TWI220986B - Method and apparatus for initializing multi-layered recording layer type optical recording medium - Google Patents

Method and apparatus for initializing multi-layered recording layer type optical recording medium Download PDF

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Publication number
TWI220986B
TWI220986B TW091123318A TW91123318A TWI220986B TW I220986 B TWI220986 B TW I220986B TW 091123318 A TW091123318 A TW 091123318A TW 91123318 A TW91123318 A TW 91123318A TW I220986 B TWI220986 B TW I220986B
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Taiwan
Prior art keywords
layer
initialization
layers
recording
recording medium
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TW091123318A
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Chinese (zh)
Inventor
Tsuyoshi Komaki
Tetsuro Mizushima
Jiro Yoshinari
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Tdk Corp
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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
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/26Apparatus or processes specially adapted for the manufacture of record carriers
    • 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
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/2403Layers; Shape, structure or physical properties thereof
    • G11B7/24035Recording layers
    • G11B7/24038Multiple laminated recording layers
    • 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
    • G11B7/24Record carriers characterised by shape, structure or physical properties, or by the selection of the material
    • G11B7/26Apparatus or processes specially adapted for the manufacture of record carriers
    • G11B7/268Post-production operations, e.g. initialising phase-change recording layers, checking for defects
    • 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
    • G11B2007/0003Recording, reproducing or erasing systems characterised by the structure or type of the carrier
    • G11B2007/0009Recording, reproducing or erasing systems characterised by the structure or type of the carrier for carriers having data stored in three dimensions, e.g. volume storage
    • G11B2007/0013Recording, reproducing or erasing systems characterised by the structure or type of the carrier for carriers having data stored in three dimensions, e.g. volume storage for carriers having multiple discrete layers

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Optical Recording Or Reproduction (AREA)
  • Manufacturing Optical Record Carriers (AREA)
  • Optical Record Carriers And Manufacture Thereof (AREA)

Abstract

A method for initializing a multi-layered recording layer type optical recording medium including a plurality of layers (L1, L0); each containing a recording layer to be initialized by irradiation of light, which layers are stacked in this order on one side of a substrate via a spacer layer (12) formed between the layers (L1, L0). Initialization of one layer (L0) among the plurality of layers (L0, L1) is performed by applying light from the layer (L0) side by using an object lens (31) having numerical aperture NA which satisfies an equation [TH*NA >= 9] wherein TH (mum) is thickness of a spacer layer (12) adjacent to the surface of the substrate (2) side in the layer (L0). Thus, it is possible to uniformly initialize the layers (L1, L0) containing the recording layers.

Description

1220986 __案號91123318___^ 月 日修正 , 五、發明說明(1) " 發明所屬之技術領域: 本發明是有關於一種具有形成於基板之一表面上分別 包括記錄層之複數層、與形成於上述複數層間之間隔層之 多層記錄層光記錄媒體之初始化方法、及初始化裝置。 先前技術: 光記錄媒體以高密度、大容量等優點受到注目,目前 已應,於各式各樣的用途。特別是可將所記錄之資訊抹除 及進行再記錄之重複讀寫式光記錄媒體,因其可進行資料1220986 __Case No. 91123318 ___ ^ Amendment on the day of the month, V. Description of the invention (1) " Technical field to which the invention belongs: The invention relates to a method of forming a plurality of layers including a recording layer formed on one surface of a substrate, and forming An initializing method and an initializing device for a multilayer recording layer optical recording medium with a spacer layer between the plurality of layers. Prior art: Optical recording media have attracted attention due to their advantages such as high density and large capacity, and they have been applied to a variety of applications. In particular, a rewriteable optical recording medium that can erase recorded information and perform re-recording, because it can carry out data

的修復及更新,且可重複進行重複讀寫,故於光記錄媒體 之廣L乏用途的應用上尤其受到重視。此種光記錄媒體中磁 光式Z錄媒體(M0 )與相變化型光記錄媒體等均已被開發及 商品化。 其、中,利用相變化進行可重複讀寫之相變化型光記錄 媒體(以下均以「光記錄媒體」表示)中,目前發明人已開 ^有^層貧積結構之光記錄媒體1,如第5圖所示。光記錄媒 η ίϊ:之一表面(圖中之上方表面)起依序形成反射 層3、s己錄層4、與作為透光層之覆蓋層5等所堆積構成。It can be repaired and updated, and can be read and written repeatedly, so it is particularly valued for the wide application of optical recording media. Among such optical recording media, magneto-optical Z recording media (M0) and phase change optical recording media have been developed and commercialized. Among them, in the phase-change type optical recording medium (hereinafter referred to as "optical recording medium") that can be repeatedly read and written by using phase change, the present inventors have developed an optical recording medium with a ^ layer poor structure. As shown in Figure 5. Optical recording medium η: One surface (upper surface in the figure) is formed by stacking a reflective layer 3, a recording layer 4, and a cover layer 5 as a light transmitting layer in order.

基板2之材質係利用聚碳酸酯等之樹脂材料,以射出成形 作出所欲厚度的平板形狀(例如為圓盤狀)。於基板2之^ 面(圖中之上方表面)上形成循執伺服用之凹槽等的細微凹 凸(未繪示)。反射層3例如利用A1、Ag4Ni等金屬,形成 於基板2之具有細微凹凸之表面上。記錄層4包括第一 ^呆蠖 層4a、相變化材料層4b與第二保護層4c,上述各層虹The material of the substrate 2 is a flat plate shape (for example, a disc shape) having a desired thickness by injection molding using a resin material such as polycarbonate. On the ^ surface (upper surface in the figure) of the substrate 2 are formed minute recesses (not shown) such as grooves for non-compliant servo. The reflective layer 3 is formed on the surface of the substrate 2 with fine unevenness using a metal such as A1 or Ag4Ni. The recording layer 4 includes a first dummy layer 4a, a phase-change material layer 4b, and a second protective layer 4c.

