DATA STORAGE MEDIUM AND METHODS FOR RECORDING AND READING OF DATA

Abstract: An optical data storage medium with burn-film having changeable optical properties, for example, changeable reflective power as a result of sufficiently intense illumination, due to hole-burning in the film, is provided with optical structures close to the burn-film for focusing and positioning during recording and reading of individually interpretable data bits (spots). The optical structures are preferably monodisperse, transparent spheres with a diameter in the range of 1-100 mu m. Illumination is performed selectively from a number of predetermined angles ( THETA i, phi j) during recording and reading, and the number of individual data spots under each sphere corresponds roughly to the number of angles.

Description: DATA STORAGE MEDIUM AND METHODS FOR RECORDING AND READING OF DAT The present invention relates to an optical data storage medium and methods for recording and reading data on/from said medium. More specifically, a concept is described for optical storage of information on data carriers such as fiches, cards or tape. The data carrier's surface is completely or partly covered with focusing microstructures adjacent to a layer which is able to change its optical properties when exposed to intense light. (In the following, this layer will for simplicity in most cases be referred to as the "burn-film". This expression does not imply any particular embodiment of the layer, which can be of the reversible or the irreversible type, see below.) During recording of data, such local changes are created in the layer by having the microstructures focusing the light, thus obtaining a high light intensity on the layer. During reading of data, the optical microstructures may operate as an active optical component assisting the reading equipment. By using e.g. transparent microspheres (typical diameter: 1 to 100 urn) as focusing elements disposed over an optically absorbing film, a tight focusing and a high data storage capacity can be achieved without the complexity and the expenses that otherwise would be required for a recording and reading system which focuses directly on the light absorbing layer. Using oblique illumination through the microspheres, possibilities arise for storage of a high number of data bits at each microsphere position, as well as for hierarchically built data bases, in certain cases combined with data protection. Easy prerecording on mass produced data carriers becomes possible. During reading of data the microspheres function as auxiliary optics, which makes it possible e.g. to read large blocks of data without the use of a laser. Storage of data by means of laser beams which produce local change of the optical properties of a thin film on a planar substrate are well known, for example from SPIE vol. 329 (1982) , SPIE vol. 490 (1984) , SPIE vol. 695 (1986) , SPIE vol. 899 (1988) , SPIE vol. 1078 (1989) . The change in optical properties can be reversible, whereby the stored data can be deleted and replaced by new data. Alternatively, the change in optical properties can be irreversible, whereby it becomes impossible to delete and/or rerecord new data. Storage media of the latter type are often referred to as WORM (Write Once Read Many Times) media. A usual method of preparation of WORM media consists of depositing on the substrate, which is a plastic disc, a thin fil of a low melting point metal such as Te. During data storage each bit is represented by the physical status of the specific film area assigned for the storage of said bit (one elementary data storage cell with its address) , i.e. whether that area has been irreversibly changed due to exposure to light or whether it is unchanged. To our knowledge, all practical optical data storage systems are so far based on reflection from the burn- film. The irreversible change consists in such a% case of an increase or a decrease of the reflectivity of each cell when a focused laser beam heats the burn-film. In the film is thereby created a hole through which the light can pass, or the film is smoothened so that its reflectivity increases. Several other processes can be used, e.g. local deformation of the substrate which influences the reflectivity. Reading is most commonly performed by examining the reflectivity of each cell by means of a focused laser beam scanning the surface of the data carrier systematically. This laser beam is too weak to influenc the reflectivity. From NO patent application 86.4041 (= DE 3536739) a data storage medium of the optical type is known, which medium is equipped with focusing optical structures integrated in the medium together with and on top of a material the optical properties of which can be changed by irradiation with light. This known data carrier is however only adapted for storage of visible data, i.e. images which are visually perceptible and which consist of spots that are to be interpreted together in order to create an image. "Tilt-images" can be created due to the optical structures, i.e. a lens raster or array, because the lenses are able to direct light to defined small areas underneath the lenses, depending on the direction of illumi¬ nation. The lenses are however, relatively large, the variation range for the lens diameter is indicated to be 150-500 um, recommended about 400 urn. Thus, the technique described does not relate to a data storage medium for optimized "close packing" of e.g. digital, independently interpretable data bits, but only a spot-structured image storage of the directly visible type. Only irreversible recording of data is described in NO patent application 86.4041. A main objective for the use of optical data storage media instead of magnetic ones is the very high storage density which can be achieved, combined with good long-time stability (e.g. immunity against magnetic fields) . Optical data storage is however subject to both fundamental and practical limitations, and a trade-off must be made between different desired features, of which the most important are: 1) Large number of stored bits per unit area 2) Low laser energy for recording of each bit 3) High contrast when reading information 4) Fast recording and reading 5) Short "random access" time 6) Robust and stable data storage medium 7) Inexpensive data storage medium 8) Inexpensive recording and reading equipment 9) Moderate requirements for precise focusing (distance control) Today's techniques have various limitations/problems. Consider first the recording and reading systems: If a high data storage density is desired it is necessary to use a laser beam for data recording which is focused on the burn-film by means of very high speed optics (lens with low f-number) . Theoretically, the light beam can under optimum conditions be focused to a diameter of about the wave length of the light which is applied. Practical systems have been realized which come very close to that, with focal point diameters of 0.5-1 μm. However, under such strong focusing the requirements for the mechanical control of the lens become very strict: Lens to burn-film distance must be controlled precisely: On either side of the focal point the