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    • 22. 发明申请
    • Optical recording medium
    • US20060072409A1
    • 2006-04-06
    • US10519282
    • 2003-06-27
    • Tatsuya KatoTatsuhiro KobayashiHiroyasu Inoue
    • Tatsuya KatoTatsuhiro KobayashiHiroyasu Inoue
    • G11B7/00
    • G11B7/1267G11B7/0045
    • It is an object of the present invention to provide a method for determining the power of a laser beam which can determine the recording power of the laser beam so that jitter of a reproduced signal obtained by reproducing data recorded in a data rewritable type optical recording medium can be controlled within a tolerance even when cross erasing of data occurs and that the reproduced signal having the highest level can be obtained. The method for determining the power of a laser beam according to the present invention includes the steps of recording a first test signal in a data rewritable type optical recording medium while varying a level of the recording power of the laser beam, measuring, for each of the levels of the recording power of the laser beam, an amplitude A0 of a reproduced signal obtained by reproducing the first test signal before the first test signal is influenced by cross erasing of data, an amplitude A1 and jitter J1 of a reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data and an amplitude As and jitter Js of a reproduced signal obtained by reproducing the first test signal after an influence of cross erasing of data on the first test signal was saturated, calculating a first parameter for each of the levels of the recording power of the laser beam as a function of the difference between the amplitude A0 of the reproduced signal obtained by reproducing the first test signal before the first test signal is influenced by cross erasing of data and the amplitude A1 of the reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data, calculating a second parameter for each of the levels of the recording power of the laser beam as a function of the difference between the amplitude A1 of the reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data and the amplitude As of the reproduced signal obtained by reproducing the first test signal after the influence of cross erasing of data on the first test signal was saturated, calculating a third parameter for each of the levels of the recording power of the laser beam as a function of the difference between the jitter Js of the reproduced signal obtained by reproducing the first test signal after the influence of cross erasing of data on the first test signal was saturated and the jitter J1 of the reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data, obtaining a value of the first parameter corresponding to a value of the second parameter when the third parameter is equal to a tolerance, thereby determining a critical parameter, recording a second test signal in the data rewritable type optical recording medium while varying a level of the recording power of the laser beam, judging whether or not signal characteristics of a reproduced signal obtained by reproducing the second test signal recorded in the data rewritable type optical recording medium satisfy reference conditions, measuring, for each of the levels of the recording power of the laser beam, when the signal characteristics of the reproduced signal obtained by reproducing the second test signal recorded in the data rewritable type optical recording medium satisfy the reference conditions, an amplitude AA0 of the reproduced signal obtained by reproducing the second test signal before the second test signal is influenced by cross erasing of data and an amplitude AA1 of the reproduced signal obtained by reproducing the second test signal after the first test signal was once influenced by cross erasing of data, calculating a fourth parameter based on the amplitudes AA0 and AA1 of the reproduced signals obtained by reproducing the second test signals as a function of the difference between the amplitude AA0 of the reproduced signal obtained by reproducing the second test signal before the second test signal is influenced by cross erasing of data and the amplitude AA1 of the reproduced signal obtained by reproducing the second test signal after the first test signal was once influenced by cross erasing of data, comparing the critical parameter and the fourth parameter, and determining the recording power of the laser beam at which the fourth parameter was obtained as an optimum recording power when the fourth parameter is equal to or lower than the critical parameter.
    • 24. 发明授权
    • Optical recording medium
    • 光记录介质
    • US6040030A
    • 2000-03-21
    • US153294
    • 1998-09-15
    • Hajime UtsunomiyaTatsuya KatoHiroyasu Inoue
    • Hajime UtsunomiyaTatsuya KatoHiroyasu Inoue
    • G11B7/00G11B7/0045G11B7/005G11B7/0055G11B7/006G11B7/007G11B7/125G11B7/30B32B3/00
    • G11B7/006G11B7/00718G11B7/00454G11B7/00557Y10S428/913Y10S430/146Y10T428/21
    • A method for recording/reproducing an optical recording medium of phase change type is provided. The method enables a high density recording while increase in the cross erase is suppressed. The method also enables an accurate tracking while increase in the crosstalk is suppressed. The method is adapted for use with an optical recording medium of phase change type comprising a substrate having a thickness of up to 0.8 mm wherein lands and grooves on opposite sides of the land are formed on the surface, and both the lands and the grooves are used as recording tracks, and the medium is overwritten at a recording power Pw (mW) and an erasing power Pe (mW) which meet the relation: (Pw/Pe).times.k.sup.2 .ltoreq.8.5, when the medium has a recording track pitch P (.mu.m), the recording/reproducing optical system has a numerical aperture NA, and the recording/reproducing light has a wavelength .lambda. (.mu.m) which meet the relation: k=(.lambda./NA)/P.gtoreq.1.78.
