1. Field of the Invention
The present invention relates to a hologram recording apparatus for recording a hologram in a so-called coaxial system.
2. Description of the Related Art
As a hitherto known hologram recording apparatus, an apparatus is disclosed in Japanese Laid-open Patent Publication No. 2006-113296. The hologram recording apparatus disclosed in the document is configured for recording a hologram in a hologram recording medium in a so-called coaxial system. In such a hologram recording apparatus of the coaxial system, light from a light source is converted into parallel light by a collimating lens, and then divided into recording light (signal light) and reference light through a spatial light modulator, further, the recording light and reference light are converged into the hologram recording medium through the same objective lens.
As for the spatial light modulator, a central pixel region is to be a region for producing the recording light, and a peripheral pixel region is to be a region for producing the reference light. In the central pixel region and the peripheral pixel region, a plurality of pixels are formed in a lattice-shape with a uniform pitch. As shown in
However, according to the hitherto known hologram recording apparatus described above, when the peripheral pixel region in the spatial light modulator is enlarged, the central pixel region becomes relatively down-sized, thereby causing a decrease in the amount of recording information accordingly. Also, because the luminous flux width W of the reference light R becomes larger in addition to the incident angle of the reference light R being large, an area where the recording light S and the reference light R are not overlapped on the hologram recording medium B, that is an idle exposed area, becomes enlarged. Therefore, it has been difficult to satisfy both conditions of desirably making the recording light S and the reference light R interfere with each other and enhancing the recording density.
Accordingly, the present invention has been made under the aforementioned circumstances. The object of the present invention is to provide a hologram recording apparatus, capable of enhancing recording density while desirably making recording light and reference light interfered with each other.
According to one aspect of the present invention, a hologram recording apparatus for recording a hologram comprises a light source emitting a light, an objective lens and a spatial light modulator. The spatial light modulator comprises a light modulating region, which comprises a central pixel region being formed on the spatial light modulator and comprising a plurality of first pixels, and a peripheral region being formed so as to surround the central region and comprising a plurality of second pixels, where the plurality of second pixels including a pixel being larger than each of the first pixels. A first part of the light passed through the central pixel region and a second part of the light passed through the peripheral pixel region incident on the objective lens, wherein the hologram is recorded with the first and the second lights.
According to another aspect of the present invention, a hologram recording apparatus is a hologram recording apparatus for recording a hologram by dividing light from a light source into recording light and reference light through a spatial light modulator, and emitting the recording light and reference light through the same objective lens onto a hologram recording medium; wherein the spatial light modulator has a light modulating region including a plurality of pixels; the light modulating region is divided into a central pixel region where a part of the light from the light source is led to the objective lens as the recording light, and a peripheral pixel region where the rest or another part of the light is led to the objective lens as the reference light; and a plurality of pixels which are included in the peripheral pixel region includes larger pixels than a plurality of pixels which are included in the central pixel region.
Preferably, the peripheral pixel region is further divided into a plurality of regions, and the outer region includes the larger pixels in the regions.
Preferably, an average area of a plurality of pixels which are included in the peripheral pixel region is larger than an average area of a plurality of pixels which are included in the central pixel region.
Preferably, a light blocking region is provided between the central pixel region and the peripheral pixel region.
Preferably, the peripheral pixel region is formed in a concavo-convex shape so that a predetermined phase difference is produced between the adjacent pixels.
Preferably, the average pixel areas Ss and Sr satisfy the relationship Ss<Sr<6.25 Ss, assuming that Ss is the average pixel area of the central pixel region, and Sr is the average pixel area of the peripheral pixel region.
Other features and advantages of the present invention will become apparent from the following detailed description taken in conjunction with the accompanying drawings.
Hereinafter, a preferred embodiment of the present invention will be specifically described with reference to the drawings.
The light source 1 includes, for example, a semiconductor laser device. The light source 1 outputs relatively narrow-spectrum coherent laser light at the times of recording and reproducing.
The collimating lens 2 converts the laser light outputted from the light source 1 into parallel light. The laser light, which has become parallel light, enters a spatial light modulator 3.
The spatial light modulator 3 includes, for example, a transmissive liquid crystal panel. The spatial light modulator 3 has, as shown in
As shown in
The reproducing objective lens 5 has basically the same optical properties as the recording objective lens 4, and leads the reproducing light P produced at the time of producing to the image pickup device 6.
The image pickup device 6 includes, for example, a CCD area sensor or a CMOS area sensor. The image pickup device 6 converts the received reproducing light P into a digital signal, and reads out two-dimensional information recorded as a hologram in the hologram recording medium B.
