The transition/crossover from an insulator to a QH state of the filling factor ν > 2 in an ideal spinless 2DES can be denoted as the direct I-QH transition [16 19].
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We found that there are two opposite effects which control the final dispersion state of these filled elastomers during the polymerization.
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However, with increasing fluence there appears a positive contribution affecting the normal exponential recovery of state filling.
The recovery of state filling signal as seen for the shorter probing wavelengths (340 nm, 370 nm) in Fig. 2consists of two distinct temporal components, a fast and a much slower component.
This recorded time sequence is then modified according to the material flow characteristics and the state of die fill to satisfy the requirement of material utilization and forging quality.
An estimation of exciton life-time can be calculated by numerical fitting of the transient absorption curves using an exponential decay (to model the population of filled states in the LUMO).
