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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.
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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 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.
Particle size versus ground time clearly shows the existence of a size-induced regime transition (i.e., regime I and II).
We found two distinct particle size regimes (i.e., regime I and II), which were further confirmed by our thermoelectric measurements.
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).
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.
Furthermore, the global and the local fluid dynamic properties are related to the prevailing flow regime, i.e., the homogeneous flow regime and the heterogeneous flow regime.
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