IMPROVEMENTS RELATING TO DATA STORAGE AND RECORDING

Abstract: An optical data storage medium is disclosed for use in an optical read/write system using an optical read wavelength of W, the medium including a textured region having raised areas and depressed areas disposed in a regular array with a period (pitch) not greater than W. The medium comprises a substrate; a layer or a plurality of zones of magneto-optic material; and a layer or a plurality of zones of an optically reflective material (which may or may not be the same as and/or constituted by the magneto-optic material). The magneto-optic material is disposed so as to be accessible to incident optical radiation. In one embodiment, the texture is shallow, being generally in the range 10 to 50 nanometers. In a second embodiment, the depth of the texture is at least one tenth of the value of W. The texture can take the form of a grating, or of crossed gratings, or be defined between an array of protuberances; structures with sinusoidal, square-wave (top-hat) or saw-tooth profile are advantageous.

Description: nIMPROVEMENTS RELATING TO DATA STORAGE AND RECORDINGn This invention relates to a data storage medium, and to methods of recording data and. reading recorded data from such a medium. In particular, the invention is concerned with magneto-optic techniques. In information storage and retrieval systems, the following characteristics are desirable: (1) to minimise the size of a distinguishable feature in the record (in digital records this is a "bit"); (2) to minimise the energy requirements to write one bit; (3) to maximise the writing speed or number of bits written per second; (4) to maximise the reading speed of recorded information; (5) to maximise the signal level obtained when reading recorded information; (6) to maximise the signal-tonoise ratio during reading, and (7) to maximise the readout contrast. Several magneto-optic techniques are in theory suitable for use in information storage. These include magnetic writing (i.e. recording) followed by optical reading of the recorded material; thermomagnetic writing/magnetic reading; and thermomagnetic writing/optical reading. The present invention is directed particularly to systems using optical reading or thermomagnetic writing (or both). Where the writing step is a thermomagnetic step, the physical effect produced in the medium by writing (i.e. by the recording process) is, at least in part, magnetic and may for example involve local heating of the medium by the absorption of incident electromagnetic radiation. It is one object of the present invention to provide a magneto-optic memory structure with high sensitivity to writing radiation so that the energy requirement for writing one bit is reduced and the writing speed increased. Where the readout of magneto-optic memory structures is optical, it may be achieved by observing the change in polarisation state of electromagnetic radiation scattered from the surface. The scattering may be direct transmission or reflection, or scattering in other directions. When the readout radiation is linearly polarised, the change in polarisation state of the scattered light may usually closely be described as a rotation of the polarisation direction. This is closely equivalent to the addition of a polarisation component orthogonal to the incident polarisation in the scatter beam (the added component being the so-called magneto-optic" component). This magneto-optic component with orthogonal polarisation "carries" the readout information, but is generally of very small intensity. The scattered component with polarisation parallel to that of the incident radiation, which carries no information, is however, very large. These factors lead to low readout signal-to-noise ratio and low readout contrast which thus limits the usefulness of known magneto-optic memories by reducing the ability to extract stored information from them. In digital storage where "bits" are stored, this results in a "Bit Error Rate" which is larger than is desired for many applications. It is a second object of the present invention to provide means by which the readout signal-to-noise ratio and contrast may be improved in order to improve the readout "Bit Error Rate". It is a third object of the present invention to realise the improvements in recording sensitivity and readout "Bit Error Rate" using a magnetic-optic structure that may be formed by reliable production techniques. There are known in the art several multilayer magneto-optic structures which provide improvements in recording sensitivity and readout reliability. These structures consist of combinations of magneto-optic, dielectric and metallic layers deposited in a closely-planar thin-film form. They absorb a significant fraction of the writing illumination, giving higher writing sensitivity. They also aim to increase the intensity of the (information-carrying) magneto-optic component of the scattered radiation, and decrease the intensity of the "ordinary" reflected radiation (i.e. that component polarisastion parallel to the incident radiation), giving