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Nanosegregation processes can be viewed as changes in the nearest (first and second) environment of a certain atom, which under favourable conditions lead to further ordering of phase.
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Doping CuO/MgO system with K2O decreased the degree of ordering of CuO and MgO phases [16].
The order of phase transition is examined by computing Navard and Cox ratio from the peak heights of the DSC thermograms recorded.
These higher orders of phase transition certainly exist as their non-detection is simply the general belief that all orders of phase transition greater than 2 can always be attributed to field fluctuations [10, 11].
The validity of Ehrenfest classification of orders of phase transition has been a subject of debate [18, 19].
Motivated by this, we developed a Landau-like theory based on Ehrenfest classification of orders of phase transition [15, 16].
Within the Ehrenfest classification of orders of phase transition, we propose a continuous (>2) phase transition for studying the dependence of M on the Fe-Pn layer separation.
Equation 1 can be generalized to Landau-like form for orders of phase transition >2 as F p M, z = ∫ d d r M 2 p − 2 { − a p M 2 + b p M 4 + c p ∇ M 2 + M 2 Γ M, z } ∀ p > 2 Open image in new window (2).
The order of phases in the clusters varied depending on the location of the specific arrhythmogenic substrate responsible for the arrhythmia.
Similarly, a reversal error reversed the serial order of Phases II and III, or followed a Phase II stroke with a late Phase I ellipse stroke, and after a reversal mutant mice were nearly 50% more likely than wild-type mice to go on to complete a strong form of Phase IV.
The crystallite size and ordering of CuO phase decrease to (4 nm) by ZnO-doping (<0.08 mol) for samples calcined at 350 550 °C.
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