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The main objective of this design is to extend the T1 relaxation dispersion range covered by electronic field-cycling to higher frequencies.
Reaction order with respect to hydrogen decreases with H/Ru, whilst reaction order with respect to CO2 changes slightly within examined dispersion range.
We see no high-k waves in the elliptical dispersion range for this subwavelength unit cell structure [58].
Therefore, we hypothesize that the combination of the short lifespan and the dispersion range of the pollinator could counter-select any partial preference of the insect.
Furthermore, the active dispersion range was consistent with the intrinsic proton exchange rates (700 10,000 s−1) measured by Liepinsh and Otting from OH and NH groups of several amino acid side chains under physiologic conditions [31].
For quantitative variables, measures of central tendency were calculated (average and median), as well as measures of dispersion (range and standard deviation).
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In this interval, the second-order dispersion for the c axis ranges from 35 fs2/mm to -14 fs2/mm, and the third-order dispersion ranges from 36 fs3/mm to 142 fs3/mm.
For the b axis the second-order dispersion ranges from 35 fs2/mm to -15 fs2/mm and the third-order from 73 fs3/mm to 185 fs3/mm.
Pd/Al2O3 with different Pd dispersion ranging from 0.11 to 0.41 was obtained by the treatment under reducing atmosphere at 400 800 °C for various hours.
Negative dispersion ranging from −183 to −281 ps/(nm km) in S + C bands is achieved with the refractive index differences between matrical material and cylindrical inclusions no more than 0.03.
The choice for these dispersion ranges was based on microscopic observations [6, 9, 10].
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