Patent Document

[0001]    The present application claims priority under 35 U.S.C. 119 and 35 U.S.C. 365 to Korean Patent Application No. 10-2006-0034999, filed on Apr. 18, 2006, which is hereby incorporated by reference in its entirety. 
       BACKGROUND OF THE INVENTION 
       [0002]    1. Field of the Invention 
         [0003]    The present invention relates to an apparatus for optical pickup and more particularly, to an apparatus for optical pickup which minimizes offset element occurring between the recorded and non-recorded pattern when object lenses are configured off-axis along the tracks on the optical storage medium is disclosed. 
         [0004]    2. Description of the Related Art 
         [0005]    Optical storage media such as optical disks optically record data and are in shape of palm-size disk. Those media are loaded on a driver for data to be recorded thereto or to be read therefrom by optical apparatus inside the driver. 
         [0006]    There exist various optical storage media, for example, CD (Compact disc), DVD (Digital Versatile Disc), BD (Blu-ray Disc). Also, there are sub groups of DVD, such as DVD-RW, DVD+RW, DVD-RW. The kinds of those media are increasingly diversifying. 
         [0007]    In prior arts, various technologies have been developed to trace the track and groove on the optical storage media. Among those technologies, one uses three beams to trace the track and groove. In this case, especially when the three branched-off beams are located off-axis along the tracking direction, there is a problem that offset elements will occur over large areas near the boundary of recording and non-recording pattern of the optical storage media. 
         [0008]    In making such various image sensors, efforts are being made to improve. 
       SUMMARY OF THE INVENTION 
       [0009]    The present invention relates to an apparatus for optical pickup which effectively minimizes offset elements without being affected by the difference between the times when the beams enter the recording and non-recording area and the difference between the positions where the object lenses are located when those beams are located off-axis along the inner tracks and outer tracks. 
         [0010]    Advantages, objects, and features of the invention will be set forth in part in the description which follows and in part will become apparent to those having ordinary skill in the art upon examination of the following or may be learned from practice of the invention. The objectives and other advantages of the invention may be realized and attained by the structure particularly pointed out in the written description and claims hereof as well as the appended drawings. 
         [0011]    To achieve these objects and other advantages and in accordance with the purpose of the invention, as embodied and broadly described herein, there is provided an apparatus for optical pickup comprising: 
         [0012]    In another aspect of the present invention, there is provided a method for manufacturing a CMOS image sensor comprising the steps of: 
         [0013]    It is to be understood that both the foregoing general description and the following detailed description of the present invention are exemplary and explanatory and are intended to provide further explanation of the invention as claimed. 
     
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0014]    The accompanying drawings, which are included to provide a further understanding of the invention and are incorporated in and constitute a part of this application, illustrate embodiment(s) of the invention and together with the description serve to explain the principle of the invention. In the drawings: 
           [0015]      FIG. 1  shows a schematic diagram of an optical pickup  100  according to the first embodiment of the present invention. 
           [0016]      FIG. 2   a  illustrates the diffraction of light by optical storage and  FIG. 2   b  illustrates formation of a baseball which is formed by diffracted light at the optical storage. 
           [0017]      FIG. 3  shows a baseball pattern. 
           [0018]      FIG. 4  shows the first embodiment of a diffraction grating according to the present invention. 
           [0019]      FIG. 5  shows the second embodiment of a diffraction grating according to the present invention. 
           [0020]      FIG. 6  shows the third embodiment of a diffraction grating according to the present invention. 
           [0021]      FIG. 7  shows an exemplary push pull signal output which is generated by the diffraction grating of the optical pickup according to the first embodiment of the present invention. 
           [0022]      FIG. 8  shows positions where main beam and sub beams reach over the optical storage according to the present invention. 
           [0023]      FIG. 9   a  shows change of offset voltage dependent on time when there is no radial shift of object lens and  FIG. 9   b  shows change of offset voltage dependent on time when there is radial shift of object lens, in both cases the object lenses being placed on-axis. 
           [0024]      FIG. 10  shows change of offset voltage dependent on time when sub beam error occurred in which the object lenses are placed on-axis. 
