• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The dual layer pre-recorded optical disc 12 includes a transparent substrate 14, a partially reflective layer 16, a transparent spacer layer 18 and a high reflection layer 20. One data pit pattern 15 is provided on the substrate adjacent to the partially reflective layer, and the other data pit pattern 19 is provided on the spacer layer adjacent to the high reflection layer. The partially reflective layer has the general formula Au x Ag y , where it may be made of an alloy of gold and silver with 15 <x <40 and 60 <y <85. The substrate incident beam may be used to read the data encoded in either data pit pattern depending on which layer the laser 30 is focused in. Double layer disks have twice the data storage capacity of conventional single layer disks.
    公开号:KR20000064459A
    申请号:KR1019980704629
    申请日:1996-10-07
    公开日:2000-11-06
    发明作者:제프리 엠. 플로르자크；마이클 비. 하인츠
    申请人:윌리엄 데이비드 바우어, 캐씨 로버타 샘스；이메이션 콥；
    IPC主号:
    专利说明:

    Bilayer Optical Media With Partly Reflective Gold Alloy Layer
    The demand for media that increases storage capacity and performance in data storage seems to be endless. In the field of pre-recorded optical discs, such as compact discs and video discs, the increase in storage capacity is typically achieved by increasing the amount of storage per unit area of the disc. However, the maximum data storage density achievable in an optical recording system is limited by the minimum shape that the optical system can resolve. In conventional far imaging systems, the minimum resolvable shape dimension is limited by the refractive effect to the wavelength of the approximately available light source, typically a solid state laser diode. Thus, one way to increase disk storage capacity is to reduce the wavelength of the laser diode. However, although the wavelengths available from laser diodes have been steadily decreasing, the reduction has not been radicalized due to the limitations of solid state technology and materials.
    Many other techniques have been proposed for increasing the memory capacity of an optical recording system. These include: (1) high efficiency data coding schemes, i.e. pulse width modulation schemes, (2) optical and / or magnetic superresolution schemes, (3) zoned recording schemes at constant angular velocity, and (4) partial response / maximum likelihood detection. And an application data channel detection scheme such as (4) recording in both the home zone and the land zone of the disc.
    Although all of the foregoing methods for increasing the storage capacity depend on increasing the storage amount per unit area of the disk, an alternative method of increasing the storage capacity of the optical disk is to employ an additional storage layer on the disk. The layers can be recorded or reproduced independently. Thus, the approach in this case is to increase the addressable area of the disc. This approach is attractive because it has the potential to significantly increase the media storage capacity only by increasing the complexity of the media and recording system to a moderate degree. If multiple storage layers, for example two layers, are to be reproduced by an optical beam provided on one side of the disc, one of the storage layers of the disc should be reflective enough to be reproduced by the optical beam, There must be sufficient transparency to be able to penetrate the first memory layer and transition to the second memory layer.
    The present invention relates to the field of optical media technology, and more particularly to the field of optical media employing two or more information storage layers.
    1 shows an optical data storage system according to the present invention.
    2 is a graph of reflectance as a function of thickness for a partially reflective layer of gold.
    3 is a graph of the real component n of reflectance as a function of the amount of silver in a thin film layer of a gold-silver alloy according to one embodiment of the present invention.
    4 is a graph of the real component (n) of reflectance as a function of the amount of copper in a thin film layer of a gold-silver alloy according to one embodiment of the invention.
    Accordingly, the present invention provides an optical disc with a partially reflective layer and a transparent spacer layer that allows a single reproduced light beam to be focused on either of two different planes in the disc. The disk comprises a transparent substrate having a feature, for example a pattern of pit, on one of the faces of the disk. The partial reflective layer is provided adjacent to the shape pattern. A transparent polymer spacer layer is provided over the partially reflective layer and a high reflection layer is provided over the spacer layer.
    The partially reflective layer comprises a metal alloy comprising two metals, one of the two metals being gold, the other having a refractive index with a real component n and an imaginary component K, where n as measured at 650 nm ≤1 and K≥2. The metal alloy has the general formula Au x M y , where 10 <x <90 and 10 <y <90, where M is the second metal. One preferred embodiment is n ≦ 0.8 and K ≧ 0.3 for the second metal. Another preferred embodiment is n ≦ 0.65 and K ≧ 3.5.
    In one embodiment, the second metal is silver and the metal alloy has the general formula Au x Ag y , where 10 <x <90 and 10 <y <90. In other preferred embodiments, 15 <x <90, 10 <y <85, 15 <x <40, 60 <y <85, 20 <x <80, 20 <y <80, 20 <x <60, 40 <y <80, 20 <x <40, and 60 <y <80.
