Patent Publication Number: US-2006002277-A1

Title: Optical disc apparatus

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS  
      This application is based upon and claims the benefit of priority from prior Japanese Patent Application No. 2004-192939, filed Jun. 30, 2004, the entire contents of which are incorporated herein by reference.  
     BACKGROUND OF THE INVENTION  
      1. Field of the Invention  
      The present invention relates to an optical disc apparatus, which can play back preferable information with little crosstalk, when playing back information from an optical disc having information recorded in two or more recording layers.  
      2. Description of the Related Art  
      An optical disc used as an information recording medium is available in a play-only type represented by CD and DVD-ROM, a write-once type represented by CD-R and DVD-R, and a rewritable type used for an external memory of a computer and a record-playback video (video recording).  
      Nowadays, increase of the number of recording layers to two or more has been studied to increase the recording capacity of an optical disc of the next generation DVD standard. In this case, it is necessary to make an intermediate layer between the recording layers thin compared with a current DVD standard disc. However, it is known that crosstalk between layers increases when an intermediate layer is thin.  
      Concerning the crosstalk level, Japanese Industrial Standards (JIS) X 6241 (1997) defines that the ratio of A/M 2  (detector size (photodetector area] to the detection lateral magnification square) is 100 μm 2 &lt;A/M 2 &lt;144 μm 2  , as a specification of an optical head used for playing back information of a DVD standard optical disc.  
      It is necessary to make an intermediate layer thin compared with a current two-layer DVD-ROM disc for increasing the recording capacity of a new standard disc called a next-generation DVD (hereinafter, referred to as HD DVD) among the DVD standard optical discs having two or more recording layers.  
      However, if A/M 2  for a current DVD standard optical disc is applied to HD DVD without modifications, inter-layer crosstalk increases in a rewritable two-layer disc (HD DVD-RW) and causes a problem of failing to obtain a preferable playback signal.  
      Further, as the diameter R of an optical beam focused on an optical disc through an objective lens fluctuates by f (RI)(f indicates a function including other factors) under the influence of Rim Intensity (RI) indicating the relation between an incident light flux diameter and an aperture diameter of an objective lens used for an optical head of an optical disc drive, it is difficult to ignore the influence of RI. Thus, an optical disc drive and optical head taking account of the influence of RI on A/M 2  are not yet in practical use.  
     BRIEF SUMMARY OF THE INVENTION  
      According to an aspect of the present invention, there is provided an optical disc apparatus comprising:  
      a light source;  
      an objective lens which focuses a light from the light source on at least one of recording layers of a recording medium having at least two recording layers;  
      a photodetector which receives a light reflected on one of recording layers of a recording medium having at least two recording layers, and outputs a signal corresponding to the intensity of the light; and  
      a condenser lens which focuses a light reflected on one of recording layers of a recording medium having at least two recording layers on the photodetector,  
      wherein the objective lens and condenser lens satisfies A/M 2 &lt;100 μm 2  when A/M 2  is defined by assuming that the area of a light-receiving surface of the photodetector is A, the focal length of the objective lens is fo, the focal length of the condenser lens is fc, and fc/fo is M.  
    
    
     BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWING  
      The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate embodiments of the invention, and together with the general description given above and the detailed description of the embodiments given below, serve to explain the principles of the invention.  
       FIG. 1  is a schematic illustration for explaining an example of a recording medium (an optical disc) applicable to an optical disc drive and optical head unit according to an embodiment of the present invention;  
       FIG. 2  is a schematic illustration for explaining an example of an optical disc apparatus and an optical head unit according to an embodiment of the present invention;  
       FIGS. 3A  to  3 C are schematic illustrations for explaining a cause of inter-layer crosstalk occurring when a reflected laser beam is obtained from two recording layers by using the optical disc shown in  FIG. 1  and optical disc drive shown in  FIG. 2 ;  
       FIG. 4  is a graph for explaining the relation between the inter-layer crosstalk explained in  FIG. 3  and the magnitude of A/M 2  defined by the area A of a photodetector to receive a reflected laser beam and the lateral magnification M of a light-receiving system to pass the reflected laser beam (the ratio of a focal length fc of a condenser lens to a focal length fo of an objective lens); and  
       FIG. 5  is a graph showing the correction of the magnitude of A/M 2  defined by the area A of a photodetector to receive a reflected laser beam and the lateral magnification M of a light-receiving system to pass the reflected laser beam (the ratio of a focal length fc of a condenser lens to a focal length fo of an objective lens), taking account of Rim Intensity (RI) showing the relation between the objective lens aperture diameter and incident light beam diameter. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION  
      Hereinafter, an embodiment of the present invention will be explained in detail with reference to the accompanying drawings.  
