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It is carried out by immersing the glass in a bath of molten alkali salt (generally a nitrate) at temperatures below the transition range.
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Due to the trapped conformations, configurational entropy becomes smaller, and the associated stretch exponent drops to half of its value below the glass transition range.
Half-life is influenced predominantly by age and blood lipid TCDD concentration at the time of subsequent sampling, with linear equations providing good fit to the data above and below a transition range of 400 700 ppt.
The presence of OA, EPA or DHA suppresses or blurs the pre-transition, induces a shift of the main transition to lower temperatures, and widens the transition temperature range.
For a large range of compositions this system reveals macroscopic Lo/Ld phase coexistence below the transition temperature T c, while above T c they are homogenously mixed.
The introduction of directional micropores increased the swelling ratio below the transition and decreased the swelling ratio above the transition, thereby also enhancing the volume transition.
These detectors are operated at a temperature well below the transition temperature of the superconductor.
And well below the transition, the "thermal cloud" is gone, and only the BEC remains.
Nevertheless, the β phase usually persists below the transition temperature.
Salter et al. 45 find that the flexoelectric difference (e1− e3) in the compound 4-cyanoresorcinol bisbenzoate is negative throughout the nematic-phase range and takes values varying from around −10 pcloseclose to the isotropic transition to approximately 17 pCm−1 around 10 K below the transition.
However, below the transition temperature, where only the α from was expected, both forms crystallized.
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