Moreover, since the energy of rotational motion does not depend on angle φ, the only effect of this on the partition function of the molecule would be to reduce it by a factor of 2. We thus obtain, in the classical approximation,11 (27)jnuc-rot(T)=(2SA+1)2T2Θr. Obviously, ...
Consequently, there are no quasi-minimal rotational surfaces of parabolic type in this class. 2− II. Let + ( ) = 0, = 0. In this case the mean curvature vector field is 11 − H = 1 1 2 1 which implies again that H H = 0 if and only if H = 0. Consequently, there are...
the vast majority of the eigenvalues live on the unit circle, where the global density localises. The potential (1.26) is not in the general class of suitable potentials we consider above, cf. Def.1.1. Hence the bulk and edge behaviour differ from Theorem1.2. Recall that ...
a light source would be directed onto the rotor R from a position above the substrate. The light source could be any type of optical signal. The rotor plate could also serve as a paddle for inducing and/or detecting fluid motion in microfluidics systems, as a gated catalyst in wet chemistr...
Quasi-minimal rotational surfaces in pseudo-Euclidean four-dimensional spaceHence,σ(zu;zu) =x′1x′′2−x′′1x′2√1 + (r′)2n1+r′′√1 + (r′)2n2;σ(zu;zv) = 0;σ(zv;zv) =−r√1 + (r′)2n2:With respect to the orthonormal frame field{X;Y}we get the formulas:...
He developed the first prototype of a 6DoF strong-motion accelerograph system. Three single-axis analogue gyroscope (Systron Donner, Concord, USA, Model QRS11-00010-200) has been used in [82], which had frequency response between DC and 60 Hz. The recorded peak ground rotation rates around ...