       FIG. 1  is a schematic illustration of an example of an optical disc suitable for recording or playing back information with an optical head unit of the present invention to be explained with reference to  FIG. 2 .  
      As shown in  FIG. 1 , an optical disc (a recording medium)  1  has a first information recording layer  3  including a phase change recording film, on a first substrate  2  made of polycarbonate.  
      On the first information recording layer  3 , an intermediate layer  4  having a predetermine transmittivity against a wavelength of laser beam emitted from a semiconductor laser unit  20  of an optical head unit  11 , is stacked. On the intermediate layer  4 , a second information recording layer  5  is stacked. The intermediate layer  4  is usually made of adhesive or UV-curable resin. The second information recording layer  5  is covered by a second substrate  6  made of polycarbonate.  
      In the optical disc  1 , the information recording layers  3  and  5  may be a play-only layer composed of a reflection film made of metal, or a record-playback layer composed of phase change film. Further, in the optical disc  1 , only one of two recording layers  3  or  5  may be a play-only layer and the other may be a record-playback layer.  
      As described above, the optical disc  1  can be formed either by stacking the first substrate  2  and second substrate  6  in order, or by bonding two substrates having the information recording layer  3  (or  5 ) with a predetermined thickness to the intermediate layer to be faced to each other  4  by means of adhesive material. The substrate with the information recording layer formed on one side is about 0.6 mm thick, and the whole optical disc is about 1.2 mm thick (a reference substrate thickness).  
      The optical disc  1  is a so-called single-sided two-layer disc. The first information recording layer  3  is a semitransparent having a predetermined transmittivity against a wavelength of laser beam emitted from the semiconductor laser unit  20 . Therefore, the first information recording layer  3  can transmit a light as well as reflecting a certain amount of light. Thus, when light is radiated to the optical disc  2  from the direction of the substrate  2 , information can be recorded on one of the information recording layers  3  and  5 , or information can be played back from one of the recording layers, by adjusting a focus to one of the first and second recording layers  3  and  5  (by controlling the distance between the objective lens  24  and optical disc  1 ).  
      The intermediate layer  4  has a function to optically isolate the information recording layer  3  (or  5 ) from the other information recording layer  5  (or  3 ), while the information of one information recording layer  3  (or  5 ) is being played back. In this sense, two information recording layers  3  and  5  are preferably separated as far as possible, and the intermediate layer  4  is preferably thick. However, in that case, accurate playback of both layers by single optical system becomes hard.  
      Namely, when the thickness from the surface of the substrate  2  to the center of the intermediate layer  4  is defined as a load of an objective lens described later with reference to  FIG. 2 , an aberration corresponding to a thickness error of the half thickness of the intermediate layer  4  occurs, in any case of recording or playing back information in/from the information recording layer  3  (or  5 )  
      Therefore, from the viewpoint of reducing aberration in the optical system, the intermediate layer  4  is preferably thin. Namely, the thickness of the intermediate layer  4  is decided at a trade-off point between an aberration of the recording/playing back optics and a crosstalk between the information recording layers  3  and  5 .  
       FIG. 2  is a schematic illustration for explaining an example of an optical head unit, which records information in the optical disc shown in  FIG. 1 , or plays back information from the optical disc.  
      As shown in  FIG. 2 , an optical head unit  11  has a semiconductor laser (a light source)  20  to output a laser beam or a violet light beam of 400-410 nm. A wavelength of the laser beam is preferably 405 nm.  
      A laser beam  100  emitted from the semiconductor laser  20  is collimated by a collimator lens  21 . The collimated parallel beam passes through a polarizing beam splitter  22  and quarter-wavelength plate  23 , and is guided by the objective lens  24  to the recording surface of the optical disc  1  explained later with reference to  FIG. 2 .  
      The laser beam  100  guided to the optical disc  1  is focused on one of the first and second recording layers, by the convergence given by the objective lens  24  and the distance between the objective lens and optical disc  1 .  
      The laser beam  100  focused on the recording layer of the optical disc  1  is reflected on the recording layer, returned to the objective lens  24  as a reflected laser beam  101 , and returned to a polarizing beam splitter  22  through the quarter-wavelength plate  23 .  
      The reflected laser beam  101  returned to the polarizing beam splitter  22  is reflected toward the condenser lens  25  on the polarizing surface of the polarizing beam splitter  22 , and forms an image on the light-receiving surface of a photodetector  26  as a converging beam having a beam spot size corresponding to the focal length defined by the convergence given by the condenser lens  25 .  