laser beam diverges very quickly and in a distance of z/2 from the focus the diameter is doubled (provided a Gaussian light beam, see fig. 1) . z can be interpreted as a measure of "depth of field" which is correlated to the beam diameter w at the focal point and the light wave length λ by the equation: z = π w 2 /λ (1) Since w is very small in this connection, z lies only in the range 1-10 μm, which means that the distance between lens and storage medium must be controlled with corresponding precision. Possible deviations from planarity in the data storage medium and variations in the optical thickness of the protective film covering the burn-film, entail that the distance in practice must be servo-controlled during the fast relative movement between storage medium and lens. Furthermore, the position of the burn-film is critical. When storing data on rotating discs, the burn-spots are typicall positioned in a spiral pattern or in concentrical tracks, or in straight stripes when storing on cards. In both cases, the burn-spots must be placed as close to one another as possible in order that a high storage density be achieved; a typical distance between spots being from a few μm down to approx; 1 μm. The requirements for the positioning of the lens become correspondingly stringent and imply in practice that the data storage medium beforehand has received optical "guide-tracks" which can be followed during recording and reading by a control servo. During the reading of data, corresponding fundamental limitations apply as during recording: In order to be able to detect the small burn-spots and to discern them from one another, the use of either a laser beam with focusing properties and positioning as mentioned above for recording is required, or an imaging system. In the latter case the resolving power requirements imply that the lens must be positioned with a distance precision corresponding to the one which applies when a laser beam is used. To summarize: Recording and reading systems which operate with burn-spot diameters of approx. 1 μm or less require in practice a laser as a light source, optical components of high quality, sophisticated mechanical control-systems as well as data carriers with well controlled mechanical and optical properties (cf. below). With regard to commercial competition, this probably has little consequence for larger stationary units in controlled environments, but it may represent a considerable handicap for small, possibly mobile recording and reading units, particularly in difficult environments (vibra¬ tions, dust etc). The data storage medium itself is also encumbered with limitations and problems: a potential disadvantage of small burn-spot sizes lies in a possible interference of recording and reading due to small dust particles or the like. In principle, this problem can be solved by depositing a transparen protective film onto the burn-film. Provided that the protective film is thick enough, the laser beam due to its strong focusing, will have such a large diameter on the surface of the protective film, that small particles only obscure a small part of the beam (fig. 2). This however, requires high quality of the optical properties of the protective film: A general requirement exists for flatness and refractive index constancy in order to avoid focus displacement; this requirement becomes more severe in the case of small burn spots. Thin and flexible data carriers like optical tapes, fiches or cards represent a particularly big problem. The necessary stiffness/flatness can not be built into the data carrier itself, and shadowing effects from (dust) particles cannot be appreciably reduced through focusing as shown in fig. 2. For recording and reading on/from data storage systems which are based on measuring light reflected from the burn-film, it is usual to apply polarisation sensitive beam¬ splitters. This means that a protective film in addition to being homogenous, etc. , also has to be free from double refraction. This excludes large groups of materials which otherwise would have been eligible e.g. rolled or extruded plastic foils. Reading by means of reflection from the burn-film requires in addition that it posesses a not insignificant reflection capability. Since the film at the same time must be able to absorb enough radiation during the recording phase, the choice of film material and film thickness is significantly restricted, and a sufficiently good control of reflection/absorption during the production process must be taken care of. In order to avoid the above mentioned problems and to achieve adaption to special market niches, optical data storage systems have been introduced, based on relatively large burn- spots, i.e. 2.5-25 μm in diameter. In US patent 4.542.288 and US patent 4.284.716 Drexler et al. describe an optical data carrier of credit card size, where burn-spots are recorded along a series of straight tracks on a foil with burn-film which is bonded to the card. The burn-spot size is typically from 2.5-7 μm and upwards in diameter, with a distance of 12 μm between the burn tracks. This leads to a significantly lower data storage density than described in the introduction of this application, and the capacity of the card is thus only 2-4 megabytes. On the other hand, recording and reading becomes relatively uncritical, and it becomes possible to employ, e.g. an incoherent light source (light emitting diode) for reading. It is intended to introduce optical data cards which are rigid and inexpensive enough to have user characteristics comparable to ordinary credit cards. A potential problem associated with large burn-spots is the required heating of considerably larger areas by the laser during recording: For example, changing the burn-spot diameter from 0.7 μm to 7 μm leads to an increase of the spot area by a factor of 100. In order to avoid a dramatic and unacceptable increase in the requirements for the laser power or pulse energy, it is therefore necessary to lower the recording threshold of the burn-film (threshold for controlled thermal damage during exposure to laser light) considerably in relation to what is acceptable in stronger focused systems. Drexler et al. have developed a burn-film consisting of silver micropar- tides in gelatin, which, through chemical treatment, reaches an optimized surface reflection and has a very low recording threshold. Even though Drexler et al. by use of their special burn- film and the large burn-spot area have achieved technical solutions which are suited for large and important markets, this has resulted in a lowered data storage capacity, which lies approx. 