; the second diagram is the light source energy and The relationship diagram between the luminous parameters; the third diagram is the initial sampling diagram of bottom curve fit in the present invention; the fourth diagram is the diagram of the minimum square positioning process of the present invention; The fifth figure is a graph of the final processing result of the bottom curve fit of the present invention; the sixth figure is a preferred application example of the method of the present invention; the seventh figure is between the conventional laser element and the lens of the optical disc drive The relationship between the energy of the laser light source and the luminous parameters; Figure 8 is a graph of the energy parameters of various light sources of the conventional optical disc drive laser components due to lens assembly offset; Figure 9 is the light source feedback of the conventional optical disc drive laser components The waveform diagram of curve BHO; the tenth diagram is a waveform diagram of the conventional optical disc drive laser writing curve PLT; the eleventh diagram is the waveform diagram of the conventional optical disc drive laser element emission parameter curve RRF; the twelfth diagram is The waveform diagram of the input power FPDO of the conventional optical disc drive laser component; Figure No. Explanation: 1. Creative part ----------- installation— (please read the precautions on the back before filling in page m)
1T 絲 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 504675 燃i A7 B7 五、發明説明()1T silk This paper size is applicable to Chinese National Standard (CNS) A4 specification (210X297 mm) 504675 Burn i A7 B7 V. Description of invention ()
10 發光參數控制器 20 雷射電力控制器 30 雷射元件 40 拾取元件 50 參數回饋元件 60 第一感測單元 70 第二感測單元 80 補償器 一 100 輸入多(η)種不同的發光參數PW —---------裝-- (請先閱讀背面之注意事項再填頁) 1005電力控制系統 110讀回相對於發光參數PWi〜PWn的回饋訊號Si〜Sn 120對回饋訊號S1〜Sn進行底部曲線定位(bottom curve fit) 初步取樣運算 130 最小化(least squares fit)運算 140重作步驟100〜130 150取得最終最佳的發光參數 160參數寫入光碟機之雷射電力控制系統 BHO 光源回饋曲線 BHO” 光源回饋數10 Luminous parameter controller 20 Laser power controller 30 Laser element 40 Pick-up element 50 Parameter feedback element 60 First sensing unit 70 Second sensing unit 80 Compensator 100 Input multiple (η) different light emitting parameters PW ----------- Installation-- (Please read the precautions on the back before filling in the page) 1005 Power control system 110 Read back the feedback signal Si ~ Sn 120 relative to the light emission parameter PWi ~ PWn 120 feedback signal S1 ~ Sn performs bottom curve fit initial sampling calculation 130 minimum squares fit calculation 140 repetition steps 100 to 130 150 to obtain the final best light emission parameters 160 parameters written to the laser power control system of the optical disc drive BHO light source feedback curve BHO "number of light source feedback
Fit 定位 PLT 電力輸入曲線 PLT” 電力輸入參數 PW 發光參數 PW!〜PWn發光參數 6 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 訂 經濟部智慧財產局員工消費合作社印製 5恭 没!: 經濟部智慧財產局員工消費合作社印製 Κ Α7 〜…——一J_^B7_ 五、發明説明() RRF(I) 發光函數 RRF5(I) 發光函數 RRF(a) 函數點 RRF’(a) 函數點 RRF(b) 函數點 RRF(c) 函數點 RRF’(c) 函數點 Si〜Sn 回饋訊號 V 誤差矩陣 V(I) 誤差函數 二、習知部份 A1〜A3 反射點 BHO 光源回饋曲線 F 發光參數 FPDO 輸入電力 PW 電力參數 PHO 鏡頭曲線 PLT 電力輸入曲線 RRF 發光參數曲線 X 雷射元件 Y 鏡頭 <發明之詳細說明〉 首先請參閱第一圖所示,為本發明方法的流程圖,其 7 ---------—裝-- (請先閲讀背面之注·^事項再填頁) 訂 線 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐)Fit Positioning PLT Power Input Curve PLT ”Power input parameters PW Luminous parameters PW! ~ PWn Luminous parameters 6 This paper size is applicable to China National Standard (CNS) A4 specifications (210X297 mm) Order printed by the Ministry of Economic Affairs Intellectual Property Bureau employee consumer cooperatives 5 Congratulations !: Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs Κ Α7 ~ ...