    In yet another embodiment, the second metal is copper. In this embodiment, the metal alloy preferably has the general formula Au x Cu y , where 80 <x <90 and 10 <y <20. In another embodiment of the invention, the metal alloy has gold, silver and copper and has the general formula Au x Ag y Cu z , where 20 <x <75, 20 <y <75 and 5 <z <20. .
    In one embodiment of the invention, the substrate comprises polycarbonate and the spacer layer comprises a photopolymer. The second shape pattern or the pit pattern may be provided on a surface of the spacer layer adjacent to the high reflection layer. The spacer layer preferably has a thickness in the range of about 5 to 100 μm.
    The invention also includes an optical storage system comprising the above-mentioned medium. The system also includes a photodetector positioned to detect a focused laser beam positioned to be incident through the substrate into the medium, a means for adjusting the focus position of the laser beam on the partially reflective or high reflective layer, and a reflected laser beam exiting the medium. It includes.
    The present invention also includes a dual layer pre-recorded optical disc having the above-mentioned partially reflective layer as well as a storage system incorporating such a disc.
    An optical data storage system 10 according to the present invention is shown in FIG. The optical storage medium 12 includes a highly reflective thin film layer on the transparent substrate 14, the partially reflective thin film layer 16 on the first data pit pattern 15, the transparent spacer layer 18, and the second data pit pattern 19. 20). As shown in FIG. 1, an optical laser 30 emits a light beam towards the medium 12. As shown in FIG. Light from the light beam reflected by the thin film layer 16 or thin film layer 20 is sensed by a detector 32 that detects modulation of light intensity based on the presence or absence of pits at specific points on the thin film layer.
    While the patterns 15 and 19 are also called "data pit patterns", the pit patterns 15 and 19 are pit that can store information, for example data, servo or tracking information, format information, and the like. Or any pattern consisting of grooves.
    The ability to read the first or second pit patterns 15, 19 independently is based on the relatively limited depth of focus characteristics of a typical optical disc reading system. Lenses employed in typical optical recorders / players to form diffraction limited laser emission points on the media storage layer have moderately large (04 to 0.6) numerical apertures to improve resolution and increase memory density. Such a lens exhibits a depth of focus of about 2 μm (i.e., a range of focus fluctuations in which the focal spot size remains roughly limited in diffraction) (large focus fluctuations cause the size of the irradiated spot to grow rapidly). As a result, if the partially reflective thin film layer 16 exhibits sufficient transmission and the distance separating the two tapered pit patterns 15 and 19 is large compared to the optical focus depth, it is "cross-talk" from another data pit pattern. It is possible to focus the laser 30 on either data pit pattern while keeping it low enough to tolerate. Thus, the light from the laser 30 is reflected back towards the detector 32 by both layers 16 and 20, and only the layer where the laser is focused is strongly modulated to reflect the intensity of the reflected light to enable data reading. .
    The data pit patterns 15, 19 on the medium 10 first focus the focus on one of the reflective layers 16, 20 and then convert the data of the entire layer before converting the focus position to focus on the other reflective layer. By reproducing, it can be reproduced most easily. Alternatively, it may be desirable to switch the focus position one or more times before fully reproducing the data contained in one of the data fit patterns 15, 19. In either case, the use of two data pit patterns separated by the transparent layer 18 effectively doubles the data storage capability of the optical recording medium 10.
    Another configuration may include two transparent substrates, each having a different molded or replicated data pit pattern on one surface. The metallic semi-reflector layer described herein is deposited on the first data pit pattern on the first substrate, and the high reflective layer is deposited on the second data pit pattern on the second substrate. The two cladding substrates are then bonded to each other with a transparent binder, which may also be a photopolymer or other polymeric material, in such a way that a uniform space is provided between the two bonding surfaces. Other means of using the metallic quasi-reflector layer described herein to construct an optical storage medium comprising two or more information surfaces that can be addressed by an optical beam incident on one side of the disk structure are known in the art. If you are skilled, you will know clearly.
    The transparent layer 14 may be a polymeric material suitable for an optical disk substrate that sufficiently supports the molding of the data pit pattern 15, such as polycarbonate or amorphous polyolefin. Alternatively, it is possible to use a flat substrate, for example of glass or polymethylmethacrylate, and to form the data pit pattern 15 by photopolymer replication.