2 orders of magnitude below other optical data storage systems. At present, data storage applications seem to have been targeted that can be met within the 2-4 megabytes capacity of this card limit (e.g. patient journals) , but there is no doubt that this low data storage density in the future will be considered as even more limiting and unacceptable, also with regard to small and distributed data systems. Finally it is until now unclear to which extent the highly sensitive and chemically special burn-film may have poorer stability when exposed to strong influences from adverse environments (heat, light, chemical attacks) than burn-films made from e.g. tellurium. A main objective of the present invention is to provide an optical data carrier and methods for recording and reading which, in spite of high data storage density, impose modest requirements upon the recording and reading equipment with respect to power and precision. The object is achieved according to the invention by manufacturing an optical data storage medium of the type which is precisely defined in claims 1-15, and by applying recording and reading processes for data on the medium, as presicely defined in claims 16-20. The invention shall now be further described by means of examples of embodiments. It shall also be explained with the aid of the following figures: Fig. 1 shows schematically the basic relationship between the degree of focusing and the depth of field as described above. Fig. 2 shows how a protective film on top of a burn-film reduces the influence of impurities or defects on the surface as described above. Fig. 3 illustrates the effect of optical structures such as transparent spheres over the burn-film, compared with traditional set-ups. Fig. 4 shows more detailed how a hole can be created in the burn-film in various positions underneath one single transparent sphere by varying the direction of the incident light beam. Fig. 5 shows experimentally produced burn-patterns achieved through the use of transparent spheres. Fig. 6 shows an alternative type of optical structures, i.e reflecting microstructures under the burn-film. Fig. 7 illustrates retro-reflection from the burn-film by means of a transparent sphere. Fig. 8 is a schematic drawing showing the principle of a reading method where diffused light is applied from the bottom side of the data storage medium. Fig. 9A shows an alternative reading method applying directional light from the top side of the medium. Fig. 9B shows images taken from the bottom side of the medium, for various directions of light incident on the top side Fig. 10A shows the experimental result of simple trickling of spheres onto a pre-pitted substrate. Fig. 10B shows the corresponding results after deposition by means of dry brushing. Fig. 11 A, B, C illustrate various methods for deposition of transparent spheres into pits on a substrate. Fig. 12 shows one example of a complete data storage mediu with transparent spheres in pits. Fig. 13 illustrates the possibility of recording through o single sphere from several directions by screening or parallel displacement of the light beam at the entrance to the optical system. Fig. 14A is a schematic drawing showing an arrangement for reading with directional light, and Fig. 14 B, C, D show examples of detector systems for use in the arrangement of Fig. 14 A. By incorporating focusing structures into the data storage medium, the same advantages can be achieved as when applying large burn-spots, without the need to reduce the high data storage density. At the same time possibilities for technical solutions and applications are accessible, which are not within reach with traditional data storage media. Fig. 3 shows a schematic drawing of a memory medium according to this invention: A carrier layer of e.g. plastic is coated with a thin burn-film, which is covered with microlenses, e.g. small, transparent spheres which are spread on top of the film or adjacent to it, preferably in a certain pattern. During recording of data a laser beam is directed toward one sphere at a time; the beam only having to be sufficiently in focus to hit single spheres. The light is thereafter focused in the actual sphere and illuminates a small spot of the burn-film underneath the spher , which causes a change of the optical properties of the burn-film at this spot, e.g. a hole is created in the burn- film (a "burn-spot") through which light can pass. The presence or non-presence of a burn-spot represents one information bit (logical "0" or "1") . The medium's role as "auxiliary optics" is illustrated in principle on the drawing, through the comparison with a traditional medium without microlenses. It shows that small burn-spots with corresponding low power/energy requirement for the laser beam can be combined with relatively large spheres and corresponding uncritical focusing and positioning of the beam. The problem still remains, that large spheres, in analogy with large burn-spots, as mentioned above, give low data storage density as long as only one burn-spot relates to each sphere. However, by illuminating the spheres from other directions, burn-spots will occur at many points underneath one given sphere, see fig. 4. Writing of burn-spots by illuminating at skew-angles thus enables each sphere to store several bits, depending on how many burn-positions can be assigned to each sphere. When each sphere has the coordinates x, y in the plane, and the skew-angle is defined by the polar-coordinates Θ, φ, the complete address of each bit-position on the storage medium can be written (x, y, θ, φ ). The number of possible burn-directions (®i. <pj) for each sphere can be interpreted as a "multiplex factor" N. Present experiments indicate practically achievable values for N up to 25, possibly more. Fig. 5 shows an example where light has been sent through a large number of spheres in the same way using 5 different angles in the same plane. The corresponding burn-holes in the film are formed in line (one burn-hole is weaker than the rest, due to an unintentionally less intense laser beam) , with good individual definition. This result shows that it is possible to produce under each sphere, for example, a group of approx. 17 well defined burn-holes (2 Bytes plus control hole, see below). Reading consists in determining the addresses which have a burn-spot, which implies determination of the local change of the optical reflection or transmission properties of the burn- film. Principal and technical aspects in connection therewith will be discussed in the following. The focusing microstructures can have many forms: Light-refracting structures may be placed in front/on top of the data storage film as shown in fig. 4. Such structures can include e.g. : Discrete optical elements, immobilized in relation to the data-storage-film (spheres, convex lenses, Fresnel structures) . Stamped surface patterns in the transparent layer. Controlled refractive index variations in a completel or partly transparent layer. Light reflecting structures may be placed behind/under the data storage film, so that the light, after passing through the film (assumed partly transparent) , is reflected and focused against the film backside, see fig. 6. The burn-film can be of the irreversibly changeable type, or it may be reversible if different light intensities are applied for recording, erasing and reading. Reversible optical burn-materials are known for example from the article "Organo- metallic materials for erasable optical storage" by Hoffman and Potember, Applied Optics, vol. 28, p. 1417-1421, 1989. Other, well known reversible burn-films are of the type magneto- optical, phase-changing, blistering, among others. Two main alternatives exist for reading