EP1145234A1 - Optisches aufzeichnungsmedium vom phasenwechsel-typ und verfahren zur seiner herstellung - Google Patents
Optisches aufzeichnungsmedium vom phasenwechsel-typ und verfahren zur seiner herstellungInfo
- Publication number
- EP1145234A1 EP1145234A1 EP99961386A EP99961386A EP1145234A1 EP 1145234 A1 EP1145234 A1 EP 1145234A1 EP 99961386 A EP99961386 A EP 99961386A EP 99961386 A EP99961386 A EP 99961386A EP 1145234 A1 EP1145234 A1 EP 1145234A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- layer
- optical recording
- phase change
- type optical
- recording medium
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 162
- 238000000034 method Methods 0.000 title claims description 35
- 238000004519 manufacturing process Methods 0.000 title claims description 22
- 239000010410 layer Substances 0.000 claims abstract description 434
- 239000000758 substrate Substances 0.000 claims abstract description 71
- 229910000618 GeSbTe Inorganic materials 0.000 claims abstract description 35
- 229910017629 Sb2Te3 Inorganic materials 0.000 claims abstract description 35
- 229910005900 GeTe Inorganic materials 0.000 claims abstract description 27
- 239000002356 single layer Substances 0.000 claims abstract description 5
- 238000002310 reflectometry Methods 0.000 claims description 99
- 238000002425 crystallisation Methods 0.000 claims description 81
- 238000011282 treatment Methods 0.000 claims description 45
- 239000013078 crystal Substances 0.000 claims description 30
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 20
- 229910052681 coesite Inorganic materials 0.000 claims description 19
- 229910052906 cristobalite Inorganic materials 0.000 claims description 19
- 229910052682 stishovite Inorganic materials 0.000 claims description 19
- 229910052905 tridymite Inorganic materials 0.000 claims description 19
- 238000000151 deposition Methods 0.000 claims description 14
- 229910000765 intermetallic Inorganic materials 0.000 claims description 12
- 230000008021 deposition Effects 0.000 claims description 6
- 229910000838 Al alloy Inorganic materials 0.000 claims description 5
- 229910052581 Si3N4 Inorganic materials 0.000 claims description 3
- 229920005668 polycarbonate resin Polymers 0.000 claims description 2
- 239000004431 polycarbonate resin Substances 0.000 claims description 2
- 238000004544 sputter deposition Methods 0.000 description 30
- 230000008025 crystallization Effects 0.000 description 20
- 229910052984 zinc sulfide Inorganic materials 0.000 description 19
- 229910045601 alloy Inorganic materials 0.000 description 16
- 239000000956 alloy Substances 0.000 description 16
- 230000000052 comparative effect Effects 0.000 description 12
- 238000011156 evaluation Methods 0.000 description 12
- 229910018321 SbTe Inorganic materials 0.000 description 11
- 239000011241 protective layer Substances 0.000 description 11
- 238000010276 construction Methods 0.000 description 9
- 239000000203 mixture Substances 0.000 description 9
- 239000004033 plastic Substances 0.000 description 9
- 238000009826 distribution Methods 0.000 description 6
- 239000004417 polycarbonate Substances 0.000 description 5
- 229920000515 polycarbonate Polymers 0.000 description 5
- 239000007789 gas Substances 0.000 description 4
- 238000001746 injection moulding Methods 0.000 description 4
- 238000001755 magnetron sputter deposition Methods 0.000 description 4
- 239000012790 adhesive layer Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 230000001105 regulatory effect Effects 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 238000000137 annealing Methods 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 239000002131 composite material Substances 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 230000006866 deterioration Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000011835 investigation Methods 0.000 description 2
- 238000001659 ion-beam spectroscopy Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 150000004767 nitrides Chemical class 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 238000001179 sorption measurement Methods 0.000 description 2
- 238000007738 vacuum evaporation Methods 0.000 description 2
- IRPGOXJVTQTAAN-UHFFFAOYSA-N 2,2,3,3,3-pentafluoropropanal Chemical compound FC(F)(F)C(F)(F)C=O IRPGOXJVTQTAAN-UHFFFAOYSA-N 0.000 description 1
- 229910001316 Ag alloy Inorganic materials 0.000 description 1
- KLZUFWVZNOTSEM-UHFFFAOYSA-K Aluminum fluoride Inorganic materials F[Al](F)F KLZUFWVZNOTSEM-UHFFFAOYSA-K 0.000 description 1
- 239000004593 Epoxy Substances 0.000 description 1
- ISWSIDIOOBJBQZ-UHFFFAOYSA-N Phenol Chemical compound OC1=CC=CC=C1 ISWSIDIOOBJBQZ-UHFFFAOYSA-N 0.000 description 1
- NRTOMJZYCJJWKI-UHFFFAOYSA-N Titanium nitride Chemical compound [Ti]#N NRTOMJZYCJJWKI-UHFFFAOYSA-N 0.000 description 1
- 239000005083 Zinc sulfide Substances 0.000 description 1
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 238000010961 commercial manufacture process Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- PMHQVHHXPFUNSP-UHFFFAOYSA-M copper(1+);methylsulfanylmethane;bromide Chemical compound Br[Cu].CSC PMHQVHHXPFUNSP-UHFFFAOYSA-M 0.000 description 1
- 239000012467 final product Substances 0.000 description 1
- 150000002222 fluorine compounds Chemical class 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 229910003437 indium oxide Inorganic materials 0.000 description 1
- PJXISJQVUVHSOJ-UHFFFAOYSA-N indium(iii) oxide Chemical compound [O-2].[O-2].[O-2].[In+3].[In+3] PJXISJQVUVHSOJ-UHFFFAOYSA-N 0.000 description 1
- 230000010365 information processing Effects 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- ORUIBWPALBXDOA-UHFFFAOYSA-L magnesium fluoride Chemical compound [F-].[F-].[Mg+2] ORUIBWPALBXDOA-UHFFFAOYSA-L 0.000 description 1
- 229910001635 magnesium fluoride Inorganic materials 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000001247 metal acetylides Chemical class 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 229920003986 novolac Polymers 0.000 description 1
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 1
- BPUBBGLMJRNUCC-UHFFFAOYSA-N oxygen(2-);tantalum(5+) Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Ta+5].[Ta+5] BPUBBGLMJRNUCC-UHFFFAOYSA-N 0.000 description 1
- 229920005672 polyolefin resin Polymers 0.000 description 1
- 239000000047 product Substances 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 230000002441 reversible effect Effects 0.000 description 1
- 238000012552 review Methods 0.000 description 1
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 229910010271 silicon carbide Inorganic materials 0.000 description 1
