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No ASE was observed for F8BT under 390 nm excitation for either the rotaxinated and the conventional blend, most likely as a result of the lower absorption cross section of F8BT at 390 nm with respect to the polyrotaxane in the "threaded" case and due to the complete absence of optical gain in the spectral region of F8BT emission in the unthreaded blend Figure 2d
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No ASE was observed for F8BT under 390 nm excitation for either the rotaxinated and the conventional blend, most likely as a result of the lower absorption cross section of F8BT at 390 nm with respect to the polyrotaxane in the "threaded" case and due to the complete absence of optical gain in the spectral region of F8BT emission in the unthreaded blend (Figure 2d).
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