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The fluorescence lifetimes range from ∼100 ps to ∼2 ns.
The electronic properties of TiO2 can be easily tuned by linking a PS to its surface.
Then, the relaxation is conducted for 100 ps to assure the system reaches equilibrium.
In [89], data were simulated with different timing resolutions (from 300 ps to non-TOF-PET).
We take 500 ps to tune the resonator, which is at least 10× better that competing designs.
The crystal was first annealed at 300 K and 0 pressure for 100 ps to reach equilibrium.
In particular, the temperature dependence of the transition from a self-trapped Ps to the Bloch state was investigated.
Transmissions from PS to mother were most frequently observed (30 episodes), followed by transmissions from PS to father (20 episodes), and from PS to JH or PS to PS (18 episodes) (Fig. 2).
Transient FWM measurements versus τ12 were taken for nonzero τ23 = 1 ps to exclude nonresonant nonlinearities.
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The introduction of multiple branch points with long side chains allows the LCB-PS to resist the elastic-driven decohesion.
The fluorescent response of G-PS to intracellular glucose changes was tested with HeLa cells.
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