KR100225108B1 - Optic-magneto recording medium - Google Patents

Optic-magneto recording medium Download PDF

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KR100225108B1
KR100225108B1 KR1019950001801A KR19950001801A KR100225108B1 KR 100225108 B1 KR100225108 B1 KR 100225108B1 KR 1019950001801 A KR1019950001801 A KR 1019950001801A KR 19950001801 A KR19950001801 A KR 19950001801A KR 100225108 B1 KR100225108 B1 KR 100225108B1
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South Korea
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recording
film
magneto
layer
recording medium
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KR1019950001801A
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Korean (ko)
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KR960030150A (en
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안용진
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윤종용
삼성전자주식회사
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    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10584Record carriers characterised by the selection of the material or by the structure or form characterised by the form, e.g. comprising mechanical protection elements
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10586Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material

Abstract

본 발명은 단파장용 광자기 디스크에 관한 것으로서, 좀 더 상세하게는 기판상에 유전체막, 기록막, 절연막, 및 반사막이 순차적으로 적층된 광자기 기록매체에 있어서, 상기 기록막을 NdTbFeCo로 구성된 재생층 및 희토류-리치 타입의 TbFeCoCr로 구성된 기록층으로 형성시켜 기록재생 싸이클 반복후에도 기록재생특성 및 보자력의 감소가 거의 나타나지 않으며, 기록자구의 크기에 있어서도 거의 변화가 없는 광자기기록 매체에 관한 것이다.The present invention relates to a short-wavelength magneto-optical disk, and more particularly, to a magneto-optical recording medium in which a dielectric film, a recording film, an insulating film, and a reflective film are sequentially stacked on a substrate, wherein the recording film is made of NdTbFeCo. And a rare earth-rich type recording layer composed of TbFeCoCr, which shows little decrease in recording / reproducing characteristics and coerciveness even after repeated recording / reproducing cycles, and almost no change in the size of the recording domain.

Description

단파장용 광자기 기록 매체Short wavelength magneto-optical recording media

제1도는 종래의 광자기 기록 매체를 개략적으로 도시한 단면도.1 is a sectional view schematically showing a conventional magneto-optical recording medium.

제2도는 본 발명에 따른 광자기 기록 매체를 개략적으로 도시한 단면도.2 is a sectional view schematically showing a magneto-optical recording medium according to the present invention.

제3도는 본 발명 및 종래의 기술에 따른 광자기 기록 매체의 기록/소거 싸이클에 대한 기록파워의 변화를 나타낸 그래프.3 is a graph showing a change in recording power for a recording / erase cycle of a magneto-optical recording medium according to the present invention and the prior art.

제4도는 본 발명 및 종래의 기술에 따른 광자기 기록 매체의 기록/소거 싸이클에 대한 기록재생특성의 변화를 나타낸 그래프.4 is a graph showing the change of recording / playback characteristics with respect to the recording / erasing cycle of the magneto-optical recording medium according to the present invention and the related art.

제5도는 본 발명 및 종래의 기술에 따른 광자기 기록 매체의 기록/소거 싸이클에 대한 캐리어 레벨(carrier level)의 변화를 나타낸 그래프.5 is a graph showing a change in carrier level for a recording / erasing cycle of a magneto-optical recording medium according to the present invention and the prior art.