—— 一 J_ ^ B7_ V. Description of the invention () RRF (I) Luminescence function RRF5 (I) Luminescence function RRF (a) Function point RRF ' (a) Function point RRF (b) Function point RRF (c) Function point RRF '(c) Function point Si ~ Sn Feedback signal V Error matrix V (I) Error function II. Known part A1 ~ A3 Reflection point BHO light source feedback curve F light emission parameter FPDO input power PW power parameter PHO lens curve PLT power input curve RRF light emission parameter curve X laser element Y lens < detailed description of the invention> Please refer to the first figure for the method of the invention 7 ----------- installation-(please read the notes on the back, ^ matters, and then fill in the pages) Alignment This paper size is applicable to China National Standard (CNS) A4 specification (210X297) %)
中’該步驟包含有: (100)輸人多⑷種不同的發光參數PW,即在光碟機的資料 寫入模式TM PWl〜PWn(如第二圖所示)等多個不同的發 光參t輪人雷射元件使之對光碟片作資料寫人之動作,· (11〇):回相對於發光參數pw!〜pwn的回饋訊號Sl〜 sn(如第一圖所不),在光碟機的讀取模式下,讀回發射的 光源訊號; (12〇)對回饋訊號Sl〜Sn進行底郜曲線定位(bottom curve fit)初步取樣運算,即對回饋訊號S1〜&所構成的曲線進行 曲線定位運算的取樣動作; (130)最小化(least squares _運算,將上述步驟12〇所運算 而得的值進行最小化運算,取得新的發光參數; (140)重作步驟ι〇〇〜13〇 ; (150)取得最終最佳的發光參數; (160)參數寫入光碟機之雷射電力控制系統。 經 濟 部 智 慧 財 產 局 員 X 消 費 合 社 印 製 請再配合第三圖,以下為了再闡明第一圖所示方法的 各步驟詳細運算内容,茲再配合以圖式來作進一步的說 明,其中,在第三圖所示者,是該第一圖所示的發光參數 PWi-PWn相對的回饋訊號Sl〜Sn,所構成的曲線圖,進 行底部曲線定位(bottom curve fit)初步取樣運算,首先,則 給予此曲線定義一個函數為發光函數RRF(I),1=1〜n,此 時則遵循取樣規則為: <1>當RRF(I)SRRF(I+1)時,即兩點間斜率為正(上昇)時, 則使RRF,(I+1)=RRF(I),即強迫下一個點為原來的點 8 本紙張尺度適用中國國家標隼(CNS ) A4規格(210X297公釐) 504675 經濟部智慧財產局員工消費合作社印製 A7 ____:___B7_五、發明説明() 之直: <2>當RRFi i) > RRF(卜[)3等·則舌.點間钭孟為負(下降丨時, 則:吏RRFVi+h=RRF( 1+丨)·也就是令該下一洇點的值 不變·保持其原來的it, 如在第三S中則擧制函數點RRF(a)、RRF(b)、RRF(c)三 點, · [<a,b*c<n,知a,b,c三個笪在i與η間,其中, 函數點RRF(a)之前的钭孟為負(下降),各函數點保持原 渣,而函數點RRF(a)到函數點RRF(b)間之钭至為正(上昇) 之狀態·故各函數點的{£則被強迫保持在RRF(a),形成新 的函數點RRF’(、a·):而函數點RRF(b)至函數點RRF(:c)間之 钭系為負ί下降),此時其間的各函數點值均維持其原值不 變,而在函數點RRF(c)以後的斜率則為正值(:上昇),故強 迫其值為RRF(c),即形成新的函數點RFF(c)。 請再參閉第西圖所示,在經過第三圖所示的底部面線 定位運算後,得到新的曲線,吾人給予定義新的發光函數 為RFF(:I),1=1〜η,並再對此發光函歎RFF’(I)進行最,!、 化的運算處理,其運算階數並不限制,在本發明t是列舉 以五階的運算為其實施例,則其算方程式則如下所列: RRF'(I)則可作五階展開成(A)式: RRF^AOfAirV Α3Γ3丁 A4f+Vi.............···.......*··,(Α) 9 (請先閱讀背面之注意事項再填, 頁 *裝- 、1Τ 線 本紙張尺度適用中國國家標準(CNS ) A4規格( 210X 297公釐) 5 67 04 5 A7 B7 五、發明説明( 其口,誤差函數ν(ί)為定垃irtt)的誤差,再將此RFF’(:I)以 矩;^來表示之·扣化成(B)式: RRF.This step includes: (100) Entering a plurality of different light-emitting parameters PW, that is, a plurality of different light-emitting parameters such as the data writing mode TM PW1 to PWn (as shown in the second figure) of the optical disc drive. The wheel laser device makes the data write action on the disc, (11〇): the feedback signal Sl ~ sn (as shown in the first picture) relative to the light emitting parameters pw! ~ Pwn, In the reading mode, read back the emitted light source signal; (12) Perform a preliminary sampling calculation of the bottom curve fit on the feedback signals Sl ~ Sn, that is, the curve formed by the feedback signals S1 ~ & Sampling action of