Optical reproduction medium and method of reproducing data stored therein

Abstract: The present invention provides an improved light-reproduction medium storing data therein to be reproduced by detecting light transmitted therethrough and/or light reflected therefrom. The light-reproduction medium comprises a substrate formed on a surface thereof with at least two recording pits, and may have (i.e. the phrase should read "...at least two recording pits, and may have a magnetic film (4)...") a magnetic film (4) formed on the surface of the substrate (1). The recording pits (2a,2b,2Aa,2Ab,2B,2Ca,2Cb,2Da,2Db) have different level from the surface of the substrate (1), each of the recording pits having a cross-section selected from at least two different shapes. The present invention provides a light-reproduction medium having memory density several times greater than a conventional CD-ROM without changing CD-ROM fabrication technique and an optical head structure, resulting in significantly increased capacity of an optical disc or an optical card.

Description: The invention relates to a light-reproduction medium, in particular to a light-reproduction medium such as an optical disc and an optical card to be used to reproduce data stored therein by projecting lights thereto and analyzing lights reflected therefrom. The invention also related to a method of reproducing data stored in a light-reproduction medium, and a reproduction apparatus for reproducing data stored in a light-reproduction medium. In particular, the invention relates to a light-reproduction medium capable of accomplishing highly densified recording. Various attempts have been made to highly density a light-reproduction medium such as CD-ROM which is an optical disc used only for data regeneration. An example of CD-ROM is illustrated in Figs. 1A and 1B which a plan view of a part thereof and a cross-sectional view taken along the line B1-B1 in Fig. 1A. As illustrated, CD-ROM comprises a substrate 1 formed on a surface thereof with a plurality of recessed portions each of which acts as a recording pit 2, and a reflection film 7 covering the surface of the substrate 1. In operation, lights are projected to the surface of the substrate 1 with one of an optical head or the CD-ROM being moved in a direction indicated with an arrow Y, and lights reflected from the substrate 1 are detected. Then, the reflected lights are detected to thereby identify recessed or raised portions of the surface of the substrate 1 of which the recording pit 2 is constituted. The thus detected light intensity is converted into signals, and thus data stored in the CD-ROM are reproduced. Hereinbelow, though not explained each time, an optical disc such as CD-ROM is to be moved relative to an optical head between a top and a bottom of a figure, namely in a direction indicated with the arrow Y in Fig. 1A, for instance. For fabrication of such CD-ROM as above mentioned, there is used a basic pattern board called a stamper which is formed on a surface thereof with recessed and raised portions acting as recording pits storing data therein. By injection mold technology, the recessed and raised portions are copied on a polycarbonate substrate, and then a reflection film formed from metal such as aluminum is deposited on the polycarbonate substrate. The stamper is fabricated with exposure technology called mastering, and hence, the memory density of CD-ROM depends upon how fine recording pits can be fabricated with the mastering. In order to meet the demand of highly densified light-reproduction medium in these days, one considered solution is to fabricate a recording pit in a smaller size. To this end, it is necessary to fabricate the recessed and raised portions of the stamper in a smaller size, which in turn requires a smaller-sized mastering. However, there is limitation to the reduction of size of mastering, and hence it is almost impossible to carry out higher density of a light-reproduction medium. Thus, a new technique for accomplishing higher density of a light-reproduction medium needs to be developed in place of the mastering. For instance, Japanese Unexamined Patent Publication No. 47-26104, which is based on Dutch application No. 7103233 filed on March 11, 1971, has suggested a circular disc shaped data carrier which contains aural and video signals encoded to optical signs or which contains the aural and video signals in swirl arrangement, and also has suggested a reader for the data carrier. EP-A-0,633,565 describes an optical disk on which information is readable based on a laser light reflected by an information recording surface. The information recording surface includes a surface transformed portion on which a plurality of transformed shapes, each corresponding to the information, are arranged so that the polarization conditions of light reflected by the transformed shapes differ according to the information. EP-A-0,594,193 describes an optical disk on which there are formed a plurality of concavo-convex pits, multivalued data stored on the disk corresponding to the depth of the pits. EP-A-0,553,548 describes an optical disk having a recording surface on which a plurality of tracks are formed, and information pits formed on the tracks. Each pit has a first pit portion having a first level from the recording surface and a second pit portion having a second level lower than the first. EP-A-0,553,573 describes an optical disk on which information is recorded in the form of an information pit. The information pits have a plurality of pit portions each of which is formed as a combination of pit fragments, each having a predetermined pit height. EP-A-0,546,525 describes an optical disk including at least one tracking groove and a plurality of pits arranged in between the spaces divided by the tracking groove. EP-A-0,479,577 describes an optical disk having