* 도면의 주요부분에 대한 부호의 설명* Explanation of symbols for main parts of the drawings

1, 11 : 기판 2, 12 : 유전체막1, 11 substrate 2, 12 dielectric film

3, 13 : 기록막 4, 14 : 절연막3, 13: recording film 4, 14: insulating film

5, 15 : 반사막 16 : 재생층5, 15: reflective film 16: reproduction layer

17 : 기록층17: recording layer

본 발명은 단파장용 광자기 기록 매체에 관한 것으로서, 좀 더 상세하게는 기판상에 유전체막, 기록막, 절연막 및 반사막이 순차적으로 적층된 구조를 가지는 광자기 기록 매체에 있어서, 상기 기록막을 기록층과 재생층으로 형성시키고, 상기 기록층을 희토류-리치 타입(RE-rich type)으로 형성시켜 단파장 레이저 영역에서 기록재생 싸이클 반복후에도 기록재생특성 및 보자력의 감소가 거의 나타나지 않으며, 기록자구의 크기에 있어서도 거의 변화가 없는 광자기 기록 매체에 관한 것이다. 이하 본 발명에 사용된 용어 광자기 기록 매체 는 광자기 디스크 와 동일한 의미로 혼용하여 사용한다.The present invention relates to a short-wavelength magneto-optical recording medium, and more particularly, to a magneto-optical recording medium having a structure in which a dielectric film, a recording film, an insulating film, and a reflective film are sequentially stacked on a substrate, wherein the recording film is a recording layer. And a recording layer formed of a rare-earth type (RE-rich type), the recording and reproducing characteristics and the coercivity are hardly reduced even after repeating the recording and reproducing cycle in the short wavelength laser region. The present invention relates to a magneto-optical recording medium having almost no change. Hereinafter, the term magneto-optical recording medium used in the present invention is used interchangeably with the same meaning as the magneto-optical disk.

일반적으로 광자기 디스크의 기록막은 희토류 원소와 천이원소가 합금된 박막으로 형성되며, 희토류 원소와 천이원소의 부격자의 자화값의 차가 되는 페리(Ferri) 자성체이다. 기록막에서 천이원소의 자화가 우세한 박막을 천이금속-리치(TM-rich) 기록막, 희토류 원소의 자화가 우세한 경우를 희토류-리치(RE-rich)기록막이라 한다.In general, a recording film of a magneto-optical disk is formed of a thin film in which rare earth elements and transition elements are alloyed, and is a Ferri magnetic material which is a difference between the magnetization values of the sublattices of the rare earth elements and transition elements. The thin film in which the magnetization of the transition element predominates in the recording film is called the transition metal-rich (TM-rich) recording film, and the case in which the magnetization of the rare earth element is superior is called a rare-earth (RE-rich) recording film.

일반적으로 광자기 디스크에 정보를 기록하는 원리는 열자기적 특성을 이용하며, 정보의 재생은 자기광학 특성을 이용한다.In general, the principle of recording information on a magneto-optical disk uses thermomagnetic characteristics, and the reproduction of information uses magneto-optical characteristics.

광자기 디스크에 정보를 기록하는 원리는 기판에 수직자화막을 형성시켜, 기록막에 레이저광이 조사될 때 기록막의 수직방향에 대해 평행 또는 반평행하게 자구(magnetic domain)를 형성시켜 정보를 기록, 재생 및 소거하는 기술이다. 즉, 광자기 기록막에 집적된 레이저광이 조사된 국부적으로 큐리온도 이상으로 온도가 상승되어 자화를 잃게 되고 외부자계가 인가되면 레이저광이 조사된 부분의 자화가 외부자계와 같은 방향으로 자구를 형성시키므로서 정보의 기록이 가능하다. 또한, 정보의 재생은 커-효과(kerr effect)를 이용하는데, 이는 입사된 레이저광이 기록막에서 반사될 때, 편광면의 회전이 기록막의 자화상태에 따라 다르게 된다. 즉, 자화가 기록막의 상방향으로 되어 있을때 편광면이 +θk 회전한다고 하면, 자화가 하방향으로 되어 있는 경우에 편광면이-θk 회전하게 되는데, 자화의 방향에 따라서 반사된 레이저광은 서로 2θk의 편광면이 회전하게 된다. 이 차이를 광 검출기에서 전기적 신호를 재생하는 것이 광자기 디스크의 재생원리이다.The principle of recording information on a magneto-optical disk is to form a vertical magnetization film on a substrate, and to record information by forming a magnetic domain parallel or antiparallel to the vertical direction of the recording film when laser light is irradiated onto the recording film. It is a technique for reproducing and erasing. In other words, when the laser beam integrated on the magneto-optical recording film is irradiated locally, the temperature is raised above the Curie temperature, and the magnetization is lost. It is possible to record information by forming. Also, the reproduction of information uses a Kerr effect, which is that when the incident laser light is reflected on the recording film, the rotation of the polarization plane varies depending on the magnetization state of the recording film. That is, if the polarization plane is rotated + θk when the magnetization is in the upper direction of the recording film, the polarization plane is rotated by -θk when the magnetization is in the downward direction, and the laser beams reflected along the direction of magnetization are 2θk from each other. The polarization plane of is rotated. Reproducing this difference in the photodetector is the principle of reproduction of the magneto-optical disk.