      The light-receiving part of the photodetector is usually divided into several sections, each of which outputs a current corresponding to the light intensity. The current outputted from each light-receiving section is converted into a voltage by a not-shown I/V amplifier, and processed by a processor  27  to be usable as a HF (playback) signal, focus error signal and track error signal. The HF (playback) signal is converted into a predetermined signal format, or outputted to a temporary storage or external storage through a given interface. The size of the light-receiving section of the photodetector  26  is defined, so that the A/M 2  which is determined by the area “A” of the light-receiving section of the photodetector and the lateral magnification M of the light-receiving system (the ratio of the focal length fc of the condenser lens to the focal length fo of the objective lens), becomes a predetermined value as explained hereinafter with reference to  FIG. 3 .  
      The focus error signal and track error signal among those obtained by the processor  27  are converted by a servo driver  28  into signals usable as a focus control signal and track control signal to operate an actuator  29 , which displaces the position of the objective lens  24 , and supplied to the actuator  29 . Therefore, the objective lens  24  held by the actuator  29  is optionally moved in the vertical direction to approach to and separate from the information recording layer  3  (or  5 ) of the optical disc  1 , and/or in the disc radial direction. Namely, the objective lens  24  is controlled by the servo driver  28  to follow the information track on the optical disc  1 .  
      Next, description will be given on optimization of the elements of the optical head unit  11  for recording or playing back information in/from a new-standard optical disc called a next-generation DVD (hereinafter referred to as HD DVD).  
      Assuming that the wavelength of a light source (the output of a semiconductor laser unit) is 405 nm and the numerical aperture NA of the objective lens  24  is 0.65, the suitable thickness of the intermediate layer  4  of the optical disc  1  is 15-25 μm as a specification of HD DVD considering the trade-off mentioned above. Conditions on the thickness of the intermediate layer  4  described below are applicable to an optical disc having more than three information recording layers or a disc having two or more intermediate layers.  
      Description will now be given on an inter-layer crosstalk upon playback of a two-layer optical disc with reference to  FIGS. 3A  to  3 C.  
       FIGS. 3A-3C  are schematic illustrations of the light-receiving system of the optical head unit of  FIG. 2 , or the path of the reflected laser beam  101 .  FIG. 3A  shows the case when the information of the information recording layer  5  (L 1 ) far from the objective lens  24  is played back.  FIG. 3B  shows the case when the information of the information recording layer  3  (L 0 ) near the objective lens  24  is played back (or, recorded).  
      As shown in  FIG. 3A , the reflected laser beam  101  (solid line) from the information recording layer  5  (L 1 ) becomes parallel beam after passing through the objective lens  24 , and is focused by the condenser lens  25  onto the photodetector  26 .  
      The photodetector  26  detects the focused laser beam reflected from the target information recording layer (L 1  in this case). However, the optical disc  1  generates (reflects) a certain amount of reflected laser beam as indicated by a dotted line even in the information recording layer  3  (L 0 ). The reflected laser beam from the recording layer other than the target information recording layer is called a crosstalk beam.  
      Unlike the reflected laser beam indicated by a solid line, the crosstalk beam (a dotted line) becomes a diverging beam, not a parallel beam, after passing through the objective lens  24 , and is led to the photodetector  26  as a so-called defocused beam, though it is given convergence by the condenser lens  25 .  
      Thus, as shown in  FIG. 3C , a part (a central part) of the crosstalk beam is radiated to the photodetector  26  (a dotted circle). This crosstalk beam is put (superposed) on the laser beam signal from the target information recording layer  5 , as a noise component, and defined as an inter-layer crosstalk.  
      Likewise, in  FIG. 3B , the reflected laser beam from the information recording layer  5  (L 1 ) becomes a crosstalk beam with respect to the reflected laser beam from the information recording layer  3  (L 0 ). (The illustration of the beam on the photodetector is the same as  FIG. 3C , and omitted.)  
      The difference between the crosstalk beams shown in  FIG. 3A  and  FIG. 3B  is whether the luminous flux after passing through the objective lens  24  is a converging beam or a diverging beam. As explained in  FIG. 3A , the beam becomes a defocused beam on the photodetector  26 , and causes an inter-layer crosstalk.  
      An inter-layer crosstalk is defined by the ratio of the parts of a crosstalk beam radiated to the photodetector  26 , as described above. Thus, as far as all parts of a converging beam from a target information recording layer can be received on the photodetector  26 , the crosstalk influence is less when the photodetector size is small. When the size of the photodetector  26  is constant, the inter-layer crosstalk element becomes small if the crosstalk beam size is large.  