- LIVNPJMFVYWSIS-UHFFFAOYSA-N silicon monoxide Chemical compound [Si-]#[O+] LIVNPJMFVYWSIS-UHFFFAOYSA-N 0.000 description 1
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 1
- 229910052814 silicon oxide Inorganic materials 0.000 description 1
- 229910052950 sphalerite Inorganic materials 0.000 description 1
- 150000004763 sulfides Chemical class 0.000 description 1
- 229910001936 tantalum oxide Inorganic materials 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- DRDVZXDWVBGGMH-UHFFFAOYSA-N zinc;sulfide Chemical compound [S-2].[Zn+2] DRDVZXDWVBGGMH-UHFFFAOYSA-N 0.000 description 1
Classifications
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- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
- G11B7/253—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates
- G11B7/2531—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates comprising glass
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
- G11B7/253—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates
- G11B7/2533—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates comprising resins
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
- G11B7/253—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates
- G11B7/2533—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates comprising resins
- G11B7/2534—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of substrates comprising resins polycarbonates [PC]
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
- G11B7/256—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of layers improving adhesion between layers
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording 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
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/252—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers
- G11B7/258—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of reflective layers
- G11B7/2585—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of layers other than recording layers of reflective layers based on aluminium
Definitions
- the present invention relates to a phase change-type optical recording medium in which recording of information is made utilizing phase change by light, and a process for manufacturing the same.
- a phase change-type optical recording medium utilizes, to recording and erasing of information, a reversible structural change or a phase change between amorphous and crystal states or phases of a recording layer derived from difference of thermal history of heating and cooling by light or laser beam application. More specifically, a portion of a recording layer is melted and rapidly cooled to make it amorphous for recording, and is kept at a temperature higher than the crystallization temperature of the recording layer for a certain time period to make it crystalline for erasing. It is estimated that the temperature of the recording layer of GeSbTe, as a typical example, becomes to about 600°C when being recorded and to more than about 170°C when being erased. Reading or reproduction of a signal is done by using a difference of reflectivity between the amorphous and crystal phases.
- the phase change-type optical recording medium has a high information processing speed as well as a high recording capacity.
- the phase change-type optical recording system has an advantage of low cost since the structure of a drive such as an optical head is simpler than a drive for a magneto-optical recording medium.
- the crystal phase of a recording layer is used as the erase state of information, and a high laser power is applied to melt and rapidly cool the- recording layer to make it amorphous and to use the amorphous phase of a recording layer as the record state of information.
- recording layers of phase change- type optical recording media are amorphous as-deposited, i.e., immediately after it is deposited, for example, by sputtering, media including a recording layer are entirely annealed to make the recording layer crystalline, i.e., the erase state.
- the entire annealing is carried out, for example, by application of a laser beam having, for example, a width of 1 - 2 ⁇ m and a length of 100 ⁇ m at about 1 to a recording layer of a recording medium usually with a plurality passes.
- This annealing is called as "initial-crystallization", “post- crystallization”, or simply “initialization”.
- a typical manufacturing process of a phase change-type optical recording medium comprises injection molding of a plastic substrate, sputtering for depositing a stack of layers including a recording layer, optionally coating an organic protective layer on the stack of layers, initial-crystallization, assembling with a casing, inspecting and shipping, in this order.
- Two discs comprising a 0.6 mm-thick substrate and a stack of layers including a recording layer are bonded to each other, when a double-sided recording medium, for example, as of a DVD-RAM disc, is manufactured. In this case, the two discs are usually bonded to each other with an adhesive after an organic protective layer is coated, but the organic protective layer is sometime eliminated.
- a phase change-type optical recording medium has a basic recording layer structure comprising a lower dielectric layer, a recording layer, an upper dielectric layer and a reflective layer, which layers are formed by sputtering or other thin film depositing method.
- "Rapid cooling structure phase change-type optical disc using ZnS-Si0 2 dielectric” shows the structure of a typical phase change- type optical recording medium which is commercially used.
- This structure comprises a polycarbonate substrate (usually a thickness of 0.6 mm or 1.2 mm) /a lower dielectric layer (ZnS # Si0 2 )/a recording layer (GeSbTe)/an upper dielectric layer (ZnS'Si0 2 )/a reflective layer (Al alloy) /an adhesive layer.
- a focused laser beam for initial-crystallization, writing and reading is usually applied to the recording layer through the plastic substrate.
- This type of medium usually has a structure in which the layers are formed on a substrate in the order reversed to the above-mentioned usual order, i.e., in the order of a substrate/a reflective layer/a lower dielectric layer/a recording layer/an upper dielectric layer.
- a proposed structure of an optical head for this type medium is similar to a head of a hard disc that is, a flying head in which an objective lens is mounted on a slider since an objective lens should be very close to the surface of a medium.