한편, 광자기 디스크는, 제1도에 도시된 바와 같이, 외경이 130㎜(또는 90㎜)이고, 홈(groove)이 1.6㎛ 간격으로 형성된 기판(1)상에 유전체막(2)/기록막(3)/절연막(4)/반사막(5)을 스퍼터링(sputtering)방식으로 순차적으로 적층시켜 제조하며, 기록용량이 10E8 BYTE/㎠으로 기억용량이 매우 높다.On the other hand, the magneto-optical disk, as shown in FIG. 1, has a dielectric film 2 / recorded on a substrate 1 having an outer diameter of 130 mm (or 90 mm) and grooves formed at intervals of 1.6 mu m. The film 3 / insulation film 4 / reflection film 5 are sequentially stacked by sputtering, and the recording capacity is 10E8 BYTE / cm 2, which is very high.

그러나, 종래의 광자기 디스크는 TbFeCo를 기록막(3)으로 사용하여 VKWKD 830㎚(또는 780㎚)의 레이저 다이오드를 광원으로 사용하여 기록, 재생할때 기록막(3) TbFeCo는 커회전각이 약 0.3deg 정도이나, 파장이 감소함에 커회전각이 감소하여 파장이 절반인 415㎚이하가 되면 0.2deg이하가 되어 기록, 재생특성이 현저하게 감소되는 문제점이 있었다.However, in the conventional magneto-optical disk, the recording film 3 TbFeCo has a large rotation angle when recording and reproducing using the TbFeCo as the recording film 3 and using the laser diode of VKWKD 830 nm (or 780 nm) as the light source. However, when the wavelength is reduced, the rotation angle decreases as the wavelength decreases. When the wavelength is less than 415 nm, which is half the wavelength, the recording and reproduction characteristics are significantly reduced.

따라서, 본 발명은 상술한 문제점을 해결하기 위한 것으로서, 기록막을 기록층 및 재생층으로 형성시킴에 따라 단파장에서 커회전각이 커서 기록 및 기록재생특성이 우수한 광자기 디스크를 제공하는데 그 목적이 있다.Accordingly, an object of the present invention is to provide a magneto-optical disk having excellent recording and recording / reproducing characteristics due to a large rotation angle at a short wavelength as the recording film is formed of a recording layer and a reproduction layer. .

상기의 목적을 달성하기 위한 본 발명의 광자기 기록 매체는 기판상에 유전체막, 기록막, 절연막, 및 반사막이 순차적으로 적층된 광자기 기록매체에 있어서, 상기 기록막을 NdTbFeCo로 구성된 재생층 및 희토류-리치 타입의 TbFeCoCr로 구성된 기록층으로 형성시킨 것으로 이루어진다.The magneto-optical recording medium of the present invention for achieving the above object is a magneto-optical recording medium in which a dielectric film, a recording film, an insulating film, and a reflective film are sequentially stacked on a substrate, wherein the recording film is a reproduction layer and rare earth composed of NdTbFeCo. -Made of a recording layer composed of a rich type TbFeCoCr.

이하, 본 발명의 구성을 첨부한 도면을 참조하여 좀 더 구체적으로 살펴보면 다음과 같다.Hereinafter, the configuration of the present invention will be described in more detail with reference to the accompanying drawings.

