Abstract:
The present invention relates to an apparatus for reading from and/or writing to holographic storage media with a simplified common aperture setup. 
     According to the invention an apparatus for reading a data page from and/or writing a data page to a holographic storage medium, with a coaxial arrangement of one or more reference beams and an object beam or a reconstructed object beam, has one or more spatial light modulators for generating the one or more reference beams by modulating a light beam with a modulation pattern having a spatial frequency higher than the spatial frequency of the data page.

Description:
FIELD OF THE INVENTION 
       [0001]    The present invention relates to an apparatus for reading from and/or writing to holographic storage media, and more specifically to an apparatus for reading from and/or writing to holographic storage media using a simplified common aperture setup. 
       BACKGROUND OF THE INVENTION 
       [0002]    In holographic data storage digital data are stored by recording the interference pattern produced by the superposition of two coherent laser beams, where one beam, the so-called ‘object beam’, is modulated by a spatial light modulator and carries the information to be recorded. The second beam serves as a reference beam. The interference pattern leads to modifications of specific properties of the storage material, which depend on the local intensity of the interference pattern. Reading of a recorded hologram is performed by illuminating the hologram with the reference beam using the same conditions as during recording. This results in the reconstruction of the recorded object beam. 
         [0003]    One advantage of holographic data storage is an increased data capacity. Contrary to conventional optical storage media, the volume of the holographic storage medium is used for storing information, not just a few layers. One further advantage of holographic data storage is the possibility to store multiple data in the same volume, e.g. by changing the angle between the two beams or by using shift multiplexing, etc. Furthermore, instead of storing single bits, data are stored as data pages. Typically a data page consists of a matrix of light-dark-patterns, i.e. a two dimensional binary array or an array of grey values, which code multiple bits. This allows to achieve increased data rates in addition to the increased storage density. The data page is imprinted onto the object beam by the spatial light modulator (SLM) and detected with a detector array. 
         [0004]    Currently mainly three solutions for holographic storage systems are discussed. In the collinear system, as disclosed for example in EP 1 624 451, separate parts of the objective lens aperture are used for the object beam and the reference beam, respectively. This arrangement is a so-called coaxial system, i.e. the object beam and the reference beam run along the same axis. This system uses a kind of shift multiplexing as a multiplexing method. 
         [0005]    In the off-axis recording system, as disclosed for example in U.S. Pat. No. 6,721,076, the object beam and the reference beam do not share the same optical path. In this system angle and polytopic multiplexing are used. 
         [0006]    The basic idea of the common aperture recording system, which is described, for example, in WO 2006/003077, is that the object beam and the reference beam(s) fill the full aperture of the objective lens. The common aperture system is hence a special type of coaxial system. For read-out the beams are separated in the focal plane, i.e. the Fourier plane of the reconstructed hologram image. This is different from the collinear concept, where the object beam and the reference beam only fill a distinct part of the aperture and, as a consequence, are separated in the image plane of the hologram. The common aperture system allows to achieve a higher data capacity, but the setup is more complex and instable, as the object beam and the reference beam(s) have to be separated, formed and joined. 
       SUMMARY OF THE INVENTION 
       [0007]    It is an object of the invention to propose an apparatus for reading from and/or writing to holographic storage media with a simplified common aperture setup. 
         [0008]    According to the invention, this object is achieved by an apparatus for reading a data page from and/or writing a data page to a holographic storage medium, with a coaxial arrangement of one or more reference beams and an object beam or a reconstructed object beam, which has one or more spatial light modulators for generating the one or more reference beams by modulating a light beam with a modulation pattern having a spatial frequency higher than the spatial frequency of the data page. 
         [0009]    The idea of the invention is to generate the object beam and the reference beam(s) for the common aperture recording system with one or more spatial light modulators. This is achieved by using special pixel patterns, where the data patterns, which code the binary data, are modulated with a reference beam pattern of a higher spatial frequency than the maximum spatial frequency of the data pattern. Thus the object beam and the reference beam can be separated in the Fourier domain, which is the basic principle of the common aperture system. The invention allows to realize the common aperture system without the need to separate and join the object beam and the reference beam by optical means. Both beams use the same optical path. The setup is thus much simplified and the system becomes more stable with regard to shocks and vibrations. In addition, the requirements for the coherence length of the laser can be lowered, because the optical path lengths for the object beam and the reference beam are automatically nearly the same. 