    • 提供了一种用于记录/再现相变型光记录介质的方法。 该方法能够进行高密度记录,同时抑制交叉擦除的增加。 该方法还能够进行精确的跟踪,同时抑制串扰的增加。 该方法适用于包括厚度高达0.8mm的基板的相变型光记录介质,其中在该表面上形成有焊盘相对两侧的焊盘和凹槽,并且焊盘和凹槽均为 用作记录轨道,并且当介质具有记录轨道间距时,记录功率Pw(mW)和满足关系式(Pw / Pe)xk2 <8.5的擦除功率Pe(mW)被覆盖介质 P(μm),记录/再现光学系统具有数值孔径NA,并且记录/再现光具有满足以下关系的波长λ(μm):k =(λ/NA)/P>/=1.78 。
    • 25. 发明授权
    • Laser beam power modulation pattern decision method, device for recording data onto optical recording medium, and optical recording medium
    • 激光束功率调制模式决定方法,用于将数据记录到光记录介质上的装置和光记录介质
    • US07254101B2
    • 2007-08-07
    • US10516701
    • 2003-06-02
    • Tatsuya KatoHideki HirataHiroyasu Inoue
    • Tatsuya KatoHideki HirataHiroyasu Inoue
    • G11B15/52
    • G11B7/1267G11B7/00456G11B7/2403G11B7/243G11B7/258
    • It is an object of the present invention to provide a method for determining a pattern for modulating the power of a laser beam which can determine a pattern for modulating the power of a laser beam so that data can be recorded in a write-once type optical recording medium with a laser beam having a low recording power at a high linear recording velocity. The method for determining a pattern for modulating the power of a laser beam according to the present invention includes the steps of determining pulse train patterns by fixing a recording power at a predetermined level and varying the level of a bottom power, modulating the power of the laser beam in accordance with the pulse train patterns to record first test signals in the optical recording medium, reproducing the first test signals, determining the optimum level of the bottom power based on the amplitude of the thus reproduced first test signals, determining pulse train patterns by fixing the bottom power at the optimum level and varying the level of the recording power, modulating the power of the laser beam in accordance with the pulse train patterns to record second test signals in the optical recording medium, reproducing the second test signals and determining the optimum level of the recording power based on at least one of jitter and error rates of the thus reproduced second test signals.
    • 本发明的目的是提供一种用于确定用于调制激光束的功率的图案的方法,该方法可以确定用于调制激光束的功率的图案,使得数据可以以一次写入型光学 以高线性记录速度具有低记录功率的激光束的记录介质。 根据本发明的确定用于调制激光束的功率的图案的方法包括以下步骤:通过将记录功率固定在预定水平并改变底部功率的电平来调节脉冲串模式的功率 激光束根据脉冲序列图案在光学记录介质中记录第一测试信号,再现第一测试信号,基于这样再现的第一测试信号的幅度确定底部功率的最佳电平,确定脉冲串模式 通过将底部功率固定在最佳水平并改变记录功率的水平,根据脉冲串模式调制激光束的功率,以将第二测试信号记录在光学记录介质中,再现第二测试信号并确定 基于由此再现的抖动和错误率中的至少一个的记录功率的最佳电平 nd测试信号。
    • 26. 发明授权
    • Optical recording medium
    • 光记录介质
    • US07142492B2
    • 2006-11-28
    • US10519693
    • 2003-06-27
    • Tatsuhiro KobayashiTatsuya KatoHiroyasu Inoue
    • Tatsuhiro KobayashiTatsuya KatoHiroyasu Inoue
    • G11B7/00
    • G11B7/1267G11B7/0045
    • A method for determining the recording power of a laser beam so that jitter from a reproduced signal obtained by reproducing data recorded in a data rewritable type optical recording medium can be controlled within an acceptable tolerance even when cross erasing of data occurs. The power of a laser beam is measured for each level of the recording power of the laser beam. Critical parameters are calculated for each level of the recording power of the laser beam. The critical parameters are projected onto a data rewritable type optical recording medium for recording data therein. Direct overwriting required for saturating an influence of cross erasing of data is performed x times in one embodiment to determine a critical parameter. A data recording apparatus storing a critical parameter used for determining the power of a laser beam is associated with ID data for identifying the kind of optical recording medium. A data recording apparatus storing an optimum recording power used for determining the power of a laser beam is also associated with ID data for identifying the kind of optical recording medium.