광자기 디스크에 있어서, 데이타 전송속도의 고속화 및 고밀도화가 과제이며 미국, 일본 및 유럽에서 이의 연구가 활발히 진행되고 있다. 광자기 디스크의 고밀도를 이루기 위해서는 짧은 레이저 파장을 사용하여야 하며, 단파장에서 커회전각이 커서 기록 및 재생특성이 우수하여야 한다.Background Art In the magneto-optical disk, high data transfer speeds and high density are the subjects, and researches are actively conducted in the US, Japan, and Europe. In order to achieve high density of magneto-optical disk, short laser wavelength should be used, and it should be excellent in recording and reproducing characteristics because of large rotation angle at short wavelength.

따라서, 본 발명의 광자기 기록 매체는 상술한 조건을 만족시키기 위하여, 제2도에 도시된 바와 같이, 기판(11)상에 유전체막(12), 재생층(16) 및 기록층(17)으로 구성된 기록막(13), 절연막(14) 및 반사막(15)이 순차적으로 적층된 구조를 갖는다.Therefore, the magneto-optical recording medium of the present invention has a dielectric film 12, a reproduction layer 16 and a recording layer 17 on the substrate 11, as shown in FIG. The recording film 13, the insulating film 14, and the reflective film 15 constituted of the above structure are sequentially stacked.

본 발명에 따르면, 상기 기판(11)은 상기 기판(11)은 광자기 디스크의 제조에 통상적으로 사용되는 것을 모두 사용할 수 있다. 상기 유전체막(12)은 SiN으로 이루어지며, 그 두께는 500∼650Å이며, 기록층(17)은 희토류-리치 타입의TbFeCoCr을 사용하는데, 그 두께는 130∼200Å이 바람직하다. 또한 본 발명에 사용되는 절연막(14)은 SiN으로 두께는 200∼400Å이며, 반사막(15)은 AlTi로 두께 약 400-600Å이며, 반사막(15)은 AlTi로 두께 약 400-600Å으로 이루어진다. 이때, 상기 재생층(16) 및 기록층(17)의 두께가 80Å이하이면 광자기 특성이 열화되고, 200Å이상이면 기록감도가 나빠진다.According to the present invention, the substrate 11 may be any substrate that is commonly used in the manufacture of magneto-optical disks. The dielectric film 12 is made of SiN, and its thickness is 500 to 650 Å. The recording layer 17 uses rare earth-rich type TbFeCoCr, whose thickness is preferably 130 to 200 Å. In addition, the insulating film 14 used in the present invention is SiN, 200-400 GPa thick, the reflecting film 15 is AlTi approximately 400-600 GPa, and the reflective film 15 is AlTi, approximately 400-600 GPa. At this time, when the thickness of the reproduction layer 16 and the recording layer 17 is 80 kPa or less, the magneto-optical characteristic deteriorates, and when the thickness of the reproduction layer 16 and the recording layer 17 is 200 kPa or more, the recording sensitivity becomes worse.