curve positioning operation; (130) Minimize (least squares _ operation, minimize the value obtained by the operation calculated in the above step 120) to obtain a new light-emitting parameter; (140) Repeat step ι〇〇 ~ 13〇; (150) Get the final best luminous parameters; (160) The parameters are written into the laser power control system of the optical disc drive. Member of the Intellectual Property Bureau of the Ministry of Economic Affairs X Consumer Co., Ltd. Please cooperate with the third picture. Clarify the detailed operation of each step of the method shown in the first figure Let ’s further cooperate with diagrams for further explanation. Among them, the one shown in the third figure is a graph of the feedback signals Sl ~ Sn relative to the light-emitting parameters PWi-PWn shown in the first figure. To perform the bottom curve fit (bottom curve fit) preliminary sampling operation, first, a function is given to this curve to define the light-emitting function RRF (I), 1 = 1 ~ n. At this time, the sampling rule is followed: < 1 > When RRF (I) SRRF (I + 1), that is, when the slope between two points is positive (rise), then make RRF, (I + 1) = RRF (I), that is, forcing the next point to be the original point 8 Paper size is applicable to China National Standard (CNS) A4 specification (210X297 mm) 504675 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs A7 ____: ___ B7_ V. Description of the invention (): < 2 > When RRFi i) > RRF (Bu [) 3, etc., then the tongue. When the point between points is negative (falling, then: RRFVi + h = RRF (1+ 丨) · That is, the value of the next point is unchanged. · Keep its original it, as in the third S, the three function points RRF (a), RRF (b), and RRF (c), [< a, b * c < n, know a, b, c three 笪 between i and η, In the above, 钭 Meng before the function point RRF (a) is negative (falling), each function point remains the original slag, and the state between the function point RRF (a) and the function point RRF (b) is positive (rising). · So {£ at each function point is forced to stay at RRF (a), forming a new function point RRF '(, a ·): and the relationship between the function point RRF (b) and the function point RRF (: c) The value of each function point during this time remains the same, and the slope after the function point RRF (c) is positive (: rise), so it is forced to be RRF (c ), Forming a new function point RFF (c). Please refer to the second graph shown in the figure. After the bottom face line positioning operation shown in the third graph, a new curve is obtained. We give a new definition of the luminous function as RFF (: I), 1 = 1 ~ η, Then, the luminous function sigh RFF '(I) is performed most, and the calculation order is not limited. In the present invention t is a fifth-order operation as an example, the calculation equation is Then it is listed as follows: RRF '(I) can be expanded to the fifth order as (A): RRF ^ AOfAirV Α3Γ3 丁 A4f + Vi ................... ... * · ,, (Α) 9 (Please read the precautions on the back before filling in, page * installed-, 1Τ thread The paper size applies the Chinese National Standard (CNS) A4 specification (210X 297 mm) 5 67 04 5 A7 B7 V. Explanation of the invention (the error function ν (ί) is the error of the fixed irtt), and then this RFF '(: I) is expressed in terms of moments; ^ is deducted into (B) formula: RRF .