tracking tracks and recording tracks interposed between the tracking tracks. The width of the recording tracks in a specific region is larger than that in another region. It is an object of the at least the preferred embodiments of the present invention to providing a light-reproduction medium capable of accomplishing higher densification thereof without mastering technology. It is another such object to provide a method of reproducing data stored in a light-reproduction medium, and a reproduction apparatus for reproducing data stored in a light-reproduction medium both without mastering technology. In one aspect, the present invention provides a light-reproduction medium comprising a substrate with recording pits formed on a surface thereof, at least two of said recording pits having a different cross-sectional profile in a plane perpendicular to a direction (A) in which the light-reproduction medium is moved relative to an optical head, characterised in that the respective cross-sectional profiles of said at least two pits are selected from a rectangular shape, a triangular shape, and a trapezoidal shape. It is possible to detect a difference in cross-sectional shape by utilizing mutually perpendicular polarized lights, thereby increasing multiplicity of stored data and accomplishing higher densification. A magnetic film may be formed on the surface of the substrate. The at least two of the recording pits may have a different width in said plane perpendicular to a direction in which the light-reproduction medium is moved relative to an optical head. It is possible to detect a difference in width by utilizing mutually perpendicular polarized lights, thereby increasing multiplicity of stored data and accomplishing higher densification. The at least two recording pits may be asymmetrical in shape about an axis passing through a midpoint thereof and parallel to the direction A. The at least two recording pits may have a different level from the surface of the substrate. It is possible to detect a difference in cross-sectional shape by measuring received light intensity at a side facing to the axis, thereby increasing multiplicity of stored data and accomplishing higher densification. Lands or grooves may be formed on said surface in a region in which said at least one recording pit is not formed, the lands or grooves extending in a direction in which the light-reproduction medium is moved relative to an optical head and having a depth measured normal to the surface of a substrate which is different to that of said at least one recording pit. Preferably, the lands or grooves have a depth of 1/10 to 1/30 of a wavelength of an incident light or an integral number of 1/4 of a wavelength of an incident light. It is possible to increase multiplicity in a region where recording pits are not formed, thereby accomplishing higher densification. In a second aspect, the present invention provides a method of reproducing data stored in a light-reproduction medium, comprising the steps of: (a) projecting mutually perpendicularly intersected polarized lights to a light-reproduction medium including a substrate with recording pits formed in a surface thereof, at least two of the recording pits having a different cross-sectional profile in a plane perpendicular to a direction (A) in which the light-reproduction medium is moved relative to an optical head, characterised in that the respective cross-sectional profiles of said at least two pits are selected from a rectangular shape, a triangular shape, and a trapezoidal shape and (b) reproducing data from polarized lights reflected from or transmitted through the light-reproduction medium. The inventor has found that if polarized lights are projected to a groove or a land composed of magnetic substance, the reflected lights have peculiar characteristics. On the assumption that when polarized Gaussian beam is projected to magnetic substance having a groove or a land formed thereon, an intensity of lights scattered from the magnetic substance is represented with R, and Kerr rotation angle represented with , Fig. 2 shows the dependency of a product R  on a shape of the groove or land. Hereinbelow, the term "a cross-section of a groove or a land" means a cross-section of a recording pit as viewed in a direction perpendicular to a direction in which a light-reproduction medium is moved relative to an optical head. As illustrated with an axis of abscissa in Fig. 2, it is assumed that a cross-section of a groove or a land is varied from a V-shape to a rectangle. A left end of the abscissa indicates a V-shape, and a right end indicated a rectangle. A groove or a land comprises an inclined portion and a flat portion. The axis of abscissa in Fig. 2 indicates a half width of the flat portion in the case that an entire width of a groove or land of which the recording pit is constituted is fixed. The data shown in Fig. 2 is that obtained when a groove or land is relatively wide, namely when a width of a groove or land of a recording pit is twice as long as a wavelength of an incident light. It is understood in Fig. 2 that a product R  is quite different in dependence on s-polarization, p-polarization, incidence to a land, or incidence to a groove when the groove or land is not rectangular in shape. On the other hand, it is also understood that a product R  keeps almost the same when the groove is rectangular in shape. Herein, an orientation of s-polarization means a direction parallel to the groove or land, whereas an orientation of p-polarization means a direction perpendicular to the groove or land. In view of the above mentioned phenomenon, it is understood that it is possible to detect whether a recording pit is constituted of a rectangular or V-shaped groove or land by concurrently radiating s- and p-polarized lights to magnetic substance having recessed and raised portions, and