of data from the data storage medium, namely measuring the light that is reflected from the medium, or the light that is transmitted through it: Reflection: A laser beam scans the addresses of interest o the data storage medium. The illumination of the spheres is performed under the same conditions as during recording, but the beam intensity is now adjusted so that it is too weak to affect the burn-film. In a properly designed data storage medium, the light that is reflected from the burn-film hits the sphere from the bottom side and is focused in such a manner that the light returns in the direction from which it entered (Fig. 7) . The reflected light can be separated from the incident light beam by means of a beam splitter, and the intensity is measured by a photo-detector. This is a well known technique which is used in a majority of existing optical data storage systems. At addresses with a burn-spot, the reflection becomes weaker (stronger for some types of burn-films) than otherwise, whereby the logical state "0" or "1" of each single address is determined. Transmission: In this case, light is only allowed to pass through the burn-film in positions where burn-spots exist. In analogy with the reflection case, the addresses of interest can be scanned with a laser beam, while at the same time recording through which ones light passes to a photo-detector which is placed on the back/bottom (in the following the front/top is defined as the side where the spheres are placed) . The special data storage media disclosed here, however, permit new and in many cases very simple reading methods to be used. Two concepts are described in the following; in one case illumination is provided from the back, in the other case from the front: Under "Spatial filtering in the Fourier plane" (see Fig. 8) the data storage medium is illuminated with a broad, diffuse light beam from the back. Light source can be for example a lamp or a light emitting diode. Each burn-spot then acts as a light source under each sphere, with a position in relation to the sphere which causes the light after passing through the sphere to follow the direction which the laser beam had during recording. Address determination is effected in two steps: a lens first focuses the illumination in one plane (Fourier plane) where light from all burn-spots which were recorded under a given direction (Θ, φ) passes through the same point, characteristic for that burn-direction. Thereafter, the light which passes through each of these characteristic points, is separated by means of a hole mask (e.g. time controlled electro-optically) , mirror or the like. For each light bundle an imag__T of the data storage medium will be created in a plane behind the Fourier plane, where burn-spots which were recorded in a given direction (Θ, φ) appear bright against a dark background. The surface position (x, y) on the area can thereby be determined by means of one or more photo detectors. In this manner a complete address-set (x, y, Θ, φ) can be obtained for each direction (Θ^, φj) which is accessible for data storage in the given medium. An alternative reading method may be termed "directional illumination" , where the data storage medium is illuminated from the side where the spheres are located. Only light with an angle of incidence towards the spheres corresponding to one of the directions which were applied during recording, will be able to pass through a burn-spot, see fig. 9A. By illuminating a larger area of the data storage medium using the angle of incidence (0^, φj) , it becomes possible to determine from the backside of the medium which burn-spot positions (x, y) on the medium that has this direction in its address. This is illu¬ strated in fig. 9B, where a group of four holes has been burned under each one of some neighbouring spheres. As shown, it is possible by means of directional illumination to have the light pass selectively through holes which correspond to each of the four burn-directions. By systematically illuminating in all accessible burn-directions, it is therefore possible to determine the logical state "0" or "1" for complete address sets (x, y, Θ, φ) . During recording and (in certain cases) reading, the laser beam has to be positioned and oriented at such an angle that ea single sphere is struck correctly. In analogy with today's optical data storage techniques, this might be achieved with a system that directs a weak (which means not intense enough to affect the burn-film) laser beam to the desired address by mea of an optical control track or guide in the burn-film. These tracks or guides must have an unequivocal spatial relationship to the sphere positions, and could have higher or lower reflectivity than the rest of the burn-film. Alternativel one can make use of the fact that the spheres are immobilized in relation to the burn-film, in a pattern that can serve as a coordinate reference in the plane. Provided that the burn-film is sufficiently reflecting, the modification of the weak laser beam reflection when the beam strikes the spheres could be applied as guidance criterion. One disadvantage of such techniques is, that they are not applicable for systems based on light that is transmitted through burn-spots in data carriers. As far as we know, reading by reflection is the only method employed with optical data storage systems which are at present on the market. In US pat. no. 4.542.288 Drexler claims that data storage on reflecting media is advantageous because, e.g. automatic focusing is easier to implement. This is not surprising, since the burn- film does not allow light to pass through. In our case, however, optical guide marks can be establish in a very simple manner, and these marks can be applied in both reflection and transmission based systems: After the data storage medium has been manufactured, it is exposed to a strong light flash from a laser or a flash lamp which exposes a large area of the data storage medium simultaneously. The light strikes the plane where the spheres are deposited in a directio perpendicular to the plane, and the intensity is controlled such that changes in the burn-film only take place in a small area in the center under each sphere. The sphere's lens effect thus causes a small well defined burn-spot to be made, similar to burn-spots which are obtained during laser recording of data (laboratory experiments have shown that this is relatively easi achieved) . Burn-spots created during the light flash are thereby automatically positioned correctly each in relation to its sphere. At spheres that are located somewhat off their nominal position, the burn-spot is formed correspondingly displaced. If a sphere were lacking in a given position on the data storage medium, no positioning burn-spot would be formed at that point. In data storage media where the burn-spot is a hole in the burn-film through which light can pass, it is possible to create, e.g. by illumination of the medium from the opposite side of the burn-film, a well defined light source related to each sphere, which can be used for automatic positioning and focusing during recording and reading of data. It should be pointed out that the