    • 一种用于确定激光束的记录功率的方法,使得即使当数据发生交叉擦除时,也可以通过再现记录在数据可重写型光学记录介质中的数据而获得的再现信号的抖动被控制在可接受的公差内。 针对激光束的记录功率的每个级别测量激光束的功率。 针对激光束的记录功率的每个级别计算关键参数。 将关键参数投影到用于在其中记录数据的数据可重写型光学记录介质上。 在一个实施例中,执行用于饱和数据交叉擦除的影响所需的直接重写x次以确定关键参数。 存储用于确定激光束的功率的临界参数的数据记录装置与用于识别光学记录介质的种类的ID数据相关联。 存储用于确定激光束的功率的最佳记录功率的数据记录装置也与用于识别光学记录介质的种类的ID数据相关联。
    • 27. 发明授权
    • Optical recording method and optical recording medium
    • 光记录方法和光记录介质
    • US06999392B2
    • 2006-02-14
    • US09971703
    • 2001-10-09
    • Tatsuya KatoHajime UtsunomiyaHiroyasu InoueHiroshi ShingaiYoshitomo Tanaka
    • Tatsuya KatoHajime UtsunomiyaHiroyasu InoueHiroshi ShingaiYoshitomo Tanaka
    • G11B7/00G11B7/24
    • G11B7/24085G11B7/00454G11B7/006
    • Increase of jitter in a phase change optical recording medium is suppressed with no extreme decrease in the crystallization speed of the recording layer when the medium is overwritten at a high linear velocity. In addition, in a disk-shaped medium operated at a constant angular velocity, the overwriting is accomplished with the increase of jitter suppressed over the entire area of the medium. Provided is an optical recording method for recording a disk-shaped optical recording medium having a phase change recording layer which is rotated at a constant angular velocity, wherein amorphous recorded marks are formed in the recording layer. In this method, the minimum recorded mark is formed such that WL/ML incrementally or gradually decreases from the radially inner side to the radially outer side of the optical recording medium, when the minimum signal has a length of SL, and when the minimum recorded mark corresponding to said minimum signal has its maximum width of MW, EW is 0.1 MW; the position on the leading edge side of the recorded mark at the width of EW is designated effective leading edge; and the position on the trailing edge side of the recorded mark at the width of EW is designated effective trailing edge; the distance between the effective leading edge and the effective trailing edge is designated effective length ML; and the distance between the effective leading edge and the position at which the width starts to decrease on the trailing edge side is designated WL.
    • 当以高线速度重写介质时,抑制了相变光记录介质中的抖动的增加,而在记录层的结晶速度没有极度降低的情况下。 另外,在以恒定的角速度操作的盘形介质中,通过在介质的整个区域上抑制的抖动的增加来实现重写。 提供了一种用于记录具有以恒定角速度旋转的相变记录层的盘形光学记录介质的光学记录方法,其中在记录层中形成非晶体记录标记。 在该方法中,形成最小记录标记,使得W L L / M L L从光记录介质的径向内侧向径向外侧逐渐地逐渐减小 当最小信号具有长度为S L L时,当对应于所述最小信号的最小记录标记具有M W的最大宽度时,E W 为0.1MW; 记录标记的前缘侧的位置在E 的宽度被指定为有效前沿; 并且在E&lt; W&gt;宽度的记录标记的后缘侧的位置被指定为有效后缘; 有效前沿和有效后沿之间的距离被指定为有效长度M L L; 并且有效前沿与后缘侧宽度开始减小的位置之间的距离被指定为W L L。
    • 28. 发明申请
    • Optical recording medium
    • US20060013089A1
    • 2006-01-19
    • US10519693
    • 2003-06-27
    • Tatsuhiro KobayashiTatsuya KatoHiroyasu Inoue
    • Tatsuhiro KobayashiTatsuya KatoHiroyasu Inoue
    • G11B7/12
    • G11B7/1267G11B7/0045
    • It is an object of the present invention to provide a method for determining the power of a laser beam which can determine the recording power of the laser beam so that jitter of a reproduced signal obtained by reproducing data recorded in a data rewritable type optical recording medium can be controlled within a tolerance even when cross erasing of data occurs and that the reproduced signal having the highest level can be obtained. The method for determining the power of a laser beam according to the present invention includes the steps of recording a first test signal in the data rewritable type optical recording medium while varying a level of the recording power of the laser beam, reproducing the first test signal recorded in the data rewritable type optical recording medium, measuring, for each of the levels of the recording power of the laser beam, an amplitude A0 of a reproduced signal obtained by reproducing the first test signal before the first test signal is influenced by cross erasing of data, an amplitude A1 and jitter J1 of a reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data and an amplitude As and jitter Js of a reproduced signal obtained by reproducing the first test signal after an influence of cross erasing of data on the first test signal was saturated, calculating a first parameter for each of the levels of the recording power of the laser beam as a function of the difference between the amplitude A0 of the reproduced signal obtained by reproducing the first test signal before the first test signal is influenced by cross erasing of data and the amplitude A1 of the reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data, calculating a second parameter for each of the levels of the recording power of the laser beam as a