         [0010]    According to a further aspect of the invention, the above advantages are likewise achieved by a method for writing a data page to a holographic storage medium using a coaxial arrangement of one or more reference beams and an object beam, which has the step of generating the one or more reference beams by modulating a light beam with a modulation pattern having a spatial frequency higher than the spatial frequency of the data page. 
         [0011]    Similarly, the above advantages are also achieved by a method for reading a data page from a holographic storage medium using a coaxial arrangement of one or more reference beams and a reconstructed object beam, which has the step of generating the one or more reference beams by modulating a light beam with a modulation pattern having a spatial frequency higher than the spatial frequency of the data page. 
         [0012]    Preferably, a single spatial light modulator is provided for modulating the light beam with a superposition of the data page and the modulation pattern. This has the advantage that the cost of the optical setup is reduced, as only one spatial light modulator is necessary. 
         [0013]    Alternatively, two spatial light modulators are provided for modulating the light beam in series with the data page and the modulation pattern. Ideally both spatial light modulators are arranged in parallel close to each other in the object plane. It is not significant whether the modulation pattern or the data page are imprinted on the light beam first. This solution has the advantage that different types of spatial light modulators may be used, e.g. having different pixel sizes or different switching times. In addition, the spatial light modulator for imprinting the modulation pattern can likewise be static, i.e. it may have a fixed modulation pattern. In this case a simple phase or amplitude mask is preferably employed. 
         [0014]    Preferentially, the data pixels of the data page are formed by groups of pixels of the one or more spatial light modulators. This easily allows to use the same spatial light modulator or at least the same type of spatial light modulator for imprinting both the modulation pattern and the data page on the light beam. 
         [0015]    Advantageously, the reconstructed object beam is separated from the one or more reference beams by a spatial filter. This spatial filter is located in a Fourier plane. As the object beam and the one or more reference beams have different spatial frequencies, they are spatially separated in and close to the Fourier plane. Consequently, a spatial filter such as an aperture allows to separate the beams in a cheap and efficient way. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0016]    For a better understanding the invention shall now be explained in more detail in the following description with reference to the figures. It is understood that the invention is not limited to this exemplary embodiment and that specified features can also expediently be combined and/or modified without departing from the scope of the present invention. In the figures: 
           [0017]      FIG. 1  shows a known transmission type apparatus for reading from and writing to holographic storage media during the writing operation, 
           [0018]      FIG. 2  shows the apparatus of  FIG. 1  during the reading operation, 
           [0019]      FIG. 3  illustrates a common aperture apparatus for reading from and/or writing to holographic storage media according to the invention, 
           [0020]      FIG. 4  illustrates an example of a data pattern, where each data pixel is formed by 3×3 SLM pixels, 
           [0021]      FIG. 5  illustrates a modulation pattern for generating reference beams, 
           [0022]      FIG. 6  shows the data page resulting from the superposition of the data pattern and the modulation pattern, 
           [0023]      FIG. 7  illustrates the intensity distribution resulting from the data page of  FIG. 6  in the focal plane of a first Fourier lens, 
           [0024]      FIG. 8  shows the intensity distribution of a reconstructed object beam in the focal plane of a third Fourier lens after spatial filtering, 
           [0025]      FIG. 9  illustrates the intensity distribution of the reconstructed object beam in the image plane on the array detector, 
           [0026]      FIG. 10  shows the image obtained by the array detector, 
           [0027]      FIG. 11  illustrates the histogram of the detector values of  FIG. 10 , and 
           [0028]      FIG. 12  depicts retrieval of the initially stored binary data through slicing. 
       
    
    
     DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS 
       [0029]    In the following description reference is made to transmission type holographic storage systems with two reference beams. Of course, the idea is also applicable to reflection type holographic storage systems, where the data is recorded and read from only one side of the holographic storage medium. Furthermore, only a single reference beam or more than two reference beams may be used. 