optical control mark not necessarily needs to be located centrally under each sphere, but can be achieved with oblique illumination. It can be of advantage that certain data are recorded before a user starts the first recording. When the data storage medium is delivered to the user, it is as mentioned above, typically equipped with optical control guides for focusing and positioning of the recording and reading systems. Also, various other types of information may have been stored, for example, address or control codes. Elementary pre-recorded information of that type becomes common to all users of a certain type of optical data storage medium, for example one category of data card. However, in addition it may be of interest for many users to prerecord user specific information which is duplicated on a great number of identical cards. Such users may be organizations, insurance companies etc. , which wish to store expiration data, user codes or the like on cards that are sent to members as the end users. Alternativel , it may concern data programs, which are distri¬ buted in great numbers etc. In principle recording of such information is possible with a standard equipment for recording, which either is used directly or is modified with respect to automatic handling of the cards. This may, however, become very time consuming and may be expensive: the number of cards to be prerecorded can be very large (from thousands to millions) , and in certain cases it will at the same time be of interest to store considerable amounts of data (e.g. data programs) on each card. On this background it is desirable to have a cheaper and more efficient alternative to standard laser recording. As far as we know, there exists at present in the technical and scientific litterature no technical solution to this problem. Admittedly, Drexler discloses in US pat. no. 4.542.288 pre¬ recording of data on cards by means of photolithography, laser recording or surface molding. However, this has to be done before the card is sealed and sent to the users, and is in most cases probably limited to simple basic information as discussed above. A seemingly simple alternative is to apply masking technique in analogy with the light exposing step in photolitho¬ graphy: A mask which has holes where burn-spots are desired, is placed over a data storage medium and in register with it (which means, the mask is placed with the holes in correct position in relation to the data storage medium) . The data storage medium is then illuminated through the holes in the mask thereby obtaining burn-spots in the right places. However, two problems arise: First, the light's wave nature causes it to spread fan-like behind the holes, and the shadow pattern becomes blurry. The deviation from the geometric shadowing increases, the smaller the holes, and the larger the distance from the shadowing mask. Practical optical data storage media are typically equipped with a protective film of 150-500 μm in thickness. This means in practice that recording through a mask on media that have been through the complete manufacturing process (i.e. are covered with protective film) cannot be performed by means of mask-technique as long as the burn-spot size is supposed to stay well below approx. 4 - 8 μm in diameter. Thus, all of todays data storage media are excluded, with the possible exception of media with particularly low data storage density. As far as we know, only Drexler Technology Corp.'s Lasercard may be of relevance in this connection. The other problem is less fundamental, but of great practical and economic importance: Reading of data requires that the light intensity and the pulsation energy are suffi¬ ciently high at the point where the burn-spot is to be created. When using the mask technique a large area (which means the whole mask) is exposed simultaneously and the light source must be sufficiently intensive over that complete area. This can mean, that instead of a flash lamp a relatively strong laser beam may be required, which easily can become a dominating and prohibitive cost element in recording equipment, intended for markets where users are numerous, each with their own equipment ("distributed users") . In the present invention these problems are circumvented: First, only light spots of the size of the focusing optical structure need to be defined during illumination through the mask. The dimensions of the structures and the thickness of the protective film are adjusted to each other, while simultaneously a high data storage density is maintained by applying many directions for recording and reading, as discussed before. Second, the structures (e.g. spheres) collect light energy over a large part of their cross section and concentrate it in a considerably smaller area (burn-spot) . Thereby the power/energy requirements of the light source are reduced. The focusing micro-optics (e.g. spheres) in the data storage medium itself may thus be viewed as an integral part of the optical reading and recording systems. Micro-optics can have an "assisting role" so that the requirements for the remaining optical and mechanical system-components can be reduced, but they can also lead to qualitatively new possibili¬ ties in optical data storage. In the following both types of advantages/possibilities are shortly summarized: a) High data storage density combined with an uncritical positioning and focusing during recording and reading: Not the burn-spots, but the considerably larger focusing optical structures (spheres) define the optical and mechanical requirements for the recording and reading equipment. This leads to an increased depth of focus and lower requirements for positioning with subsequent simplifications and cost reductions for recording and reading systems, as well as for the data storage medium itself (planeness etc.). In typical difficult environments, an optical data storage system based on integrated optical structures (e.g. spheres) in the data storage medium will be less critical and tolerate more vibrations, temperature changes and other physical disturbance parameters. This can be of importance in airplanes and for military use. b) Possibilities for prerecording of data by means of mask technique, cf. above: Each optical structure, e.g. sphere, on a data storage medium which is to be illuminated selectively through holes in the mask, is so large that diffraction-effects behind the holes can be tolerated. This includes practical media with a protecti film. At the same time, the structures collect light from an area which is considerably larger than the area of the burn- spot, which permits the use of correspondingly weaker light sources. c) Oblique recording and reading permit directed data accessibility and increase data security: The reading equipment must be adapted to the same angles (Qj . . φj) which were defined during recording. It is fully possible to supply different user groups with equipment which only can read at some of the angles, but not all which were used during recording. The angles which are not accessible for a certain user group can, for example, store information which only is meant to be read by other user groups. The