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The quantum yield for the reaction between OX and triethanolamine is too low for the implementation of the device configuration in Fig. 1. As a result, we have not studied this photochemical process in polymer matrices. Instead, we have focused our attention on the photoinduced reaction between OX and triethylamine, which is significantly more efficient.
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The emitted radiation is not sufficiently intense to encourage the photochemical reaction between OX and triethylamine. Consistently, the state of the photosensitive layer does not change significantly even after thousands of emission readings.
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The detected emission intensity decreases by ca. 2% after 1000 excitation cycles. It follows that ca. 6610 excitation cycles would, presumably, lower the detected intensity to the logic threshold. Thus, a binary 0 cannot be read more than 6610 times. In principle, this limitation can be overcome by selecting a fluorophore with an excitation wavelength in a spectral region where the photosensitive layer does not absorb.
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