           [0025]      FIG. 11  shows change of offset voltage dependent on time when sub beam error occurred and there is radial shift of object lens in which the object lenses are placed on-axis. 
           [0026]      FIGS. 12   a  and  12   b  show change of offset voltage dependent on time when there is radial shift of object lens by 1 au and 5 au respectively in which the object lenses are placed off-axis. 
           [0027]      FIG. 13   a  shows change of offset voltage dependent on time when there is radial shift of object lens by 5 au and sub beam error occurred in which the object lenses are placed on-axis and  FIG. 13   b  shows change of offset voltage dependent on time when there is radial shift of the object lens by 5 au and sub beam error occurred in which the object lenses are placed off-axis. 
           [0028]      FIG. 14  shows change of offset voltage dependent on time given the same conditions as those of  FIG. 13   b  measured in an optical pickup according the present invention. 
           [0029]      FIG. 15  shows a schematic diagram of an optical pickup  200  according to the second embodiment of the present invention. 
       
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
       [0030]    Reference will now be made in detail to the preferred embodiments of the present invention, examples of which are illustrated in the accompanying drawings. Wherever possible, the same reference numbers will be used throughout the drawings to refer to the same or like parts. 
         [0031]      FIG. 1  shows an optical pickup  100  according to the embodiment of the present invention. 
         [0032]    Referring to  FIG. 1 , the optical pickup  100  according to the first embodiment of the present invention comprises light source  110 , collimate lens  120 , beam splitter  130 , diffraction grating  140 , wavelength plate  150 , object lens  155 , condensing lens  160  and light detecting means  170 , and an optical storage  180  may be placed before the object lens  155 . 
         [0033]    The light source  110  generate laser beam and the collimate lens  120  transforms the light generated by light source  110  into a parallel beam. 
         [0034]    The beam splitter  130  which is a light dividing means transmits the incident light from collimate lens  120  depending on the polarizing direction of the light or reflects the light reflected by the optical storage  180  to the condensing lens  160 . 
         [0035]    The transmission light through beam splitter  130  passes through the diffraction grating  140  and then is transformed to a circularly polarized light by quarter wavelength plate  150 . 
         [0036]    The circularly polarized light passes through the object lens  155  and is reflected by the optical storage  1380  having land and groove structure and goes back to the object lens  130 . 
         [0037]    The reflected light is transformed to a parallel beam by the object lens  130  and then is polarized by quarter wavelength  150  so that its polarizing direction is reversed. And then the light is diffracted by the diffraction grating  140 . 
         [0038]    The diffraction grating  140  diffracts and divides the reflected light by the optical storage  180  into a main beam and two sub beams, in which the diffracted lights of main beam and sub beams form a baseball pattern as shown in  FIG. 3 . 
         [0039]    The diffraction grating  140  comprises two grating pattern regions which have different polarization direction from each other. The first grating pattern performs diffracting and dividing of the reflected light by the optical storage and excludes the AC signal causing area i.e. the region which the sub beam region and the main beam region overlap. The second grating pattern covers the region which the sub beam region and the main beam region overlap and diffracts the lights to a direction different from case of the first grating pattern. The diffracted light by the second grating pattern does not enter the light detecting means and is excluded from error detecting process. 
         [0040]    The detailed structures of the diffraction grating  140  will be described below with reference to  FIG. 4  and the following drawings. 
         [0041]    The main beam out of the divided by the diffraction grating  140  is 0 th  beam and is detected as an MPP signal at the light detecting means  170 , the sub beams thereof are +1st beam and −1st beam and detected as first SPP signal and second SPP signal at the light detecting means  170  respectively. 
         [0042]    The diffracted light from the diffraction grating  140  is reflected by beam splitter  130  and transmits to the light detecting means via condensing lens  160 . 
         [0043]    The light detecting means  170  is a light-to-electrical conversion device such as Photo Diode, receives 0 th  beam, +1 st  beam −1 st  beam and generates MPP signal, first SPP signal and second SPP signal and detects TES (Track Error Signal) therefrom. 
