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In the overdoped regime, the material behaves as a reasonably conventional metal, with a large Fermi surface3,4.
When sectioned, this material behaves as a solid, continuous molecular sieve membrane.
But the surface of the material behaves as a very good conductor, like a metal, allowing electrons to travel freely.
In all cases, the material behaves as a paramagnet above the characteristic transition temperature; it acquires a macroscopic magnetic moment only when an external field is applied.
Therefore, in using this method of analysis, the material behaves as if the structure does not deform until it collapses plastically.
Two different previously developed devices were utilized to measure thermal expansion: in the upper part of the cryogenic temperature range where the material behaves as a fluid, and in the lower part of the cryogenic temperature range where the material behaves as a solid for all practical applications.
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Certain nuclei in the test material behave as tiny bar magnets and line up with the field.
The current vs. voltage characteristics of the tungstite NRs showed that the material behaved as a Schottky diode with a breakdown electric field of 3.0 × 105 V m−1.
These prismatic samples, composed by 30%, 50 % and 70 of RAP in weight in relation to the base material, behave as beams, under the specific essays.
Due to the surface effects, the latter model does work as a combination of two subsystems, i.e. the bulk material behaving as a Cauchy continuum, and the boundary surface operating as a membrane-like boundary layer, each subsystem being in (local and global) equilibrium by its own.
It is then recorded that Mn2+ (3d5) ions, which are introduced into Ga2O3 Mn (host material), behave as the luminescence activator in the Ga2O3 Mn material [22].
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com