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Microscopy and differential scanning calorimeter (DSC) were used to study the phase transition of samples collected from the mixer at different times and temperatures during processing.
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However, the transition of sample 2 is between 3° and 10°.
The transition of sample 2 is broader than sample 1, which is relative to the Fig. 4 results.
Figure 5 shows, for example, the GaAsBi PL transition of sample 1, which is strongly asymmetric, together with the Gaussian fitting of the two exciton recombination-related peaks.
The type-I transition of sample #8 displayed an average shift of Δλ = 1.2 ± 2.0 nm and up to Δλ = 6.5 nm for outliers.
However, sample #7 and the type-II transition of sample #8 displayed roughly linear Δλ– F due to symmetry breaking (i.e., the relative orientation of the applied field with respect to the type-II asymmetry of the structure).
Even larger shifts (as large as Δλ = 13.1 nm, Figure 3 ) were observed for the type-II transition of sample #8 (this sample has ∼730 nm type-I transition and ∼630 nm type-II transition due to an asymmetric type-II interface), with an average shift of Δλ = 3.5 ± 3.1 nm.
The transition of sample from the acidic gastric (pH 2) to the mild alkaline intestinal environment (pH 7.4) caused a significant decrease in the amount of anthocyanins as compared with the initial samples, wherein the higher anthocyanins stability was observed for red cabbage (67.7% recovery versus 13.2% for anthocyanin-rich extract)— Table 1.
The transition of the samples is defined through the construction of a sequence of intermediate distributions, which are sampled through application of a resample-move scheme.
For the model of area percolated, the transition of two samples is 1°~4° and 1°~8°, respectively.
This may contribute to the diffuse phase transition of the samples.
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