2186-5255-PFl(N).ptc2186-5255-PFl (N) .ptc

1220986 修正 號 9112^1« 五、發明說明(2) 4b、4a係依此順序形成於反射層3上。其中第一保護層“ 與第二保護層4c之材質例如為氧化鋁或ZnS_Si〇2等介電材 料,相變化材料層4b之材質例如為GeTeSb、InSbTe或 AgGelnSbTe等材料。覆蓋層5之材質例如利用透光性樹脂 材料,形成於第一保護層4a上。 光纪錄媒體1中,以設定為記錄功率之記錄用雷射光 束由覆蓋層5側起對記錄層4進行照射,由於其可使包括相 變化材料層4b之記錄層4於非結晶狀態與結晶狀態間產生 可逆性之相變化,故可進行記錄記號的形成及去除。換言 之’當以記錄功率之雷射光束照射記錄層4 (尤其是相變化 材料層4b)時,被照射的部分加熱到溫度超過熔點後急速 冷卻(淬火)而形成非結晶化狀態,因而形成對應於記錄信 號之記錄記號;當記錄功率之雷射光束照射記錄層4時, 記錄層4被照射的部分加熱到溫度超過結晶化溫度後緩慢 進行冷卻(退火)而形成結晶化狀態,因而 除。當讀取時,以讀取功率之雷射光束(使用比千進二 時具較低功率之雷射光束)進行照射時,利用非結晶狀態 ^、、、、。曰曰狀態間卩現著光學常數變化而產生變化之光反射率的 差異 來判別5己錄冗號的有無,以進行資料的讀取。 在製作光記錄媒體1時,首先以射出成形形成表面且 有凹槽等之細微凹凸的圓盤狀基板2。接著,於基板2之表 面上形成反射層3,之後於反射層3上形成記錄層4。此時 =變化材料層4b與第一、第二保護層4a、4c一般係以濺鍍 /形成。然後,例如利用旋塗法於記錄層4上形成覆蓋層 第6頁 2186.5255.PFl(N).ptc 1220986 _累號 91123318 五、發明說明(3) 5。記錄層4中之相變化材料層4b於剛形成時為非結晶狀 η λ用者並不能進行記錄。因此,4 了使光記錄媒 體1在使用者可立刻直接使用之狀態下出貨,於 =媒體1時須對記錄層4(尤其是相變化材料層扑)進行初始 ^步驟。故於形成覆蓋層5後,需進行記錄層4之初始化 二驟。於是,以與讀取用或記錄用雷射光束之昭射方向同 一方向(亦即由覆蓋層5侧),利用高功率(初始化功率)之 雷射光束(以下以「初始化用雷射光束」表示)照射,進行 記錄層4之初始化步驟。此時,此初始化用雷射光束一般 係藉由數值孔徑NACmimericai aperture)約為〇 4(例如為 〇· 34)之物鏡,對光記錄媒體】進行照射。如此即完成了具 有初始化記錄層4之光記錄媒體1。 、為了符合更大容量之光記錄媒體之開發與商品化的要 f,發明人目前正從事以光記錄媒體!為基礎、且具更大 容量之光記錄媒體丨丨的開發。關於此光記錄媒體丨^之說明 請對照第6圖。圖中與光記錄媒體丨具相同結構之部份均以 相同符號標示,其說明亦不重複敘述。 ^此光記錄媒體11,亦即單面多層(例如兩層)記錄層型 光記錄媒體(以下以「多層記錄層型光記錄媒體」表示), 如圖所示,於基板2之一表面(圖中之上表面)上依序形成 包括反射層3與記錄層彳之以層、作為透光層之間隔層12、 記錄層14(以下以「L〇層」表示)、與作為透光層之覆蓋層 5。間隔層12之>厚度TH通常設定為2〇 ,其L〇層側的表面 上形成有凹槽等之細微凹凸。記錄層丨4包括第一保護層1220986 Amendment No. 9112 ^ 1 «V. Description of the Invention (2) 4b and 4a are formed on the reflective layer 3 in this order. The material of the first protective layer and the second protective layer 4c is, for example, a dielectric material such as alumina or ZnS_SiO2, and the material of the phase change material layer 4b is, for example, GeTeSb, InSbTe, or AgGelnSbTe. The material of the cover layer 5 is, for example, A light-transmitting resin material is used to form the first protective layer 4a. In the optical recording medium 1, the recording layer 4 is irradiated with the recording laser beam set to the recording power from the cover layer 5 side. The recording layer 4 including the phase-change material layer 4b generates a reversible phase change between the amorphous state and the crystalline state, so that recording marks can be formed and removed. In other words, 'When the recording layer 4 is irradiated with a laser beam of recording power ( Especially when the phase-change material layer 4b), the irradiated part is heated to a temperature exceeding the melting point, and then rapidly cooled (quenched) to form an amorphous state, thereby forming a recording mark corresponding to the recording signal; when the laser beam of the recording power is irradiated When recording layer 4, the irradiated portion of recording layer 4 is heated to a temperature exceeding the crystallization temperature, and then slowly cooled (annealed) to form a crystalline state. When reading, when using a laser beam with a reading power (using a laser beam with a lower power than 1000 times) to irradiate, use the amorphous state ^ ,,,,. The difference of the light reflectance caused by the change of the optical constant is used to judge the presence or absence of 5 digits to read the data. When the optical recording medium 1 is produced, the surface of the optical recording medium 1 is first formed by injection molding with grooves. Subtle uneven disk-shaped substrate 2. Next, a reflective layer 3 is formed on the surface of the substrate 2, and then a recording layer 4 is formed on the reflective layer 3. At this time = the changing material layer 4b and the first and second protective layers 4a, 4c is generally sputtered / formed. Then, for example, a cover layer is formed on the recording layer 4 by using a spin coating method. Page 6 2186.255255.PFl (N) .ptc 1220986 _ tired number 91123318 5. Description of the invention (3) 5. Record The phase-change material layer 4b in layer 4 was amorphous η λ at the time of formation and cannot be recorded by the user. Therefore, the optical recording medium 1 is shipped in a state where the user can directly use it immediately. For media 1, the recording layer 4 (especially the phase change material layer The initial step is performed. Therefore, after the cover layer 5 is formed, the initialization step of the recording layer 4 needs to be performed. Therefore, the same direction as the radiating direction of the reading or recording laser beam (that is, from the cover layer 5 side) ), Using a high-power (initialization power) laser beam (hereinafter referred to as "initialization laser beam") to perform the initialization step of the recording layer 4. At this time, the laser beam for initialization is generally irradiated to an optical recording medium through an objective lens having a numerical aperture (NACmimericai aperture) of about 0.4 (for example, 0.34). Thus, the optical recording medium 1 having the initial recording layer 4 is completed. In order to meet the requirements of the development and commercialization of larger-capacity optical recording media, the inventor is currently engaged in optical recording media! Based on the development of optical recording media with greater capacity. About the description of this optical recording medium, please refer to FIG. 6. In the figure, parts having the same structure as the optical recording medium are marked with the same symbols, and descriptions thereof are not repeated. ^ This optical recording medium 11 is a single-sided multilayer (eg, two-layer) recording layer type optical recording medium (hereinafter referred to as a "multilayer recording layer type optical recording medium"), as shown in the figure, on one surface of the substrate 2 ( The upper surface in the figure) includes a reflective layer 3 and a recording layer, a spacer layer 12 as a light transmitting layer, a recording layer 14 (hereinafter referred to as "L0 layer"), and a light transmitting layer. The cover layer 5. The > thickness TH of the spacer layer 12 is usually set to 20, and fine irregularities such as grooves are formed on the surface of the L0 layer side. Recording layer 4 includes a first protective layer

2186-5255-PFl(N).ptc 第7頁 1220986 -^---案號91123318_年月日 你正 , 五、發明說明(4) 一 _ -----2186-5255-PFl (N) .ptc Page 7 1220986-^ --- Case No. 91123318_Year Month Date You are five. Description of the invention (4) One _ -----

