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- W123211091 abstract "As shown in Sect. 1.2, for high sounding frequencies, vector equation (1.11) splits up into three scalar equations, and it is sufficient to consider the equation for one component of the field $$Delta E + {k^2}varepsilon left( {r,k} right)E = 0$$(3.1), where $$varepsilon left( {r,w} right) = 1 - frac{{4pi {r_e}Nleft( r right)}}{{{k^2}left( {1 + i{nu _{eff}}left( r right)/omega } right)}},{kern 1pt} {kern 1pt} {kern 1pt} {kern 1pt} {kern 1pt} {kern 1pt} {kern 1pt} {kern 1pt} k = frac{{2pi f}}{c} = frac{w}{c}$$is the wave number, v eff (r) is the efficient electron collision frequency, N(r) is electron concentration, and the “ion” contribution to the dielectric permittivity may be neglected [Ginzburg, 1961]. The relation for ɛ has the same form both in the SI and cgs systems; only the expression for r e varies." @default.
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- W123211091 date "2003-01-01" @default.
- W123211091 modified "2023-09-27" @default.
- W123211091 title "Inverse Scattering Problems" @default.
- W123211091 doi "https://doi.org/10.1007/978-3-662-05221-1_4" @default.
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