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The general expression for the ponderomotive Hamiltonian is used to obtain the quasi-static quasi-neutral density change caused by the ponderomotive force of a cold magnetoplasma wave of arbitrary frequency and polarization: δn (x) =−[‖E(x) ‖2−‖B(x) ‖2] /4π (Te+Ti).
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Kaufman et al. (1979) studied this question.
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