The above and other features and advantages of the present invention will become more apparent by describing in detail exemplary embodiments thereof with reference to the attached drawings in which:
Hereinafter, an optical information processing apparatus, an optical information recording method, and an optical information reproducing method according to exemplary embodiments of the present invention will be described with reference to the attached drawings. The optical information processing apparatus according to the exemplary embodiments of the invention can be embodied as an optical information reproducing apparatus by excluding the structure of an optical information detector, while the optical information processing apparatus can be embodied as an optical information recording apparatus by excluding the structure of a light modulator and partially modifying the structure of an optical system. Accordingly, in the following description, the optical information processing apparatus will be described without distinguishing the recording apparatus and the reproducing apparatus.
As shown in
The light modulator 130 may be employed a reflecting type spatial light modulator as an example a digital micro-mirror device (DMD).
The light modulator 130 provides a signal beam pattern 131 and a reference beam pattern 132 for modulating a beam. Accordingly, the beam reflected by the reflecting mirror 120 is reflected and is supplied as a signal beam S and a reference beam R by the light modulator 130. In the light modulator 130, the signal beam pattern 131 is formed at the center portion of the light modulator 130 and the reference beam pattern 132 is formed around the signal beam pattern 131 in the light modulator 130.
The optical information processing apparatus further includes a beam splitter 140 guiding the signal beam S and the reference beam R coaxially traveling to an optical information storage medium 190 from the light modulator 130. The beam splitter 140 transmits a P polarized beam and reflects an S polarized beam. A shutter 141 and an optical information detector 150 are disposed beside the beam splitter 140. The optical information detector 150 may be a charge-coupled device (CCD), a complementary metal-oxide semiconductor (CMOS), or an optical device capable of detecting light. The shutter 141 is shut at the time of recording optical information and is opened at the time of reproducing optical information.
A reflecting mirror 160 reflecting the signal beam S and the reference beam R to the optical information storage medium 191 is disposed in an optical axial path of the beam splitter 140. A quarter-wavelength (λ/4) plate 170 is disposed next the reflecting mirror 160 and an objective lens 180 is disposed next the quarter-wavelength plate 170. The quarter-wavelength plate 170 converts the P polarized beam passing through the beam splitter 140 into a circularly polarized beam. Accordingly, the beam irradiated to the optical information storage medium 190 through the objective lens 180 is an S polarized beam.
The optical information storage medium 190 is disposed next the objective lens 180. The optical information storage medium 190 can be made of photopolymer. A reflecting plane 191 is formed on the surface of the optical information storage medium 190 opposite to the surface to which the beam is irradiated. The reflecting plane 191 reflects the beam passing through the optical information storage medium 190 in the opposite direction.
On the other hand, as shown in
In the exemplary embodiment, the optical information detector 150 is located beside the coaxial path of the beam traveling toward the optical information storage medium from the light modulator 130. Accordingly, a reproduced beam reproduced from the optical information storage medium 190 in response to the reference beam R at the time of reproducing optical information is reflected by the reflecting plane 191 of the optical information storage medium 190 and travels to the beam splitter 140 through the optical path of the reference beam R. Since the reproduced beam is an S polarized beam after passing through the quarter-wavelength plate 170, the reproduced beam is reflected by the beam splitter 140 and travels to the optical information detector 150. The optical information detector 150 decodes the optical information of the reproduced beam. On the other hand, the optical information detector may be located in the traveling direction of the beam passing through the optical information storage medium 190 at the time of recording optical information. In this case, it is not necessary to form the reflecting plane 191 in the optical information storage medium 190.
In the exemplary embodiment of the invention, the reference beam pattern 132 is provided in a variety of shapes for multiplexing record and reproduction of the optical information. Here, the multiplexing record means that optical information is superposed and recorded at the same position, and the multiplexing reproduction means that a plurality of optical information pieces recorded at the same position are reproduced.
Hereinafter, the reference beam pattern 132 formed in the light modulator 130 according to the exemplary embodiment of the invention will be described in more detail. The reference beam pattern 132 and the signal beam pattern 131 are formed in different areas of the light modulator 130. The optical information can be recorded and reproduced by allowing the signal beam S and the reference beam R generated from the patterns to interfere with each other on the optical information storage medium 190.
An experimental example thereof will be described hereinafter.
It is assumed that the angle between the pectinate patterns is 12 degree, the thickness of the optical information storage medium 190 is 200 μm, the wavelength of the beam is 405 nm, and the focal length of the objective lens 110 is 5 mm. In this condition, it was concluded that optical information can be multiplexed by rotating the reference beam pattern 132 by a rotation angle of 2 degree or more. This conclusion is established in the following description. The below-mentioned graphs illustrate results of the experimental examples of the exemplary embodiment.
