On the covariant theory of plasma oscillations

1978 ◽  
Vol 23 (17) ◽  
pp. 626-628
Author(s):  
Kwok-Kee Tam ◽  
K. Kuen Tam
1969 ◽  
Vol 47 (10) ◽  
pp. 1057-1060 ◽  
Author(s):  
Kwok-Kee Tam ◽  
John O'hanlon

A covariant theory of plasma oscillations for a many-component plasma in the presence of an external magnetic field is formulated.


1968 ◽  
Vol 46 (16) ◽  
pp. 1763-1767 ◽  
Author(s):  
Kwok-Kee Tam

A covariant theory of plasma oscillations in the absence of an external field is formulated by considering a plasma as the limit of an infinite number of relativistic streams.


1966 ◽  
Vol 89 (5) ◽  
pp. 39-47 ◽  
Author(s):  
D.A. Kirzhnits ◽  
Yurii E. Lozovik

2015 ◽  
Vol 60 (3) ◽  
pp. 232-246 ◽  
Author(s):  
V.N. Gorev ◽  
◽  
A.I. Sokolovsky
Keyword(s):  

Author(s):  
M. Born

The theory of lattice deformations is presented in a new form, using the tensor calculus. The case of central forces is worked out in detail, and the results are applied to some simple hexagonal lattices. It is shown that the Bravais hexagonal lattice is unstable but the close-packed hexagonal lattice stable. The elastic constants of this lattice are calculated.


1971 ◽  
Vol 5 (2) ◽  
pp. 239-263 ◽  
Author(s):  
Z. Sedláček

Small amplitude electrostatic oscillations in a cold plasma with continuously varying density have been investigated. The problem is the same as that treated by Barston (1964) but instead of his normal-mode analysis we employ the Laplace transform approach to solve the corresponding initial-value problem. We construct the Green function of the differential equation of the problem to show that there are branch-point singularities on the real axis of the complex frequency-plane, which correspond to the singularities of the Barston eigenmodes and which, asymptotically, give rise to non-collective oscillations with position-dependent frequency and damping proportional to negative powers of time. In addition we find an infinity of new singularities (simple poles) of the analytic continuation of the Green function into the lower half of the complex frequency-plane whose position is independent of the spatial co-ordinate so that they represent collective, exponentially damped modes of plasma oscillations. Thus, although there may be no discrete spectrum, in a more general sense a dispersion relation does exist but must be interpreted in the same way as in the case of Landau damping of hot plasma oscillations.


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