Ma、相變化材料層14b與第二保護層14c,上述各層“^^、 1 4b、1 4a係以此順序形成於間隔層丨2之具有細微凹凸的表 面上。雖然各層14a、14b、14c與對應之各層4a、4b、4c 的材質與厚度均相異,但卻具有相同之功能。覆蓋層5之 材質為樹脂材料,且形成於L〇層上。 ‘ 即使是光記錄媒體11,於此製造過程中仍需進行記錄 · 層4、1 4之初始化步驟。如第7圖所示,與光記錄媒體工相 同’於形成覆蓋層5後,以與對光記錄媒體1之初始化時所 使用之具相同數值孔徑NA之物鏡21,進行初始化步驟。具 體地《兒’以初始化用雷射光束L 由覆蓋層5侧起對^ 1層 ,照射:來進行包括記錄層“L1層的初· 著如圖所不’對L〇層照射初始化用雷射光束k,進行L〇層 之初始化。如此完成了具有經初始化之L1層與L0層的光記 錄媒體1 1。 ° 、本發明人檢討上述之多層記錄層光記錄媒體之初始化 方法’發現下列急需改進之缺點。亦即,如第7圖所示, 此初始化方法中對形成於間隔層1 2上之L0層進行初始化 時’照射L0層所使用之初始化用雷射光束Lin中之一部分的 雷射光束lpe ’會通過L0層與間隔層12達以層,而雷射光束 Lp、E中之=部份的雷射光束LRE會被L1層所反射。此時被反射· 的雷射光束LRE與照射L0層所使用之初始化用雷射光束lin間 會因,=層12之厚度不均而產生干涉現象。因此,層吸 收之光1會有部份不相同,結果造成L〇層各部分的發熱量 不同(L0層上產生發熱不均)。因此,由於反射之雷射光束Ma, the phase change material layer 14b, and the second protective layer 14c. The above-mentioned layers "^^, 14b, and 14a are formed in this order on the surface of the spacer layer 2 with fine unevenness. Although each layer 14a, 14b, 14c The materials and thicknesses of the corresponding layers 4a, 4b, and 4c are different, but they have the same function. The material of the cover layer 5 is a resin material and is formed on the layer L0. 'Even for the optical recording medium 11, in During the manufacturing process, the recording and layer 4 and 14 initialization steps are still required. As shown in Fig. 7, it is the same as that of the optical recording medium. After the cover layer 5 is formed, it is the same as when the optical recording medium 1 is initialized. The objective lens 21 having the same numerical aperture NA is used to perform the initialization step. Specifically, the laser beam L for initialization is used to face ^ 1 layer from the cover layer 5 side and irradiated: to perform the initial process including the recording layer "L1 layer" · Initialize the L0 layer by irradiating the laser beam k for initialization to the L0 layer as shown in the figure. Thus, the optical recording medium 11 having the initialized L1 layer and the L0 layer is completed. ° The present inventors reviewed the initialization method of the above-mentioned multilayer recording layer optical recording medium 'and found that the following shortcomings are in urgent need of improvement. That is, as shown in FIG. 7, when the L0 layer formed on the spacer layer 12 is initialized in this initialization method, 'a part of the laser beam lpe of the initialization laser beam Lin used for irradiating the L0 layer is irradiated' It will pass through the L0 layer and the spacer layer 12 and the laser beam Lp, E = part of the laser beam LRE will be reflected by the L1 layer. At this time, the reflected laser beam LRE and the initialization laser beam lin used to irradiate the L0 layer may cause an interference phenomenon due to the uneven thickness of the layer 12. Therefore, the light 1 absorbed by the layer may be partially different, which results in different amounts of heat generation in each portion of the L0 layer (heat unevenness on the L0 layer). Therefore, due to the reflected laser beam

第8頁 1220986 案號 91123318 五、發明說明(5) LEe的再照射,L 0層,尤其是記錄層1 4中之相變化材料層 1 4b可能會產生不均勻之結晶狀態,而無法進行良好之初 始化步驟,故最好能針對此缺點作改善。 多層記錄層型媒體之初始化裝 錄媒體具有形成於基板之一表 發明内容: 因此,為了改善上述缺 一種多層記錄層光記錄媒體 層之各層進行均勻的初始化 的係提供一種多層記錄層型 吕己錄層之各層進行均勻的初 本發明提供一種多層記 法,上述多層記錄層型光記 面上分別包括記錄層之複數 L0(N為1以上之整數)、與形 其中上述記錄層以光照射進 記錄媒體之初始化方法包括 從上述L 0層側對上述複數層 光,以進行初始化,其中與 面相鄰接之上述間隔層的厚 係使用上述數值孔徑NA與上 式之上述物鏡·· ΤΗ X NA — 9 〇 此外,本發明提供一種 置,上述多層記錄層型光記 點,本發明之主要目的係提供 之初始化方法,可對包括記錄 步驟。再者,本發明之另一目 媒體之初始化裝置,可對包括 始化步驟。 錄層光記錄媒體之初始化方 錄媒體具有形成於基板之一表 層LN、L(N-1 )、…、L2、L1、 成於上述複數層間之間隔層, 行初始化,上述多層記錄層光 :使用具數值孔徑NA之物鏡, 中之層LM(N 21)照射雷射 上述層LM之靠上述基板側之表 度為TH(//m)時,上述雷射光 述厚度TH之關係滿足下列方程Page 8 1220986 Case No. 91123318 V. Description of the invention (5) After re-irradiation of LEe, the phase change material layer 14b in the layer L0, especially the recording layer 14 may produce an uneven crystalline state, which cannot be performed well. Initialization step, it is best to improve on this shortcoming. Initialization of a multi-layer recording layer type recording medium has a substrate formed on the substrate. SUMMARY OF THE INVENTION Therefore, in order to improve the above-mentioned lack of a multi-layer recording layer, the optical recording medium layers are uniformly initialized, and a multi-layer recording layer type Lu Ji is provided. The present invention provides a multilayer notation in which each layer of the recording layer is uniform. The multilayer recording layer type optical recording surface includes a plurality of recording layers L0 (N is an integer of 1 or more), and the recording layer is illuminated by light. The initialization method of the recording medium includes initializing the plurality of layers of light from the L 0 layer side to initialize, wherein the thickness of the spacer layer adjacent to the surface uses the numerical aperture NA and the above-mentioned objective lens of the above formula. · T X X NA — 〇 In addition, the present invention provides a multi-layer recording layer type optical recording device, the main purpose of the present invention is to provide an initialization method, which can include a recording step. Furthermore, the initialization device of another medium of the present invention may include an initialization step. The initial recording layer of the recording optical recording medium has a surface layer LN, L (N-1), ..., L2, L1 formed on one of the substrates, and a spacer layer formed between the plurality of layers. When using an objective lens with a numerical aperture NA, the middle layer LM (N 21) is irradiated with the laser. The surface of the layer LM on the substrate side is TH (// m). The relationship between the thickness and the thickness of the laser light satisfies the following equation.

第9頁 1220986 _案號91123318_年月日 修正 五、發明說明(6) 面上分別包括記錄層之複數層LN、L(N-1 ).....L2、L1、 L0(N為1以上之整數)、與形成於上述複數層間之間隔層, 其中上述記錄層以光照射進行初始化,上述多層記錄層型 媒體之初始化裝置包括:具數值孔徑N A之物鏡,用以由上 述L0層側對上述複數層中之層LM(N -μ -1)照射雷射光來 進行初始化,其中與上述層LM之靠上述基板侧之表面相鄰 接之上述間隔層的厚度為TH( 時,上述物鏡之數值孔 徑NA與上述厚度TH之關係會滿足下列方程式: ΤΗ X NA . 9。Page 9 1220986 _Case No. 9123318_Year Month Day Amendment V. Description of Invention (6) The plural layers including recording layers LN, L (N-1), ..., L2, L1, L0 (N is An integer of 1 or more), and a spacer layer formed between the plurality of layers, wherein the recording layer is initialized by light irradiation, and the initialization device of the multilayer recording layer type medium includes: an objective lens having a numerical aperture NA, used by the L0 layer The layer LM (N-μ -1) of the plurality of layers is irradiated with laser light for initialization, wherein the thickness of the spacer layer adjacent to the surface of the layer LM on the substrate side is TH (when the above The relationship between the numerical aperture NA of the objective lens and the thickness TH described above will satisfy the following equation: τ X NA .9.

