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By F. Balasa

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Hereafter, we explain the algorithm by using a one-dimensional translation effect in the pixel-matched system with a simplified channel model. A received pixel Cm(k, l) can be represented as a function of two adjacent spatial light modulator pixels, A(k-1, l) and A(k, l), as shown in Fig. 6 and Eq. (7). 24 Data Storage Fig. 6. Illustration of one-dimensional translation effect with parameter σ (Menetrier & Burr, 2003). Cm k , l    ffCCD 2  ff CCD 2  ff CCD 2  ff CCD 2   Ak , l h  x   , y   Ak  1, l h  x    1, y  dxdy 2 (7) Rewriting Eq.

5. Grayscale encoding Fig. 2(d) shows that the THG signal depends on the number of pulses. This can be used to encode the information onto a grayscale. Using an acousto-optic modulator, the number of pulses is well controlled. As presented in the Fig. cm-2 is linear with the number of pulses between 1104 and 5 104 pulses. Considering the readout error, the encoding becomes possible with a 16 levels grayscale (4 bits). Optical data storage in photosensitive glasses and spin state transition compounds 39 Fig.

2003). This phenomenon was explained using the so-called domino effect (Koshino & Ogawa, 1998): When the concentration of the local excited HS state is higher than a critical Optical data storage in photosensitive glasses and spin state transition compounds 41 value, all the system commutes from an LS to an HS state. According to these experiments, one may wonder if a single laser pulse may also induce the same phenomena in a cooperative iron(II) SCO material. , 2003). , 2004). Compared to the experiments reported on valence tautomeric compounds, our results indicated that the final state reached after a laser excitation is neither a pure HS nor a pure LS state, but it is instead a “mixture” of HS/LS domains.

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