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Instead, double-walled lamellae become the most stable phase for P3AT molecules with 25% GD.
Therefore, the most stable phase, α-Al2O3, is the only possible candidate to reproduce the IR absorption feature at 13.55 ± 0.05 μm (Supplementary Note 1).
While γ hydride is the most stable phase, it is very close in energy to the δ phase.
Al5Cu2Mg8Si6 with a lower hardness and elastic modulus exhibits the most stable phase at elevated temperatures, which is correlated with its good creep resistance.
It is shown that due to the limitation in the size of the system, a phase transition which could occur in a macroscopic sample is inhibited and situations may be realized where a metastable phase may be formed in preference to the most stable phase.
In the MD method, however, the crystalline-glassy phase transformation is taking place through a single stage by introducing numerous lattice imperfections to the stable crystalline powders and this leads to raising of the free energy from the most stable phase (tetragonal-Zr2Pd) to a less stable phase (glassy) that is obtained after 216 259 ks of MD time.
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Well known among the various boron allotropes, the most stable phases of the boron bulk are the α-rhombohedral (α-B) and β-rhombohedral (β-B) boron[28].
Solvent drop grinding and most cooling crystallization experiments (using solvents that do not form homosolvates; see Supporting Information) led to the thermodynamically most stable phases at room temperature (AH-II° and MH-I°).
Among these phases, monoclinic structured β-Ga2O3 is the most stable form with a wide bandgap of 4.9 eV [14].
Based on these results, it is suggested that with the described synthesis route only the Ni3Sn2 phase is formed as the most stable intermetallic phase in the Ni-Sn system.
Consequently, the Al2O3 nuclei have higher possibility to overcome a large barrier to form the most stable corundum phase.
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