- phase change-type optical recording media use a chalcogene alloy such as GeSbTe and AglnSbTe for a recording layer.
- a dielectric layer used comprises a ZnS-based layer such as ZnS » Si0 2 or a nitride-based layer such as GeN.
- a reflective layer used comprises an Al alloy, Au, an Ag alloy, etc.
- the initial-crystallization of a phase change- type optical recording medium is carried out using a specialized initial-crystallization apparatus equipped with a high power optical head emitting a high power laser beam. Specifically, a disc is being rotated while an optical beam focused on the plane of a recording layer is moved in the radial direction to effect the initial- crystallization to the entire surface of a disc.
- This initial-crystallization involves two problems as below:
- An initial-crystallization apparatus is expensive and an initial-crystallization treatment requires a long time period. Usually, an initial- crystallization treatment takes several tens of seconds per disc, typically 40 to 120 seconds, which is significantly longer than a cycle time of injection molding of a plastic substrate and sputtering, each taking about ten and several seconds. As a result, a number of expensive initial-crystallization apparatus are required in one commercial manufacture line for manufacturing phase change-type optical recording media.
- a recording layer tends to have un-uniform crystal state, more specifically un-uniform crystal grain size.
- the initial-crystallization is carried out at a higher power for a higher production rate, the un-uniformity of the crystal grains becomes larger.
- the measurable phenomenon is a variation of reflectivity of a medium or disc in one rotation of a medium, the phenomenon is considered to have a relation with the un-uniform crystal grain size.
- a medium with this type of variation after the initial- crystallization treatment has a large variation in timing of detecting a reproduction signal (large jitter), and has a severe deterioration after repetition of overwrite (increase in jitter), which are critical disadvantages of a recording medium.
- the variation of reflectivity of a medium in a rotation of a medium should be not more than 7%.
- the variation of reflectivity of a medium in a rotation of a medium can be measured by the amplitude of reproduction signals (SUM signal) using an electrical characteristic evaluating apparatus. If the initial-crystallization is carried -out at a lower speed or is repeated at a lower power, a recording layer with excellent initial-crystallization state of uniform crystal grain size can be obtained.
- SUM signal amplitude of reproduction signals
- a phase change-type optical recording medium in which recording of information is made utilizing phase change by light comprising: substrate; a first dielectric layer on said substrate; a phase change-type optical recording layer made of GeSbTe wherein the molar ratio of Sb:Te is less than 0.6 on said first dielectric layer; a second dielectric layer on said phase change-type optical recording layer; and a reflective layer either on the second dielectric layer or between said substrate and said first dielectric layer; wherein an intermediate layer is further disposed between said first dielectric layer and said phase change-type optical recording layer and/or between said phase change-type optical recording layer and said second dielectric layer, said intermediate layer being a single layer of Sb 2 Te 3 or GeTe or a laminate layer ⁇ f Sb 2 Te 3 and GeTe, said intermediate layer being in direct contact with said phase change-type optical recording layer.
- phase change-type optical recording medium according to ( 1 ) , wherein said intermediate layer is disposed between said first dielectric layer and said phase change-type optical recording layer, and said phase change-type optical recording layer is in the as- deposited state without an initial-crystallization treatment.
- phase change-type optical recording medium according to (1) - (3), wherein said phase change-type optical recording medium has not more than 7% of a variation from a median of reflectivity, in a rotation of said medium, when said phase change-type optical recording layer is in the crystal state.
- phase change-type optical recording medium according to (1) - (4), wherein said phase change-type optical recording layer of GeSbTe has an atomic ratio of Ge:Sb:Te of about 1:2:4 or about 2:2:5.
- phase change-type optical recording medium according to (1) - (5), wherein said intermediate layer is a layer of Sb 2 Te 3 .
- phase change-type optical recording medium according to (1) - (6), wherein said intermediate layer is an intermetallic compound layer or a laminated layer of two or more intermetallic compounds.
- phase change-type optical recording medium according to (1) - (7), wherein said recording medium has a first reflectivity for writing and a second reflectivity higher than said first reflectivity for erasing, and said first reflectivity is attained when said phase change-type optical recording layer is amorphous .
- (9) The phase change-type optical recording medium according to (1) - (7), wherein said recording medium has a first reflectivity for writing and a second reflectivity lower than said first reflectivity for erasing, and said first reflectivity is attained when said phase change-type optical recording layer is amorphous .
- phase change-type optical recording medium according to (1) - (9), wherein said first and second dielectric layers are made of at least one selected from the group consisting of Si0 2 , ZnS, Si 3 N 4 , and a combination of Si0 2 and ZnS, and said recording medium further comprises a substrate of a polycarbonate resin and a reflecting layer of an aluminum alloy.
- a process for manufacturing a phase change-type optical recording medium in which recording of information is made utilizing phase change by light comprising the steps of: providing a substrate; forming a first dielectric layer on said substrate; depositing a phase change-type optical recording layer made of GeSbTe wherein the molar ratio of Sb:Te is less than 0.6 on said first dielectric layer; forming a second dielectric layer on said phase change-type optical recording layer; forming a reflective layer either on the second dielectric layer or between said substrate and said first dielectric layer; wherein said process further comprises a step of depositing an intermediate layer between said first dielectric layer and said phase change-type optical recording layer and/or between said phase change-type optical recording layer and said second dielectric layer, said intermediate layer being made in direct contact with said phase change-type optical recording layer, said intermediate layer being a single layer of Sb 2 Te 3 or GeTe or a laminated layer of Sb 2 Te 3 and GeTe.
- R d stands for the reflectivity of said optical recording medium having the phase change-type optical recording layer in the as-deposited state without an initial-crystallization treatment
- R a stands for the reflectivity of said optical recording medium having the phase change-type optical recording layer in the amorphous state used for writing
- R c stands for the reflectivity of said optical recording medium having the phase change-type optical recording layer in the crystal state used for erasing.
