Three-body components of collision-induced light scattering by rare gases

1990 ◽  
Author(s):  
Daniel Coffman ◽  
Lothar Frommhold ◽  
Massimo Moraldi
2012 ◽  
Vol 136 (10) ◽  
pp. 104104 ◽  
Author(s):  
Li-Yan Tang ◽  
Zong-Chao Yan ◽  
Ting-Yun Shi ◽  
James F. Babb ◽  
J. Mitroy

2011 ◽  
Author(s):  
Tetsuo Nishikawa ◽  
Kazuhiro Tanaka ◽  
Atsushi Hosaka ◽  
Kanchan Khemchandani ◽  
Hideko Nagahiro ◽  
...  

1994 ◽  
Vol 49 (6) ◽  
pp. 4602-4609 ◽  
Author(s):  
Silvia Pestelli ◽  
Ubaldo Bafile ◽  
Lorenzo Ulivi ◽  
Marco Zoppi

1958 ◽  
Vol 25 (2) ◽  
pp. 210-213
Author(s):  
L. E. Goodman ◽  
A. R. Robinson

Abstract The well-known noncommutativity of three-dimensional finite rotations has long been a curiosity in mechanics since, in actual solution of dynamical problems, the angular velocity, which is conveniently representable as a vector, plays a more natural role. In modern inertial guidance systems, however, the orientation of a body in space, i.e., a rotation, is of primary engineering interest. In this paper a simple method of determining orientation from the time history of three body components of angular velocity is developed by means of a new theorem in kinematics. As a special case of this theorem it is shown that a gyro subjected to a regime of rotations which returns it to the original space orientation will, in general, produce a residual signal. It will have experienced a nonzero and easily calculated mean angular velocity about its input axis. Some implications of the theorem for the design of inertial guidance systems and for the testing of gyros are discussed.


1996 ◽  
Vol 74 (6) ◽  
pp. 1180-1186 ◽  
Author(s):  
Sean A.C. McDowell ◽  
Ashok Kumar ◽  
William J. Meath

Formulae for the computation of isotropic and anisotropic dipolar dispersion energy coefficients, for two-body and three-body interactions involving H2, N2, CO, and the rare gases, are presented in an average energy approximation. These coefficients are computed to within 1% of the reliable values for these coefficients, which are obtained by using the relevant dipole oscillator strength distributions, with the exception of a few that are recorded in tabular form. The input data required for these formulae are the isotropic and anisotropic polarizabilities and average energies for the interacting species. The results provide the first reliable anisotropic triple-dipole dispersion energy coefficients for interactions involving molecules. Key words: non-additive, anisotropic, interaction energies, triple-dipole dispersion energies.


1991 ◽  
Vol 72 (2) ◽  
pp. 345-352 ◽  
Author(s):  
S.M. El-Sheikh ◽  
G.C. Tabisz ◽  
L. Ulivi

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