function of the difference between the amplitude A1 of the reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data and the amplitude As of the reproduced signal obtained by reproducing the first test signal after the influence of cross erasing of data on the first test signal was saturated, calculating a third parameter for each of the levels of the recording power of the laser beam as a function of the difference between the jitter Js of the reproduced signal obtained by reproducing the first test signal after the influence of cross erasing of data on the first test signal was saturated and the jitter J1 of the reproduced signal obtained by reproducing the first test signal after the first test signal was once influenced by cross erasing of data, obtaining a value of the first parameter corresponding to a value of the second parameter when the third parameter is equal to a tolerance, thereby determining a critical parameter, recording a second test signal in the data rewritable type optical recording medium while varying a level of the recording power of the laser beam, judging whether or not signal characteristics of a reproduced signal obtained by reproducing the second test signal recorded in the data rewritable type optical recording medium satisfy reference conditions, measuring, for each of the levels of the recording power of the laser beam, when the signal characteristics of the reproduced signal obtained by reproducing the second test signal recorded in the data rewritable type optical recording medium satisfy the reference conditions, an amplitude AA0 of the reproduced signal obtained by reproducing the second test signal before the second test signal is influenced by cross erasing of data and an amplitude AA1 of the reproduced signal obtained by reproducing the second test signal after the first test signal was once influenced by cross erasing of data, calculating a fourth parameter based on the amplitudes AA0 and AA1 of the reproduced signals obtained by reproducing the second test signals as a function of the difference between the amplitude AA0 of the reproduced signal obtained by reproducing the second test signal before the second test signal is influenced by cross erasing of data and the amplitude AA1 of the reproduced signal obtained by reproducing the second test signal after the first test signal was once influenced by cross erasing of data, comparing the critical parameter and the fourth parameter, and determining the recording power of the laser beam at which the fourth parameter was obtained as an optimum recording power when the fourth parameter is equal to or lower than the critical parameter.
    • 30. 发明授权
    • Optical recording medium including protruding winding parts used as prepits
    • 光记录介质,包括用作预凹坑的突出的绕组部分
    • US06665260B2
    • 2003-12-16
    • US09899152
    • 2001-07-06
    • Tatsuya KatoHajime UtsunomiyaHiroyasu InoueHideki Hirata
    • Tatsuya KatoHajime UtsunomiyaHiroyasu InoueHideki Hirata
    • G11B724
    • G11B7/24085G11B7/00745G11B7/261
    • In an optical recording medium wherein grooves or lands formed on the supporting substrate are used for the recording tracks, and wherein prepits are also formed, production of the supporting substrate and high density recording are facilitated. This medium comprises a supporting substrate and a recording layer on the substrate wherein the surface of the supporting substrate on which the recording layer is formed is formed with alternating continuous convex portions and continuous concave portions which are substantially parallel to each other. The adjacent continuous convex portions are connected by bridging convex portions extending in transverse direction, and the bridging convex portion has a planar configuration that its width is minimum at or near the center between the adjacent continuous convex portions. The supporting substrate is produced by using a master disk which has a resist layer formed with mother patterns of each of the continuous convex portions, continuous concave portions, and prepits. In the production of the master disk, the resist layer is intermittently irradiated with one exposure beam, and the area irradiated is used as the mother pattern of the continuous concave portions or convex portions, and the area which was not irradiated is used as the mother pattern of the prepits.
    • 在其中形成在支撑基板上的槽或焊盘用于记录轨道的光记录介质中,并且还形成预凹坑,便于生产支撑基板和高密度记录。 该介质包括支撑衬底和衬底上的记录层,其中形成有记录层的支撑衬底的表面形成有彼此基本平行的交替的连续凸部和连续凹部。 相邻的连续凸部通过在横向延伸的桥接凸部连接,并且桥接凸部具有在相邻的连续凸部之间的中心处或其附近的宽度最小的平面构造。 支撑基板通过使用具有形成有连续凸部,连续凹部和预凹坑中的每一个的母体图案的抗蚀剂层的母盘来制造。 在母盘的制造中,用一个曝光束间歇地照射抗蚀剂层,照射的面积用作连续凹部或凸部的母体图案,未照射的区域用作母体 预制图案。