根據本發明之多層記錄層光記錄媒體之初始化方法及 初始化裝置’當進行層之初始化步驟時,若與該層之 靠基板侧之表面相鄰接之間隔層的厚度為TH( V m)時,使 用滿足式(ΤΗ X NA -9)之數值孔徑NA的物鏡,由L0層側照 射雷射光來進行初始化,如此可降低相隔於間隔層而鄰接 之層L(M + 1)所反射之反射光的影響,故可對層以進行均勻 的初始化。因此,可製造出具有高可靠性之初始化的多層 記錄層型光記錄媒體。Initialization method and initialization device for optical recording medium of multilayer recording layer according to the present invention 'When performing the initialization step of a layer, if the thickness of the spacer layer adjacent to the surface of the layer on the substrate side is TH (V m) The objective lens with numerical aperture NA satisfying the formula (TΗ X NA -9) is initialized by irradiating laser light on the L0 layer side, so that the reflection reflected by the layer L (M + 1) adjacent to the spacer layer can be reduced. The effect of light, so the layer can be uniformly initialized. Therefore, an initialized multilayer recording layer type optical recording medium with high reliability can be manufactured.

本發明提供一種多層記錄層光記錄媒體之初始化方 法,上述多層記錄層型光記錄媒體具有形成於基板之一表 面上分別包括記錄層之複數層LN、[(Nd )、···、L2、、 L0(N為1以上之整數)、與形成於上述複數層間之間隔層, 其中上述記錄層以光照射進行初始化,本發明之初始化方 法包括:使用具數值孔徑^值在〇. 55以上之物鏡,由上述 L0層側對上述複數層中之層照射雷射光,以The invention provides a method for initializing a multilayer recording layer optical recording medium. The above-mentioned multilayer recording layer type optical recording medium has a plurality of layers LN, [(Nd), ..., L2, each including a recording layer formed on one surface of a substrate. L0 (N is an integer of 1 or more), and a spacer layer formed between the plurality of layers, wherein the recording layer is initialized by light irradiation, and the initialization method of the present invention includes: using a numerical aperture ^ value of 0.55 or more The objective lens irradiates laser light from the L0 layer side to one of the plurality of layers, so that

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案號 91123318 五、發明說明(7) 進行初始化。 再者,本發明提供一種多層記錄層型媒體之初始 置,上述多層記錄層型光記錄媒體具有形成於基板之一 面上分別包括記錄層之複數層LN、[(Ν-〗)、···、L2 L0(N為1以上之整數)、與形成於上述複數層間之間、 其中上述記錄層以光照射進行初始化,上述多層記^ 媒體之初始化裝置包括:具數值孔#ΝΑ之物鏡:用以、二: 述L—0層側對上述複數層中之層LM(N^Md)照射雷射光上 進仃化,其中上述物鏡之數值孔徑NA值在0· 55以上。 初二ίΓΐ之多層記錄層光記錄媒體之初始化方法及 •以上的物鏡,從L0層側照射雷射光來進行初始 化 光Si於:ΐΐ?:隔於間隔層而鄰接之層所反射之反射 =二=”記錄層之_進行均句的初始化。 記錄媒體。&八咼可靠性之初始化的多層記錄層型光 實施方式: 以下請參照所附之圖式 記錄媒體之初始化方法之較佳j : t月之多層記錄層光 光記錄媒體1、1 1具相π a _ Η乍詳細說明。圖中與 其說明亦不重複敘述。 1 1刀勺以相同符唬標不, 請參照第1、6圖,光訪絲碰赚,, 錄媒體11具有以本發明之多層Case No. 91123318 V. Description of the invention (7) Initialization. Furthermore, the present invention provides an initial setting of a multilayer recording layer type medium. The above-mentioned multilayer recording layer type optical recording medium has a plurality of layers LN, [(N-〗), ... , L2 L0 (N is an integer of 1 or more), and formed between the plurality of layers, wherein the recording layer is initialized by light irradiation, and the above-mentioned multi-layer recording medium initialization device includes: an objective lens with a numerical hole # ΝΑ: In two, the L-0 layer side irradiates laser light on the layer LM (N ^ Md) of the plurality of layers, and the numerical aperture NA of the objective lens is above 0.55. The second stage of the initialization method of the optical recording medium of the multilayer recording layer and the objective lens above, the laser light is irradiated from the L0 layer side to initialize the light. Si: Si ?: reflection reflected by the adjacent layer separated by the spacer layer = two = ”__ Initialize the uniform sentence of the recording layer. Recording medium. &Amp; Hachiman reliability initialization of multilayer recording layer type optical implementation: Please refer to the attached diagram for the initialization method of the recording medium. The multi-layered recording layer optical recording media 1 and 1 of t month have a detailed description of π a _. At first glance, its description is not repeated. 1 1 knife and spoon are marked with the same sign. Please refer to sections 1 and 6. Figure, optical access, touch recording, recording medium 11 has multiple layers according to the present invention

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^ =層光記錄媒體之初始化方法完成初始化之記錄層,其 ^ 基板2之具有細微凹凸形成之表面(圖中之上方表面) 依序形成L1層、間隔層12、與間隔層12相鄰接之l〇層、 與覆蓋層5等所堆積構成。 接著將對本發明之光記錄媒體丨丨之初始化裝置Μ作說 明’請參照第2圖。 初始化裝置Μ包括軸承馬達ΜΤ、讀寫頭PU、軸承伺服 SPS、傳動伺服TRS、聚焦循軌伺服FTS、與控制裝置CNT。 轴承馬達MT係由軸承伺服SPS控制,使光記錄媒體丨丨在線 速度一定的條件下進行轉動,後續會再作描述。 讀寫頭PU由形成一體之雷射光射出端與雷射光接受端 所組成’以控制裝置CNT控制雷射驅動源驅動雷射光(兩者 均未纟會示於圖中)朝光記錄媒體11方向,對光記錄媒體1 ^ 射出設定為初始化功率之雷射光束Lin。此外,讀寫頭pu還 包括物鏡31與分光鏡(未繪示),用以將雷射光束Lin集中於 光記錄媒體11之L1層、L0層上。具體地說,以聚焦循軌伺 服FTS對物鏡3 1進行聚焦循軌控制,使初始化用雷射光束 LIN集中於光記錄媒體11之L1層、L〇層上。此時,若光記錄 媒體11中之間隔層12的厚度為TH( 時,物鏡31係使用 滿足下列方程式(1)之數值孔徑NA所構成。 ΤΗ X NA ^ 9 ...........................⑴ 如前述,間隔層12的厚度TH —般係設定為20 /zm,或 至少在1 6. 5 // m以上。因此,若間隔層丨2所形成之厚度例 如為1 6 · 5 // m時,則物鏡3 1使用可滿足上式(丨)之數值孔徑^ = Layer optical recording medium initialization method The recording layer that has been initialized is completed. ^ The surface of the substrate 2 with the slight unevenness (the upper surface in the figure) is sequentially formed with the L1 layer, the spacer layer 12, and the spacer layer 12 adjacent to each other. The 10 layers and the cover layer 5 are stacked. Next, the initialization device M of the optical recording medium 丨 丨 of the present invention will be explained 'Please refer to FIG. 2. The initialization device M includes a bearing motor MT, a read-write head PU, a bearing servo SPS, a transmission servo TRS, a focus tracking servo FTS, and a control device CNT. The bearing motor MT is controlled by the bearing servo SPS, which makes the optical recording medium 丨 丨 rotate at a constant line speed, which will be described later. The read-write head PU is composed of a laser light emitting end and a laser light receiving end that are integrated to control the laser driving source to drive the laser light through the control device CNT (both are not shown in the figure) toward the optical recording medium 11 A laser beam Lin set to an initialization power is emitted to the optical recording medium 1. In addition, the read-write head pu also includes an objective lens 31 and a beam splitter (not shown) for focusing the laser beam Lin on the L1 layer and the L0 layer of the optical recording medium 11. Specifically, the focus tracking servo FTS performs focus tracking control on the objective lens 31 so that the initialization laser beam LIN is focused on the L1 layer and the L0 layer of the optical recording medium 11. At this time, if the thickness of the spacer layer 12 in the optical recording medium 11 is TH (, the objective lens 31 is configured using a numerical aperture NA that satisfies the following equation (1). ΤΗ X NA ^ 9 ........ ......... As mentioned above, the thickness TH of the spacer layer 12 is generally set to 20 / zm, or at least 1 6. 5 // m or more. Therefore, if the thickness of the spacer layer 丨 2 is, for example, 1 6 · 5 // m, the numerical aperture of the objective lens 3 1 that can satisfy the above formula (丨) is used.