angles (Θ-^, φj) need not be defined before recording. Thus, completely manufactured media can be delivered from factories and thereafter be used for recording at user-specifie sets of angles. Reading is thereafter only possible by applying the same angles. This represents a certain protection against reading with "pirate equipment". d) The medium is well suited for data-reading by transmission: The task of easy establishing of optical guide marks can probably be solved by illuminating the data storage medium in such a manner that burn-spots only are created where optical structures with focused light are located. Furthermore, less stringent requirements for focusing and imaging (see a) herein above) means that the relatively large optical path lengths through the data storage medium, which must be expected during reading with transmission, can be tolerated. A considerable advantage in using transmission instead of reflection consists in the large freedom of choice of the burn- film. It no longer needs to possess a controlled reflection ability, but can independently thereof be optimized with respect to burn-threshold, stability and production costs. Further, possibilities arise to use films with special proper¬ ties, for example reversible burn-films, fluorescent dyes which are bleached in the burn-spot area during recording, or dyes which only can be recorded or read at one or more defined wave lengths. A potentially important advantage with transmission is tha double refraction in the data storage medium, which was mentioned earlier as a problem, has little or no importance. e) Simple and fast reading: Because of their special properties, data storage media wi spheres can be used in new types of reading equipment based on extended surface illumination of the medium (i.e. not laser scanning) combined with imaging in a detection system which, for example, can be an electronically scanned matrix which contains a large number of single detector elements, see below. Such reading systems can be very simple and compact, and allow parallel reading from several areas on the data storage medium simultaneously. When employing large detector matrices, etc. it becomes possible to achieve high reading speed and short "random access" time (today's data storage systems have the disadvantage of slow random access due to the need for mechani movement of the laser, the data storage system and/or the optics, during reading). It is no trivial task to manufacture a data storage mediu according to the invention, for example of the types with transparent spheres as optical structures. The spheres have to be placed as monolayer onto the burn-film itself or in a small well defined distance from it; they have thereafter to be fastened and protected. In practice the spheres must probably also be positioned with high precision in a predefined pattern. Several techniques for controlled positioning can be of interest, see further down. So far results from practical tests suggest, that it will be possible to achieve good technical solutions of the problem concerning positioning of the spheres. One might expect that focusing microstructures, e.g. hemispheric elevations which are stamped into a transparent layer over the burn-film, can replace the spheres. In analogy with production processes for compact discs (CD) , for example, such structures could be stamped in large numbers by means of a master. Closer studies show, however, that the use of stamped or pressed structures require that certain non-trivial problems be solved, cf. below. Factors favoring the sphere solution compared to stamped o pressed structures are partly connected with the focusing, partly with the energy situation during recording of data: The number of recording directions (Θ^, φj) which can be assigned to each focusing element, N, is an essential factor. A high N implies strict requirements on the shape of the focusing element and its surface quality. More important here is probably the small distance tolerances (μm or less) between the focusing element and burn-film, which have to be observed over macroscopic distances (some cm) . If stamping or pressing is applied to a transparent layer on top of the burn-film, which itself is mounted on a plastic material, it may prove difficult to achieve a correct distance to the burn-film over the whole data storage medium in practice. In addition, the burn-film must not be locally deformed during stamping/pressing, even if the structure to be made (e.g. hemisphere) has a profile height which is comparable with the distance to the burn-film. When spheres are used, however, it is relatively easy to achieve full control of the focal conditions, provided that the spheres are monodisperse and have small deviations from perfect spherical shape. - In general, it is desireable to employ the lowest possible power/energy per recorded data bit. The focal distance of a stamped/pressed hemispheric area is about twice as large as of a sphere of corresponding size, and the burn-spot area about four times larger. To a first approximation the sphere alterna¬ tive is more advantageous by a factor of 4. This situation is further improved by a factor of about 2, because burn-films which are related to stamped/pressed focusing structures are in contact with solid material on both sides, while sphere-based data storage media typically have air on one side of the burn- film and solid material on the other. In sum, this means that data storage media with stamped/pressed focusing elements require more power/energy for recording than media with spheres. In addition to dimensioning the recording laser, this can be of importance for achieving the smallest possible size of the bum-spot, the fastest possible recording of each bit etc. (the "damage" process in the burn-film during reading can be highly non-linear with respect to energy or power density) . To illustrate the practical feasibility of the invention, we describe below some embodiments where critical features have been verified in practical tests. On the surface of a transparent substrate consisting of, e.g. polycarbonate, a pitted pattern is stamped/pressed with a die (a "master") . In analogy to the process for the production of compact discs [CD-records] , the master can be produced by means of photolithography, followed by vacuum deposition, followed by electrolytic coating. Also the stamping/pressing- process itself can be performed in analogy to CD production, where large scale production techniques have reached an advanced stage of development. After the pits have been stamped/pressed into the substrat a burn-film is applied onto the stamped/pressed surface. This can, for example, be done by depositing tellurium under vacuum, whereby an even, opaque layer on the bottom of each pit is obtained. One sphere is placed in each pit by trickling from the liquid phase or by dry brush application. This is a non- trivial task which, however, shall not be discussed any furthe here. Suffice it to state here that tests made until now, show practical feasibility: Substrates with pits of 1-2 μm in depth and a diameter in the range of 2-15 μm have been photolitho- graphically manufactured. Fig. 