- phase change-type optical recording layer of GeSbTe has an atomic ratio of Ge:Sb:Te of about 1:2:4 or about 2:2:5.
- intermediate layer is a layer of Sb 2 Te 3 .
- phase change-type optical recording medium is manufactured in a manufacturing line comprising at least one apparatus for depositing at least said phase change- type optical recording layer and at least one apparatus for initial-crystallization treatment, and said line includes said initial-crystallization treatment apparatus in number equal to or less than said deposition apparatus .
- Figs. 1 to 3 are cross sectional views of examples of a phase change-type optical recording medium according to the present invention.
- Fig. 4 schematically shows the line for manufacturing a phase change-type optical recording" medium.
- phase change-type optical recording medium may have a reflectivity equal or close to that of crystal state of the recording layer without an initial- crystallization treatment or with a short time initial- crystallization treatment.
- initial-crystallization treatment may be eliminated.
- initial-crystallization treatment of a recording layer may be conducted to obtain a uniform initial-crystallization, if necessary or desired, but this treatment is far easier or shorter in comparison with a phase change-type optical recording medium without an intermediate layer of the present invention.
- the phase change-type optical recording medium having the above construction of the present invention does not have disadvantages derived form the additional intermediate layer and may have very high productivity and high quality as a phase change-type optical recording medium.
- both a high quality of a phase change- type optical recording medium and a significantly improved productivity are attained.
- R d stands for the reflectivity of the recording medium having the phase change-type optical recording layer in the as-deposited state without an initial- crystallization treatment
- R a stands for the reflectivity of the recording medium having the phase change-type optical recording layer in the amorphous phase used for writing or recording
- R c stands for the reflectivity of the recording medium having the phase change-type optical recording layer in the crystal state used for erasing.
- the reflectivity of a recording medium having a phase change-type optical recording layer can be controlled to be both higher and lower in a medium having a recording layer of crystal state, than in a medium having a recording layer of amorphous state, by changing the construction of the layers other than the recording layer. In either case, therefore, the relationship of the reflectivity between media having the crystal and amorphous states of a recording layer of the present invention can satisfy the above formula.
- a medium having an as-deposited recording layer without initial-crystallization treatment of the present invention can be used as a ready usable final product supplied to the users, without any initial- crystallization treatment, or with an initial- crystallization treatment which is far shorter in time period and/or uses a lower power than a conventional one.
- a time period of initial-crystallization treatment of a 5-inch medium or disc of not more than 60 second, with a laser beam having a power of 1 W can be attained.
- a medium having a recording layer with or without initial-crystallization treatment of the present invention is advantageous in that the medium can have a variation, in a rotation of the medium, of the reflectivity not more than 7%, more preferably not more than 6%.
- This uniform reflectivity of a medium indicates uniform crystal grain size of a recording layer.
- the phase change-type optical recording layer of the present invention is made of GeSbTe wherein the molar ratio of Sb:Te is less than 0.6, more preferably not more than about 0.5. This phase change-type optical recording material allows to provide excellent performance and characteristics as a phase change-type optical recording medium.
- a phase change-type optical recording medium having the recording layer has a large jitter of reproduction signal since the recorded marks may have undesired shapes.
- preferred GeSbTe are GeSb 2 Te 4 and Ge 2 Sb 2 Te 5 .
- the atomic ratio of Ge:Sb:Te of the above preferred GeSbTe is preferably within ⁇ 5%, more preferably within ⁇ 3% from the stoichiometric ratio of 1:2:4 or 2:2:5. These GeSbTe materials are preferable since they allow a good repeated overwrite characteristic and a high speed erase.
- these materials preferably have a composition of an intermetallic compound of (GeTe) ( Sb 2 Te 3 ) or (GeTe) 2 ( Sb 2 Te 3 ) and have a high affinity with an intermetallic compound of GeTe and Sb 2 Te 3 , which therefore can be more easily crystallized when deposited on an intermediate layer of GeTe or Sb 2 Te 3 .
- the thickness of the phase change-type optical recording layer is preferably in a range of 12 to 50 nm. If it is less than 12 nm, the repetition durability is lowered. If it is more than 50 nm, the recording sensitivity decreases and the signal to noise ratio (S/N ratio) also decreases.
- the intermediate layer of the present invention is a layer of GeTe or Sb 2 Te 3 , or a laminated layer of GeTe and Sb 2 Te 3 .
- the GeTe and Sb 2 Te 3 are advantageous since they do not contain any element other than the constituent elements of GeSbTe and, therefore, they do not disadvantageously change the composition of the recording layer and have affinity with the GeSbTe of the recording layer. Further, since GeTe and Sb 2 Te 3 are intermetallic compounds, they can be easily crystallized when they are deposited or sputtered, by which crystallization of a recording layer of GeSbTe in direct contact with the intermediate layer is accelerated.
- the GeTe or Sb 2 Te 3 of the intermediate layer preferably has a composition equal or close to an intermetallic compound, i.e., preferably within ⁇ 5%, more preferably within ⁇ 3% from the stoichiometric ratio of 1:1 of GeTe or 2:3 of Sb 2 Te 3 .
- the intermediate layer may be a laminated layer of GeTe and Sb 2 Te 3 . It is possible to make the composition of the intermediate layer similar to that of the recording layer by using the laminated layer or a combination of two intermediate layers on and under the recording layer.
- the intermediate layer may be formed between the lower dielectric layer and the recording layer and/or between the recording layer and the upper dielectric layer, with the intermediate layer being in direct contact with the recording layer. It is preferable that an intermediate layer is first formed and the recording layer is then deposited on the intermediate layer, i.e., it is formed between the lower dielectric layer and the recording layer, since in this case the first deposited intermediate layer, which is preferably crystalline at least to some extent, accelerates crystallization of the recording layer when it is deposited.