2186-5255-PFKN) .ptc 第12頁 Ϊ2209862186-5255-PFKN) .ptc p.12 Ϊ220986

2為0.55的物鏡。若間隔層12所形成之厚度*i3#m時, ^使用可滿足上式(1)之數值孔徑“為〇 7之物鏡。另外, 讀寫頭PU由傳動伺服TRS控制,沿光記錄媒體丨丨之直徑方 向於其内徑側與外徑側間反覆進行移動。 由控制裝置CNT所控制之軸承伺服SPS控制軸承馬達MT 之轉動,使光記錄媒體1 1之線速度維持於一定。控制裝置 CNT用以控制讀寫頭”、軸承伺服sps、傳動伺服trs、及 聚焦循執伺服FTS等的驅動。2 is an objective lens of 0.55. If the thickness * i3 # m formed by the spacer layer 12 is used, an objective lens having a numerical aperture "0" that satisfies the above formula (1) is used. In addition, the read-write head PU is controlled by the transmission servo TRS, and it follows the optical recording medium The diameter direction moves repeatedly between the inner diameter side and the outer diameter side. The bearing servo SPS controlled by the control device CNT controls the rotation of the bearing motor MT, so that the linear speed of the optical recording medium 11 is maintained constant. The control device CNT is used to control the drive of read / write head ", bearing servo sps, transmission servo trs, and focus compliance servo FTS.

接著將對光記錄媒體1〗之初始化方法作說明,請參照 第1圖。而除初始化步驟外之光記錄媒體丨丨之製造方法, 因以相同於前述之製造方法所製作,故在此亦不再贅述。 首先’以控制裝置CNT控制軸承伺服sps驅動軸承馬達 MT ’使光記錄媒體丨丨以一定的線速度進行轉動。接著,控 制裝置CNT控制傳動伺服TRS,使讀寫頭⑼移動至初始化起 始位置,且控制聚焦循軌伺服FTS,將物鏡31之焦點位置 對準光§己錄媒體11之L1層使物鏡3丨定位。之後,以控制裝 置CNT控制傳動伺服TRS與聚焦循軌伺服FTS,使讀寫頭pu ,如從=徑側起往外徑側移動,而由覆蓋層5側對L丨層進Next, the initialization method of the optical recording medium 1 will be described, please refer to FIG. 1. Since the manufacturing method of the optical recording medium except for the initialization step is made by the same manufacturing method as above, it will not be repeated here. First, the bearing servo sps is driven by the control device CNT to drive the bearing motor MT and the optical recording medium 丨 丨 is rotated at a constant linear speed. Next, the control device CNT controls the drive servo TRS to move the read / write head 初始化 to the initial starting position, and controls the focus tracking servo FTS to align the focus position of the objective lens 31 to the light § The L1 layer of the recorded medium 11 makes the objective lens 3丨 Positioning. After that, the control device CNT controls the drive servo TRS and the focus tracking servo FTS, so that the read-write head pu moves from the diameter side to the outer diameter side, and the layer 5 side enters the L 丨 layer.

订雷射光束LIN之照射,以進行包括記錄層4之L丨層的初始 化步驟。 接著’以控制裝置CNT控制物鏡31之焦點位置對準L0 層而使物鏡31定位之後,同於上述之方法,對L〇層照射初 始化用雷射光束Lin ’以進行包括記錄層1 4之層的初始化 乂驟此時’如第1圖所示,與使用數值孔徑n A為0. 3 4之The irradiation of the laser beam LIN is ordered to perform an initialization step including the L 丨 layer of the recording layer 4. Next, after the focal position of the objective lens 31 is controlled by the control device CNT to align the objective lens 31 and the objective lens 31 is positioned, the same method described above is used to irradiate the laser beam Lin for initialization to the layer O0 to perform the layer including the recording layer 14 The initialization step at this time 'as shown in Figure 1, and the use of numerical aperture n A is 0. 3 4 之

!22〇986 案號 91123318 曰 修正 五、發明說明(1〇) 物鏡時相同,對L0層所照射之初始化用雷射光束LIN中之一 部份的雷射光束LPE,會通過L0層與間隔層12達L1層。而達 Ll層之雷射光束LPE中之一部份雷射光束LRE會被L1層(尤其 疋L1層中之反射層3)所反射而照射至L 0層。此時,由於物 鏡3 1之數值孔徑N A大於物鏡2 1之數值孔徑N A,因此照射l 〇 層之雷射光束LRE之束徑DI遠大於使用物鏡21時之束徑 DI (如第1、7圖所示)。換言之,使用物鏡31時,被L1層反 身于的雷射光束LRE會充分地被分散。 因此,將初始化用雷射光束LIN之雷射功率設定為定 值’以進行L0層之初始化時,被L1層反射而照射至L0層之 單位面積的雷射光束LRE的照射量,會遠小於使用物鏡2 1時 之單位面積之雷射光束LRE的照射量。如此,使用物鏡3 1來 進行初始化時,雖然被L1層反射之雷射光束LRE與照射L0層 之雷射光束LIN間會因前述之間隔層12的厚度不均而產生干 涉現象’但由於雷射光束Lre之照射能量已被分散而充分地 被降低’故不會發生L丨層所吸收之光量部分不相同的現象 。因此,可避免因雷射光束Lre之再照射至L〇層中之已完成 初始化的部分時,所產生結晶化狀態不均勻的問題,進而 可對LO層進行良好的初始化。 發明人將間隔層丨2之厚度TH設定為定值(20//m)、且 使用具不同數值孔徑NA之各物鏡的情況下,對L〇層之初始 化的良否作確認。此實驗結果列於第3圖中。根據圖中所 示之實驗結果,當使用數值孔徑NA值在0. 45以下之物鏡進 行初始化時,其初始化狀態之判定為不佳;而使用數值孔! 22〇986 Case No. 91123318 Amendment V. Description of the Invention (1) The objective lens is the same. The laser beam LPE, which is a part of the initialization laser beam LIN irradiated by the L0 layer, passes through the L0 layer and the interval. Layer 12 reaches L1. A part of the laser beam LPE up to the L1 layer is reflected by the L1 layer (especially the reflection layer 3 in the L1 layer) and irradiates the L 0 layer. At this time, because the numerical aperture NA of the objective lens 31 is larger than the numerical aperture NA of the objective lens 21, the beam diameter DI of the laser beam LRE irradiated to the 10th layer is much larger than the beam diameter DI when the objective lens 21 is used (such as the first and seventh examples). As shown). In other words, when the objective lens 31 is used, the laser beam LRE reflected by the L1 layer is sufficiently dispersed. Therefore, when the laser power of the initialization laser beam LIN is set to a constant value 'for initialization of the L0 layer, the irradiation amount of the laser beam LRE per unit area reflected by the L1 layer and irradiated to the L0 layer will be much smaller than The amount of irradiation of the laser beam LRE per unit area when the objective lens 21 is used. In this way, when the objective lens 31 is used for initialization, although the laser beam LRE reflected by the L1 layer and the laser beam LIN irradiating the L0 layer may interfere with each other due to the uneven thickness of the spacer layer 12 described above, The radiant energy of the light beam Lre has been dispersed and sufficiently reduced, so that the phenomenon that the amount of light absorbed by the L 丨 layer is not the same will not occur. Therefore, the problem of non-uniform crystallization caused by the laser beam Lre being irradiated to the portion of the L0 layer that has been initialized can be avoided, and the LO layer can be well initialized. When the inventors set the thickness TH of the spacer layer 2 to a constant value (20 // m) and used various objective lenses with different numerical apertures NA, it was confirmed whether the initialization of the L0 layer was good or not. The results of this experiment are listed in Figure 3. According to the experimental results shown in the figure, when an objective lens with a numerical aperture NA value of 0.45 or less is used for initialization, the initialization state is judged to be poor; and a numerical aperture is used.