10A shows spheres with a diameter of 7.1 μ which were deposited by means of trickling from the liquid phase to a matrix of pits, each with a diameter of about 5 μm. Despite of the simple non-optimized process, a high filling degree was achieved. A corresponding result was obtained by the dry brush method, see Fig. 10B, which shows spheres with a diameter of 6.4 μm of the same pitted pattern. Data storage media with pits can be manufactured on several levels of sophistication: Fig. 11A shows the simple case where the spheres are in the pits, directly on the burn- layer. In Fig. 11B the pit diameter is adapted to the size of the sphere, such that the latter is kept in the optimal focusing distance relative to the burn-layer at the bottom of the pit. This requires use of monodisperse spheres. In Fig. 11C the bottom of the pit is shaped like a part of a spherical surface, concentric with the sphere. Thereby ideal focusing on the burn-layer is achieved for all angles of incidence, as well as perfect retro-reflex for systems based on reading with reflection. After deposition of the spheres, the medium is encapsulate with a protective film of, e.g. transparent polycarbonate, see Fig. 12. A relevant total thickness of the memory medium is 0.8 mm, an ISO-standard for credit cards. Oblique recording does in practice not necessarily imply large technical complication. A simple technique, which permits illumination of one and the same sphere from many directions without readjustment of the light beam in each direction is shown on the principle sketch on Fig. 13: All incident beams, that are parallel with each other, wil af er having passed through the illumination optics, be refracted in such a manner that they strike the same point (the sphere center) from different directions. Only a fraction of the illumination optics aperture is used for each direction. This is achieved by having a laser beam with limited diameter strike different positions on the aperture, depending on the desired light direction towards the sphere. Alternatively, partial screening of the fully illuminated aperture can be applied. In both cases it is possible to choose the direction without mechanical movement of components (not discussed furhter here) . The principle solution of Fig. 13 requires a reasonable choice of parameters and components, where the f-number and aperture of the optics are adapted to the sphere diameter, illumination angles and their tolerance. Again it turns out that large spheres make it easier to find practical solutions. With respect to reading with directional illumination, one of the techniques which was mentioned above in connection with reading under light transmission shall be discussed: A simple light source such as a LED illuminates the data storage ' medium from a direction (Q , φj) which corresponds to one of the reading angles, see Fig. 9A, B and Fig. 14A. A large area on the medium with many spheres is illuminated simul¬ taneously from the side on the burn-film where the spheres are placed. The light has almost plane-wave-character at each single sphere, and the focusing in the sphere deviates little from the one during the preceding recording with the laser beam. After focusing in the sphere, the light will pass through the burn-film, provided a burn-spot (a "hole") had previously been created in that direction during the recording of data. Light that passes through the holes in the burn-film is recorded by means of a simple optical system which does not need to resolve each hole: since the direction (θ-j_, φj) under which the illumination takes place is already known, it is sufficient to determine at which sphere positions (x, y) light is transmitted. This can be done, for example, by means of a detector matrix with one or more detector elements, assigned to each sphere position by "proximity" (Fig. 14B) , optical fiber (Fig. 14C) or imaging (Fig. 14D) . The number of detector elements per matrix can be large (CCD-matrices for TV cameras contain several hundred thousand elements) . Thereby correspondingly large blocks of the data storage medium can be read quickly by electronic scanning, and the whole medium can be covered by a small number of mechanica displacements. Intermediate solutions are conceivable: An alternative to large detector matrices which "stare", are, for example, detector arrays which scan. If the medium is not too broad (e.g. tape) the matrix can cover the whole width of it. Mechanical displacement can in that case be obtained by pulling the medium in one' direction, preferably continously. Large matrices, however, place more stringent requirements on reading system and data storage medium, and it becomes e.g. more difficult to achieve register between the sphere's position and the assigned detector element for all sphere positions in the block. In this connection, the data storage system according to the invention offers special advantages: It is considerably easier to achieve register with a lower number of relatively large focusing structures (spheres) , than with a larger number of smaller data spots in a traditional optical data storage medium. Indeed, simple imaging analysis shows that in many relevant cases, there is a dichotomy where the one is practical achievable while the other is not. Solutions based on redundanc (several detector elements assigned to each focusing structure or burn-spot on the data storage medium) , or fast-scan near nominal positions will hardly change this fundamental situation After illumination in a given direction (Θi, φj) this LED can be turned off, and another LED is turned on, which provides reading in a new direction (θ^, <pτ , etc. until all directions in question have been covered. This can be done in a very fast sequence, while the data storage medium is immobile during the illumination cycle. In practice light sources can be used which turn on and off with such a speed that the relative displacemen between the medium and the reading equipment during the illumination cycle is negligible, even at relative speeds up to many m/s. By employing mutually spectrally adapted light source/ detector element pairs, possibilities arise for simultaneous parallel reading of data in several directions. It is evident that reading equipment in many sub-categories can easily be manufactured, where each category only has illumination possibilities in a smaller number of reading directions (see paragraph C concerning control of data acces¬ sibility) . Finally it should be remarked that, even if the data storag technique which is the essential feature in the present invention, concerns in principle visually non-readable data spots which are read and interpreted independently, there is actually no hindrance to achieve additional indications which also are visible to the eye, by using the same technique. In the latter case, visible features are produced through correla¬ tion of data points in macroscopic areas to create visible images by "cooperation". Such images can be visible from all, or only a limited number of directions. Of course, a practical data storage medium (card) can be additionally equipped with visual indications which are created by printing.