      The crosstalk beam size on the photodetector  26  is determined by the lateral magnification M of the light-receiving system, as described before. When the aperture radii of the objective lens  24  and condenser lens  25  are the same, the lateral magnification M is determined by the ratio of the focal length fc of the condenser lens  24  to the focal length fo of the objective lens  25 , and obtained from an equation M =fc/fo.  
      Therefore, assuming that the area of the light-receiving part of the photodetector  26  is A and the lateral magnification of the light-receiving system is M, a value of A/M 2  can be defined as an index almost proportional to an inter-layer crosstalk. The A/M 2  concerning a current DVD-standard optical disc has been disclosed in the aforementioned prior art document, Japanese Industrial Standards (JIS) X 6241: 1997. The value of A/M 2  has a range of 100&lt;A/M 2 &lt;144 μm 2 .  
       FIG. 4  is a graph plotting A/M 2  in the horizontal axis and an inter-layer crosstalk in the vertical axis.  
      As seen from  FIG. 4 , there is a certain relationship as explained before between the level (magnitude) of inter-layer crosstalk and the thickness of the intermediate layer  4  in the optical disc  1 . It is obvious that when the intermediate layer  4  is thin, the inter-layer crosstalk is increased. In  FIG. 4 , the curve a indicates the case when the thickness of the intermediate layer  4  is 15 μm. Likewise, the curve b indicates the case when the thickness of the intermediate layer  4  is 20 μm, the curve c indicates the case when the thickness of the intermediate layer  4  is 25 μm, and the curve d indicates the case when the thickness of the intermediate layer  4  is 30 μm. The curve z is drawn to compare the thickness (40 μm) of the intermediate layer  4  in a current DVD-standard optical disc.  
      In a current DVD-standard optical disc, a maximum value of A/M 2  is 144 μm 2 , and it is seen that the maximum inter-layer crosstalk is 10.2% (0.102).  
      By applying this maximum value of inter-layer crosstalk to a next-generation optical disc of the present invention, it is known that A/M 2 &lt;27 μm 2  when the intermediate layer  4  is 15 μm thick, A/M 2 &lt;47 μm 2  when the intermediate layer  4  is 20 μm thick, A/M 2 &lt;73 μm 2  when the intermediate layer  4  is 25 μm thick, and A/M 2 &lt;104 μm 2  when the intermediate layer  4  is 30 μm thick. It is seen from the above that when the value of A/M 2  is small, the inter-layer crosstalk level can be decreased.  
      Therefore, a small value of A/M 2  is better from the viewpoint of inter-layer crosstalk. Concerning HD DVD, it is preferable to make the value of A/M 2  smaller than a current DVD standard, that is, A/M 2 &lt;100 μm 2 .  
      More concretely, when the intermediate layer  4  is 20 μm thick, it is desirable from the viewpoint of decreasing an inter-layer crosstalk to satisfy A/M 2 &lt;47 μm 2  as a specification of light-receiving system in an optical head unit (an optical disc drive) suitable for the optical disc  1  of the present invention.  
      A lower value of A/M 2  is desirable from the viewpoint of inter-layer crosstalk, and a lower limit value cannot be defined. On the other hand, a lower limit value of the area A of the photodetector  26  and an upper limit value of the detection lateral magnification M can be practically defined. The size of the photodetector  26  is at least a square having a 40 μm side (A=1600 μm 2 ). On the other hand, a maximum value of lateral magnification M is determined by a maximum value of fc (the focal length of the condenser lens  25 ). Then, considering the influence of fc on the size of the optical head  11 , it is appropriate to set a maximum of 120 mm (the same size as a disc) as an upper limit. Therefore, when fo (the focal length of the objective lens  24 ) is 3 mm, M=40.  
      Based on the above values, the lower limit of A/M 2  is A/M 2 =1600/40 2 =1.0. Therefore, it is necessary to satisfy 1&lt;A/M 2 &lt;47 μm 2  as a specification of the light-receiving system in the optical disc drive of the present invention.  
      Nowadays, it is well known that the influence of Rim Intensity (RI), which indicates the relation between the incident luminous flux diameter and the aperture diameter of the objective lens  25 , cannot be ignored as a factor responsible for the characteristics of the optical head unit  11  (particularly, the objective lens  24 ).  
      RI is a value to express the optical intensity at the aperture rim of a lens as a ratio (or percentage) to the intensity at the center of optical beam, with respect to a laser beam coming into a lens, and is one of parameters to express the optical characteristics of a beam applied to an objective lens.  
