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- W2081262011 abstract "With use of the Lie transform technique, a simple and compact but quite general expression is derived for the ponderomotive scalar and vector potentials ${ensuremath{phi}}^{mathrm{av}}$ and ${stackrel{ensuremath{rightarrow}}{mathrm{A}}}^{mathrm{av}}$ in the covariant form $({stackrel{ensuremath{rightarrow}}{mathrm{A}}}^{mathrm{av}},i{ensuremath{phi}}^{mathrm{av}})={{A}^{mathrm{av}}}_{ensuremath{mu}}=ensuremath{-}frac{1}{2}〈{F}_{ensuremath{mu}ensuremath{nu}}{ensuremath{zeta}}_{ensuremath{nu}}〉$. The four-vector ${ensuremath{zeta}}_{ensuremath{nu}}$ is the particle excursion in four-dimensional space due to the rf electric and magnetic fields, ${F}_{ensuremath{mu}ensuremath{nu}}$ is the high-frequency electromagnetic tensor, and the brackets denote an average over the high-frequency phase $stackrel{ensuremath{rightarrow}}{mathrm{k}}ifmmodecdotelsetextperiodcenteredfi{}stackrel{ensuremath{rightarrow}}{mathrm{x}}ensuremath{-}ensuremath{omega}t$." @default.
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- W2081262011 date "1981-01-26" @default.
- W2081262011 modified "2023-09-27" @default.
- W2081262011 title "Covariant Form of the Ponderomotive Potentials in a Magnetized Plasma" @default.
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- W2081262011 doi "https://doi.org/10.1103/physrevlett.46.240" @default.
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