         [0044]      FIG. 2   a  illustrates the diffraction of light by optical storage. 
         [0045]    As shown in  FIG. 2   a , the incident light into optical storage  180  is diffracted by the track structure of land/groove on the optical storage  180  with a certain angle θ and forms 0 th , +1 st  and −1 st  beams. And the 0 th , +1 st  and −1 st  beams form circular pattern(S). 
         [0046]    The size of circular pattern formed by 0 th , +1 st  and −1 st  beams may be equivalent to EPD (Entrance Pupil Diameter) of the object lens placed right before the optical storage and can be calculated by the following equation. 
         [0000]        EPD= 2 ×f×NA   (Equation 1) 
         [0047]    Wherein “f” is focal length of object lens, 
         [0048]    “NA” is Numerical Aperture. 
         [0049]      FIG. 2   b  illustrates forming of a baseball which is formed by diffracted light at the optical storage  180 . 
         [0050]    As shown in  FIG. 2   b , when a circular patterned beam is incident into the optical storage  180 , it is diffracted to form three beams b 1 , b 2 , b 3 . 
         [0051]    The circular patterns formed by side beams b 1 ,b 3  are shifted from the central pattern by the central beam b 2 , wherein the amount of shift can be calculated by the following equation. 
         [0000]      Shift=the dimension of the sub beam× f×λ÷TP    
         [0052]    wherein “the dimension of the sub beam is +1 or −1, 
         [0053]    “f” is focal length of object lens, 
         [0054]    “λ” is the wavelength of the sub beam 
         [0055]    “TP” is the track pitch of the optical storage. 
         [0056]    Reflected by the optical storage  180 , three beams b 1 , b 2 , b 3  from a baseball patter as shown in  FIG. 3 . 
         [0057]    The size and overlapping area is dependent upon the kind of the optical storage  180 . For example, the overlapping area tends to be relatively large in case of BD (Blu ray disk) or DVD RW. 
         [0058]    The baseball pattern P 1 , P 2 , P 3  formed by reflection at the optical storage  180  is transformed to a parallel beam by object lens  155 , and passes through wavelength plate  150  and diffraction grating  140 . 
         [0059]      FIG. 4  shows a plane view of the first embodiment of a diffraction grating according to the present invention which may be used in the optical pickup  100  in  FIG. 1 . 
         [0060]    In the optical pickup  100  according to one embodiment of the present invention, the structure of diffraction grating  140   a  is equivalent to circular patterns P 1 , P 2 , P 3 . Beams passing through sub beam (±1 st  beam) region (P 4 , P 6 ) and the overlapped region P 7  of main beam region P 5  and sub beam region P 4 , P 6  are diffracted to other direction than to the light detecting means  170  so that they are excluded from the process of detecting TES signal. 
         [0061]    The AC signal is caused by the overlapped region of sub beam region and main beam region. By preventing the AC signal from reaching light detecting means  170 , it enhance detecting the accurate TES. 
         [0062]    Referring to  FIG. 4 , assuming Y axis lies along the track direction and x axis lies along the tangential direction, in the diffraction grating  140   a , the first grating pattern A 1  covers the area except sub beam region and main beam region which overlaps with the sub beam regions and the second grating pattern A 2  covers the rest of the diffraction grating  140   a.    
         [0063]    The second grating pattern A 2  prevent the ±1 st  beam from reaching the optical storage, so that AC signal is excluded from the process of detecting TES signal. 
         [0064]      FIG. 5  shows a plane view of the second embodiment of a diffraction grating according to the present invention which may be used in the optical pickup  100  in  FIG. 1 . 
         [0065]    Referring to  FIG. 5 , similarly to the first embodiment, the second embodiment of diffraction grating  140   b  comprises the first grating pattern A 3  and the second grating pattern A 4 . The first grating pattern A 3  is in the shape of rectangle which does not overlap with circular pattern of sub beam P 4 , P 6 . The second grating pattern A 4  covers the rest of the diffraction grating  140   a.    