第14頁 2186-5255-PFl(N).ptc 1220986 月 修正 曰 案號 9112331« 五、發明說明(11) 二^ Ϊ f0· 55以上之物鏡進行初始化時,其初始化狀態之 為圭。因此,只要將物鏡之數值孔徑Μ值設定在〇 55 、隹—肖^可對包括圯錄層14之10層與包括記錄層4之1^1層 ^好的初始化。另外,若考慮間隔層12之厚度Η至少 j# m以上的話,只要使用數值孔徑ΝΑ值在0· 55以上 、私Γ L便可滿足上式⑴。目此,光記錄媒體11在進行 =I:只要使用數值孔徑NA值在〇·55以上之物鏡,就 可對LI f與=層進行良好的初始化步驟。如此,便可製造 tΪ同可罪性之初始化的多層記錄層型光記錄媒體。另 夕’右間隔層12形成具13/^之薄的厚度丁Η的話,由於只 有使用數值孔徑ΝΑ值為〇·7的物鏡時才能滿足上式(1),故 八要使用數值孔徑ΝΑ值為〇. 7以上的物鏡,就可對[丨層與 L0層進行良好的初始化步驟。 ” 如上所述,根據此初始化方法與初始化裝置,使用數 值孔徑ΝΑ值為0· 55之物鏡31來進行L〇層之初始化步驟時, 可避免因位於L0層下層(離入射光較遠的層)位置之u層反 射初始化用雷射光束LIN所造成之初始化不均勻的問題。因 此,具有形成於基板2之表面上之反射層3、及對初始化用 雷射光束lin之照射方向來說為反射層3之上層的以層與L〇 層等所形成之光記錄媒體n,當其進行初始化步驟時',因 L0層(尤其是相變化材料層4b )具有均勻之結晶化狀態,因 此可對L1層之上層的L0層進行確實且良好的初始化。 此外,本發明並不只限於上述之實施例,也可作適當 的變更。例如,如第4圖所示,本發明亦適用於包括記錄 2186-5255-PFl(N).ptc 第15頁 1220986 修正 曰 五、發明說明(12) 層之層為三層以上(例如分別包括記錄層丨4之[〇層與匕丄 層、及包括記錄層4之L2層)所形成之光記錄媒體^中之l〇 層與L1層的初始化步驟。此時,光記錄媒體41係由義板2 之表面上依序形成L2層、具厚度為TH之間隔層12(以%以 「下層間隔層12」表示)、L1層、幾乎與下層間隔層12且 相同結構之間隔層12、L0層與覆蓋層5等所層積構成,^ 中L2層與光記錄媒體1中之li層具有相同結構;u層與門 隔層12相鄰接,其結構幾乎與光記錄媒體n中之L〇層相曰 =^LO層與間隔層12相鄰接,其結構幾乎與11層相^。 當光記錄媒體4 1進行初始化時,使用下層間隔層丨2之 TH與數值孔徑NA之關係可滿足上式(1)之物鏡51。之後,又 依序對L2層、U層與L0層照射初始化用雷射光束k,而依 序進行包括記錄層4之L2層、包括記錄層14之!^層與包括 記錄層1 4之L0層的初始化步驟。此外,若各間隔層之厚 度TH至少於16· 5 //m以上的話,則物鏡51使用可滿足上式 (1)之數值孔徑NA值為〇·55以上之物鏡。 工 根據此初始化方法,如第4圖所示,當進行^ 1層之初 始化時,由於將被L2層反射而照射至li層之雷射光\Lre的 束徑DI加大,故可充分降低雷射光束^對以層之單位=積 照射量。因此,可使以層(尤其是!^層中之相變化材料層 14b)具有均勻之結晶狀態,進而可對L2層之上層的Li層進 行確實且均勻的初始化。此外,進行L〇層之初始化步驟 時’被L2層(尤其是l 2層中之反射層3)反射而照射至L〇層 之雷射光束LRE的束徑DI遠大於進行li層之初始化時之雷射Page 14 2186-5255-PFl (N) .ptc 1220986 Month Amendment Case No. 9112331 «V. Description of the Invention (11) When the objective lens above 0 Ϊ f0 · 55 is initialized, its initialization state is Gui. Therefore, as long as the numerical aperture M value of the objective lens is set to 055, 隹 —Xiao ^ can initialize the 10 layers including the recording layer 14 and the 1 ^ 1 layer including the recording layer 4. In addition, if the thickness 间隔 of the spacer layer 12 is at least j # m or more, the above formula ⑴ can be satisfied as long as the numerical aperture NA value is 0.55 or more and the private Γ L is used. For this reason, the optical recording medium 11 is performing = I: As long as an objective lens having a numerical aperture NA value of 0.55 or more is used, a good initialization step can be performed on the LI f and = layers. In this way, a multilayer recording layer type optical recording medium that is initialized with different guilt can be manufactured. In addition, if the right spacer layer 12 is formed to have a thin thickness of 13 mm, since the above formula (1) can be satisfied only when an objective lens with a numerical aperture NA value of 0.7 is used, it is necessary to use a numerical aperture NA value. For an objective lens of 0.7 or more, a good initialization step can be performed for the [丨 layer and the L0 layer. As mentioned above, according to this initialization method and initialization device, when using the objective lens 31 with a numerical aperture NA value of 0.55 to perform the initialization step of the L0 layer, it is possible to avoid being located under the L0 layer (the layer farther from the incident light) ) The u-layer reflects the initialization unevenness caused by the laser beam LIN for initialization. Therefore, having the reflective layer 3 formed on the surface of the substrate 2 and the irradiation direction of the laser beam lin for initialization is The optical recording medium n formed by the layer and the L0 layer above the reflective layer 3 when the initialization step is performed, since the L0 layer (especially the phase change material layer 4b) has a uniform crystalline state, it can be The L0 layer above the L1 layer is surely and well initialized. In addition, the present invention is not limited to the above-mentioned embodiment, and can be appropriately modified. For example, as shown in FIG. 4, the present invention is also applicable to including records 2186-5255-PFl (N) .ptc Page 15 1220986 Amended Fifth, the description of the invention (12) The layer is more than three layers (for example, including the [0 layer and the dagger layer of the recording layer, respectively, and including the recording layer Layer 2 of L2 ) Initialization steps of the 10 layer and the L1 layer in the formed optical recording medium ^. At this time, the optical recording medium 41 is formed by sequentially forming an L2 layer with a thickness of TH of the spacer layer 12 on the surface of the sense board 2. Expressed in% as "lower spacer layer 12"), L1 layer, spacer layer 12, which is almost the same structure as lower spacer layer 12, L0 layer and cover layer 5, are laminated, L2 layer and optical recording medium 1 The li layer has the same structure; the u layer is adjacent to the gate spacer layer 12, and its structure is almost the same as the L0 layer in the optical recording medium n. The ^ LO layer is adjacent to the spacer layer 12, and its structure is almost 11 layers. When the optical recording medium 41 is initialized, the relationship between the TH of the lower spacer layer 2 and the numerical aperture NA can satisfy the objective lens 51 of the above formula (1). After that, the L2 layer, the U layer, and the L0 layer were sequentially irradiated with the laser beam k for initialization, and the L2 layer including the recording layer 4, the! ^ Layer including the recording layer 14 and the L0 including the recording layer 1 4 were sequentially performed. Layer initialization steps. In addition, if the thickness TH of each spacer layer is at least 16 · 5 // m or more, the objective lens 51 uses an objective lens having a numerical aperture NA value of 0.55 or more that satisfies the above formula (1). According to this initialization method, as shown in Figure 4, when the ^ 1 layer is initialized, the beam diameter DI of the laser light \ Lre reflected by the L2 layer and irradiated to the li layer is increased, so the lightning can be sufficiently reduced. The radiation beam ^ is the unit of the layer = the product irradiation amount. Therefore, the layer (especially the phase-change material layer 14b in the ^ layer) can have a uniform crystalline state, and the Li layer above the L2 layer can be reliably and uniformly initialized. In addition, when the initialization step of the L0 layer is performed, the beam diameter DI of the laser beam LRE that is reflected by the L2 layer (especially the reflective layer 3 in the 12 layer) and irradiates to the L0 layer is much larger than when the initialization of the li layer is performed. Laser