    The transparent spacer layer 18 is a polymer such as a photocurable polymer having a complex refractive index having a real component n ranging from about 1.45 to 1.6 and an imaginary component K of less than 10 −4 , more preferably less than 10 −5. Can be. The transparent spacer layer 18 should be thick enough to allow the laser 30 to focus anywhere on the data fit patterns 15, 19 with minimal crosstalk. It may be varied at a thickness that is preferably in the range of about 5 to 100 μm, more preferably about 10 to 60 μm.
    The high reflection layer 20 may be a metal layer exhibiting high reflection force at a laser wavelength used to reproduce data. Currently available laser diode light sources emit at wavelengths ranging from about 600 to 850 nm. Aluminum, gold, silver, copper and alloys thereof may exhibit a moderately high reflectivity within the above wavelength range. The high reflection layer 20 preferably has a reflectance of at least 70%, more preferably 80%.
    In order to minimize the complexity and cost of the optical data storage system 10, it is preferable that the average read signal levels from each of the data pit patterns 15 and 19 be about the same. The apparent reflectivity from layers 16 and 20 should be approximately the same, as seen by detector 32.
    As used herein, the terms "apparent reflectivity" or "apparent reflectance" are primarily optical readings when focused to a point on the flat area of layer 16 or layer 20. It refers to a fraction of the luminosity incident on the transparent substrate 14, which can be sensed by the photodetector of the device. Assume that the reading device consists of a laser, a properly designed optical path, and a photodetector. Further, assume that the optical element in the optical path closest to the transparent substrate 14 is a high (> 0.4) numerical aperture objective lens. As used herein, the terms “internal surface reflectivity” or “internal surface reflectance” refer to an interface (eg, between the transparent substrate 14 and the partial reflective layer 16) in the reflective media structure. The interface or the fraction of the luminosity incident on the interface between the spacer layer 18 and the high reflection layer 20.
    In order to evaluate the required reflectivity from the partially reflective layer 16, the high reflection layer 20 is made of aluminum that reflects about 80 to 85% of the light incident on the inner surface between the spacer layer 18 and the high reflection layer 20. Suppose it is done. Further assume that the reflectance real component n of the spacer layer 18 is 1.5, and the substrate 14 is a polycarbonate with a real component n of reflectance of 1.57, and reflection at air and substrate interface does not contribute to the read signal. . Further, assuming that the partial reflective layer 16 is an ideal material that exhibits no absorption, the reflectivity of about 0.35 observed on the inner surface between the substrate 14 and the partial reflective layer is determined by the apparent reflectivity from the layers 16 and 20. It can be seen that the balance is brought about. Partial reflective layer 16 that exhibits no absorption is ideal, but substantial partial reflective layer material tends to exhibit some absorption. When choosing a hypothetical partial reflecting layer that absorbs 25% of unreflected light and defines it as the upper limit for acceptable absorption, an internal reflectivity of about 0.25 is required to balance the reflectivity of layers 16 and 20. . Thus, the above examples limit the range for internal reflectivity at the interface between substrate 14 and layer 16 to about 0.25 to 0.35. Considering attenuation due to reflection at the substrate and air interface, the range corresponds to the apparent reflectivity of about 0.24 to 0.33 as seen by the optical reading device.
    Preferred material for the partially reflective layer 16 is gold. Gold is a preferred material because of its low real component of refractive index and environmental stability (see Example 1). However, the disadvantage of using gold is its cost. Applicants have found that it is possible to alloy gold with other less expensive metals to reduce the overall cost of the partially reflective layer. The metal to be alloyed does not have to be environmentally stable like gold (because gold provides environmental stability to the alloy. Secondly, the material to be alloyed is also a low refractive index real component, such as gold). ), The real component of the refractive index must not be virtually elevated by the addition of the element to be alloyed in. Third, the material to be alloyed should be significantly less expensive than gold.
    The metal alloy of the partially reflective layer should contain at least about 10 atomic%, more preferably at least about 15 atomic% and most preferably at least about 20 atomic% gold relative to 100 atomic% alloy.
    The metal alloy preferably has the general formula Au x M y , where 10 <x <90 and 10 <y <90, where M is the second metal. The second metal (M) has a refractive index having a real component (n) and an imaginary component (K), where it is preferably n ≦ 1 and K ≧ 2, as measured at 650 nm, more preferably n ≦ 0.8 And K ≧ 3, most preferably n ≦ 0.65 and K ≧ 3.5. One preferred metal for the second metal (M) is silver. This alloy has the formula Au x Ag y , preferably 10 <x <90 and 10 <y <90, more preferably 15 <x <90 and 10 <y <85, still more preferably 20 <X <80, 20 <y <80, even more preferably 20 <x <60, 40 <y <80, most preferably 20 <x <40 and 60 <y <80.