         [0066]    Preferably, one side of the first grating pattern A 3  is in contact of the circular pattern of sub beam as shown in the  FIG. 5 . The width and length of the rectangle is variable within the scope of the present invention. 
         [0067]      FIG. 6  shows a plane view of the third embodiment of a diffraction grating according to the present invention which may be used in the optical pickup  100  in  FIG. 1 . 
         [0068]    Referring to  FIG. 6 , similarly to the first embodiment, the third embodiment of diffraction grating  140   c  comprises the first grating pattern A 5  and the second grating pattern A 6 . The first grating patter A 5  comprises two horizontally long rectangles, each of rectangles being placed in the top and the bottom respectively. 
         [0069]    Similarly, the first grating patter P 5  does not overlaps with the circular patterns of sub beams P 4 , P 6  and the second grating pattern A 6  covers the rest of the diffraction grating  140   a.    
         [0070]    The one side of the first grating pattern A 5  passes through upper or lower two of four intersection points at which the circular pattern of main beam and those of sub beams. The width and length of the rectangle of the first grating pattern is variable within the scope of the present invention. 
         [0071]      FIG. 7  shows push-pull signals MPP generated by 0 th  and SPP1 and SPP2 generated by ± 1   st  beams after being reflected by track structure on the optical storage and transmitting the first, second or third diffraction grating  140   a ,  140   b ,  140   c  of present invention. Note that there is substantially no AC signal in the push-pull signals generated by ±1 st  beam. By transmitting the diffraction gratings  140   a ,  140   b ,  140   c  of present invention DC offset is excluded from the signal detected by the light detecting means  170  which will be described with reference to  FIG. 9   a  and the following drawings. 
         [0072]    Meanwhile, tracking error level from tracking error signal detected by the light detecting means  170  can be calculated by the following equation. It is noted the tracking error level is improved by the present invention since the AC signal of SPP signal is excluded before it reaches the optical storage. 
         [0000]      Tracking error level= MPP  signal−k×(the first  SPP 1 signal+the second  SPP  signal)  (Equation 3)       Wherein “k”=DC level of MPP signal÷(2×DC level of SPP signal)         
         [0074]    The first grating patterns A 1 , A 3 , A 5  just pass the main beam b 2  without phase shift, and shift the phase of the sub beams B 1 , B 3 , so that the phase-shifted sub beams are excluded from the process of detecting tracking error signal. 
         [0075]    The gratings of the second grating patterns A 2 , A 4 , A 6  have different direction from those of the first grating patterns A 1 , A 3 , A 5 , for example, by 90° so that they can divert beam towards a certain position other than light detecting means  170 . 
         [0076]      FIG. 8  shows positions where main beam and sub beams reach over the optical storage according to the present invention. 
         [0077]    The main beam B 2  is on the border line between the unrecorded area U and recorded area R and the sub beams are shifted by about ½ TP from the border line, which corresponds to the track lines on the optical storage. 
         [0078]      FIG. 9   a  shows change of offset voltage dependent on time when there is no radial shift of object lens and  FIG. 9   b  shows change of offset voltage dependent on time when there is radial shift of object lens, in both cases the object lenses being placed on-axis. Before time=0 along time axis, it represent offset voltage in the unrecorded area, and after time=0 along time axis, offset voltage in the unrecorded area. 
         [0079]    The difference between the unrecorded area U and recorded area R appears as difference of reflection ratio. When applying DDP method using three beams, comparing  FIGS. 9   a  and  9   b , there occurs a voltage level difference between the unrecorded area and the recorded area by the radial shift of object lens, i.e. by moving object lens over the optical storage. 
         [0080]    There is no change of offset voltage level between before and after t=0 when there is no radial shift of object as shown in  FIG. 9   a , while there occurs a difference of offset voltage level between before and after t=0 when there is radial shift of object as shown in  FIG. 9   b.    
         [0081]      FIG. 10  shows change of offset voltage dependent on time when sub beam error occurred in which the object lenses are placed on-axis. 
         [0082]    In  FIG. 10 , sub beam error occurred, so that sub beam was de-tracked towards 0 th  beam by 10 TP. As such, offset voltage level change was increased near t=0. 