Claims: P A T E N T C L A I M S 1. An optical data storage medium for the storage of data in a number of elementary cells in the form of localized areas which are read and interpreted individually, said medium including a wholly or partially light absorbing film, here termed the burn-film, said burn-film being able to change locally and possibly reversibly its optical properties under the influence of strong localized illumination, ' said ability being applied for recording data on said medium, characterized by optical structures with characteristical dimensions less than 100 μm in at least two mutually orthogonal directions, positioned in close proximity to the burn-film for refractive influence on and/or control of the illumination towards the burn-film, said optical structures constituting an integral part of the data storage medium. 2. The optical medium of claim 1 wherein the optical structur consist of structural modulations in an essentially transparent film above the burn-film. 3. The optical medium of claim 2 wherein the modulations are surface modulations of mechanical/geometrical character. 4. The optical medium of claim 2 wherein the modulations are bulk modulations of the complex optical refractive index induced by the introduction or removal of ions or molecules in defined localized regions of the film. 5. The optical medium of claim 1 wherein the optical structur consist of a reflective layer positioned at an adjusted distanc underneath the burn-film, said burn-film being partly transpare to said illumination, and said reflective layer having geometri modulations. 6. The optical medium of any of the previous claims wherein the optical structures are designed for concentrating or focusing incident light beams on the burn-film. 7. The optical medium of claim 1 wherein the optical structure consist of a plurality of separate, totally or partially transparent and optically refracting objects placed above the burn-film. 8. The optical medium of claim 7 wherein the optically refracting objects are spheres. 9. The optical medium of claim 8 wherein the spheres have essentially the same diameter and bulk properties. 10. The optical medium of claim 8 or 9 wherein the spheres lie in contact with the burn-film. 11. The optical medium of claim 8 or 9 wherein the spheres lie above depressions or pits in a substrate with the burn-film covering the bottom of the depressions. 12. The optical medium of claim 11 wherein the dimensions of the depressions are adapted to the sphere diameter for achieving optimum focusing of the illumination on the burn-film. 13. The optical medium of claim 11 or 12 wherein the bottom of each depression is shaped concentrically in relation to a sphere which lies in a stable position on top of the depression. 14. The optical medium of any one of claims 8-13 wherein the sphere diameter is in the range 1-100 μm. 15. The optical medium of any of the previous claims wherein the optical properties of the burn-film have been changed locall through intense pre-illumination which via the optical structure is localized to a particular region of that burn-film area which is assigned to each respective optical structure, said pre- illumination being adapted for striking a predetermined number of said structures in a uniform manner, said particular burn-fil regions being generated for guidance and control purposes in connection with subsequent recording and reading of data on/from said medium. 16. A method for recording data on an optical data storage medium of the type described in any one of the previous claims, c h a r a c t e r i z e d b y directing intense illuminatio selectively toward the medium from a number of different directions, each respective illuminated optical structure thereby effecting the reversible or irreversible change of said optical properties of said burn-film selectively in a correspon ding number of localized areas relating to each optical structure. 17. A method according to claim 16 wherein the medium is illuminated through a mask, allowing light to pass through only to certain of said optical structures. 18. A method according to claim 16 wherein the various directions of the illumination are achieved by parallel translation of a light beam through various parts of the entrance side of one and the same optical focusing system, by selectively exciting permanently positioned, separate light sources or by selective partial blocking of a broad light beam at the entrance side, causing the light to pass through differe parts of the focusing system. 19. A method for reading of data from an optical data storage medium of the type indicted in any one of claims 1-15 wherein determination of the position of reversibly or irreversibly changed localized areas in the burn-film is done by supplying diffuse illumination toward said data storage medium, by spatia filtering of light emerging from said medium in an area spaced from an optically transforming system placed outside said medium, and by imaging of said medium in a focal plane of the optically transforming system, with light corresponding to separate predefined directions from said optical structures. 20. A method for reading data from an optical medium of the type indicated in any one of the claims 1-15 wherein determi¬ nation of the position of reversibly or irreversibly changed localized areas in the burn-film is performed by illuminating said medium from predetermined selective directions, and read¬ out correlated with each direction, of light emerging from said medium, by means of light detector single elements or a light detector matrix in one or two dimensions, possibly operating in a scanning mode.

Inventors: NORDAL PER-ERIK, NORDAL, PER-ERIK
Applicants: DYNO PARTICLES AS, DYNO PARTICLES A.S
Application year: 1991
Main classification: G11B7
IPC codes: G06K19, G11B7