Γ 1 1 1 1 1 | 1 1/2 1/4 1/8 1/16 ! | 1 1/3 1/9 υη ι/si I 1/a1 l/n: i/n,^ Ι/ά4 AO Al A2 Λ3 A4Γ 1 1 1 1 1 | 1 1/2 1/4 1/8 1/16! | 1 1/3 1/9 υη ι / si I 1 / a1 l / n: i / n, ^ Ι / ά4 AO Al A2 Λ3 A4
VIVI
Va •(B) (請先閱讀背面之注意事項再填HI頁) 装. 經濟部智慧財產局員工消費合作社印製 再將矩瘴弍簡化得到(c)弍如下: RRF=HA+V··.................(c) 再將上述(:c)式申的誤差矩陣v予以作最小化處理,而得 到(D)式為: Q(COST FUNCTION )=1/2 VTV=1/2(RJRF-HA)T(RRJF-HA).........(D) 將上列強(D)式對A作偏徵分處理到(E)式,得到誤差矩障 V小化處理的值為0,代回(C)式中,並再作如(F)式所示 的化簡處理: Ρ Θ l/2(RRF:HA)T(RRF-HA)=(RRF:HA)r(-H)=0· •(E) 絲Va • (B) (Please read the notes on the back before filling in the HI page) Pack. Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs, and then simplify the moment (c): as follows: RRF = HA + V ·· ....... (c) Minimize the error matrix v applied by the above (: c) formula, and get the formula (D): Q (COST FUNCTION) = 1/2 VTV = 1/2 (RJRF-HA) T (RRJF-HA) ......... (D) Use the above strong (D) formula to bias A to ( E), the value of the minimization of the error moment barrier V is 0, and it is replaced in the formula (C), and then simplified as shown in the formula (F): ρ Θ l / 2 (RRF: HA) T (RRF-HA) = (RRF: HA) r (-H) = 0 · (E) Silk
P A HTRRF=HTBLA..............(F) ίο 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 504675 經濟部智慧財產局員工消費合作社印製 ..丨 A7 : _B7______ 五、發明説明() 而得·到最終的i G)式: Α ·=[1-ΗΤ广HTRRF:·····......(G) 該(.G )弍中顯示了底部曲線定位處理所得到相關於發光函 數RRF([)的矩H敦A、故吾人可將其最後的關係弍定 出為(Η)弍: · RRF(I>=HA,..................(H) 而重覆以工第一圖〜弟四圖的运鼻步隸,即第'一圖所示的 步骤100〜130 ’ gp可得到再經第二次底部西線定位運算所 得的新的發光參數RRF” ’其值經過二次的底部曲線定位 運异後’已完全消除光碟機鏡片組裝偏差所成的擾動因 素,為一最佳化的發光參數值,可使光碟機的雪射元件輸 出最大的光源能量3 請再參閱第五圖所示,同理可得,将上述第八圖所示 的光源回讀垚線BHO及電力輸入西線PLT經過本發明上 述的方法運算,¾理後·即可得到已消除光碟機之鏡頭組裝 偏差所造成之擾動因素之光源S饋數BHO”及電力輸入參 數PLT”,而這些運算方法、方程式及矩陣皆可用計算機 程式來代之,且可寫入光碟機的雷射發光之電力控制系統 100的相關控制元件中*其詳細的應用情形在以下將有深 入及進一步的說明,而該計算機程式或軟體益非為本發明 _ a___ 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閱讀背面之注意事項再填 頁) •裝. 訂 線· 504675 A7 B7 五、發明説明() 所欲主張的範缚及標的’故不予詳列及說明。 請再配合第六圖所示’是本發明的方法,在實際應用 於光碟機的雷射發光之電力控制系統100,之情形,其中, 該電力控制系統則包含一發光參數控制器(reference optical process controller,簡稱 R.〇.p.C)1〇、雷射電力控 制器20、雷射元件30、拾取元件40、參數回饋元件5〇、 第一感測單元60及第二感測單元70,其中雷射元件3〇為 為雷射二極體所構成,受雷射電力控制器20的控制而產生 光源能量(發光);拾取元件40及參數回饋元件50皆為光 二極體所構成,可用來感測雷射元件30所發出的雷射光束 反射的訊號,並分別送入第一感測單元60及第二感測單元 70中作感測訊號之處理,而該發光數控制器1〇則主要藉 由其輸出的發光參數來與第一感測單元60所反饋的訊號 作負回授運算,再將其運算結果送上述的雷射電力控制5| 20,以作為雷射元件30發光的控制依據。 而經第二圖〜第五圖本發明方法所列的運算方程式、 矩陣及運算方式,是可以用計算機程式或軟體方式寫入一 經濟部智慧財產局員工消費合作社印製 補償器80中,其輸出端與第二感測單元70所輪出的回饋 訊號運算後送入該發光參數控制器1〇中,而經補償器8〇 的運算結果,可得到得已消除光碟機鏡頭組裝偏差造成之 擾動因素的最佳化發光參數RRF”、光源回饋數Bii〇 ”及電 力輸入參數PLT”等參數資料,提供給整個電力控制系統 1 〇〇 ’作為雷射元件30輸出光源能量的最佳化控制依據, 並儲存於該電力控制系統1〇〇,的記憶體中(圖未顯示),而 ___ 12 本紙張適用中^^標準(CNs ) A4規格(210X297公釐) ㈣一' 6'ΓΧ 5 5 71 81‘ I ί τ!PA HTRRF = HTBLA .............. (F) ίο This paper size applies to Chinese National Standard (CNS) A4 (210X297 mm) 504675 Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs .. 丨 A7: _B7______ 5. Description of the invention () and get the final i G) Formula: Α · = [1-ΗΤ 广 HTRRF: ···· ............ (G) 该 (. G) 弍 shows the moment H and A related to the luminous function RRF ([) obtained from the bottom curve positioning process, so we can determine its final relationship as (Η) 弍: RRF (I > = HA ............ (H) Repeat the first step of the first picture ~ the fourth step of the nose step, that is, step 100 shown in the first picture ~ 130 'gp can obtain the new luminescence parameter RRF obtained by the second bottom west line positioning operation "' its value after the second bottom curve positioning and different operation 'has completely eliminated the disturbance caused by the disc assembly lens assembly deviation The factor is an optimized luminous parameter value, which can make the snow light emitting element of the optical disc drive output the maximum light source energy. 3 Please refer to the fifth figure again. It can be obtained by the same reason. Reading line BHO and power input After the western line PLT is calculated by the above method of the present invention, after processing, the light source S feed number BHO ”and the power input parameter PLT” that have eliminated the disturbance factors caused by the lens assembly deviation of the optical disc drive, and these calculation methods, Both the equations and the matrix can be replaced by computer programs, and can be written into the relevant control elements of the laser light-emitting power control system 100 of the optical disc drive. * The detailed application situation will be described in depth and further below, and the computer The program or software is not the invention_ a___ This paper size applies the Chinese National Standard (CNS) A4 specification (210X297 mm) (Please read the precautions on the back before filling in the page) • Binding. 504675 A7 B7 V. Explanation of the invention () The desired binding and the subject matter “are not listed and explained in detail. Please cooperate with the sixth figure” is the method of the present invention, which is actually applied to the power control system of laser light emission of optical disc players. 100, where the power control system includes a reference optical process controller (R.〇.pC) 1〇, laser power control 20. Laser element 30, pickup element 40, parameter feedback element 50, first sensing unit 60 and second sensing unit 70, where laser element 30 is formed by a laser diode and is subject to laser Light source energy (light emission) is generated by the control of the power controller 20; the pickup element 40 and the parameter feedback element 50 are both composed of light diodes, and can be used to sense signals reflected by the laser beam emitted by the laser element 30, and respectively Sent to the first sensing unit 60 and the second sensing unit 70 for processing of the sensing signal, and the luminous number controller 10 mainly feedbacks with the first sensing unit 60 through the output light parameter The negative signal is used for negative feedback calculation, and then the calculation result is sent to the above laser power control 5 | 20 as the basis for controlling the light emission of the laser element 30. The calculation equations, matrices, and calculation methods listed in the method of the present invention through the second to fifth figures can be written into a compensator 80 printed by a consumer cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs using a computer program or software. The feedback signal output from the output terminal and the second sensing unit 70 is calculated and sent to the light-emitting