calculating a difference between outputs. When a recording pit has a rectangular cross-section, a differential output is zero, whereas when a recording pit has a V-shaped cross-section, a differential output is a certain finite value. The concurrent radiation of s- and p-polarized lights means radiation of polarized lights oriented to a direction other than a direction parallel or perpendicular to a direction in which a light-reproduction medium is moved relative to an optical head. Hereinbelow, a direction in which a light-reproduction medium is moved relative to an optical head is referred to simply as a direction Y. An incidence angle of polarized lights is preferably 45 degrees relative to the direction Y. Thus, it is possible to obtain doubled multiplicity of a recording pit by additionally forming a magnetic film on a substrate to be fabricated in accordance with a conventional CD-ROM fabrication method, and forming the substrate with two types recording pits, namely a rectangular cross-sectional one and a V-shaped cross-sectional one. Fig. 3 illustrates the same phenomenon as Fig. 2. However, the data shown in Fig. 3 is that obtained when a groove or land of a recording pit is relatively narrow, namely when a width of a groove or land is equal to about 1/2 of a wavelength of an incident light. The tendency in Fig. 3 is essentially different from the tendency in Fig. 2 in that a product R  is different in dependence on s-polarization, p-polarization, incidence to a land, or incidence to a groove even when the groove or land is rectangular in shape. In view of this fact, it is understood that a width of a groove or land can be detected as to whether it is large or small by concurrently radiating s- and p-polarized lights and measuring a difference in outputs in the case that a recording pit has almost rectangular cross-section. That is, if a width of a groove or land is great relative to a wavelength of an incident light, a differential output is equal to zero or almost zero, as illustrated in Fig. 2, whereas if a width of a groove or land is small relative to a wavelength of an incident light, a differential output is equal to a certain finite value, as illustrated in Fig. 3. In general, it is preferable that one of grooves or lands have a width greater than 1/2 of a wavelength of an incident light, and the other have a width smaller than 1/2 of a wavelength of an incident light. Thus, it is possible to obtain doubled multiplicity in a recording pit by additionally forming a magnetic film on a substrate such as conventional CD-ROM, and varying a width of a recording pit to be greater or smaller than a threshold value. If a recording pit formed on a substrate such as conventional CD-ROM without the above mentioned magnetic substance is formed to have a cross-section which is asymmetrical about an axis passing through a midpoint of the recording pit and parallel to the direction Y, quantity of reflected lights is also asymmetrical about the axis. Hence, a combination of a recording pit having an asymmetrical cross-section and another recording pit having a cross-section obtained by rotation of the former recording pit by 180 degrees about an axis thereof provides a pair of recording pits having different symmetry with respect to reflected light quantity. Accordingly, it is possible to identify two different recording pits by using a photodetector divided into two sections in a direction parallel to the above mentioned axis, and measuring a difference between these two sections. This means that the multiplicity of a recording pit is doubled. Thus, it is possible to increase the multiplicity of a recording pit or recording pits in the above mentioned ways, however, a region where a recording pit or recording pits is (are) not formed remains to have the multiplicity of one (1). In order for such a region to have an increased multiplicity and keep a difference from a recording pit in quantity of reflected lights, it is necessary for such a region to have a groove or land which has the same configuration as a recording pit and which is quite shallower or lower than a recording pit, or have a groove or land which has the same configuration as a recording pit and which has depth or height equal to several times multiplied 1/4 of a wavelength of an incident light. Since quite shallow groove and low land have almost the same reflection intensity as a flat surface, they do not lose a difference from a recording pit in quantity of reflected lights. A groove or land having depth or height equal to k-number (k is an integer greater than 1) times multiplied 1/4 of a wavelength of an incident light would have reflection intensity of almost zero when k is an odd number, whereas would have the same reflection intensity as a flat groove or land when k is an even number. Thus, the groove or land would not lose a difference from a recording pit in reflection intensity. Accordingly, the formation of a groove or land in a region in which a recording pit or recording pits is (are) not formed in a conventional substrate in accordance with the above mentioned conditions increases the multiplicity in such a region with a difference from a recording pit or recording pits in quantity of reflected lights being maintained. Thus, it is possible to increase memory density by t-number times relative to conventional CD-ROM (t is equal to the number corresponding to the multiplicity). Among various optical systems for reproducing data stored in a light-reproduction medium, an optical system which is of type of measuring a difference between s- and p-polarized lights can divide lights into s-polarization and p-polarization, for instance, by disposing a half-wave plate between an objective lens constituting a part of reproduction optical system of conventional optical magnetic disc medium and a polarized-beam splitter disposed closest