As shown in
On the other hand, noises generated due to the multiplexing of the reference beam patterns 132 and 132′ are not completely removed. However, the problem with the noises can be effectively solved by increasing the thickness of the optical information storage medium 190.
In the experimental example, 30 pectinate patterns are formed by setting the angle between the pectinate patterns to 12 degree, the thickness of the optical information storage medium 190 is 1000 μm, the wavelength of the beam is 532 nm, and the focal length of the objective lens 110 is 5 mm. The recording data were recorded and reproduced using analog signals for the purpose of easy distinguishment and understanding. For the distinguishment of the reproduced optical information, “A” was recorded and reproduced in
As described in the exemplary embodiments, the reference beam pattern may be modified in a variety of shapes as long as the reference beam patterns have no correlation with each other. Here, “no correlation” means that a different reference beam pattern is not superposed at the same pixel or position of the light modulator 130. The distance between the reference beam patterns or the gap between the reference beam pattern and the signal beam pattern can be embodied variously depending upon the numerical apertures of the objective lens 180. That is, when the numerical aperture is large, the resolution is high and thus the distance can be reduced. On the other hand, when the numerical aperture is small, the resolution is low and thus the distance can be increased.
The light modulator 220 includes a liquid crystal display device. Examples of the liquid crystal display device constituting the light modulator 130 can include a thin film transistor liquid crystal display device (TFT LCD) which is a typical active matrix type and a super twisted nematic (STN) LCD, a ferroelectric LCD, a polymer dispersed (PD) LCD, and a plasma addressing (PA) LCD which are passive matrix types.
In the light modulator 220, the signal beam pattern 131 is formed at the central portion of the light modulator 220 and the reference beam pattern 132 is formed around the signal beam pattern 131 of the light modulator 220 (see
A reflecting mirror 240 is disposed next to the beam splitter 230. A quarter-wavelength (λ/4) plate 250 and an objective lens 260 are disposed in the traveling direction of the beam reflected by the reflecting mirror 240. The quarter-wavelength plate 250 converts a P polarized beam into a circularly polarized beam. Accordingly, the beam irradiated to the optical information storage medium 270 through the objective lens 260 is a circularly polarized beam. A reflecting plane 271 is formed on the surface of the optical information storage medium 270 opposite to the surface to which the beam is irradiated. The reflecting plane 271 reflects the beam passing through the optical information storage medium 270 in the opposite direction. Accordingly, a reproduced beam at the time of reproducing optical information is reflected by the reflecting plane 271 and then travels to the optical information detector 290. The operating states are similar to those in the above-mentioned exemplary embodiment.
Hereinafter, an optical information recording method and an optical information reproducing method according to an exemplary embodiment of the invention will be described. The methods may be performed by the configuration of the above-mentioned optical information processing apparatus, or may be performed by optical information processing apparatuses according to modified embodiments having a technical concept equal or similar to that of the above-mentioned optical information processing apparatus. The configuration of the optical information processing apparatus referred to in the following description can be understood with reference to the exemplary embodiment shown in
The reference beam R and the signal beam S are coaxially formed by the use of the reference beam pattern 132 and the signal beam pattern 131 formed in the light modulator 130 and then travel toward the optical information storage medium 190. Specifically, the signal beam pattern 131 is formed in the central portion of the light modulator 130 and the first reference beam pattern 132 is formed in the peripheral portion of the signal beam pattern 131 with a predetermined gap therefrom.
The reference beam R and the signal beam S emitted from the light modulator 130 are irradiated to the optical information storage medium 190 through the reflecting mirror 160 and the objective lens 180. The signal beam S is incident on the central portion of the objective lens 180 and the reference beam R is incident on the circumferential portion of the objective lens 110. Since a convex lens is used as the objective lens 180, the objective lens 180 focuses the beams on the optical information storage medium 190. That is, since the refraction angle of the signal beam S incident on the central portion of the objective lens 180 is different from the refraction angle of the reference beam R incident on the circumferential portion of the objective lens 180, the reference beam R and the signal beam S are focused on a recording area in the optical information storage medium 190 and thus the optical information of the signal beam S is recorded by means of the interference between the reference beam R and the signal beam S as shown in
Now, the optical information multiplexing recording method according to an exemplary embodiment of the invention will be described in more detail.
First, optical information is recorded in one track T1 of the optical information storage medium 190 by the use of a first reference beam pattern. The recording areas A11, A12, A13, and A14 in the same track T1 partially overlap with each other. A gap between the overlapping recording areas Ann is located at a null position between side lobes. The gap may be located at a second or next null position, or may be located at a first null position between a main lobe and the side lobes depending upon the diffraction efficiency.