         [0083]      FIG. 11  shows change of offset voltage dependent on time when sub beam error occurred and there is radial shift of object lens in which the object lenses are placed on-axis. Note that offset voltage level change was even more increased near t=0. 
         [0084]      FIGS. 12   a  and  12   b  show change of offset voltage dependent on time when there is radial shift of object lens by 1 au (arbitrary unit) and 5 au respectively in which the object lenses are placed off-axis. 
         [0085]    Comparing  FIGS. 12   a  and  12   b , it is noted that the more radial shift there is, the more serious the offset voltage level change gets. 
         [0086]    In on-axis configuration in which two objects are along the radial direction, ±1 st  beams are shifted from the 0 th  beam by ½ TP and the shift amount is fixed with the object lens moving, so that there occurs relatively small amount of offset change. In contrast, in off-axis configuration in which two objects are along the track direction, ±1 st  beams are shifted from the 0 th  beam by ½ TP and the shift amount varies depending the distance from the center of optical storage, so that there can occur very large amount of offset level change. 
         [0087]      FIG. 13   a  shows change of offset voltage dependent on time when there is radial shift of object lens by 5 au and sub beam error occurred in which the object lenses are placed on-axis and  FIG. 13   b  shows change of offset voltage dependent on time when there is radial shift of the object lens by 5 au and sub beam error occurred in which the object lenses are placed off-axis. 
         [0088]    Comparing  FIG. 13   a  and  FIG. 13   b , it is noted that there occurs more serious offset voltage level change near t=0 in  FIG. 13   b  than  FIG. 13   a.    
         [0089]      FIG. 15  shows change of offset voltage dependent on time detected by using the optical pickup according to the present invention, given the same conditions as those of  FIG. 13   b  measured in an optical pickup according the present invention. 
         [0090]    Comparing  FIG. 14  and  FIG. 13   a  or  13   b , it is noted that the amplitude of AC signal is slightly changed at t=0 but there is substantially no offset voltage level change near t=0. 
         [0091]      FIG. 15  shows a schematic diagram of an optical pickup  200  according to the second embodiment of the present invention. 
         [0092]    Referring to  FIG. 15 , the optical pickup  200  according to the second embodiment of the present invention comprises light source  210 , collimate lens  220 , beam splitter  230 , wavelength plate  250 , object lens  255 , diffraction grating  240 , condensing lens  260  and light detecting means  270 , and an optical storage  280  may be placed before the object lens  255 . 
         [0093]    The structure of the second embodiment of the optical pickup of  FIG. 15  is similar to the second embodiment of  FIG. 1 , but is different in that the diffraction grating  240  is positioned between beam splitter  230  and condensing lens  260 . 
         [0094]    The optical pickup according to the first embodiment of the present invention of  FIG. 1  can employ all of three embodiment of diffraction gratings  140   a ,  140   b ,  140   c , while the optical pickup according to the second embodiment of the present invention of  FIG. 15  cannot employ second embodiment of diffraction grating  140   b.    
         [0095]    Referring to  FIG. 5 , when there is radial shift of object lens, i.e. object lens moves along the radial direction, which is corresponds to the horizontal direction of the paper in  FIG. 5 , the first grating pattern region A 3  of the second embodiment of diffraction grating  140   b  can intrude the second grating pattern region A 4 . In this case, there may be a significant error in detecting tracking error signal, which makes the second embodiment of the diffraction grating unavailable. 
         [0096]    Detailed description regarding other components in  FIG. 15  will be the same as that of  FIG. 1  and is omitted. 
         [0097]    The optical pickup according to the present invention provides following advantages: 
         [0098]    The offset voltage level change can be prevented when off-axis configuration is employed and the object moves over the border of unrecorded area and recorded area. 
         [0099]    It is possible to alleviate the offset voltage level change without being affected by radial shift, sub beam error etc. and without DPP level and light efficiency being degraded when performing tracking servo over HD DVD, DVD-R, DVD-RW, BD which have different track structures.

Technology Category: 3