to the objective lens. In addition, if only a conventional photodetector for regeneration is divided into two sections, it is possible to read out data stored in asymmetrically shaped recording pits. In addition, the disposition of a half-wave plate is compatible with the division of a photodetector. When both a half-wave plate and an optical system including a polarized-beam splitter for dividing lights into s- and p-polarized lights are to be used, in general, two photodetectors are used. In such a case, each of the photodetectors is divided into two sections in the direction Y. When an optical system including a Wollaston prism for dividing lights into s- and p-polarized lights is to be used, a single photodetector is used. In such a case, the photodetector is to be divided into four sections in the direction Y. Preferred features of the present invention will now be described, purely by way of example only, with reference to the accompanying drawings, in which:- Fig. 1A is a plan view illustrating conventional CD-ROM; Fig. 1B is a cross-sectional view taken along the line B1-B1 in Fig. 1A; Fig. 2 shows the dependency of R  on a cross-sectional shape of a groove or land when a groove or land has a relatively wide width, wherein R represents an intensity of lights scattering from magnetic substance, and  represents Kerr rotation angle the scattering lights; Fig. 3 shows the dependency of R  on a cross-sectional shape of a groove or land when a groove or land has a relatively narrow width; Fig. 4A is a plan view illustrating recording pits made in accordance with the first embodiment of the present invention; Fig. 4B is a cross-sectional view taken along the line B4-B4 in Fig. 4A; Fig. 5 is a schematic view illustrating a configuration of a light-reproduction apparatus made in accordance with the present invention; Fig. 6A is a plan view illustrating a variation of a recording pit illustrated in Fig. 4A; Fig. 6B is a cross-sectional view taken along the line B6-B6 in Fig. 6A; Fig. 6C is a cross-sectional view taken along the line C6-C6 in Fig. 6A; Fig. 7A is a plan view illustrating another variation of a recording pit illustrated in Fig. 4A; Fig. 7B is a cross-sectional view taken along the line B7-B7 in Fig. 7A; Fig. 7C is a cross-sectional view taken along the line C7-C7 in Fig. 7A; Fig. 8A is a plan view illustrating still another variation of a recording pit illustrated in Fig. 4A; Fig. 8B is a cross-sectional view taken along the line B8-B8 in Fig. 8A; Fig. 8C is a cross-sectional view taken along the line C8-C8 in Fig. 8A; Fig. 9A is a plan view illustrating recording pits made in accordance with the second embodiment of the present invention; Fig. 9B is a cross-sectional view taken along the line B9-B9 in Fig. 9A; Fig. 9C is a cross-sectional view taken along the line C9-C9 in Fig. 9A; Fig. 10A is a plan view illustrating recording pits made in accordance with the third embodiment of the present invention; Fig. 10B is a cross-sectional view taken along the line B10-B10 in Fig. 10A; Fig. 10C is a cross-sectional view taken along the line C10-C10 in Fig. 10A; Fig. 11A is a plan view illustrating another recording pits made in accordance with the third embodiment of the present invention; Fig. 11B is a cross-sectional view taken along the line B11-B11 in Fig. 11A; Fig. 11C is a cross-sectional view taken along the line C11-C11 in Fig. 11A; Fig. 12A is a plan view illustrating still another recording pits made in accordance with the third embodiment of the present invention; Fig. 12B is a cross-sectional view taken along the line B12-B12 in Fig. 12A; Fig. 12C is a cross-sectional view taken along the line C12-C12 in Fig. 12A; Fig. 13A is a plan view illustrating yet another recording pits made in accordance with the third embodiment of the present invention; Fig. 13B is a cross-sectional view taken along the line B13-B13 in Fig. 13A; and Fig. 13C is a cross-sectional view taken along the line C13-C13 in Fig. 13A. Preferred embodiments in accordance with the present invention will be explained hereinbelow with reference to drawings. Hereinbelow will be explained the first embodiment with reference to Figs. 4A and 4B. A substrate 1 is formed on a surface thereof with recording pits 2a and 2b, similarly to conventional CD-ROM. The recording pits 2a and 2b have a different length in a direction Y in which a light-reproduction medium is moved relative to an optical head. On the surface of the substrate 1 are deposited a dielectric film 3, a magnetic film 4 and a dielectric film 5 on this order in such a thickness as the films 3, 4 and 5 do not change a cross-sectional shape of the recording pits 2a and 2b. Although the recording pits 2a and 2b are shaped into grooves in the following description, the recording pits may be shaped into lands. Although the single magnetic film 4 is sandwiched between upper and lower dielectric films 3 and 5, there may be formed multi-layered magnetic films. The magnetic film 4 may be deposited directly on the substrate 1. As an alternative, a reflection film (not illustrated) may be deposited on the uppermost film or dielectric film 5. The magnetic film 4 may be composed of amorphous alloy including rare earth metals and iron family transition metals, periodical multi-layered film comprising iron family transition metals and noble metals, MnBi alloy, or oxide magnetic substance. It is in particular preferable to use a film composed mainly of TbFeCo. It is also preferable for the magnetic film 4 to contain at least one element having corrosion resistance such as Ti, Cr, Ni, Ta and Pt. The substrate 1 may be made of either synthetic resin such as polycarbonate and acrylic resin or glass. As an alternative, the substrate 1 may be covered with such synthetic resin or glass. The substrate 1 is preferably shaped into a disc or card. The recording pit 2a has a rectangular