Next, at the time of recording optical information in the second track T2 adjacent to the first track T1, the optical information is recorded by the use of the reference beam generated from a different reference beam pattern having no correlation with the previously used reference beam pattern. The neighboring recording areas A21 and A22 partially overlap with each other and also partially overlap with the recording areas A11 and A12 of the first track T1. The gap between the tracks T1 and T2 is located at a null position between the side lobes of the recording areas A11 and A12 formed in the first track T1. Subsequently, optical information is recorded in the third track T3 so as to partially overlap with the second track T2 by the use of the reference beam used for recording the optical information in the first track T1, and then optical information is recorded in the fourth track by the use of the reference beam used for recording the optical information in the second track.
Optical information is recorded in the recording areas A11 and A12 of the first track T1 in the optical information storage medium 190 by the use of a reference beam generated from a first reference beam pattern. Optical information is recorded in the recording areas A21 and A22 of the second track T2 adjacent to the first track T1 by the use of a reference beam generated from a second reference beam pattern having no correlation with the first reference beam pattern. Optical information is recorded in the recording areas A31 and A32 of the third track T3 by the use of another reference beam generated from a third reference beam pattern. Then, optical information is recorded in the fourth track by the use of the reference beam used for recording the optical information in the first track. The neighboring recording areas A partially overlap with each other and also partially overlap with the recording areas A in the previous track T. Here, the gap between the tracks T is located at a null position between the side lobes of the recording areas A of the previous track T.
Optical information is recorded in the second track T2 by the use of two reference beam patterns having no correlation with each other in the same way as recording the optical information in the first track T1. The reference beam patterns have no correlation with the reference beam pattern used for recording the optical information in the first track T1.
Subsequently, optical information is recorded din the third track T3 by the use of the two reference beams used for recording the optical information in the first track T1 in the same way as recording the optical information in the first track T1. Optical information is recorded in the fourth track in the same way as recording the optical information in the second track T2. Then, optical information is recorded in the next tracks by repeating these operations. As a result, since the optical information is recorded in the recording areas A adjacent to each other and overlapping with each other among the recording areas A by the use of the reference beam patterns having no correlation with each other, it is possible to reduce noises at the time of reproducing the optical information as well as to enhance the recording density of the optical information. On the other hand, the first reference beam pattern 132 and the second reference beam pattern 132′ for multiplexing record may be formed in ring shapes having different diameters, fan shapes formed at different positions, circular comb shapes disposed at different angles, or partial comb shapes formed at different positions. The reference beam patterns may be formed in other shapes.
Two methods can be used to multiplex and record the optical information while changing the reference beam patterns 132 and 132′. In one method, first, optical information is recorded in all the recording areas of the optical information storage medium 190 while changing the optical information of the signal beam S by the use of the reference beam R generated from the first reference beam pattern 132. Thereafter, optical information is superposed and recorded in all the recording areas of the optical information storage medium 190 while changing the optical information of the signal beam S by the use of the second reference beam pattern 132′.
In the other method, optical information is superposed and recorded in a recording area of the optical information storage medium 190 by the use of reference beams R generated from a plurality of different reference beam patterns 132 and 132′, and then optical information is superposed and recorded in another recording area by the use of the different reference beams R.
On the other hand, the reference beam patterns 132 and 132′ for reproducing optical information should be in the same shape as the reference beam patterns 132 and 132′ used for recording the corresponding optical information. In other words, when a shape of reference beam patterns 132 and 132′ is used for recording optical information, the same shape of reference beam pattern 132 and 132′ as used for recording the optical information should be used to reproduce the corresponding optical information. Here, the same shape means that the beam having the same reference pattern, phase, and wavelength should be irradiated, but not that the beam should be irradiated through the same optical system from the same light source.
In the optical information recording method according to the exemplary embodiments of the invention, since optical information can be superposed and recorded in the same recording area by coaxially irradiating the reference beam and the signal beam to the optical information storage medium, it is possible to further enhance the recording density of optical information.
In the optical information processing apparatus, the optical information recording method, and the optical information reproducing method according to the invention, by allowing the reference beam and the signal beam to coaxially travel so as to record optical information and varying the reference beam pattern to a variety of different reference beam patterns having no correlation with each other so as to provide a variety of reference beams, it is possible to more efficiently multiplex the optical information and to enhance the storage density of the utilization efficiency of the holographic optical information.
Number | Date | Country | Kind |
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10-2006-0031304 | Apr 2006 | KR | national |
10-2006-0037382 | Apr 2006 | KR | national |