Improvement to holographic data storage using optimized phase mask
Holographic data storage has the advantages of high parallelism, fast access, and large capacity. The storage capacity is represented by the stored pages and pixels in each page. Due to the 3-D nature of the holographic medium, many pages of data may be multiplexed by various methods. For optimal us...
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creator | You-Seok Bae Jianwen Yang Sang-II Jin Soo-Young Lee Cheol-Hoon Park |
description | Holographic data storage has the advantages of high parallelism, fast access, and large capacity. The storage capacity is represented by the stored pages and pixels in each page. Due to the 3-D nature of the holographic medium, many pages of data may be multiplexed by various methods. For optimal use of the dynamic range of the medium, various phase masks are used to uniform the Fourier spectrum. The design of these masks is based on statistical properties of the input pixels. But, the interpixel cross talk, which is dominated by the pixels within the same page, is difficult to reduce owing to the diffraction of the limited aperture size of the medium. In the paper, we expect the spectrum to be uniform and the reconstruction error to be minimal simultaneously. Therefore, we set the targets of the spectral distribution to be constant /spl rho//sub f/ and the reconstructed amplitude /spl rho//sub 2/ equal to the input /spl rho//sub 1/. The desired /spl rho//sub f/ should be chosen so that the energy of the spectral plane would be equal to that of the input plane. We can get the transform matrix between input and Fourier plane and between input and output. |
doi_str_mv | 10.1109/CLEOPR.1999.811484 |
format | Conference Proceeding |
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The storage capacity is represented by the stored pages and pixels in each page. Due to the 3-D nature of the holographic medium, many pages of data may be multiplexed by various methods. For optimal use of the dynamic range of the medium, various phase masks are used to uniform the Fourier spectrum. The design of these masks is based on statistical properties of the input pixels. But, the interpixel cross talk, which is dominated by the pixels within the same page, is difficult to reduce owing to the diffraction of the limited aperture size of the medium. In the paper, we expect the spectrum to be uniform and the reconstruction error to be minimal simultaneously. Therefore, we set the targets of the spectral distribution to be constant /spl rho//sub f/ and the reconstructed amplitude /spl rho//sub 2/ equal to the input /spl rho//sub 1/. The desired /spl rho//sub f/ should be chosen so that the energy of the spectral plane would be equal to that of the input plane. We can get the transform matrix between input and Fourier plane and between input and output.</description><identifier>ISBN: 9780780356610</identifier><identifier>ISBN: 0780356616</identifier><identifier>DOI: 10.1109/CLEOPR.1999.811484</identifier><language>eng</language><publisher>IEEE</publisher><subject>Energy efficiency ; Holography ; Memory ; Optical diffraction ; Optical distortion ; Optical modulation ; Optical recording ; Optimized production technology ; Pattern matching ; Phase modulation</subject><ispartof>Technical Digest. CLEO/Pacific Rim '99. Pacific Rim Conference on Lasers and Electro-Optics (Cat. 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Therefore, we set the targets of the spectral distribution to be constant /spl rho//sub f/ and the reconstructed amplitude /spl rho//sub 2/ equal to the input /spl rho//sub 1/. The desired /spl rho//sub f/ should be chosen so that the energy of the spectral plane would be equal to that of the input plane. We can get the transform matrix between input and Fourier plane and between input and output.