Vertogen, The Equations of Motion for Nematics, Z

This can be simply rephrased by stating that a certain axis of the substitution group, which in general deviates slightly from the symmetry axis of this group, tends to align

Under his stochastic calculus, Peng established the existence and uniqueness of solutions for the stochastic differential equations under G-Brownian motion (G- SDEs) with

He de- veloped the existence and uniqueness of solutions for stochastic differential equations under G-Brownian motion (G-SDEs) under the Lipschitz conditions via the contraction

By applying ten typical EOSs to fit experimental compression data of 50 materials, it is shown that the SMS4 EOS gives the best re- sults; the Baonza and Morse EOSs give the second

Using the experimental data on the dielectric anisotropy, density, polarizability, dipole moment, and order parameter in the nematic phase of seven typical liquid

The well known low contrast ‘stationary’ optical texture observed in conventional experiments results from time averaging of these instant images; its wavelength is 0 = 2. Key

Time-resolved three-dimensional phase-ontrast balaned SSFP, Magneti Resonane in Mediine,.

Theorem 4 implies that there can not be wild solutions on an annulus with smooth rotational initial data that are H¨ older continuous?. Indeed, any admissible H¨ older