Photopolymer Media Simulator for Holographic Data Storage using FDTD Method and Non-Local Polymerization Driven Diffusion Model

M. Toishi, T. Tanaka, K. Watanabe
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引用次数: 1

Abstract

We simulated the holographic data storage process using a photopolymer medium taking account of the polymerization and diffusion of the monomer. We used the FDTD method to construct our simulation, which adopts a new model which includes consideration of the polymer chain length and dark reaction. We analyze the dependency of physical mameters of the photopolymer medium, such as polymer chain length and diffusion coefficient, on holographic recording. We also estimate critical physical parameters of the photopolymer medium by fitting with expimental results. 1. Introduction Holographic data storage (HDS) has application to high density archival data storage and next generation consumer optical storage (I). Recent advances of HDS are supported by the progrss of photopolymer materials 121. We should consider monomer diffision and the process of polymerizing a holographic medium which has three stages, namely, initiation, propagation, and termhation and also the, so the temporal behavior of hologram recording is relatively complicated. To simulate the holographic recording process, various simulation methods taking account of monomer diffi~sion and polymmization have been proposed (2, 31. In this paper we propose a new model to simulate the holographc recordmg of a photopolymer and construct the simulator using the fink-difference time-domain (FDTD) method. We analyze difiaction efficiency as a function of the polymer chain length, the diffusion coefficient, and the difference between the refractive indices of monomer and polymer. We also estimate various physical parameters of the photopolymer medium by fitting the theoretical model to the experimental data. 2. Numerid model of the photopolymer simulator We adopt the non-local polymerization driven diffusion model (3,4) as the polymerization model, and revise this model by consi-g he dark rwcLion and kmhaion process LLner the beam illurnhalion. The 1-~enuioml non-local diffision equation considering the dark reactim is written as n(q,t,) = Cp@p(%,t,)+Cm@m(%,t,)~~~# 3 (6)
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基于FDTD方法和非局部聚合驱动扩散模型的全息数据存储光聚合物介质模拟器
考虑到单体的聚合和扩散,我们模拟了光聚合物介质的全息数据存储过程。采用时域有限差分法进行仿真,采用了考虑聚合物链长和暗反应的新模型。我们分析了光聚合物介质的物理参数,如聚合物链长和扩散系数对全息记录的依赖性。通过与实验结果的拟合,估计了光聚合物介质的关键物理参数。1. 全息数据存储(HDS)已应用于高密度档案数据存储和下一代消费级光存储(I)。光聚合物材料的进展支持了HDS的最新进展121。由于要考虑到单体的分裂和全息介质的聚合过程有起始、传播和终止三个阶段,同时还要考虑到全息记录的时间行为相对复杂。为了模拟全息记录过程,人们提出了考虑单体扩散和聚合的各种模拟方法(2,31)。本文提出了一种模拟光聚合物全息记录的新模型,并利用时域时域差分(FDTD)方法构建了仿真器。我们分析了衍射效率是聚合物链长、扩散系数以及单体和聚合物折射率之差的函数。我们还通过将理论模型拟合到实验数据中来估计光聚合物介质的各种物理参数。2. 我们采用非局部聚合驱动扩散模型(3,4)作为聚合模型,并通过在光束光离子中加入暗光和光离子过程对该模型进行修正。考虑暗反应的1-~ enuoml非局部分裂方程为n(q,t,) = Cp@p(%,t,)+Cm@m(%,t,)~~~# 3 (6)
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