</description><subject>Energy efficiency</subject><subject>Holography</subject><subject>Memory</subject><subject>Optical diffraction</subject><subject>Optical distortion</subject><subject>Optical modulation</subject><subject>Optical recording</subject><subject>Optimized production technology</subject><subject>Pattern matching</subject><subject>Phase modulation</subject><isbn>9780780356610</isbn><isbn>0780356616</isbn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>1999</creationdate><recordtype>conference_proceeding</recordtype><sourceid>6IE</sourceid><sourceid>RIE</sourceid><recordid>eNotj81Kw0AURgdEUGpeoKt5gcSZzP9SQ9VCoCLdl5vkJhltOiEzCvr0FtqPA2d34CNkzVnBOXOPVb3ZvX8U3DlXWM6llTckc8ayM0JpzdkdyWL8ZOdJxaXW9-R5O81L-MEJT4mmQMdwDMMC8-hb2kECGlNYYED6Hf1poGFOfvJ_2NF5hIh0gvj1QG57OEbMrl6R_ctmX73l9e51Wz3Vubcm5X1pXK9A6l5iD9aattFKtJpLjr2xTacsqBKh6bAtmZYNE4brphQWobQtEyuyvmQ9Ih7mxU-w_B4uP8U_oudJ_g</recordid><startdate>1999</startdate><enddate>1999</enddate><creator>You-Seok Bae</creator><creator>Jianwen Yang</creator><creator>Sang-II Jin</creator><creator>Soo-Young Lee</creator><creator>Cheol-Hoon Park</creator><general>IEEE</general><scope>6IE</scope><scope>6IL</scope><scope>CBEJK</scope><scope>RIE</scope><scope>RIL</scope></search><sort><creationdate>1999</creationdate><title>Improvement to holographic data storage using optimized phase mask</title><author>You-Seok Bae ; Jianwen Yang ; Sang-II Jin ; Soo-Young Lee ; Cheol-Hoon Park</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i87t-f279f5a46f4efa887cb653c6141ef78bd58a52eabdec2064b03716b238ea28c03</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>1999</creationdate><topic>Energy efficiency</topic><topic>Holography</topic><topic>Memory</topic><topic>Optical diffraction</topic><topic>Optical distortion</topic><topic>Optical modulation</topic><topic>Optical recording</topic><topic>Optimized production technology</topic><topic>Pattern matching</topic><topic>Phase modulation</topic><toplevel>online_resources</toplevel><creatorcontrib>You-Seok Bae</creatorcontrib><creatorcontrib>Jianwen Yang</creatorcontrib><creatorcontrib>Sang-II Jin</creatorcontrib><creatorcontrib>Soo-Young Lee</creatorcontrib><creatorcontrib>Cheol-Hoon Park</creatorcontrib><collection>IEEE Electronic Library (IEL) Conference Proceedings</collection><collection>IEEE Proceedings Order Plan All Online (POP All Online) 1998-present by volume</collection><collection>IEEE Xplore All Conference Proceedings</collection><collection>IEEE Electronic Library (IEL)</collection><collection>IEEE Proceedings Order Plans (POP All) 1998-Present</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>You-Seok Bae</au><au>Jianwen Yang</au><au>Sang-II Jin</au><au>Soo-Young Lee</au><au>Cheol-Hoon Park</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Improvement to holographic data storage using optimized phase mask</atitle><btitle>Technical Digest. CLEO/Pacific Rim '99. Pacific Rim Conference on Lasers and Electro-Optics (Cat. No.99TH8464)</btitle><stitle>CLEOPR</stitle><date>1999</date><risdate>1999</risdate><volume>2</volume><spage>389</spage><epage>390 vol.2</epage><pages>389-390 vol.2</pages><isbn>9780780356610</isbn><isbn>0780356616</isbn><abstract>Holographic data storage has the advantages of high parallelism, fast access, and large capacity. The storage capacity is represented by the stored pages and pixels in each page. Due to the 3-D nature of the holographic medium, many pages of data may be multiplexed by various methods. For optimal use of the dynamic range of the medium, various phase masks are used to uniform the Fourier spectrum. The design of these masks is based on statistical properties of the input pixels. But, the interpixel cross talk, which is dominated by the pixels within the same page, is difficult to reduce owing to the diffraction of the limited aperture size of the medium. In the paper, we expect the spectrum to be uniform and the reconstruction error to be minimal simultaneously. Therefore, we set the targets of the spectral distribution to be constant /spl rho//sub f/ and the reconstructed amplitude /spl rho//sub 2/ equal to the input /spl rho//sub 1/. The desired /spl rho//sub f/ should be chosen so that the energy of the spectral plane would be equal to that of the input plane. We can get the transform matrix between input and Fourier plane and between input and output.</abstract><pub>IEEE</pub><doi>10.1109/CLEOPR.1999.811484</doi></addata></record> |
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identifier | ISBN: 9780780356610 |
ispartof | Technical Digest. CLEO/Pacific Rim '99. Pacific Rim Conference on Lasers and Electro-Optics (Cat. No.99TH8464), 1999, Vol.2, p.389-390 vol.2 |
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language | eng |
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source | IEEE Electronic Library (IEL) Conference Proceedings |
subjects | Energy efficiency Holography Memory Optical diffraction Optical distortion Optical modulation Optical recording Optimized production technology Pattern matching Phase modulation |
title | Improvement to holographic data storage using optimized phase mask |
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