또한, 본 발명의 기록막(13)은 기록을 담당하며 높은 보자력 값을 가지는 기록층(17)과, 높은 커회전각을 갖는 재생층(16)의 2층막으로 구성되며, 재생층은 NdXTby(Fe100-ZCoZ)100-x-y, 20≤x≤27, 13≤y≤18, 10≤z≤30등을 사용하고, 기록층으로는 희토류-리치 타입의 TbaCrb(Fe100-CCoC)100-a-b, 26≤a≤32, 3≤b≤8, 10≤c≤30을 사용하는 것이 바람직하다. 이때, 재생층 NdXTby(Fe100-ZCoZ)100-x-y에서 이의 함량인 x가 27보다 클 경우에는 원하는 수직자화값을 갖는 기록막의 형성이 용이하지 않으며, z가 30보다 클 경우에는 큐리온도가 상승되어서 정보의 기록시 높은 기록파워가 필요되므로 기록감도가 나빠진다. 또한, 기록층 TbaCrb(Fe100-CCoC)100-a-b에서 Tb의 함량인 b가 8보다 클 경우 기록막의 보자력이 4koe가 되므로 기록층으로서 필요한 보자력보다 감소되어 수직자기이방성 특성이 감소된다.In addition, the recording film 13 of the present invention is composed of a recording layer 17 which is responsible for recording and has a high coercivity value, and a two-layer film of a reproduction layer 16 having a high Kerr rotation angle, and the reproduction layer is Nd X. Tb y (Fe 100-Z Co Z ) 100-xy , 20 ≦ x ≦ 27, 13 ≦ y ≦ 18, 10 ≦ z ≦ 30, etc., and a rare earth-rich type of Tb a Cr b ( Fe 100-C Co C ) 100-ab , 26 ≦ a ≦ 32, 3 ≦ b ≦ 8, 10 ≦ c ≦ 30, preferably used. At this time, in the reproduction layer Nd X Tb y (Fe 100-Z Co Z ) 100-xy , when its content x is larger than 27, formation of a recording film having a desired vertical magnetization value is not easy, and when z is larger than 30 In this case, the Curie temperature is increased so that high recording power is required for recording information, resulting in poor recording sensitivity. Further, the recording layer Tb a Cr b (Fe 100- C Co C) is large when the recording film coercive force than that of the content of Tb in the 100-ab b 8 is lower than 4koe coercive force is therefore needed as the recording layer perpendicular magnetic anisotropy properties Is reduced.

한편, 본 발명의 단파장용 광자기 디스크는 기록막(13)을 기록층(17)과 재생층(16)으로 분리하여 기록층(17)은 수직자기 이방성을 담당하는 층으로, 재생층(16)은 광자기 효과를 담당하는 층으로 각각 80∼130Å으로 제조하므로서 종래의 광자기 디스크에 비해 단파장 레이저에서 커회전각이 우수하다. 또한, 기록층(17)을 희토류-리치 타입으로 제조하므로써 기록/재생 사이클에 따른 신뢰성 테스트에서도 기록재생특성과 기록파워의 감소가 거의 없으며, 기로된 자구의 크기가 일정하게 유지되는 효과가 있는 것이다.On the other hand, the short-wavelength magneto-optical disk of the present invention separates the recording film 13 into the recording layer 17 and the reproduction layer 16, and the recording layer 17 is a layer responsible for vertical magnetic anisotropy, and the reproduction layer 16 ) Is a layer responsible for the magneto-optical effect, which is 80 to 130 각각 each, and has a larger rotation angle in a short wavelength laser than a conventional magneto-optical disk. In addition, since the recording layer 17 is manufactured in the rare earth-rich type, the recording and reproducing characteristics and the recording power are hardly reduced even in the reliability test according to the recording / reproducing cycle, and the size of the predetermined magnetic domain is kept constant. .

이하, 실시예 1 및 비교에 1을 통하여 본 발명의 효과를 좀 더 구체적으로 살펴보지만, 하기예에 본 발명의 범주가 한정되는 것은 아니다.Hereinafter, the effects of the present invention will be described in more detail with reference to Example 1 and 1, but the scope of the present invention is not limited to the following examples.

[실시예 1]Example 1

폴리카보네이트 기판(11)상에 직류 마그네트론(DC Magnetron)방식으로 유전체막(12), 재생층(16), 기록층(17), 절연막(14) 및 반사막(15)을 순차적으로 형성시켜 본 발명의 광자기 디스크를 제조하였다.The dielectric film 12, the regeneration layer 16, the recording layer 17, the insulating film 14 and the reflective film 15 are sequentially formed on the polycarbonate substrate 11 by a DC magnetron method. Magneto-optical disks were prepared.