         [0030]    An exemplary setup of a known common aperture apparatus for reading from and writing to holographic storage media is shown in  FIG. 1 . For simplification only the principal rays of the light beams are illustrated. A source of coherent light, e.g. a laser diode  1 , emits a light beam  2 , which is collimated, expanded and filtered by a beam expander and filter arrangement  3 . The light beam  2  is then divided into two separate light beams  5 ,  6  by a beam splitter  4 . The first light beam  5 , the so called “object beam”, passes a beam shutter  7  and is directed by two mirrors  8 ,  9  towards a spatial light modulator (SLM)  10 . The SLM  10  modulates the light beam  5  to imprint a 2-dimensional data pattern. The object beam  5  is filtered by a pair of Fourier lenses  11 ,  13  and a spatial filter  12 , which filters out the high frequency components of the object beam  5 . The object beam  5  is then focused into a holographic storage medium  15 , e.g. a holographic disk or card, by an objective lens  14 . The second light beam  6 , the reference beam, also passes a beam shutter  16  before it impinges on a partial beam generating element  17 , e.g. a bi-prism or a diffractive element. The partial beam generating element  17  generates two or more partial reference beams  6   a ,  6   b  from the reference beam  6 . The partial beam generating element  17  is designed in such a way that the foci of the two partial reference beams  6   a ,  6   b  lie besides the focal area of the object beam  5 . The partial reference beams  6   a ,  6   b  are coupled into the optical path of the object beam  5  by a beam coupling element  18 , e.g. a beam splitter, and focused into the holographic storage medium  15  by the objective lens  14 . At the intersection of the object beam  5  and the partial reference beams  6   a ,  6   b  an interference pattern appears, which is recorded in a photo-sensitive layer of the holographic storage medium  15 . 
         [0031]    As shown in  FIG. 2 , the stored data are retrieved from the holographic storage medium  15  by illuminating a recorded hologram with the partial reference beams  6   a ,  6   b  only. For this purpose the object beam  5  is blocked by the beam shutter  7 . The partial reference beams  6   a ,  6   b  are diffracted by the hologram structure and produce a copy of the original object beam  5 , the reconstructed object beam  19 . This reconstructed object beam  19  is collimated by an objective lens  20  and directed onto a 2-dimensional array detector  24 , e.g. a CCD-array. A further pair of Fourier lenses  21 ,  23  and a further spatial filter  22  block the partial reference beams  6   a ,  6   b . The spatial filter  22  is advantageously also used for filtering out the high frequency components of the reconstructed object beam  19 . The array detector  24  allows to reconstruct the recorded data. 
         [0032]    In order to simplify the generation of the reference beams  6   a ,  6   b  and the separation of the reference beams  6   a ,  6   b  and the reconstructed object beam  19 , the main idea of the invention is to generate the object beam  5  and the reference beams  6   a ,  6   b  with the SLM  10 . The SLM  10  may be a phase or amplitude SLM. It is likewise possible to apply more than one SLM  10  in series. The corresponding common aperture setup is illustrated in  FIG. 3 . The setup is essentially the same as the setup of  FIG. 1 . However, the reference beam path is omitted, which simplifies the optical setup. Instead, the reference beams  6   a ,  6   b  are generated by modulating the data pattern with an additional pattern, which mainly consists of higher spatial frequencies than the data pattern. This is either done by the same SLM  10  as used for imprinting the data page on the light beam  2 , or by an additional SLM  10 a (indicated by the dashed rectangle). Of course, in the latter case the SLM  10  can likewise be used for imprinting the modulation pattern, whereas the additional SLM  10   a  imprints the data page. The high frequency modulation pattern acts as a reference beam  6   a ,  6   b  for the common aperture holography. As a consequence, the spatial filter  12  is modified such that it does not filter out the spatial frequencies of the modulation pattern, i.e. the diameter of the aperture is increased. Of course, it is likewise possible to modify the spatial filter  12  in such way that only one reference beam  6   a ,  6   b  is passed. In the figure, the spatial separation of the object beam  5  and the reference beams  6   a ,  6   b  is for illustration purposes only. 