- initial-crystallization treatment an intermediate layer on the recording layer or between the recording layer and the upper dielectric layer is also effective.
- this initial-crystallization treatment can be shorter in time period or can use a lower power than a conventional case or a medium without an intermediate layer.
- a combination of two intermediate layers formed both on and under the recording layer is regulated to have a specific average composition, for example, the same composition as the recording layer.
- the formation method of the intermediate layer of the present invention is not particularly limited, and includes vacuum evaporation, sputtering, ion beam sputtering, CVD, etc.
- the same process as used for forming the other layers such as the recording layer and dielectric layers is preferred from the viewpoint of continuity of the manufacturing process, and sputtering is particularly preferable from the viewpoints of adhesion with the underlying layer, control of an alloy composition, uniform layer thickness distribution, uniform composition distribution, etc.
- the deposition conditions including deposition rate and sputtering gas pressure may be suitably selected considering the productivity and internal stress of the deposited layer.
- the thickness of the intermediate layer is preferably in a range of 1/40 to 1/4, more preferably 1/20 to 1/5 based on the thickness of the recording layer.
- the thickness of the intermediate layer is less than 1/40 of the thickness of the recording layer, it is not easy to deposit a crystalline intermediate layer by sputtering or other method and therefore the effect of the intermediate layer may not appear. If the thickness of the intermediate layer is more than 1/4 of the thickness of the recording layer, the intermediate layer may possibly be melted and mixed with the recording layer to disadvantageously change the composition of the recording layer, resulting in deterioration of characteristics, such as recording sensitivity, by repeated overwrite.
- the substrate of a medium in the present invention may be any known substrate used for a phase change-type optical recording medium, for example, a transparent substrate of polycarbonate, polyolefin resin or glass.
- a transparent substrate of polycarbonate, polyolefin resin or glass is an injection molded polycarbonate disc having a thickness of about 0.6 to 2.0 mm and a diameter of about 60 to 120 mm.
- the transparency of the substrate is not essential if a laser beam need not pass through the substrate.
- the first and second dielectric layers or lower and upper dielectric layers used in the present invention may be any dielectric layer transparent to a laser used and preferably has heat resistance and a high refractive index.
- oxides, nitrides, sulfides, carbides and fluorides of metals, and composites thereof may be used.
- silicon oxide, indium oxide, tantalum oxide, aluminum oxide, silicon nitride, aluminum nitride, titanium nitride, zinc sulfide, magnesium fluoride, aluminum fluoride, silicon carbide, and composites thereof can be mentioned, although it is not limited to these.
- a transparent dielectric having a refractive index of near 2.1 for example, ZnS*Si0 2 which is obtained by sputtering a mixed target comprising ZnS (e.g., 80 mol%) and Si0 2 (e.g., 20 mol%) in an argon gas.
- the thickness of the dielectric layers is different between the lower and upper dielectric layers and depends on the medium construction and the refractive index.
- the dielectric layer may be formed by a known method including vacuum evaporation, sputtering, ion beam sputtering, CVD, etc. However, it is preferable that all the layers of a recording medium are formed using a same method for the continuity of the manufacturing process.
- the reflective layer used in the preset invention can be disposed on the second or upper dielectric layer or between the substrate and the first or lower dielectric layer, depending on the side of incidence of a laser beam.
- a preferred example of the reflective layer is an Al alloy with a few or several % of Ti or Cr.
- a thin Au layer for example, is used when a medium is to have a construction in which the light adsorption of the crystal phase of the recording layer should be greater than the light adsorption of the amorphous phase of the recording layer.
- An organic protective layer may be optionally provided on the top of the medium.
- any additional layers for example, a heat insulating layer or an adhesive layer, may be included in the medium of the present invention if desired as long as the features and advantages of the present invention are not lost.
- Figs. 1 to 3 show examples of the constructions of a phase change-type optical recording medium of the present invention.
- the medium comprises a transparent substrate 1, and on the substrate 1, a lower dielectric layer 2, an intermediate layer 3, a recording layer 4, an upper dielectric layer 5, a reflective layer 6 and an organic protective layer 7 are deposited in this order.
- a laser beam is incident on the backside of the substrate 1 and focused on the recording layer 4.
- the medium comprises a transparent substrate 1, and on the substrate 1, a heat insulating layer 8, a reflective layer 6', a lower dielectric layer 2, an intermediate layer 3, a recording layer 4, and an upper dielectric layer 5 are deposited in this order.
- a laser beam is incident on the side of the upper dielectric layer 5 and focused on the recording layer 4. This is a layer-side-beam-incident phase-change type optical recording medium.
- the reflectivity of a medium can be controlled by the layer construction such that the medium having a recording layer in the crystal state has a reflectivity higher or lower than the same medium having the same recording layer in the amorphous state. If the reflectivity of a medium having a recording layer in the crystal state is higher than in the amorphous state, this medium is called as "high-to-low type" (from erase state to record state). If the reflectivity of a medium having a recording layer in the crystal phase is lower than in the amorphous phase, this medium is called as "low-to-high type".
- the medium is a double-sided recording medium.
- Two media or discs comprising a transparent substrate 1, a lower dielectric layer 2, an intermediate layer 3, a recording layer 4, an upper dielectric layer 5, a reflective layer 6 and an organic protective layer 7, as shown in Fig. 1, are bonded with each other with an adhesive layer 9 being applied between the two organic protective layers 7.
- the medium of the present invention may be supplied to the users as a ready usable finished product without any initial-crystallization treatment.