이때, 유전체막(12)은 SiN로 600Å, 절연막(14)은 SiN로 200Å반사막(15)은 Al-Ti로 두께를 400Å으로 하여 제조한다. SiN제조에서는 Ar과 N2의 혼합가스를 사용하여 직류 반응성 마그네트론 스퍼터링(DCreactive magnetron sputtering)방식을 사용하였고, 또한 재생층(16), 기록층(17) 및 반사막(15)은 Ar가스를 이용한 직류 마그네트론 방식으로 두께 100Å, 150Å, 및 400Å로 각각 제조하였으며, 재생층(16)은atm% 기준으로 22atm%의 Nd, 15atm%의 Tb, 50atm%의 Fe, 및 13atm%의 Co로, 기록층은 희토류-리치 타입의 TbFeCoCr을 atm% 기준으로 28.0atm%의 Tb, 53.0atm%의 Co, 및 5.5atm%의 Cr로 제조하였다. 박막 제조시의 초기 진공도는 약 3×10E-7 mbar이었으며, 사용한 타켓(target)의 크기는 지름 2인치였으며, 박막의 형성시에 균일도를 향상시키기 위해 기판을 20rpm의 속도로 회전하여 박막을 제조하였다.At this time, the dielectric film 12 is made of 600 ns of SiN and the insulating film 14 is made of SiN, and the 200 ns reflective film 15 is made of Al-Ti with a thickness of 400 ns. In the manufacturing of SiN, a DC reactive magnetron sputtering method using a mixed gas of Ar and N2 was used, and the regeneration layer 16, the recording layer 17, and the reflective film 15 were DC magnetrons using Ar gas. And a thickness of 100 kPa, 150 kPa, and 400 kPa, respectively, and the regeneration layer 16 is 22atm% Nd, 15atm% Tb, 50atm% Fe, and 13atm% Co on the basis of atm%, and the recording layer is rare earth. -Rich type TbFeCoCr was prepared with 28.0atm% Tb, 53.0atm% Co, and 5.5atm% Cr on the basis of atm%. The initial vacuum during the thin film manufacturing was about 3 × 10E-7 mbar, the target size used was 2 inches in diameter, and the thin film was manufactured by rotating the substrate at a speed of 20 rpm to improve the uniformity in forming the thin film. It was.

[비교예 1]Comparative Example 1

상기 실시예 1에서 재생층 및 기록층을 천이금속-리치의 TbFeCo로 형성시킨 것을 제외하고는 동일하게 실시하여 박막을 제조하였다.A thin film was manufactured in the same manner as in Example 1 except that the reproduction layer and the recording layer were formed of TbFeCo of transition metal-rich.

상기 실시예 1 및 비교예 1에서 제조된 박막을 VSM(vibrating sample magnetometor)을 이용하여 박막의 자기적 특성을 측정하였으며, 제3도에 디스크의 반복기록재생 횟수에 대한 기록파워의 변화를 나타내였고, 제4도에 디스크의 반복재생 횟수에 대한 기록재생특성을, 제5도에 기록재생의 반복 횟수에 대한 캐리어 레벨(carrier level)의 변화를 도시하였다.The magnetic properties of the thin films prepared in Example 1 and Comparative Example 1 were measured using a vibrating sample magnetometor (VSM), and FIG. 3 shows the change in recording power with respect to the number of times of repeated recording and reproducing of the disc. FIG. 4 shows the recording / playback characteristics with respect to the number of repetitive reproductions of the disc, and FIG. 5 shows the change of the carrier level with respect to the number of repetitions of the recording / reproduction.