    In another embodiment, the second metal M may be copper. In a preferred embodiment, this alloy has the general formula Au x Cu y , where 80 <x <90 and 10 <y <20. These ranges ensure the environmental stability of the alloy. It may also be desirable to alloy gold with both silver and copper. Such alloys preferably have the general formula Au x Ag y Cu z , where 20 <x <75, 20 <y <75 and 5 <z <20.
    The partially reflective layer 16 has a thickness in the range of about 8 to 14 nm, more preferably in the range of about 10 to 12 nm. In order to maximize the reflectance R and transmittance T of the partially reflective layer, it is necessary to minimize the absorption A of the layer (because 1 = R + T + A). The absorption of the partially reflective layer is a function of the multiplicative product of the real component (n) and the imaginary component (K) of the refractive index of the layer. To minimize absorption, the product of n · K should be minimized. For metals, K should be minimal because n is large. Partial reflective layer 16, when measured at 650 nm, preferably has n ≦ 1 and K ≧ 2, more preferably n ≦ 0.8 and K ≧ 3, most preferably n ≦ 0.65 and K ≧ 3.5 Has
    The present invention will now be described in more detail with reference to the following non-limiting examples. (All measurements are approximate.)
    Example 1
    Au thin films were prepared by direct current magnetron scattering techniques onto glass slides and polycarbonate discs. The scattering pressure was maintained at 2 mTorr and the deposition rate for Au was 7.8 nm / min. A series of Au films was deposited onto a glass slide to determine the dependence of reflectance / transmittance on film thickness at 650 nm wavelength. This data was also used to derive the complex refractive index of the Au film. Figure 2 shows the dependence of the reflectance and transmittance on the thickness of the film.
    From this data, it was found that the complex refractive index of the Au film was n = 0.29 and K = 3.72 at 650 nm. This refractive index was then used to predict the reflectance and transmittance of the polycarbonate / Au / photopolymer structure that gave a partial reflectance of at least 0.20 and had a transmittance sufficient to obtain a reflectance of 0.20 from the high reflection layer. The predicted thickness was 11 nm. The polycarbonate disc was scattered coated with Au film and then sealed coated with a photopolymer of about 11 μm. Reflectance and transmittance of the disk were measured on a parallel light spectrophotometer. At λ = 650 nm, R was 0.227 and T was 0.685. These values of R and T achieve a desired target of at least 0.20 for reflections from the partially reflective and high reflective layers. The sample disc was then exposed to an environment of 85% relative humidity at 80 ° C. The adhesion of the Au film to the polycarbonate substrate and the photopolymer was excellent. The variation in reflectance and refractive index of the gold partial reflector disk while in this environment is plotted in Table 1 below.
    Environmental Behavior of Au Partial Reflective Layer Daytime at 85% relative humidity at 80 ° CreflectivityTransmittance 00.257 ± 0.0110.618 ± 0.019 One0.259 ± 0.0140.658 ± 0.018 20.267 ± 0.0080.608 ± 0.006
    Within the measurement error, the reflectance and transmittance of the Au film did not decrease over time in an environment of 85% relative humidity at 80 ° C. Therefore, the stability of the Au film under such severe conditions was excellent, indicating that the material for the partial reflector is preferred.
    Example 2
    Ag x Au 100-x films were prepared by co-depositing Ag and Au from individual magnetron generators. This deposition occurred in a vacuum system with a base pressure of 2 × 20 −7 Torr. The scattering pressure was maintained at 2 mTorr and the combined deposition rates from the two sources reached 7-17 nm / min throughout the alloy range. The atomic composition of the alloy film was controlled by varying the deposition rate of the individual sources and was mutually verified by inductively coupled plasma (ICP) composition measurements. An alloy film with a nominal thickness of 9 to 10 nm was deposited onto the glass slide to derive the components n and K of the refractive index from the measurements of the refractive index and the transmittance. The dependence of the real component of the refractive index on the Ag content in the Ag—Au alloy is shown in FIG. 3.
