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In low light-intensity (I) regime, the exponent n of I equals 1 and kVL = 0.05 cm2 s−1 mW−1.
Transmission spectrum: As discussed, the Type I regime shows high transmission in contrast to other metamaterials where absorption is a major issue.
The three-step model includes reaction between gaseous oxygen and surface complex, C(O), which is key to describing the high reaction orders widely reported in the low temperature Zone I regime.
At low substrate temperatures, 4I regime, films with equivalent bulk mass deposited thicknesses, d≥0.9 nm uniformly cover the substrate and exhibit no discernible crystalline structure for d≤1.6 nm for TS=77 K.
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This chapter reviews recent progress and development of hypernuclear physics in the S=-I regime.
The two lower molecular weight groups show a regime I-regime II transition, which translates to lower temperatures as branching is increased.
Analysis by the Lauritzen and Hoffman (L-H) equation of crystallization rate indicates a regime I-regime II break for lower defect content (3.75%) PVF2 fraction and a regime II-regime III break for higher defect content (5%and5.6%6%) PVF2 fractions.
In medium and high I regimes, n equals 0.36 and 0, kVL equals 1 cm2 s−1 mW−1 and 7 s−1, respectively.
It is interesting to note that based on the change in particle size, we discovered two different size regimes (i.e., regime I, and regime II shown in Fig. 3).
We found two distinct particle size regimes (i.e., regime I and II), which were further confirmed by our thermoelectric measurements.
Although in Fig. 3 where we observe the existence of two regimes (i.e., regime I and II) of particle size as a function of ground time, there is no correlated crystalline phase change.
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