higher readout reliability. However, further improvement is desired for many applications, especially in the application to computer memories. It is also desired to provide a structure that may be manufactured with higher yields and consequent lower manufacturing costs. The multilayer structures discussed above are difficult to manufacture to the required uniformity of properties within the total storage area of each structure, and between structures. According to one aspect of the present invention, there is provided an optical data storage medium for use in an optical read/write system using an optical read radiation of wavelength W, which medium has or includes a region which carries a surface texture including raised areas and depressed areas which are disposed in a regular array with a period (pitch) measured transversely to the mean surface level of not greater than W, wherein the medium comprises: (a) a substrate; (b) a layer or a plurality of zones of magneto-optic material; and (c) a layer or a plurality of zones of an optically reflective material (which may or may not be the same as and/or constituted by said layer or zones of magneto-optic material), the magneto-optic material being disposed in relation to the structure of the data storage medium as a whole such that it is accessible to incident optical radiation. The substrate will generally be a dielectric material, and in many embodiments will carry the textured structure. The invention also provides methods for recording (writing) and reading such a data-storage medium. The invention further provides a pre-recorded data storage medium having the structure defined above and recorded by a method in accordance with the invention. According to one embodiment of the present invention, there is provided a data storage medium comprising a substrate having a slightly textured surface coated with a thin film of a metal which conforms to the texture of the surface and, on top of said thin film of metal, a thin film of magneto-optic material which also conforms to the texture of the substrate surface. If the magneto-optic film is itself highly reflective, the thin metal film may be omitted. Preferably, the magneto-optic film has a thickness in the range of 5-100 nm. One such structure is shown by way of example in Figure 1. The depth of the texture (e.g. the peak to trough dimension where the surface is in the form of a grating) may be very small, for example in the range of 10-50 nm. Alternatively, the depth of the texture may be in the range 50-200 nm. The mean pitch of the texture will usually be smaller than or equal to the wavelength of the writing or reading radiation. The metal which constitutes the thin film between the substrate and the magneto-optic film is preferably silver, gold, copper or aluminium. This film may, for example, have a thickness in the range 10 to 100 nm. The magneto-optic film may be overcoated with a thin metallic film of, for example, silver, gold, copper or aluminium. The thickness of such an overcoating film may be in the range 5 to 30 nm. The texture of the surface may be in the form of a series of alternate grooves and ridges which are substantially parallel. For convenience, though not essentially, these may be uniformly spaced and of uniform depth and shape. Such a surface will be referred to herein as a grating since it is similar to surface relief diffraction gratings which are well known in the spectroscopic art. The texture may consist of two such gratings disposed mutually at an angle. The gratings may be disposed mutually orthogonally. ' Such a textured surface is referred to as a crossed grating. Many methods of making such gratings are known and include photolithography of an interference field, mechanical ruling and replication from a pre-existing surface. We have found that materials which are suitable for use as the magneto-optic layer include transition elements, rare earth elements, alloys of at least one rare earth element and at least one transition element, and alloys of at least one transition element and at least one semi-metal. Materials that work satisfactorily include iron, cobalt, nickel, terbium-iron, gadolinium-cobalt, and manganesebismuth. One particularly favoured material is an amorphous (glassy) alloy of terbium-iron which can possess a magnetisation normal to the film plane when prepared under favourable conditions. The dielectric constant of at least one of the magneto-optic material and the optically reflective material should preferably have a negative real part and a small imaginary part at the frequency of the radiation in question. The shallow-texture structure of this first embodiment of the invention provides increase in readout reliability when the illumination has electric vector E linearly polarised parallel to the plane of incidence as shown in Figure 2. We refer to this as polarisation in the plane of incidence. When the surface texture takes the form of a grating the readout beam polarisation should preferably also be closely perpendicular to the grating lines. (This is unnecessary when the texture