    As can be seen in FIG. 3, the real part n of the refractive index is less than 1.0 for any binary alloy of Ag and Ag. For bicomponent alloys ranging from 10 atomic% Ag to 60 atomic% Ag, the real and imaginary components of the refractive index provide a partial transmittance of at least 0.20 and a sufficient transmittance to obtain an apparent reflectance of at least 0.20 from the high reflection layer. It was used to determine the thickness of the alloy layer in the polycarbonate disc / Ag x Au 100-x / photopolymer structure having. Table 2 shows the optical parameters of the alloy film, the thickness of the alloy layer used to make the disk specimen, and the resulting partial reflector sandwich structure, as measured for an alloy containing Ag in the range of 10 to 60 atomic percent on a spectrophotometer. The reflectance and transmittance of are plotted. The refractive index and reflectance of these disks satisfy the requirement that the partial reflectivity be at least 0.20 with a sufficient transmittance to obtain an apparent reflectance of at least 0.20 from the high reflection layer.
    Ag x Au 100-x Partial Reflector Disc Characteristics for λ = 650 nm alloynKt (nm)RT Ag 10 Au 90 0.364.3490.29 ± 0.020.61 ± 0.03 Ag 20 Au 80 0.384.4290.28 ± 0.020.59 ± 0.02 Ag 30 Au 70 0.394.15100.28 ± 0.010.58 ± 0.02 Ag 40 Au 60 0.384.31100.27 ± 0.010.59 ± 0.01 Ag 50 Au 50 0.454.18100.29 ± 0.010.57 ± 0.02 Ag 60 Au 40 0.334.19100.272 ± 0.0040.56 ± 0.02
    Example 3
    Another example of an alloy having a refractive index of n <1.0 is an Au 100-x Cu x alloy. As in the Ag-Au alloy, Au-Cu alloy films were prepared by co-depositing Au and Cu from individual magnetron scattering sources. The basic pressure of the vacuum system was 2 × 10 −7 Torr and the scattering pressure was maintained at 2 mTorr. The combined deposition rates from the two sources were in the range of 12-18 nm / minute. The atomic composition of the alloy was varied by independently controlling the deposition rates of the Au and Cu sources, and the composition of the selected Au-Cu alloy was mutually verified by ICP measurements. Alloy film specimens were first deposited onto glass slides having a nominal thickness of 10 nm for the determination of the optical properties n and K. The reflectance and transmittance of the alloy film were measured by a spectrophotometer, and from these measurements, the real component (n) and imaginary component (K) of the refractive index were determined at λ = 650 nm. 4 shows the variation of n with respect to atomic% of Cu. The real part n of the refractive index for the Au 100-x Cu x film is less than 1.0 for at least x ≦ 60. Interpolation between the x'60 and x'100 data points causes n to remain below 1.0 and K to be greater than 2.0 in the range. Then, as in the Ag-Au alloy film, the polycarbonate disks / Au 100-x Cu having sufficient transmittance to result in a partial reflectance of at least 0.20 and a reflectance of at least 0.20 from the high reflection layer, as in the Ag-Au alloy film. x / was used to determine the required alloy film thickness in the photopolymer structure.
    Table 3 plots the optical parameters of the alloy as measured on a spectrophotometer, the thickness of the alloy layer, and the reflectance and transmittance of the resulting partial reflector disk. Here, the data indicate that the reflectance and transmittance of these disks with Au-Cu alloy film have a sufficient transmittance to obtain an apparent reflectance of at least 0.20 from the high reflection layer and satisfy the requirement that the partial reflectance is at least 0.20.
    Au 100-x Cu x Partial Reflector Disc Characteristics for λ = 650 nm alloynKt (nm)RT Au 90 Ag 10 0.434.24100.28 ± 0.010.55 ± 0.01 Au 80 Ag 20 0.484.17100.29 ± 0.020.54 ± 0.01 Ag 70 Au 30 0.613.88110.28 ± 0.010.52 ± 0.02 Ag 60 Au 40 0.613.93100.26 ± 0.010.52 ± 0.01 Ag 50 Au 50 0.594.16100.25 ± 0.010.55 ± 0.02 Ag 40 Au 60 0.634.05110.29 ± 0.0010.51 ± 0.02
    权利要求:
    Claims (11)
    [1" claim-type="Currently amended] A transparent substrate 14 having a shape pattern 15 on one main surface thereof,
    Adjacent to the shape pattern and comprising a metal alloy composed of gold, the first metal, and M, the second metal, the second metal having a refractive index with a real component n and an imaginary component K, where n ≦ 1 at 650 nm. And K ≧ 2, wherein the metal alloy has the general formula Au x M y , wherein 10 <x <90 and 10 <y <90;
    Transparent polymer spacer layer 18,
    An optical storage medium (12) comprising a high reflection layer (20) in sequence.