cross-section. The recording pit 2b has greater length than the recording pit 2a, extending parallel to the direction Y, and has a V-shaped cross-section which is symmetrical about an axis extending perpendicularly to the direction Y. In addition, second grooves 6 are formed on a surface of the substrate 1 in a region where the recording pits 2a and 2b are not formed. The second grooves 6 are shallower than the recording pits 2a and 2b, and extend in parallel with the direction Y. Fig. 5 illustrates a light-reproduction apparatus for reproducing the light-reproduction medium illustrated in Figs. 4A and 4B. The light-reproduction apparatus comprises (a) a first polarized-beam splitter 11 for receiving laser beam from a light source (not illustrated) and splitting the received laser beam into two beams, (b) a second polarized-beam splitter 12 for receiving split beam from the first polarized-beam splitter and further splitting it into two beams, (c) an objective lens 14 disposed in facing relation to a light-reproduction medium 10, (d) a half-wave plate 13 disposed between the second polarized-beam splitter 12 and the objective lens 14, (e) a third polarized-beam splitter 16 for receiving split beam from the second polarized-beam splitter 12 and further splitting it into two beams to transmit them to photodetectors, (f) a second half-wave plate 15 disposed between the second polarized-beam splitter 12 and the third polarized-beam splitter 16, (e) first and second photodetectors 19 and 20 for receiving split beams from the third polarized-beam splitter 16, (f) lenses 17 and 18 each disposed between the third polarized-beam splitter 16 and the first and second photodetectors 19 and 20, and (g) a signal processing circuit 21 for processing signals transmitted from the first and second photodetectors 19 and 20. In operation, laser beam emitted from a light source is projected to a surface of the light-reproduction medium 10 through the first and second polarized-beam splitters 11 and 12, the half-wave plate 13 and the objective lens 14. The light reflected from the light-reproduction medium 10 passes through the objective lens 14 and the half-wave plate 13, and then is split into two beams in the second polarized-beam splitter 12. The thus split beam passing through the second polarized-beam splitter 12 is transmitted to a servo system through the first polarized-beam splitter 11. The other split beam passes through the second half-wave plate 15, and is further split by the third polarized-beam splitter 16. The thus split beams pass through the lenses 17 and 18 to and detected by the first and second photodetectors 19 and 20 each of which is divided at a center thereof into two sections. The light-reproduction apparatus illustrated in Fig. 5 is characterized by the half-wave plate 13 in comparison with a conventional light-reproduction apparatus. The half-wave plate 13 changes polarization of light into linear polarization oriented in a direction other than direction parallel or perpendicular to a direction Y in which the light-reproduction medium 10 is moved relative to the illustrated light-reproduction apparatus. In this embodiment, the half-wave plate 13 changes polarization of light into linear polarization angled by 45 degrees to the direction Y, and causes s- and p-polarized lights to enter onto the light-reproduction medium 10. The light reflected from the light-reproduction medium 10 is changed into polarization in which the light is emitted by the half-wave plate 13. Then, the linearly polarized-light is split into s-polarized light and p-polarized light by the third polarized-beam splitter 16. The thus split lights enter the first and second photodetectors 19 and 20. Thus, the first photodetector 19 detects p-polarized light, whereas the second photodetector 20 detects s-polarized light. As mentioned earlier, each of the first and second photodetectors 19 and 20 is divided into two sections corresponding to a region closer to a center of the light-reproduction medium and a region farther away from a center of the light-reproduction medium, respectively. Hence, the first photodetector 19 outputs a signal A to the signal processing circuit 21 when p-polarized light is detected at the region of the light-reproduction medium 10 closer to a center thereof, and also outputs a signal B to the signal processing circuit 21 when p-polarized light is detected at the regions of the light-reproduction medium 10 farther away from a center thereof. Similarly, the second photodetector 20 outputs a signal C to the signal processing circuit 21 when s-polarized light is detected at a region of the light-reproduction medium 10 closer to a center thereof, and also outputs a signal D to the signal processing circuit 21 when s-polarized light is detected at the regions of the light-reproduction medium 10 farther away from a center thereof. The signal processing circuit 21 receives the signals A, B, C and D, and carries out calculation in accordance with following equations: (A+B)-(C+D), (A+C)-(B+D) and (A+B+C+D). The data stored in the light-reproduction medium 10 can be obtained from the results of the calculation. Thus, similarly to conventional CD-ROM, the light-reproduction apparatus can reproduce data stored in the light-reproduction medium 10 in dependence on a length of the recording pits 2a and 2b in the direction Y by calculating (A+B+C+D) based on the outputs transmitted from the first and second photodetectors 19 and 20. Furthermore, the difference in a cross-sectional shape between the recording pit 2a having a rectangular cross-section and the recording pit 2b having a V-shaped cross-section makes it possible to reproduce data in accordance therewith. It is possible to identify a cross-section of the recording pits 2a and 2b as to whether they are rectangle or V-shape by calculating a difference between sand