takes the form of two gratings crossed approximately at right angles). For readout of small recorded bits, typically having linear dimensions 400 nm to 5000 nm in size, readout illumination of wavelength 400 nm to 1000 nm is highly focussed and therefore impinges on the surface from a wide range of angles. This illuminating radiation has a smooth variation of intensity across this angular range. The radiation reflected from the surface also emerges in a range of angles, with a primarily smooth variation in intensity across the angular range, but over a small portion of that angular range there may be observed a strong dip in intensity. This is shown in Figures 3 (a), (b), (c). A photo-detector viewing at the angular position of this dip (through an appropriately oriented analyser) observes a much increased intensity of the information-carrying magneto-optic component. It also observes a much reduced intensity of radiation component polarised parallel to the incident radiation (the ordinary reflectivity component). As a result both the readout contrast and the readout signal-to-noise ratio are greatly improved. Accordingly, the invention further provides a method of reading data stored on a data storage medium, which method comprises monitoring the intensity of the magneto-optic signal within the angular range over which there occurs a sharp reduction (dip) in reflectivity as the surface of the medium is observed or scanned with the read-out illumination. Figure 4 shows experimentally-measured graphs of the intensity of the information-carrying component at and close to this dip in surface reflectivity. In Figure 4, plot A is for a magneto-optic layer on a shallow grating surface such as that of Figure 1; plot B is for a similar structure, but with a layer of silver on top of the magneto-optic layer; and plot C is for a planar substrate. If the surface reflectivity dip is very sharp, which occurs for highly-reflective metallic or magnetic metallic layers on the surface texture, then the position of the dip noticeably changes upon reversal of the magnetisation direction of the magnetic layer. An alternative readout method is, therefore, the measurement of the angular position of the reflectivity dip. Accordingly the invention also provides a second method of reading data stored on a data storage medium, which method comprises monitoring the angular position at which there occurs a sharp reduction (dip) in reflection from the medium as the surface thereof is observed or scanned with the read-out radiation. We have not found this approach as useful in obtaining high readout signal-to-noise ratios as the first method. The origin of the reflectivity dip is attributed to the excitation of collective electronic motion (surface polaritons or plasmons) in the magnetic film by the incident radiation, the surface texture enabling efficient coupling between the incident radiation and this collective electron motion. This shallow textured surface provides strong absorption over a narrow range of angles, giving a small improvement to writing sensitivity. We have obtained best results on readout from the shallow textured surface when the surface is in the form of a sinusoidal profile of depth 25-40 nm, and a period slightly smaller than the wavelength of the readout illumination. The magnetic film is preferably highly reflective, examples being cobalt, terbium-iron, and gadolinium-cobalt; and of thickness in the range of 5 nm to 50 nm. Under these conditions we have obtained 7.5 fold enhancement in the intensity of the magneto-optic component and a two-fold reduction in the intensity of the ordinary reflected component. For a practical erasable data storage and retrieval medium the "polar" configuration, in which the direction of magnetisation lies perpendicular to the mean surface plane, is preferred because this permits the maximum recording density. In this arrangement preferred materials for the magnetic layer are MnBi, GdCo, TbFe, GdTbFe and other rare earth-transition element alloys. According to a second embodiment of the invention there is provided a data storage medium comprising a substrate having a more deeply textured surface coated with a thin magnetic film which conforms to the texture of the surface. The texture preferably has a mean spatial dimension smaller than the wavelength of the readout radiation and preferably has a depth at least one tenth of the wavelength of the readout radiation, and more preferably at least one sixth thereof. We have found grating profile depths in the range 0.2W to 0.5W, where W is the wavelength of the writing or reading illumination, to be particularly advantageous. In the case where the surface is a surface-relief grating the mean spatial dimension is the grating pitch. The surface relief may take the form of a single grating or of two or more gratings disposed mutually at an angle. With two gratings, they may be disposed mutually orthogonally. We have found a single grating to be particularly advantageous. The thin magnetic film may be continuous or discontinuous on the textured surface. Possible