제3도로 부터, 비교예의 박막을 기록/소거 횟수가 104이 될 때 까지 완만하게 기록파워가 3mw로 감소하여 기록파워의 감소가 급속하게 나타나고, 본 발명의 박막에서는 기록파워가 4mw이상으로 유지가 되므로 기록파워의 감소가 거의 나타나지 않았고, 제4도로부터, 종래의 천이금속-리치 타입의 TbFeCo의 경우, 디스크의 반복재생 횟수 102이하에서 기록재생특성이 약 44dB에서 반복재생 횟수가 104이될 때 약 37dB까지 감소하여 기록재생특성이 현저하게 감소하며, 본 발명의 경우 기록 재생특성이 104의 싸이클 후에도 약 45dB를 유지하므로 기록재생특성의 감소가 거의 없음을 알 수 있다. 또한, 제5도로부터, 종래의 방법에 따라 제조된 박막에 비해 본 발며의 박막이 기록재생의 횟수가 증가할 수록 캐리어 레벨(carrier level)의 감소가 작아 더욱 우수함을 알 수 있다. From FIG. 3, the recording power gradually decreases to 3mw until the number of times of recording / erasing of the thin film of the comparative example reaches 10 4 , and the recording power decreases rapidly. In the thin film of the present invention, the recording power is maintained at 4mw or more. the so recorded were the power reduction in the almost open, the fourth from the road, the conventional transition metal-case of TbFeCo of a rich type, repeat number of times in the recording and reproducing characteristics in the following iteration of disk playbacks 10 2 about 44dB of 10 4 In this case, the recording and reproducing characteristics are remarkably reduced by about 37 dB. In the present invention, the recording and reproducing characteristics are maintained at about 45 dB even after 10 4 cycles. In addition, from FIG. 5, it can be seen that as the number of times of recording and reproducing the thin film of the present invention is smaller than the thin film manufactured according to the conventional method, the decrease of the carrier level is smaller, which is superior.

Claims (5)

기판상에 유전체막, 기록막, 절연막, 및 반사막이 순차적으로 적층된 광자기 기록매체에 있어서, 상기 기록막을 NdTbFeCo로 구성된 재생층 및 희토류-리치 타입의 TbFeCoCr로 구성된 기록층으로 형성시키는 것을 특징으로 하는 단파장용 광자기 기록 매체.A magneto-optical recording medium in which a dielectric film, a recording film, an insulating film, and a reflective film are sequentially stacked on a substrate, wherein the recording film is formed of a reproduction layer composed of NdTbFeCo and a recording layer composed of rare earth-rich type TbFeCoCr. Short-wavelength magneto-optical recording media. 제1항에 있어서, 상기 재생층의 두께가 80∼130Å인 것을 특징으로 하는 단파장용 광자기 기록 매체.The short-wavelength magneto-optical recording medium according to claim 1, wherein the reproduction layer has a thickness of 80 to 130 kHz. 제1항에 있어서, 상기 기록층의 두께가 130∼200Å인 것을 특징으로 하는 단파장용 광자기 기록 매체.The short-wavelength magneto-optical recording medium according to claim 1, wherein the recording layer has a thickness of 130 to 200 microseconds. 제1항에 있어서, 상기 재생층이 NdXTby(Fe100-ZCoZ)100-x-y, 20≤x≤27, 13≤y≤18, 10≤z≤30로 구성됨을 특징으로 하는 단파장용 광자기 기록 매체.The short wavelength of claim 1, wherein the regeneration layer is composed of Nd X Tb y (Fe 100-Z Co Z ) 100-xy , 20 ≦ x ≦ 27, 13 ≦ y ≦ 18, and 10 ≦ z ≦ 30. Magneto-optical recording medium. 제1항에 있어서, 상기 기록층이 TbaCrb(Fe100-CCoC)100-a-b, 26≤a≤32, 3≤b≤8, 10≤c≤30로 구성됨을 특징으로 하는 단파장용 광자기 기록 매체.2. The short wavelength of claim 1, wherein the recording layer comprises Tb a Cr b (Fe 100-C Co C ) 100-ab , 26 ≦ a ≦ 32, 3 ≦ b ≦ 8, and 10 ≦ c ≦ 30. Magneto-optical recording medium.
KR1019950001801A 1995-01-28 1995-01-28 Optic-magneto recording medium KR100225108B1 (en)

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