    [2" claim-type="Currently amended] A transparent substrate 14 having a shape pattern 15 on one main surface thereof,
    Adjacent to the shape pattern and comprising a metal alloy composed of gold and silver, the alloy having a refractive index having a real component n and an imaginary component K, where n ≦ 1 and K ≧ 2 at 650 nm; A partial reflective layer 16 having the general formula Au x Ag y wherein 10 <x <90 and 10 <y <90;
    Transparent polymer spacer layer 18,
    An optical storage medium (12) comprising a high reflection layer (20) in sequence.
    [3" claim-type="Currently amended] A transparent substrate 14 having a first data pit pattern 15 on one main surface thereof,
    Adjacent to the first data pit pattern and having a general formula Au x Ag y , wherein the partial reflective layer 16 comprises an alloy of gold and silver with 10 <x <90 and 10 <y <90;
    A second data pit pattern 19 on one main surface, the main surface being provided with a transparent spacer layer 18 provided on one side of a spacer facing the partial reflection layer,
    And a high reflection layer (20) provided adjacent to the second data pit pattern.
    [4" claim-type="Currently amended] A transparent substrate 14 having a first data pit pattern 15 on one main surface, and having a general formula Au x Ag y adjacent to the first data pit pattern, where 15 <x <40 and 60 <y <85 A partially reflective layer 16 comprising an alloy of gold and silver and a transparent polymer spacer layer having a second data pit pattern 19 on one major surface, the major surface being provided on one side of the spacer opposite the partial reflective layer. 18,
    An optical storage medium 12 sequentially comprising a high reflection layer 20 provided adjacent to the second data pit pattern,
    A focal spot laser beam 30 positioned to be incident through the substrate into the disc,
    Means for allowing the beam to be focused on the partially reflective or high reflective layer by adjusting the focal position of the laser beam,
    And a photodetector (32) positioned to detect the reflected laser beam exiting the disk.
    [5" claim-type="Currently amended] The medium or system according to claim 1, 2 or 3, or the system of claim 4, wherein n ≦ 0.65 and K ≧ 3.5.
    [6" claim-type="Currently amended] The medium according to claim 1 or 2, wherein 20 <x <80 and 20 <y <80.
    [7" claim-type="Currently amended] The medium according to claim 1, 2 or 3, wherein 20 <x <40 and 60 <y <80.
    [8" claim-type="Currently amended] The medium of claim 1 wherein the second metal is copper and the metal alloy has the general formula Au x Cu y , wherein 80 <x <90 and 10 <y <20.
    [9" claim-type="Currently amended] The method of claim 1, wherein the second metal is silver and the metal alloy further comprises copper, wherein the metal alloy has the general formula Au x Ag y Cu z , wherein 20 <x <75, 20 <y <75, 5 <z <20. The medium characterized by the above-mentioned.
    [10" claim-type="Currently amended] The medium or system of claim 1, 2 or 3, or the system of claim 4, wherein the spacer layer has a thickness in the range of about 5 to 100 μm.
    [11" claim-type="Currently amended] The medium or system according to claim 1, 2 or 3, or the system of claim 4, wherein the partially reflective layer is between 8 and 14 nm thick.
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    同族专利:
    公开号 | 公开日
    DE69606435D1|2000-03-02|
    DE69606435T2|2000-09-14|
    WO1997022968A1|1997-06-26|
    AU7258896A|1997-07-14|
    JP2000502482A|2000-02-29|
    EP0868720B1|2000-01-26|
    US5640382A|1997-06-17|
    EP0868720A1|1998-10-07|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    法律状态:
    1995-12-19|Priority to US8/574,680
    1995-12-19|Priority to US08/574,680
    1996-10-07|Application filed by 윌리엄 데이비드 바우어, 캐씨 로버타 샘스, 이메이션 콥
    1996-10-07|Priority to PCT/US1996/016046
    2000-11-06|Publication of KR20000064459A
    优先权:
    申请号 | 申请日 | 专利标题
    US8/574,680|1995-12-19|
    US08/574,680|US5640382A|1995-12-19|1995-12-19|Dual layer optical medium having partially reflecting metal alloy layer|
    PCT/US1996/016046|WO1997022968A1|1995-12-19|1996-10-07|Dual layer optical medium having partially reflecting gold alloy layer|
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