parameter controller 10, and the calculation result of the compensator 80 can be obtained to eliminate the disc assembly lens assembly deviation. The parameter data such as the optimized luminous parameter RRF ”, the light source feedback number Bii〇”, and the power input parameter PLT ”are provided to the entire power control system 100 ′ as the optimized control of the output light source energy of the laser element 30 Basis, and stored in the memory of the power control system 100, (not shown), and ___ 12 This paper is applicable ^^ Standards (CNs) A4 specifications (210X297 mm) '一' 6'Γχ 5 5 71 81 'I ί τ!
JJ
經濟部智慧財產局員工消費合作社印製 五、發明説明() ,光碟機不論是在何種鏡頭組裝偏移所造成的擾動因素 自動使該雷射元件3G獲得最佳化的輸出光源能量 =輸出控制,可大幅降低光碟機在調校及測試的人力 及成本。 舉的應用例,並不以其所揭露 =電力控制系統為限,舉凡是所有如可讀寫光碟機内 、雷射兀件之電力控制系統,皆可使用此種方法及補償控 制模式為之,而可使所有的光碟機中的雷射元件不需以大 量的人力來調校或测試,誠為一極具產業利用價值之發明。 本發明之發明精神,係在於以最為精簡有效及不完全 不以人工調校及測試方式,來對該光碟機中的雷射元件之 輸出光源能量作演除擾動因素的最佳化補償控制,使光碟 機之雷射元件無論在於寫入或讀取的模式下均提供穩定及 最佳的光源輸出。 〜 上述第-圖〜第六圖所示本發明光碟機之雷射能量之 補償方法,其中所揭示之袓關說明及圖式,係為便於闡 本發明之技術内容及技術手段’所揭示較佳實施例之 隅,並不因而拘限其範疇。並且,舉凡一切針對本發明 結構細部修飾、變更,或者是元件之等效替代、置換, 不脫離本發明之發明精神及範疇,其範圍將由以下之申 專利範圍來界定之。 明 之 當 請 13 本紙張尺度適用中國國家榡準(CNS ) A4規格(21〇χ297公釐)Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs. 5. Description of the invention (), no matter what kind of lens assembly the optical disc drive is caused by the disturbance factors, the laser element 3G automatically obtains the optimal output light source energy = output Control can greatly reduce the manpower and cost of the optical disc drive in the adjustment and testing. The application example is not limited to its disclosure = power control system. For example, all power control systems such as readable and writable optical disc drives and laser components can use this method and compensation control mode. And it can make all the laser components in the optical disc drive do not need to be adjusted or tested with a lot of manpower, which is an invention with great industrial utilization value. The inventive spirit of the present invention is to optimize and control the disturbance of the output light source energy of the laser element in the optical disc drive by using the most streamlined and effective and not completely manual adjustment and test methods. The laser component of the optical disc drive can provide a stable and optimal light source output in either a write or read mode. ~ The above figure-Figure ~ Figure 6 above shows the method for compensating the laser energy of the optical disc player of the present invention. The disclosed key descriptions and drawings are for the convenience of explaining the technical content and technical means of the present invention. The scope of the preferred embodiment is not limited thereby. In addition, all modifications or changes to the structural details of the present invention, or equivalent substitutions and replacements of the elements, without departing from the spirit and scope of the present invention, will be defined by the scope of the following patent applications. Please use 13 paper sizes to comply with China National Standards (CNS) A4 (21 × 297 mm)