- the initial-crystallization treatment of the medium can be effected in a very short time period or with a significantly lower power in comparison with a conventional medium without an intermediate layer, to complete the initial-crystallization. It is noted that in a conventional medium without an intermediate layer, an initial-crystallization treatment is essential and it requires a long time, about 3 minutes for a typical example of a 120 mm disc, and/or repeated treatments.
- the initial-crystallization treatment of the present invention may be effected using a commercially available specific initial-crystallization apparatus. For example, a laser beam having a width of 1 to 2 ⁇ m and a length of about 100 ⁇ m with a power of about 1 Watt is scanned on the recording layer. The scan can be only one pass in the present invention.
- the initial-crystallization treatment is carried out by keeping the recording layer at a temperature higher than the crystallization temperature thereof for a certain time period.
- the time period for the initial-crystallization treatment can be, for example, not more than 60 seconds in the present invention.
- Fig. 4 shows this type of manufacturing line, in which 11 denotes a sputtering apparatus, 12 a coating apparatus and 13 an initial-crystallization apparatus .
- the reflectivity of a medium of the present invention can be measured by a spectrometer or an spin- stand-type electric characteristic evaluation apparatus.
- the amorphous and crystal states or the write and erase states can be easily determined by the reflectivity of the medium.
- the crystal and amorphous states can be determined by the reflectivity at a single wavelength, but it can be more easily and surely determined by the pattern of distribution of the reflectivity depending on the wavelength.
- the variation of the reflectivity of a medium, " in a rotation of a medium can be determined using an electric characteristic evaluation apparatus having an optical head to measure the variation of the amount of the laser light returned from the medium when a reading or reproducing laser beam is applied and the medium is rotated.
- Example 1 and Comparative Example 1 On one surface of a plastic substrate having a thickness of 1.2 mm, a lower dielectric layer, an intermediate layer, a recording layer, an upper dielectric layer, a reflective layer and an organic protective layer in this order were formed to manufacture a phase change-type optical recording medium of Example 1.
- a recording medium of Comparative Example 1 a phase change-type optical recording medium without an intermediate layer was manufactured which had a construction comprising, on one surface of a plastic substrate having a thickness of 1.2 mm, a lower dielectric layer, a recording layer, an upper dielectric layer, a reflective layer and an organic protective layer in this order.
- Two kinds of plastic substrates of a polycarbonate disc having a diameter of 120 mm and an inner diameter of 15 mm were used for each of Example 1 and Comparative Example 1.
- One of the two substrates was a substrate having a plane surface for measuring the reflectivity of the medium by a spectrometer.
- the other one of the two substrates was a substrate produced by injection molding to provide continuous servo spiral grooves in an area having radius of 24 to 58 mm, for measuring the distribution of the reflectivity by an electric characteristic evaluation apparatus.
- the depth of the groove was 70 nm
- the track pitch was 1.48 ⁇ m
- the widths of the groove and land were about 0.74 ⁇ m.
- the recording layer was a 20 nm thick GeSbTe alloy layer and the intermediate layer was eliminated.
- the lower and upper dielectric layers were a
- the sputtering apparatus used was a magnetron sputtering apparatus (ANELVA SPF-430H type) in which the holder for a substrate was modified so as to set a plurality of substrates thereto.
- This apparatus allowed three targets to be set in a vacuum chamber to sputter three kinds of layers in the row.
- the target exchange was effected, after the 95 nm-thick lower dielectric layer, the 2 nm-thick intermediate layer, the 18 nm-thick GeSbTe recording layer and the 16 nm-thick upper dielectric layer were deposited sequentially.
- the two substrates were set in the vacuum chamber, which was evacuated to 8 x 10 ⁇ s Pa and an Ar gas was introduced at a flow rate of 75 SCCM and the orifice of a main valve was regulated to attain a pressure of 0.8 Pa.
- the targets used were a GeSbTe alloy, a ZnS « Si0 2 sintered body, a SbTe alloy, and the AlCr alloy, each target having a diameter of 101 mm and a thickness of 5 mm.
- the substrate was set in a plane above the target at a distance of about 120 mm and the substrate, while being self-rotated, was further rotated around a center located on the central axis of the target at a radius of 100 mm.
- the powers applied were a 500W radio frequency power for sputtering the ZnS*SiO, sintered body, a 400W direct current power for sputtering the AlCr target, and a 50W direct current power for sputtering the SbTe and GeSbTe targets.
- the deposition rates were 23.3 nm/min for the ZnS # Si0 2 layer, 10.2 nm/min for the AlCr layer, 21.1 nm/min for the SbTe layer, and 20.5 nm/min for the GeSbTe layer.
- a ultra-violet curable phenol novolak epoxy aerylate resin was coated and cured by irradiation with UV rays to obtain a phase change-type optical recording medium having an organic protective layer.
- the medium of Example 1 had a reflectivity of 35% at a wavelength of 680 nm, immediately after the sputtering was completed, i.e., at the stage of removal of the medium or the substrate with the deposited layers from the vacuum chamber. It was also confirmed by the distribution of the reflectivity on the wavelength that the recording layer was crystalline.
- the medium of Comparative Example 1 had a low reflectivity of 6% and the recording layer was amorphous when the medium was removed from the vacuum chamber, and the reflectivity of the medium increased to 35% by initial-crystallization treatment. The measurement of the reflectivity was carried out at a location with a radius of 35 mm of the medium. The reflectivity was measured by an optical fiber-type spectrometer (Device name: Photal, manufactured by Hodaka electronics).
- the initial-crystallization apparatus was a bulk eraser apparatus (LK101A type, manufactured by Shibasoku).