p-polarized lights in accordance with the equation: (A+B)-(C+D). Thus, the multiplicity of the recording pits can be increased also by the difference in a cross-sectional shape between the recording pits 2a and 2b. Accordingly, even if there are formed recording pits having the same size as conventional ones, it is possible to double the multiplicity of both the recording pits and a region in which the recording pits are not formed. As a result, it is possible to have two times greater multiplicity in a light-reproduction medium. In place of the third polarized-beam splitter 16 may be used a Wollaston prism, in which case two photodetectors are to be used in juxtaposition or there is to be used a photodetector divided into four sections in the direction Y. As an alternative, a hologram device may be substituted for such a photoelement so that the optical head may be more compact. In addition, it is allowable to project light to the light-reproduction medium 10 through the substrate 1 or the multi-layered structure 3, 4, and 5. Either lights reflected from the light-reproduction medium 10 or lights passing through the light-reproduction medium 10 may be used for detection. The recording pits 2a and 2b having rectangular and V-shaped cross-section, respectively, and the second grooves 6 may have a greater width as measured in a direction perpendicular to the direction Y relative to a wavelength of an incident light, as illustrated in Figs. 6A and 7A, to thereby utilize the characteristic shown in Fig. 2. For instance, a recording pit may have a rectangular cross-section 2Aa or a V-shaped cross-section 2Ab illustrated in Figs. 6B and 7B, respectively, and the second groove may have a cross-section 6A illustrated in Figs. 6C and 7C. As an alternative, a recording pit may have a cross-section having a shape intermediate between rectangle and V-shape. For instance, a recording pit may have a reverse trapezoidal cross-section 2B as illustrated in Fig. 8B, in which case, if a ratio of a width R of a flat portion to an entire width (R+2T) of the groove 2B is smaller than 80%, the groove 2B can be considered to be almost the same as a V-shaped groove. Figs. 9A to 9C illustrate the second embodiment of the present invention which is a variation of the first embodiment thereof. In this embodiment, a groove formed in a region where the recording pits 2a and 2Ab are formed and the second grooves 6 and 6A formed in a region where the recording pits are not formed may have a varying width which is defined as a length measured in a direction perpendicular to the direction Y. Specifically, the second grooves 6 have a narrow width smaller than a half of a wavelength of an incident light, whereas the second groove 6A has a wide width greater than a half of a wavelength of an incident light. Thus, it is possible to detect a difference in width in the recording pits and second grooves by calculation in accordance with the equation (A+B)-(C+D), utilizing the characteristics shown in Figs. 2 and 3, to thereby make it possible to further increase the multiplicity. Figs. 10A to 10C and 11A to 11C illustrate grooves formed as recording pits in accordance with the third embodiment of the present invention. The illustrated recording pits 2C have a cross-section asymmetrical about an axis passing through a center of the recording pits 2C and perpendicular to the direction Y. The recording pit 2Ca illustrated in Figs. 10A and 10B has a bottom inclined upward towards the center of the light-reproduction medium, whereas the recording pit 2Cb illustrated in Figs. 11A and 11B has a bottom inclined downward towards the center of the light-reproduction medium. The thus formed recording pits 2Ca and 2Cb bias incident lights to regions of the light-reproduction medium closer to or farther away from a center thereof in dependence on whether a bottom of the recording pits 2Ca and 2Cb is inclined upward or downward. Thus, when the light-reproduction apparatus illustrated in Fig. 5 is to be used, there is generated a difference in detected optical intensity between the regions A, C closer to a center of the light-reproduction medium and the regions B, D farther away from a center of the light-reproduction medium in the first and second photodetectors 19 and 20 each of which is divided into two sections. Accordingly, it is possible to identify whether a recording pit has a cross-section illustrated in Fig. 10B or Fig. 11B by making calculation in accordance with the equation (A+C)-(B+D). Thus, it is possible to further increase the multiplicity of the light-reproduction medium by adding the shapes of the recording pits 2Ca and 2Cb to the configuration of the first embodiment. It is allowable to use recording pits 2Da and 2Db illustrated in Figs. 12B and 13B, respectively, in place of the recording pits 2Ca and 2Cb illustrated in Figs. 10B and 11B, respectively. The recording pit 2Da comprises a portion 2Daa inclined downward to the center of the light-reproduction medium, and a horizontally flat portion 2Dab, as illustrated in Fig. 12B, whereas the recording pit 2Db comprises a horizontally flat portion 2Dbb and a portion 2Dba inclined upward to the center of the light-reproduction medium, as illustrated in Fig. 13B. If a ratio of a width of the flat portion 2Dab or 2Dbb to an entire width of the groove 2Da or 2Db is smaller than 80%, the groove 2Da or 2Db can be considered to be almost the same as a V-shaped groove. Thus, it is preferable for the recording pits 2Da and 2Db to satisfy such a ratio being smaller than 80%. Since the third embodiment has nothing to do with the characteristics as illustrated in Figs. 2 and 3 caused due to a difference between s- and p-polarized lights, when only the recording pits 2Da or 2Db formed in accordance with the third embodiment are to be used, it is not necessary to deposit the magnetic film 4 on the