2186-5255-PFl(N).ptc 第16頁 1220986 案號91123318_年月 3 __一為 五、發明說明(13) 光束徑,因此,雷射光束LRE對L0層中已完成初始化部份之 影響比對L1層進行初始化時的影響還低。所以,L0層亦可 進行良好的初始化。而且,當進行L 0層之初始化時,即使 通過L0層之一部份的雷射光束LPE被11層反射,若各間隔層 12、12之厚度TH相同,便可滿足上式(1)。因此,可在不 受被L1層所反射之雷射光束LRE的影響下,對L0層進行良 好的初始化,而製造出具有高可靠性之初始化之多層記錄 層型光記錄媒體。 產業上可利性: 如上所述,本發明之多層記錄層光記錄媒體之初始化 方法與多層記錄層型媒體之初始化裝置中,當進行層L(M) 之初始化步驟,與層L ( Μ )之靠基板侧之表面相鄰接之間隔 層的厚度為TH( //m)時,使用滿足式(ΤΗ X ΝΑ -9)之數值 孔徑NA的物鏡,從L0層側照射雷射光來進行初始化,如此 可降低相隔於間隔層而鄰接之層L(M + 1 )所反射之反射光的 影響,故可對層LM進行均勻的初始化。因此,可製造出具 有高可靠性之初始化的多層記錄層型光記錄媒體。因此, 利用本發明之多層記錄層光記錄媒體之初始化方法與初始 化裝置,可對包括記錄層之各層進行均勻初始化。2186-5255-PFl (N) .ptc Page 16 1220986 Case No. 91123318_Year 3 __ One is the fifth, the description of the invention (13) beam diameter, therefore, the laser beam LRE has completed the initialization part of the L0 layer The impact is lower than when the L1 layer is initialized. Therefore, the L0 layer can also be well initialized. Furthermore, when the initialization of the L 0 layer is performed, even if the laser beam LPE passing through a part of the L 0 layer is reflected by the 11 layers, if the thickness TH of each of the spacer layers 12 and 12 is the same, the above formula (1) can be satisfied. Therefore, the L0 layer can be well initialized without being affected by the laser beam LRE reflected by the L1 layer, and an initialized multilayer recording layer type optical recording medium with high reliability can be manufactured. Industrial Applicability: As described above, in the method for initializing the multilayer recording layer optical recording medium and the initialization device for the multilayer recording layer type medium of the present invention, when the initialization step of the layer L (M) and the layer L (M) are performed, When the thickness of the spacer layer adjacent to the surface on the substrate side is TH (// m), an objective lens with a numerical aperture NA satisfying the formula (ΤΗ X ΝΑ -9) is used, and laser light is irradiated from the L0 layer side for initialization. In this way, the influence of the reflected light reflected by the adjacent layer L (M + 1) separated from the spacer layer can be reduced, so that the layer LM can be uniformly initialized. Therefore, an initialized multilayer recording layer type optical recording medium with high reliability can be manufactured. Therefore, by using the initialization method and the initialization device of the multilayer recording layer optical recording medium of the present invention, each layer including the recording layer can be uniformly initialized.

2186-5255-PFl(N) .ptc 第17頁 1220986 案號 91123318 曰 修正 圖式簡單說明 第1圖為具有L1層與L0層之光記錄媒體11進行初始化 時之初始化方法的說明圖。 第2圖為具有L1層與L0層之光記錄媒體11進行初始化 時之初始化裝置Μ的說明圖。 第3圖為使用具不同數值孔徑ΝΑ之物鏡來進行初始化 時,L 0層之初始化的良否之實驗結果的說明圖。 第4圖為具有L2層與L1層之光記錄媒體41進行初始化 時之初始化方法的說明圖。 第5圖繪示形成一層記錄層4之光記錄媒體1之結構剖2186-5255-PFl (N) .ptc Page 17 1220986 Case No. 91123318 Modification Brief Description of Drawings Figure 1 is an explanatory diagram of the initialization method when the optical recording medium 11 having the L1 layer and the L0 layer is initialized. Fig. 2 is an explanatory diagram of the initialization device M when the optical recording medium 11 having the L1 layer and the L0 layer is initialized. Fig. 3 is an explanatory diagram of the experimental results of the initialization of the L 0 layer when the objective lens with different numerical aperture NA is used for initialization. Fig. 4 is a diagram illustrating an initialization method when the optical recording medium 41 having the L2 layer and the L1 layer is initialized. FIG. 5 shows a structural section of the optical recording medium 1 forming a recording layer 4

