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An in situ nanolamellar Ti5Si3/TiNi composite is prepared by arc melting based on the design principle of load sharing between a hard component and a phase transforming matrix.
The spectra from the north rim and the central regions are composed, at least, of 2 components: one is a thin thermal component with a temperature of about 0.4 keV and the other is a hard component represented by either a thin thermal emission model with a temperature higher than a few keV or a power-law model with a photon index of ∼2.
These experiments showed that ground-level cosmic rays consist of two components: a "soft" component which is capable of prolific generation of multiple particle events, and a "hard" component which is capable of traversing great thicknesses of lead.
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If this were the only process, the intensity of the hard component passing through a layer of solid material would decrease by the same amount as in an equivalent layer of air.
In response to these requirements, a composite coating technology has been developed, which consists of a hard metal component from the tungsten carbide family of coatings and a hard refractory oxide layer produced from a slurry coating.
While the genetic model presented here is a soft selection model (i.e., each local population contributes to the next generation independently of its mean relative fitness), the integration of demographic processes (i.e., the demo-genetic model) clearly adds a hard selection component (since the size and contribution of demes partly depend on their genetic loads).
With the individual thickness property adjusted, the multilayer was even harder than its hard component (TiC).
The spectra all exhibit the hard component without the thermal feature, and are spatially extended.
A series of hybrid polyurethane POSS materials have been synthesized on the basis of poly tetramethylene glycol) (Terathane 1400®) as soft component, 4,4′-methylenebis phenylisocyanate) (MDI) as hard component, and 1,4,4′-methylenebis phenylisocyanate
Fig. 6 Representative results of stepwise thermal demagnetization of three-axis IRM produced in steady fields at 3.0 T (hard component), 0.40 T (medium component), and 0.12 T (soft component).
HIRM, the hard component of IRM, is derived from the formula: HIRM = (SIRM + bIRM)/2, where the bIRM is usually defined as IRM-0.3T (the IRM value obtained at 300 mT back field).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com