examples of this structure are shown in Figures 5 (a), (b) and (c). In this and all subsequent Figures, 1 refers to the magnetic layer, 2 to the metallic mirror layer. According to a third embodiment of the invention there is provided a data storage medium comprising a substrate having a textured surface of similar depth, period and profile to that described in the second aspect of the invention. This textured surface is coated with a thin metallic film which in turn is coated with a thin magnetic film, both film layers conforming to the texture of the surface. Either or both film layers may be continuous or discontinuous. Examples of this structure are shown in ¯ Figures 6 (a) - (e) for the top-hat & BR< sinusoidal profiles. Advantageously, the mirror layer is, in the case of the top-hat profile embodiments, located so that the electromagnetic or optical path length between the mirror layer and the lower magneto-optic film is an odd number of quarter-wavelengths of the read or write radiation. According to a fourth embodiment of the invention a metallic thin film may be deposited on a planar substrate and coated with a dielectric layer that provides a textured surface of similar depth, period and profile to that described in the second aspect of the invention. The dielectric layer is then coated with a magnetic thin film. Either or both film layers may be continuous or discontinuous. Examples of this structure are shown in Figures 7(a) and 7(b), for the top-hat profile. According to a fifth embodiment of the invention a magnetic thin film may be deposited on a planar substrate and coated with a dielectric layer that provides a textured surface of similar depth, period and profile to that described in the second aspect of the invention. The dielectric layer is then coated with a metallic thin film. Either or both film layers may be continuous or discontinuous. Figures 7(c) and 7(d) show examples of this aspect of the invention. According to a sixth embodiment, a structure of the type defined in any of the first to fifth embodiments is overcoated with a dielectric material to a depth sufficient to give the medium a planar surface. With such a structure, the lower surface of the coating dielectric layer conforms to the textured surface of the substrate plus magneto-optic and/or metallic films. In this embodiment, relatively deep textures are preferred. Figure 8 shows an example of such a structure. In each of the second, third, fourth, fifth and sixth embodiments of the invention the surface texture may most conveniently take the form of a top-hat (square-wave) or crossed top-hat profile or sinusoidal surface-relief grating or crossed sinusoidal surface-relief grating, although other profiles, for example a triangular or sawtooth profile, are also intended to fall within the scope of this invention. In each case, we have found that particular advantage in either the writing or reading (or both) of data can be achieved when the depth of the grating lies in the range 0.2 times to 0.5 times the wavelength of the writing or reading illumination. For writing, either a crossed grating or a single grating profile confers advantage. For readout, a single grating profile is preferred. When writing on a single grating profile, we find that, for radiation linearly polarised perpendicular to the grating lines, nearly complete absorption occurs, with very little reflectivity. This high absorption occurs over a wide range of angles of incidence so that even with a very small recorded spot size for which a tightly-focussed cone of radiation is required, almost all the incident radiation energy can be utilised for thermomagnetic recording, giving very high writing sensitivity. When writing on a crossed grating profile, nearly complete absorption occurs for any polarisation of the incident radiation, again over a wide range of angles of incidence, and very high writing sensitivity is achieved. For readout from a single grating profile, readout radiation polarised perpendicular to the grating lines gives a very low intensity of the "ordinary" reflection component. Furthermore the high absorption of energy that this represents may produce a much increased magneto-optic component intensity. These combine to give a much increased polarisation rotation angle of the reflected readout illumination. Over a wide range of angles of incidence, we commonly find a fourfold or a fivefold increase in rotation angle over that obtained from a planar magneto-optic film on a planar (non-textured) substrate surface. In general, both the contrast and signal-to-noise ratio on readout from the structure are greatly enhanced. Excellent performance has been achieved with the structures illustrated in Figures 6(b), (c), (d) and (e) and Figures 7(a)-(d) as the surface texture, using writing and readout radiation polarised in the plane of incidence and perpendicular to the grating lines. For a writing and readout radiation wavelength of 633 nm the preferred pitch and depth of the sinusoidal structure is 150-400 nm, and that for the top-hat structure is 180-300 nm. The thin metallic