Next, functions of the hologram recording apparatus A will be described.
At the time of recording, laser light from the light source 1 enters the spatial light modulator 3 through the collimating lens 2. In the central pixel region 31 of the spatial light modulator 3, each pixel enters ON-OFF state according to the recording information, whereby the recording light S including a predetermined pixel pattern is produced.
On the other hand, in the peripheral pixel region 32 of the spatial light modulator 3, predetermined pixels between the pixels having a phase difference equivalent to 0 and the pixels having a phase difference equivalent to π are brought into an ON state, whereby a reference light R including a predetermined phase pattern is produced. An example of the predetermined phase pattern is, a pattern according to the determinant of the Walsh-Hadamard Transform. By varying such a phase pattern, so-called multi-phase recording is performable.
In this regard, the reference light R is led to the objective lens 4 as diffracted light according to the size of pixels (pixel pitch T) of the peripheral pixel region 32, and the recording light S is led to the objective lens 4 as diffracted light according to the size of pixels (pixel pitch t) of the central pixel region 31. As for the diffracted light from each of the pixels, the diffraction angle becomes smaller as the pixel pitch becomes larger, whereby the luminous flux density is to be large. Therefore, the reference light R is emitted onto the hologram recording medium B with a large incident angle compared with the recording light S, which can be made to interfere with the reference light R with a certain level of light intensity.
This means a luminous flux width Wr of the reference light R in relation to the luminous flux width Ws of the recording light S can be smaller than ever before. By making the luminous flux width Wr of the reference light R smaller as described above, an idle exposed area where the recording light S and the reference light R are not overlapped in the hologram recording medium B becomes smaller. Thus, the idle exposed area and the overall irradiated area become smaller, and consequently, the recording density of the hologram can be enhanced.
An optical system A′ shown in
As the configuration of the embodiment, making the pixels in the peripheral pixel region 32 larger than those in the central pixel region 31 of the spatial light modulator 3 produces optically the same functional effects as making the aperture magnification of the aperture filter F smaller in the optical system A′. In this regard, distance between a zero-order diffracted light and first-order diffracted light according to the aperture filter F is expressed by λf/T, where assuming that X is the aperture radius of the aperture filter F, λ is the wavelength of the laser light, f is the focal distance of the lens group L1 (equivalent to the distance between the spatial light modulator 3′ and the lens group L1), and T is a pixel pitch in the spatial light modulator 3′. The aperture magnification is a ratio of the aperture radius X to λf/T which is expressed by magnification. The aperture magnification can be assumed to be the ratio of the pixel pitch t of the central pixel region 31 to the pixel pitch T of the peripheral pixel region 32.
In such an optical system A′, an experiment in which the aperture magnification is varied has been carried out. It is assumed that the number of pixels in the spatial light modulator 3′ is 40000, and a reproducing signal can be received from each pixel. As the results of the experiment shown in
Thus, according to the hologram recording apparatus A of the embodiment, while the incident angle of the reference light R becomes relatively large by the objective lens 4 suitable for a coaxial system, the light intensity of the reference light R can be maintained at a predetermined level, whereby the recording light S and the reference light R can be made to desirably interfere with each other, and consequently, the hologram can be recorded at a high resolution.
Also, while the light intensity of the reference light R is to be at a predetermined level, the idle exposed area can be made smaller than ever before, whereby the irradiated area for recording the hologram can be made as small as possible, and consequently, the recording density of the hologram can be enhanced.
As for a spatial light modulator 3 shown in
According to the hologram recording apparatus with such a configuration, the second circular region 32B on the outside becoming a larger incident angle is formed so as to be larger in pixel pitch T2, whereby, while the light intensity of the reference light R from the second circular region 32B can be maintained at a predetermined level, its luminous flux width can be made further smaller. Therefore, the idle exposed area can be made further smaller.
Still further, because incident angles between the reference light R from the first circular region 32A and the reference light R from the second circular region 32B are somewhat different, so-called multi-angle recording is performable by alternately controlling the first and second circular regions 32A and 32B respectively, thus the multiplicity of the hologram can be greater and the recording density can be enhanced.
However, the present invention is not limited to the above-described embodiments.
For example, the first circular region and the second circular region may be approximately equal in pixel pitch and a light blocking region may be provided therebetween. Also, no light blocking region may be provided between the first circular region and the second circular region, or between the central pixel region and the peripheral pixel region.
Number | Date | Country | Kind |
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2007-118264 | Apr 2007 | JP | national |