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We can find that the surges of intra-coding percentage occur during the appearance of transition effects.
The appearance of transition proteins correlates with the condensation of chromatin whereas protamines remodel it into a novel torroidal conformation.
During the capping phase of acrosome development, the size of the doughnut-like chromatin domain increases, and this area often is marked by uniform nucleosome loss and the first appearance of transition protein 2 and protamine 1.
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The appearance of the transition region makes a toughness increase and stress gradient decrease.
During the process of subsequent low temperature heat treatment of precursor gel, the formation of α-Al2O3 was firstly observed at temperature as low as 400 °C without the appearance of other transition phases.
In terms of their structure and energy states, it is confirmed that the Al-centered first shell clusters play dominant role in the appearance of glass transition prior to the crystallization.
The electrolytes formulated in MOEMC are characterized by the appearance of glass-transition temperatures without encountering freezing points, and this unique low-temperature behavior has allowed us to experimentally determine their glass-transition temperatures.
In particular, the contribution that reverberations in recurrent neural networks may have in the appearance of these transitions could depend strongly on synaptic properties.
Awake state was marked by the presence of low-amplitude fast activity; SWS was identified by continuous high-amplitude slow activity and regular appearance of spindles; transitions from SWS into rapid eye movement (REM) sleep were identified by a decrease in high-amplitude slow activity, increase of theta activity and presence of spindles.
A complete analysis of our model, both with mean-field approaches and numerical simulations, shows the appearance of complex transitions between high (up) and low (down) neural activity states, driven by the synaptic noise, with permanence times in the up state distributed according to a power-law.
Typically, micro-phase separation occurs in soybean oil and LoSatSoy polymers as evidenced by the appearance of two glass transition temperatures α1 and α2; α1 (approximately 80°C) is the glass transition temperature of the crosslinked polymer, and α2 (approximately 0°C) corresponds to the solid liquid transition (glass transition) of the oil-rich phase in the bulk polymer.
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