mirror layer should have thickness adequate to be opaque but should not significantly tin-fill" the structure. Using aluminium as the mirror layer, a thickness of 15-50 nm is appropriate. Upon the crests of the structure is deposited the magnetic layer (which is, therefore, discontinuous across the surface profile), which typically is of thickness in the range of 10-50 nm, and which may be any of the rare-earth-transition element alloys discussed above for the shallow-textured surface in the first embodiment. The other structures described also provide large improvements in readout performance, but to date we have not observed enhancements as large as those provided by the structures of Figures 6(b), (d), (e) and 7(a)-(d). The sinusoidal and top-hat structures are preferred for two further production reasons. Firstly the magnetic layers on both types of profile are substantially planar so that the magnetisation direction of the recorded bits is well-defined with respect to the readout illumination, giving maximum magneto-optic signal. Secondly, these profiles may be fabricated using either photolithography of an interference field or mechanical ruling or replication from a pre-existing surface. In particular for the structures shown in Figures 5 and 6 a "master" grating profile medium can be produced by, for example, the technique of photolithography of an interference field, and electroplating, and many replicas of the profile can be produced by such techniques as embossing, casting, injection moulding, and compression moulding. This gives ease of reliable and repeatable production with high yields. The magneto-optic layers may alternatively be formed by sputtering or evaporating (at low pressure) a controlled amount of the magneto-optic material onto the textured surface at a controlled angle of deposition. Materials that we have found suitable for the dielectric (e.g. substrate) layers include polycarbonates, photoresists, polymethylmethacrylate and high-temperature nylons, and polyesters. These materials can simply replicate an existing grating surface profile, by such well known means as embossing and casting. It is possible by these means to replicate a "master" grating surface many times. The dielectric grating profile does not, therefore, have to be constructed for each memory structure. This ease of preparation of the grating profile is to be compared with the fabrication of the multilayer structures, where the fine tolerances required are difficult to achieve and must be reproduced during the manufacture of every structure. In the structures according to this invention, the fine tolerances must be satisfied for the master grating. However, once this is achieved subsequent reproduction of that grating within those tolerances is easily accomplished. The master grating may, for example, take the form of a nickel-electroplating of a grating formed by photolithography, mechanical cutting or other means. The materials listed above by way of example also can withstand without damage the elevated temperatures required for recording information onto and erasing infdrmation from the presently preferred magneto-optic materials. Other dielectric materials capable of this include glasses but it is generally less easy to replicate the grating profile of a master grating onto such materials. Materials that we have found suitable for the high-reflectivity metal layers of the structure include silver, gold, copper and aluminium. Other metals may be similarly effective.

Claims: Claims: 1. An optical data storage medium for use in an optical read/write system using an optical read radiation of wavelength W, which medium has or includes a region which carries a surface texture including raised areas and depressed areas which are disposed in a regular array with a period (pitch) measured transversely to the mean surface level of not greater than W, wherein the medium comprises: (a) a substrate; (b) a layer or a plurality of zones of magneto optic material; and (c) a layer or a plurality of zones of an optically reflective material (which may or may not be the same as and/or constituted by said layer or zones of magneto-optic material), the magneto-optic material being disposed in relation to the structure of the data storage medium as a whole such that it is accessible to incident optical radiation. 2. A medium as claimed in claim 1, wherein the magneto-optic film has a thickness in the range of 5-100 nanometers. 3. A medium as claimed in claim 1 or 2, wherein the magneto-optic film is overcoated with a thin metallic film. 4. A medium as claimed in claim 3, wherein said thin metallic film is formed of silver, gold, copper or aluminium. 5. A medium as claimed in claims 3 or 4, wherein said thin metallic film is 5 to 30 nanometers in thickness. 6. A medium as claimed in any preceding claim, wherein the texture of the surface is in the form of a series of alternate grooves and ridges which are substantially parallel. 7. A medium as claimed in claim 6, wherein said grooves and ridges are uniformly spaced and of uniform depth and shape. 