         [0033]    In the following specific embodiment a one-dimensional modulation of the data pattern is realized by generating one data pixel with several pixels of a single SLM  10 . An example of a data pattern is shown in  FIG. 4 . In this case one data pixel  30  is formed by 3×3 SLM pixels  31 . A channel bit ‘1’ corresponds to 3×3 bright pixels, whereas a channel bit ‘0’ corresponds to 3×3 dark pixels. 
         [0034]    An example of a one-dimensional amplitude modulation pattern  32  is shown in  FIG. 5 . The modulation pattern  32  consists of lines of bright pixels with a width of one pixel, which are separated by two dark pixels. As a consequence the spatial frequency of the modulation pattern  32  is higher than the spatial frequency of the data pattern. Of course, other types of modulation patterns  32  can likewise be used, as long as they exhibit a sufficiently large fraction of high spatial frequencies compared to the spatial frequency of the data pattern. For example, the modulation pattern  32  may be a 2-dimensional grating, or a stochastic or pseudo-stochastic structure such as a grating with variable line distances. Apart from an amplitude modulation pattern  32  also a phase modulation pattern may be used, e.g. a grating with a sinusoidal phase modulation. The latter has the advantage that ideally no zeroth order is generated, which simplifies the separation of the light beams  5 ,  6   a ,  6   b  in the Fourier plane. 
         [0035]    The final data page  33 , which results from the superposition of the data pattern and the modulation pattern  32 , is illustrated in  FIG. 6 . This pattern  33  is applied by the SLM  10  to the light beam  2  emitted by the light source  1 . As can be derived from the figure, in order to reduce the number of pixels of the SLM  10  the pixels are preferably adapted to the modulation pattern. In the specific example, rectangular pixels with a size corresponding to three vertically adjacent square pixels could be used. 
         [0036]    The intensity distribution in the focal plane of the first Fourier lens  11  resulting from the final data page  33  of  FIG. 6  is shown in  FIG. 7  in logarithmic scale with arbitrary units. Three regions of higher intensity can be identified. The central region is generated by the lower frequency content of the signal, i.e. mainly the data pattern. The regions at the sides of the central region result from the high-frequency content, i.e. mainly the modulation pattern  32 . This separation of the data pattern and the modulation pattern  32  is also found in the focal plane of the third Fourier lens  21  and makes it possible to separate the reconstructed object beam  19  and the reference beam  6   a ,  6   b  in this plane. 
         [0037]    For reading, only the modulation pattern  32  of  FIG. 5  is applied to the light beam  2  by the SLM  10 . The original data pattern is then reconstructed by the hologram stored in the holographic storage medium  15 . In order to filter out the reference beams  6   a ,  6   b  the aperture of the spatial filter  22  between the holographic storage medium  15  and the array detector  24  is chosen such that the intensity peaks resulting from the reference beam  6   a ,  6   b  in the focal plane of the third Fourier lens  21  are blocked.  FIG. 8  shows an intensity plot of the remaining intensity distribution in this focal plane behind the aperture of the spatial filter  22  in logarithmic scale with arbitrary units. 
         [0038]    The resulting signal intensity distribution in the image plane on the array detector  24  is depicted in  FIG. 9 . As can be seen the high-frequency content of the reference beams is completely filtered out. The data signal can thus be recovered without being disturbed by the signal of the reference beams  6   a ,  6   b . In this specific embodiment this is done by detecting the signal with an array detector  24  that is chosen and adjusted in such a way that each data pixel  30 , which consists of 3×3 SLM pixels  31 , falls on one detector pixel. The resulting image obtained by the array detector  24  is shown in  FIG. 10 . The binary data coded by the initial data pattern of  FIG. 4  are recovered by simple slicing. For this purpose an intensity level, i.e. a slice level, has to be determined. The slice level decides if a pixel value is detected as a bright or a dark pixel, i.e. as ‘1’ or ‘0’ of the channel code. For example, the slice level can be determined from the histogram of the detector values, which is shown in  FIG. 11 . It can be seen that the bright and dark pixels are well separated and a slice level can easily be determined. After slicing the initially stored binary data are retrieved. This is illustrated in  FIG. 12 .