substrate 1. All that is necessary is to deposit a reflection film on a substrate like conventional CD-ROM. Hereinbelow are described more detailed examples. An optical disc was made comprising a polycarbonate substrate having a diameter of 120 mm and multi-layers deposited on the substrate, including SiN interference film, TbFeCo magnetic film, SiN protection film and Al alloy reflection film. The light-reproduction apparatus illustrated in Fig. 5 was used as an optical system. The orientation of polarized lights to be radiated into the optical disc was set at 45 degrees relative to a direction in which the optical disc is to be moved relative to an optical head. An incident light had a wavelength of 680 nm. A plurality of grooves were formed as recording pits, some of them having a depth of 170 nm and others 21.25 nm. These grooves had rectangular or V-shaped cross-section or other shapes such as those illustrated in Figs. 4A to 13C. On regeneration of data stored in the optical disc, all signals (A+B)-(C+D), (A+C)-(B+D) and (A+B+C+D) were clearly reproduced, and all these signals had almost the same quality as conventional CD-ROM. Thus, it has been confirmed that there have been obtained a light-reproduction medium having memory density four times greater than conventional CD-ROM. There was made another optical disc having the same configuration as the previously mentioned optical disc except that grooves formed as recording pits have a depth of either 85 nm or 170 nm. On regeneration of data stored in the optical disc, all signals (A+B)-(C+D), (A+C)-(B+D) and (A+B+C+D) were clearly reproduced, and all these signals had almost the same quality as conventional CD-ROM. Thus, it has been confirmed that there have been obtained a light-reproduction medium having memory density four times greater than conventional CD-ROM. There was made still another optical disc having the same configuration as the firstly mentioned optical disc except that grooves formed as recording pits have a depth of either 170 nm or 340 nm. On regeneration of data stored in the optical disc, all signals (A+B)-(C+D), (A+C)-(B+D) and (A+B+C+D) were clearly reproduced, and all these signals had almost the same quality as conventional CD-ROM. Thus, it has been confirmed that there have been obtained a light-reproduction medium having memory density four times greater than conventional CD-ROM. There was made yet another optical disc having the same configuration as the firstly mentioned optical disc except that grooves formed as recording pits have a depth of either 170 nm or 21.25 nm. Some of these grooves had rectangular cross-section 2a and others had V-shaped cross-sections 2Ab as illustrated in Fig. 9B, and some of the grooves had a width of 680 nm and others 340 nm. On regeneration of data stored in the optical disc, signals (A+B)-(C+D) and (A+B+C+D) were clearly reproduced, and these signals had almost the same quality as conventional CD-ROM. Thus, it has been confirmed that there have been obtained a light-reproduction medium having memory density twice greater than conventional CD-ROM. The same experiment was conducted to an optical card having been made in accordance with the same specification as the above mentioned optical disc. The same results were obtained, and thus the effectiveness of the optical card was confirmed. It has been also confirmed that the same results could be obtained not only when the optical disc or card was moved relative to an optical head, but also when an optical head was moved relative to the optical disc or card. Although the recording pits are formed as grooves and the second grooves are formed in the above mentioned embodiments, it should be noted that a land or lands may be formed in place of a groove or grooves. When a land or lands are to be formed, there may be used the upside down of the shapes illustrated in Figs. 4A to 13C. It is not always necessary to form grooves or lands having more than two different cross-sections. One groove or land may be formed as a recording pit. In addition, it is allowable to form both a groove or grooves and a land or lands. It is also allowable to form both grooves having more than two different cross-sections and lands having more than two different cross-sections. It is not always necessary to concurrently project s- and p-polarized lights into a light-reproduction medium. The s- and p-polarized lights may be projected alternately for regeneration of data. Thus, the present invention provides a light-reproduction medium having memory density several times greater than a conventional CD-ROM without changing CD-ROM fabrication technique, driving method and an optical head structure, resulting in significantly increased capacity of an optical disc or an optical card. Each feature disclosed in this specification (which term includes the claims) and/or shown in the drawings may be incorporated in the invention independently of other disclosed and/or illustrated features. The text of the abstract filed herewith is repeated here as part of the specification. The present invention provides an improved light-reproduction medium storing data therein to be reproduced by detecting light transmitted therethrough and/or light reflected therefrom. The light-reproduction medium comprises a substrate formed on a surface thereof with at least two recording pits, and a magnetic film formed on the surface of the substrate. The recording pits have different level from the surface of the substrate, each of the recording pits having a cross-section selected from at least two different shapes. The present invention provides a light-reproduction medium having memory density several times greater than a conventional CD-ROM without changing CD-ROM fabrication technique and an optical head structure, resulting in significantly increased capacity of an optical disc or an optical card.