8. A medium as claimed in claim 6 or 7, wherein the texture of the surface comprises two series of grooves and ridges disposed mutually at an angle. 9. A medium as claimed in claim 8, wherein said two series of grooves and ridges are mutually orthogonal. 10. A medium as claimed in any preceding claim, wherein the magneto-optic layer is formed of a transition element, a rare earth element, an alloy of at least one rare earth element and at least one transition element, or an alloy of at least one transition element and at least one semi-metal. 11. A medium as claimed in claim 10, wherein the magneto-optic layer consists of iron, cobalt, nickel, terbium-iron, gadolinium-cobalt or manganese-bismuth. 12. A medium as claimed in any preceding claim, wherein the textured surface is of sinusoidal profile. 13. A medium as claimed in any preceding claim, wherein the depth of the surface texture (peak-to-trough) is in the range 10-50 nanometers. 14. A medium as claimed in any one of claims 1 to 12, wherein the depth of the surface texture (peak-to-trough) is in the range 50-200 nm. 15. A medium as claimed in any one of claims 1 to 12, wherein the textured surface has a mean spatial dimension smaller than W and has a depth at least one tenth of W. 16. A medium as claimed in claim 12, 13 or 14, or 15, wherein the textured surface is in the form of a grating. 17. A medium as claimed in claim 16, wherein the grating is of square-wave profile. 18. A medium as claimed in claim 16, wherein said grating is of sinusoidal profile. 19. A medium as claimed in claim 16, wherein said grating is of saw-tooth profile. 20. A medium as claimed in claim 17 or 18, wherein the magneto-optic layer is formed over the raised surface portions (lands) of the grating and over the depressed surface portions (pits) of the grating. 21. A medium as claimed in claim 17 or 18, wherein the magneto-optic layer is formed only over the raised surface portions (lands) of the grating only. 22. A medium as claimed in claim 17 or 18, wherein the magneto-optic layer is formed only over the depressed surface portions (pits) of the grating. 23. A medium as claimed in preceding claim, wherein the magneto-optic layer is formed over or under a metallic mirror layer. 24. A medium as claimed in claims 22 and 23, wherein the magneto-optic layer is formed over a metallic mirror layer, and wherein a metallic mirror layer is also present over the depressed surface portions (pits) of the grating. 25. A medium as claimed in claim 15, 16, 17 or 18, wherein a thin metallic film is formed on a planar substrate and is coated with a dielectric layer having said textured surface, the dielectric layer carrying said magneto-optic layer as a continuous or discontinuous thin film. 26. A medium as claimed in claim 15, 16, 17 or 18, wherein the magneto-optic layer is formed on a planar substrate and is coated with a dielectric layer having said textured surface, the surface of said dielectric layer being coated with a thin metallic film which is either continuous or discontinuous. 27. A medium as claimed in any one of claims 15 to 26, wherein the textured surface is sinusoidal in profile with a pitch and depth in the range 150-400 nanometers for a read-out radiation, W, of 633 nanometers. 28. A medium as claimed in any one of claims 15 to 26, wherein the textured surface is sinusoidal in profile with a pitch and depth in the range 200-550 nanometers for a read-out radiation, W, of 820 nanometers. 29. A medium as claimed in any one of claims 15 to 26, wherein the textured surface is of square-wave profile with a pitch and depth in the range 180-300 nanometers for a read-out radiation wavelength, W, of 633 nanometers. 30. A medium as claimed in any one of claims 15 to 26, wherein the textured surface is of square-wave profile with a pitch and depth in the range 240-400 nanometers for a read-out radiation wavelength, W, df 820 nanometers. 31. A medium as claimed in claim 23, 24 or 25, wherein said metallic mirror layer has a thickness in the range 15-50 nanometers. 32. A medium as claimed in any preceding claim, wherein the medium further includes an overcoating dielectric layer the lower surface of which conforms to said textured surface, and the upper surface of which is planar. 33. A method of reading data stored on an optical data storage medium as claimed in any preceding claim which comprises monitoring the angular position at which there occurs a sharp reduction (dip) in reflection from the medium as the surface thereof is observed or scanned with the read-out radiation. 34. A method of reading data stored on an optical data storage medium as claimed in any one of claims 1 to 32, which comprises monitoring the intensity of the magneto-optic signal within the angular range over which there occurs a sharp reduction (dip) in reflectivity as the surface of the medium is observed or scanned with the read-out radiation.

Inventors: HELFET, PETER ROY, HUMBERSTONE, VICTOR CAREY, PETTIGREW, ROBERT MARTIN
Applicants: PLASMON DATA SYSTEMS N.V.
Application year: 1983
Main classification: G11B7
IPC codes: G11B11, G11B7, G11C13