- the optical head used emitted a laser beam having a power of about IW on the surface of the disc, a wavelength of 810 nm, an NA (numerical aperture of objective lens) of 0.34 and a spot size of 125 ⁇ m (long axis) x 1.27 ⁇ m (short axis), and was set to have the long axis at an angle of 30° inclined from the radial direction of the disc.
- the initial-crystallization treatment was effected by rotating the disc at a constant linear speed of 5 m/sec and moving the optical head at a feed speed of 86 ⁇ m/rotation (i.e., the optical head moves 86 ⁇ m per one rotation of the disc), while the power was set to 65% (i.e., about 650 mW) of the maximum power.
- the scan was only one pass on the disc.
- the variation of the reflectivity of the grooved medium was evaluated on a circle with a radius of 35 mm.
- the evaluation was made by an electric characteristic evaluation apparatus (DDU-1000 type, manufactured by Pulstech Industries).
- the variation of the reflectivity was determined by measuring, with an osciloscope, the reflectivity of a medium for one circle.
- the variation of the reflectivity of the medium of Example 1 was 6% from the median reflectivity but that of Comparative Example 1 was 12%, disadvantageously exceeding the reference value of 7%.
- the media as shown in Table 1 were manufactured.
- the substrate, the method for manufacturing the medium, the thicknesses of the layers, and the methods for evaluation were the same as in Example 1.
- ⁇ represents
- the difference of the reflectivity between before and after the initial- crystallization was low, only 3 to 12%.
- Example 7 A layer-side-beam-incident phase-change type optical recording medium of Example 7 was manufactured with a construction of a heat insulating layer, a reflective layer, a lower dielectric layer, an intermediate layer, a recording layer and an upper dielectric layer in this order on a plastic substrate 1.2 mm thick.
- a layer-side- beam-incident phase-change type optical recording medium of Comparative Example 2 did not have an intermediate layer, that is, the construction comprised a heat insulating layer, a reflective layer, a lower dielectric layer, a recording layer and an upper dielectric layer in this order on a plastic substrate 1.2 mm thick.
- Two kinds of plastic substrates of a polycarbonate disc having a diameter of 120 mm and an inner diameter of 15 mm were used for each of Example 7 and Comparative Example 2.
- One of the two substrates was a substrate having a plane surface for measuring the reflectivity of the medium by a spectrometer.
- the other one of the two substrates was a substrate produced by injection molding to provide continuous servo spiral grooves in an area having a radius of 24 to 58 mm, for measuring the reflectivity by an electric characteristic evaluation apparatus.
- the depth of the groove was 70 nm
- the track pitch was 1.10 ⁇ m
- the widths of the groove and land were about 0.55 ⁇ m.
- the 100 nm thick heat insulating layer, the 150 nm thick reflective layer, the 20 nm thick lower dielectric layer, the 2 nm thick intermediate layer (only in Example 7), the 18 nm thick recording layer of GeSbTe, and the 95 nm thick upper dielectric layer were formed in this order.
- the recording layer was a 20 nm thick GeSbTe alloy layer and the intermediate layer was eliminated.
- the sputtering apparatus used was a magnetron sputtering apparatus (ANELVA SPF-430H type) in which the holder for a substrate was modified so as to set a plurality of substrates thereto.
- This apparatus allowed three targets to be set in a vacuum chamber to sputter three kinds of layers sequentially.
- the target exchange was effected to further deposit the 20 nm thick lower dielectric layer, the 2 nm-thick SbTe intermediate layer, the 18 nm-thick GeSbTe recording layer and the 95 nm-thick upper dielectric layer sequentially.
- the two substrates were set in the vacuum chamber, which was evacuated to 8 x 10 "5 Pa and an Ar gas was introduced at a flow rate of 75 SCCM and the orifice of a main valve was regulated to attain a pressure of 0.8 Pa.
- the targets used were a GeSbTe alloy, a ZnS*Si0 2 sintered body, a SbTe alloy, and an AlCr alloy, each target having a diameter of 101 mm and a thickness of 5 mm.
- the substrate was set in a plane above the target at a distance of about 120 mm from the target surface and the substrate, while being self-rotated, was further rotated around a center located on the axis passing through the center of the target at a radius of 100 mm.
- the powers applied were a 500W radio frequency power for sputtering the ZnS # Si0 2 sintered body, a 400W direct current power for sputtering the AlCr target, and a 50W direct current power for sputtering the SbTe and GeSbTe targets.
- the deposition rates were 23.3 nm/min for the ZnS » Si0 2 layer, 10.2 nm/min for the AlCr layer,
- the medium of Example 7 had a reflectivity of 39% at a wavelength of 680 nm, immediately after the sputtering was completed, i.e., at the stage of removal of the medium or the substrate with the deposited layers from the vacuum chamber. It was also confirmed by the distribution of the reflectivity on the wavelength that the recording layer was crystalline.
- the medium of Comparative Example 2 had a low reflectivity of 11% and the recording layer was amorphous when the median was removed from the vacuum chamber, but the reflectivity of the medium increased to 38% by conventional initial- crystallization treatment.
- the measurement of the reflectivity was carried out at a location with a radius of 35 mm of the medium.
- the reflectivity was measured by an optical fiber-type spectrometer (Device name: Photal, manufactured by Hodaka electronics).
- the initial-crystallization apparatus was a bulk eraser apparatus (LK101A type, manufactured by Shibasoku) .
- the optical head used emitted a laser beam having a power of about IW on the surface of the disc, a wavelength of 810 nm, an NA (numerical aperture of objective lens) of 0.34 and a spot size of 125 ⁇ m (long axis) x 1.27 ⁇ m (short axis), and was set to have the longitudinal axis at an angle of 30° inclined from the radial direction of the disc.