      For example, in the optical disc drive, the diameter R of a laser beam focused on an optical disc through an objective lens is can be obtained by 
 
 R= 2 ×f ( RI )×λ/ NA  
 
 (f indicates a function including other factors). Even though the objective lens  24  is almost annular (a perfect circle), if a laser beam from the semiconductor laser unit  20  is diverging and has the elliptical cross section, it is necessary to consider the direction. In this case, RI is defined including the direction as RIx or RIy. 
 
      For example, when RI(no direction)=0.6 and wavelength λ=405 nm and NA=0.65, a beam diameter R is R=0.5260 μm. when RI (no direction)=0.7 and wavelength λ=405 nm and NA=0.65, a beam diameter R is R=0.5218 μm.  
      Further, in the optical disc drive, a collimator lens  21  is used in addition to the objective lens  24 , particularly in the semiconductor laser unit  20 .  
      Therefore, in the present invention, RI that is conventionally fixed to 1.0 (an incident light intensity is uniform over a pupil) is changed, and the degree of an inter-layer crosstalk including the influence of RI is also considered.  
       FIG. 5  shows the dependence of an inter-layer crosstalk on A/M 2 , when the intermediate layer  4  in the optical disc  1  is set to 20 μm thick and RI is changed as a parameter.  
      As seen from  FIG. 5 , as a result of setting RI to 0.135 (curve A), 0.6 (curve B) and 1.0 (curve Z, a comparing example), it is confirmed that the inter-layer crosstalk value increases when RI is small (low), and decreases when RI is large (high). The RI=0.135 (a lower limit) used in  FIG. 5  can be theoretically lowered as close as possible to 0, but substantially it is about 1/e 2  (=0.135). An upper limit is theoretically 1.0 (conventional=a comparing example, without considering RI).  
      According to  FIG. 5 , when the value of A/M 2  is set as A/M 2 &lt;27 μm 2  at RI=0.135 (curve A) and A/M 2 &lt;47 μm 2  at RI=0.6 (curve B), the inter-layer crosstalk value (magnitude) can be decreased.  
      There occurs a problem that the light usage efficiency of a lens is lowered when RI is high (large). Moreover, the beam diameter of the light focused by a lens is increased when RI is low (small). Therefore, an optimum range of RI considering a trade-off is 0.55&lt;RI&lt;0.70. When RI is changed, A/M 2  is not largely changed unlike when the thickness of the intermediate layer  4  in the optical disc  1  is changed.  FIG. 5  shows an example of the intermediate layer  4  with the thickness of 20 μm, but it has been confirmed that the substantially the same effect can be obtained even if the intermediate layer  4  is 15 μm or 30 μm thick.  
      Next, a preferable value of A/M 2  will be considered.  
      When considering a lower limit value of A/M 2  assuming that the intermediate layer  4  is 15-30 μm thick, the lower limit value of A/M 2  is 2-3 μm 2 .  
      Concretely, assuming that a maximum value of fc (a focal length of the condenser lens  25 ) is almost the same as the size of an optical disc according to the method explained above and assuming that fo (a focal length of the condenser lens  24 ) is 3 mm, M=26.7 is obtained when the disk size is 80 mm. Therefore, A/M 2 =1600/26.7 2 =2.3.  
      Conversely, assuming that a maximum value of fc is almost the same as the radius, not the diameter, of an optical disc caused by miniaturization of the optical disc drive, when the outside dimension of the optical disc is 120 mm, fc=60 mm and M=20. In this case, A/M 2 =1600/20 2 =4. When the outside diameter of the optical disc is 80 mm, fc=40 mm and M=13.3. Therefore, A/M 2 =1600/13.3 2 ≈9.  
      As described hereinbefore, according to the present invention, in inter-layer crosstalk in an optical disc having two or more recording layers can be certainly decreased and good playback characteristics can be obtained, by setting the area of a photodetector to receive a reflected laser beam from an optical disc to “A”, and setting the largeness of A/M 2  defined by the lateral magnification M (the ratio of a condenser lens focal length fc to an objective lens focal length fo) of the light-receiving system to pass a reflected laser beam to 1&lt;A/M 2 &lt;47 μm 2 .  
      Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details and representative embodiments shown and described herein. Accordingly, various modifications may be made without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.  
      In the detailed description of the invention, an optical disc drive is taken as an example for explaining the embodiment of the invention. But, it is apparent that the invention is applicable also to a movie camera and portable audio equipment to contain musical data.