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First order transitions of a solvent in a gel differ from those of the solvent alone.
When applied to seeds, TMA and DMA techniques provide information consistent with existing information on glass and first order transitions.
The transitions are normally first order, although second order transitions have been suggested for several compounds such as cadmium II) and barium II) stearates [20, 58].
The higher order transitions were found to be contributing ~33%% of the power to the emission spectrum at this current density.
These spectral features between 1050 and 1100 nm were previously attributed to higher order transitions of the QW as discussed in Fig. 2.
These higher order transitions should have a very low oscillator strength in a regular QW, and their appearance with significant (i.e., non-zero) PC and EL is attributed to the strain/piezoelectric modulation of the QW by the QDs.
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As a last point of this paper, we consider second-order transitions.
As only the dipole transition leads to Raman scattering, the higher-order transitions will cause a decrease in the overall efficiency of the enhancement.
These exothermic transitions, with peak temperatures of 74 80 °C and 115 132 °C, respectively, were attributed to disorder-order transitions of different kinds.
One of the most intriguing features of IDPs is their ability to undergo disorder-to-order transitions upon binding in order to perform their function.
For first-order transitions and disordered systems, on the other hand, macroscopic energy barriers need to be overcome to prevent dynamic ergodicity breaking.
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