面圖。 第6圖繪示具有L1層與L0層之光記錄媒體11之結構剖 面圖。 第7圖為本發明人目前所使用對具有L1層與L0層之光 記錄媒體11進行初始化時之初始化方法的說明圖。 符號說明: 1、1 1、4 1〜光記錄媒體; 2〜基板; 3〜反射層; 4、14〜記錄層; 4a、14a〜第一保護層; 4b、14b〜相變化材料層; 4c、14c〜第二保護層; 5〜覆蓋層;Face view. Fig. 6 is a sectional view showing the structure of an optical recording medium 11 having an L1 layer and an L0 layer. Fig. 7 is an illustration of an initialization method currently used by the inventors when initializing an optical recording medium 11 having an L1 layer and an L0 layer. Explanation of symbols: 1, 1 1, 4 1 to optical recording medium; 2 to substrate; 3 to reflective layer; 4, 14 to recording layer; 4a, 14a to first protective layer; 4b, 14b to phase change material layer; 4c 14c ~ second protective layer; 5 ~ cover layer;

2186-5255-PFl(N) .ptc 第18頁 1220986 案號 91123318 圖式簡單說明 1 2〜間隔層; 21、31〜物鏡 Λ_η 曰 修正2186-5255-PFl (N) .ptc Page 18 1220986 Case No. 91123318 Brief description of the drawings 1 2 ~ spacer; 21, 31 ~ objective lens Λ_η

IHB 2186-5255-PFKN) .ptc 第19頁(IHB 2186-5255-PFKN) .ptc Page 19

Claims (1)

六、申請專利範圍 i —種多 層記錄層型光 別包括記錄層 1以上之整數) 述5己錄層以光 體之初始化方 使用具數 層中之層LM(N 其中與上 間隔層的厚度 孔徑NA與上述 進行:Sixth, the scope of patent application i — a kind of multi-layer recording layer type light type including the integer of 1 or more of the recording layer) The 5th recording layer uses the light body's initialization side to use the layer LM (N where the thickness of the upper spacer layer) The aperture NA is performed as described above: 層記錄層光記錄媒體之初始化方法,上述多 記錄媒體具有依序形成於基板之一表面上分 之複數層 LN、L(N —υ、…、L2、L1、L〇(N 為 、與形成於上述複數層間之間隔層,其中上 照射進行初始化,上述多層記錄層光記錄媒 法包括·· 值孔徑NA之物鏡,從上述lq層側對上述複數 2 Μ — 1 )照射雷射光,以進行初始化, 述層LM之靠上述基板側之表面相鄰接之上述 為TH(//m)時,上述雷射光係使用上述數值 厚度TH之關係滿足下列方程式之上述物鏡來 ΤΗ X NA - 9 〇 2 · 一種多層記錄層光記錄媒體之初始化方法,上述多 曰σ己錄層型光§己錄媒體具有依序形成於基板之一表面上分 別包括記錄層之複數層LN、L(N_1)、…、L2、LI、LO(N為 1以上之整數)、與形成於上述複數層間之間隔層,其中上 述記錄層以光照射進行初始化,上述多層記錄層光記錄媒 體之初始化方法包括:Layer recording layer optical recording medium initialization method, the above-mentioned multi-recording medium has a plurality of layers LN, L (N — υ, ..., L2, L1, L0 (N is, and is formed in sequence) formed on one surface of a substrate in sequence. In the spacer layer between the plurality of layers, the upper layer is irradiated for initialization. The multi-layer recording layer optical recording medium method includes an objective lens with a numerical aperture NA, and the plurality of 2 M-1 are irradiated with laser light from the lq layer side to perform Initialization, when the surface of the layer LM adjacent to the substrate side is TH (// m), the laser light uses the objective lens whose relationship between the numerical thickness and TH satisfies the following equation to obtain X NA-9. 2 · A method for initializing a multi-layer recording layer optical recording medium. The above-mentioned σ-recorded layer type optically-recorded medium has a plurality of layers LN, L (N_1), and a recording layer sequentially formed on one surface of a substrate, respectively. ..., L2, LI, LO (N is an integer of 1 or more), and a spacer layer formed between the plurality of layers, wherein the recording layer is initialized by light irradiation, and the multilayer recording layer optical recording medium initialization method package include: 使用具數值孔徑NA值在0. 55以上之物鏡,從上述L0層 側對上述複數層中之層LM(N )照射雷射光,以進行 初始化。 3 ·—種多層記錄層型媒體之初始化裝置,上述多層記 錄層型光記錄媒體具有依序形成於基板之一表面上分別包Using an objective lens having a numerical aperture NA of 0.55 or more, laser light is irradiated to the layer LM (N) of the plurality of layers from the L0 layer side to perform initialization. 3. An initialization device for a multi-layer recording layer type medium, the above-mentioned multi-layer recording layer type optical recording medium has sequentially 2186-5255-PFl(N).ptc 第20頁 1220986 _______案號 91123318 __年 月_g_ 修正____ 六、申請專利範圍 括記錄層之複數層LN、L(N-1 ).....L2、LI、L0(N為1以 上之整數)、與形成於上述複數層間之間隔層,其中上述 記錄層以光照射進行初始化,上述多層記錄層型媒體之初· 始化裝置包括: 具數值孔徑NA之物鏡,用以從上述L0層侧對上述複數 層中之層LM(N - Μ -1)照射雷射光來進行初始化, 其中與上述層LM之靠上述基板側的表面相鄰接之上述 間隔層的厚度為TH(/zm)時,上述物鏡之數值孔徑NA與上 述厚度T Η之關係會滿足下列方程式:2186-5255-PFl (N) .ptc Page 20 1220986 _______ Case No. 91123318 __Year Month_g_ Amendment ____ Sixth, the scope of the patent application includes the multiple layers LN, L (N-1) of the recording layer ... .. L2, LI, L0 (N is an integer of 1 or more), and a spacer layer formed between the plurality of layers, wherein the recording layer is initialized by light irradiation, and the initial and initial device of the multilayer recording layer type medium includes: An objective lens having a numerical aperture NA is used to initialize the layer LM (N-M -1) of the plurality of layers from the above-mentioned L0 layer side by laser light, which is adjacent to the surface of the layer LM on the substrate side When the thickness of the spacer layer is TH (/ zm), the relationship between the numerical aperture NA of the objective lens and the thickness T 满足 will satisfy the following equation: ΤΗ X ΝΑ -9。 種多層記錄層型媒體之初始化裝置 4. --------------上述多層言i 錄層型光記錄媒體具有依序形成於基板之一表面上分別達 括記錄層之複數層LN、L(N-1).....L2、L1 ^ 上之整數)、與形成於上述複數層間之間隔層,其中、上述 圮錄層以光照射進行初始化,上述多層記錄層' 始化裝置包括: 土螺體之不 具數值孔徑NA之物鏡,用以由上述l〇層側起 數層甲之層LM(N - Μ -1)照射雷射光來進行初始化、上述複 其中上述物鏡之數值孔徑ΝΑ值在〇· 55以上。’ΤΗΝΑ -9. Initialization device for a multi-layer recording layer-type medium 4. -------------- The above-mentioned multi-layer recording layer-type optical recording medium has a recording layer formed on one surface of a substrate in order, respectively. LN, L (N-1) ..... L2, an integer on L1 ^), and a spacer layer formed between the plurality of layers, wherein the recording layer is initialized by light irradiation, and the multilayer recording The layer 'initialization device includes: an objective lens without a numerical aperture NA of the earth spiral body, which is used for initialization by irradiating laser light for several layers of LM (N-M -1) from the above 10 layers, The numerical aperture NA of the objective lens is above 55. ’
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