- the initial- crystallization treatment was effected by rotating the disc at a constant linear speed of 5 m/sec and moving the optical head at a feed speed of 86 ⁇ m/rotation (i.e., the optical head moves 86 ⁇ m per one rotation of the disc), while the power was set to 65% of the maximum power, i.e., about 650 mW.
- the scan of the laser beam in this Example was one pass on the disc in contrast to a plurality of passes in the conventional initial- crystallization treatment.
- the variation of the reflectivity of the grooved medium was evaluated on a circle with a radius of 35 mm.
- the evaluation was made by an electric characteristic evaluation apparatus (DDU-1000 type, manufactured by Pulstech Industries).
- the variation of the reflectivity was determined by measuring the reflectivity of a medium for one circle.
- the variation of the reflectivity of the medium of Example 7 was 5% from the median reflectivity but that of Comparative Example 2 was 11%, disadvantageously exceeding the reference value of 7%. It was confirmed that the manufacturing process, specifically the initial-crystallization process, can be shortened and that the recording medium had excellent performance in accordance with the present invention. (Examples 8 to 12)
- the media as shown in Table 2 were manufactured.
- the substrate, the method for manufacturing the medium, the thicknesses of the layers, and the methods for evaluation were the same as in Example 7.
- ⁇ represents
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- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Chemical & Material Sciences (AREA)
- Inorganic Chemistry (AREA)
- Optical Record Carriers And Manufacture Thereof (AREA)
- Thermal Transfer Or Thermal Recording In General (AREA)
- Manufacturing Optical Record Carriers (AREA)
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
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JP36981098 | 1998-12-25 | ||
JP10369810A JP2000195110A (ja) | 1998-12-25 | 1998-12-25 | 相変化型光記録媒体の製造方法 |
PCT/JP1999/007300 WO2000039794A1 (en) | 1998-12-25 | 1999-12-24 | Phase change-type optical recording medium and process for manufacturing the same |
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EP1145234A1 true EP1145234A1 (de) | 2001-10-17 |
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Application Number | Title | Priority Date | Filing Date |
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EP99961386A Withdrawn EP1145234A1 (de) | 1998-12-25 | 1999-12-24 | Optisches aufzeichnungsmedium vom phasenwechsel-typ und verfahren zur seiner herstellung |
Country Status (8)
Country | Link |
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EP (1) | EP1145234A1 (de) |
JP (1) | JP2000195110A (de) |
KR (1) | KR20010099945A (de) |
CN (1) | CN1338099A (de) |
AU (1) | AU1801200A (de) |
CA (1) | CA2355654A1 (de) |
TW (1) | TW459224B (de) |
WO (1) | WO2000039794A1 (de) |
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Publication number | Priority date | Publication date | Assignee | Title |
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TWI246681B (en) * | 2000-12-15 | 2006-01-01 | Koninkl Philips Electronics Nv | Optical information medium and its use |
EP1293975A3 (de) * | 2001-09-13 | 2007-02-14 | TDK Corporation | Verfahren und Vorrichtung zur Herstellung von optischen Aufzeichnungsmedien |
CN101339783B (zh) * | 2003-02-19 | 2011-01-12 | 日本胜利株式会社 | 光记录方法、光记录媒体、光记录媒体记录装置、光记录装置、光盘、光盘记录再现装置 |
Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
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JPS63317939A (ja) * | 1987-06-22 | 1988-12-26 | Asahi Chem Ind Co Ltd | 光情報記録媒体 |
JPH01298545A (ja) * | 1988-05-26 | 1989-12-01 | Nippon Columbia Co Ltd | 円盤型光情報記録媒体及びその製造方法 |
JPH0825338B2 (ja) * | 1988-06-22 | 1996-03-13 | 松下電器産業株式会社 | 光学情報記録再生消去部材の記録再生消去方法 |
JPH0652578A (ja) * | 1992-07-28 | 1994-02-25 | Nippondenso Co Ltd | 光情報記録媒体 |
JPH07141693A (ja) * | 1993-09-22 | 1995-06-02 | Toshiba Corp | 情報記録媒体 |
JP3810462B2 (ja) * | 1995-12-13 | 2006-08-16 | 三菱化学メディア株式会社 | 光学的情報記録用媒体 |
DE69816073T2 (de) * | 1997-04-16 | 2004-05-19 | Asahi Kasei Kabushiki Kaisha | Verfahren zur herstellung eines optischen informationsaufzeichnungsmediums, und durch das verfahren hergestelltes optisches informationsaufzeichnungsmedium |
-
1998
- 1998-12-25 JP JP10369810A patent/JP2000195110A/ja active Pending
-
1999
- 1999-12-23 TW TW088122809A patent/TW459224B/zh not_active IP Right Cessation
- 1999-12-24 KR KR1020017008105A patent/KR20010099945A/ko not_active Application Discontinuation
- 1999-12-24 CA CA002355654A patent/CA2355654A1/en not_active Abandoned
- 1999-12-24 CN CN99816371A patent/CN1338099A/zh active Pending
- 1999-12-24 AU AU18012/00A patent/AU1801200A/en not_active Abandoned
- 1999-12-24 EP EP99961386A patent/EP1145234A1/de not_active Withdrawn
- 1999-12-24 WO PCT/JP1999/007300 patent/WO2000039794A1/en not_active Application Discontinuation
Non-Patent Citations (1)
Title |
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See references of WO0039794A1 * |
Also Published As
Publication number | Publication date |
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WO2000039794A1 (en) | 2000-07-06 |
KR20010099945A (ko) | 2001-11-09 |
TW459224B (en) | 2001-10-11 |
AU1801200A (en) | 2000-07-31 |
CA2355654A1 (en) | 2000-07-06 |
JP2000195110A (ja) | 2000-07-14 |
CN1338099A (zh) | 2002-02-27 |
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