Claims: A light-reproduction medium comprising a substrate with recording pits formed on a surface thereof, at least two of said recording pits (2a, 2b, 2Aa, 2Ab, 2B, 2Ca, 2Cb, 2Da, 2Db) having a different cross-sectional profile in a plane perpendicular to a direction (A) in which the light-reproduction medium is moved relative to an optical head, characterised in that the respective cross-sectional profiles of said at least two pits are selected from a rectangular shape (2a, 2Aa), a triangular shape (2b, 2Ab, 2Ca, 2Cb), and a trapezoidal shape (2B, 2Da, 2Db). A light-reproduction medium according to Claim 1, wherein a magnetic film (4) is formed on the surface of the substrate (1). A light-reproduction medium according to Claim 1 or Claim 2, wherein said at least two of said recording pits (2a, 2b, 2Aa, 2Ab, 2B, 2Ca, 2Cb, 2Da, 2Db) have a different width in said plane. A light-reproduction medium according to Claim 3, wherein the width includes one greater than a half of an incident light wavelength, and one smaller than a half of an incident light wavelength. A light-reproduction medium according to any preceding claim, wherein said at least two recording pits (2Ca, 2Cb, 2Da, 2Db) are asymmetrical in profile about an axis passing through a midpoint thereof and parallel to the direction A. A light-reproduction medium according to Claim 5, wherein one of the recording pits (2Ca, 2Cb, 2Da, 2Db) has a cross-section in a plane perpendicular to said direction (A) which has an upper edge inclined towards a center of the light-reproduction medium. A light-reproduction medium according to any preceding claim, wherein said at least two recording pits have a different level from the surface of the substrate. A light-reproduction medium according to any preceding claim, wherein: lands or grooves (6, 6A) are formed on said surface in a region in which said at least two recording pits (2a, 2b, 2Aa, 2Ab, 2B, 2Ca, 2Cb, 2Da, 2Db) are not formed, the lands or grooves (6, 6A) extending in a direction in which the light-reproduction medium is moved relative to an optical head and having a depth measured normal to the surface of said substrate which is different to that of said at least two recording pits (2a, 2b, 2Aa, 2Ab, 2B, 2Ca, 2Cb, 2Da, 2Db). A light-reproduction medium according to Claim 8, wherein each of the lands or grooves (6, 6A) has a width varying in a direction in which the light-reproduction medium is moved relative to an optical head. A light-reproduction medium according to Claim 8 or Claim 9, wherein the lands or grooves have a depth of 1/10 to 1/30 of a wavelength of an incident light or an integral number of 1/4 of a wavelength of an incident light. A method of reproducing data stored in a light-reproduction medium, comprising the steps of: (a) projecting mutually perpendicularly intersected polarized lights to a light-reproduction medium including a substrate (1) with recording pits (2a, 2b, 2Aa, 2Ab, 2B, 2Ca 2Cb, 2Da, 2Db) formed in a surface thereof, at least two of the recording pits (2a, 2b, 2Aa, 2Ab, 2B, 2Ca, 2Cb, 2Da, 2Db) having a different cross-sectional profile in a plane perpendicular to a direction (A) in which the light-reproduction medium is moved relative to an optical head, characterised in that the respective cross-sectional profiles of said at least two pits are selected from a rectangular shape (2a, 2Aa), a triangular shape (2b, 2Ab, 2Ca, 2Cb), and a trapezoidal shape (2B, 2Da, 2Db) and (b) reproducing data from polarized lights reflected from or transmitted through the light-reproduction medium. A method according to Claim 11, wherein the step (b) includes the steps of decomposing the polarized lights into components parallel to the direction and a direction B perpendicular to direction A, and calculating a difference between the components.

Inventors: OGAWA MASATSUGU, OGAWA, MASATSUGU
Applicants: NIPPON ELECTRIC CO, NEC CORPORATION
Application year: 1996
Main classification: G11B7
IPC codes: G11B7, G11B11