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW90106858A TW504675B (en) | 2001-03-23 | 2001-03-23 | Laser energy compensation method of CD-ROM drive |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW90106858A TW504675B (en) | 2001-03-23 | 2001-03-23 | Laser energy compensation method of CD-ROM drive |
Publications (1)
Publication Number | Publication Date |
---|---|
TW504675B true TW504675B (en) | 2002-10-01 |
Family
ID=27607834
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW90106858A TW504675B (en) | 2001-03-23 | 2001-03-23 | Laser energy compensation method of CD-ROM drive |
Country Status (1)
Country | Link |
---|---|
TW (1) | TW504675B (en) |
-
2001
- 2001-03-23 TW TW90106858A patent/TW504675B/en not_active IP Right Cessation
Similar Documents
Publication | Publication Date | Title |
---|---|---|
TWI230377B (en) | Optical recorder and laser power control method | |
TW550555B (en) | Automatic control method for generating stable laser power (ACSP) of a compact disk drive | |
CN101460986B (en) | Video display device, video display method | |
TW446937B (en) | Optical recording medium | |
TW476174B (en) | Semiconductor laser control circuit and laser light source | |
CN100401396C (en) | Optical head, optical reproduction apparatus and optical record and reproduction apparatus | |
TW504675B (en) | Laser energy compensation method of CD-ROM drive | |
TW200632897A (en) | Methods and apparatus to compensate for power output variations over time | |
TW201029007A (en) | Laser control method and laser control circuit | |
CN102388600A (en) | Method, apparatus and system for providing a color device characterization with a quality evaluation | |
TW470945B (en) | Automatic output power calibration method of the pickup head of optical storage medium | |
US8218415B2 (en) | Laser power control system and method used in optical disc writer | |
JP3165216B2 (en) | Mark edge recording method and apparatus | |
CN102708878A (en) | Method for deriving precise control over laser power of an optical pickup unit, and associated automatic power calibration circuit | |
CN102566095B (en) | Method and system for measuring gamma curves of liquid crystal spatial light modulator | |
TW513692B (en) | Calibration method of the returned light noise from the light source of optical disk driver | |
TWI352989B (en) | System and method for calibrating light emitting d | |
CN100362580C (en) | Optical head device, optical recording device, and optical recording method | |
CN1194345C (en) | Laser output power control method for optical disc drive, optical disc drive and computer system | |
US20030012102A1 (en) | Method for compensating laser energy of optical disk drive | |
TWI289844B (en) | Power control method for eliminating output power offset of a pick-up head in an optical disk drive | |
CN101083094A (en) | Optical disc apparatus and recording power control method | |
TW200938972A (en) | Device and method for providing dynamic light standard | |
CN1534639A (en) | Laser power monitoring equipment, optical recording and/or reproducing device containing said equipment | |
TWI352990B (en) | Automatically calibtating method of output power o |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
GD4A | Issue of patent certificate for granted invention patent | ||
MM4A | Annulment or lapse of patent due to non-payment of fees |