boltzmann-ginzburg-landau approach to simple models of active matter

This is sufficient to get tightness in the space of continuous functions and then almost sure convergence is a consequence of a non trivial theorem on Banach valued martingales in

2014 A model based on second rank tensor orientational properties of smectic phases is developed.. The model predicts a second order smectic A-smectic C phase transition

Nous analysons ensuite comment la nature des transitions (continues ou discontinues) et la nature des phases obtenues (états de valence pure ou mixte) sont affectées par

In the disordered state the alloys show no longer a spontaneous magnetization but a weak paramagnetism independent of the Cr concentration, which is attributed to

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L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des

The estimated Tc of the Penrose (dual Penrose) lattice is higher (lower) than that of the square lattice, although the average coordination numbers of these three

Equation (12) has all the features required to describe a second-order lamellar-to-cubic phase transition. the average principal curvatures of the bilayer. However,