Scattering of Microwaves form a Cylindrical Plasma in the Born Approximation. II.
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The scattering of a microwave, which is fed by an oscillating electric dipole, is treated in the Born approximation. When the source is a dipole poetwetez, where e_x is a unit vector in the z direction, the scattered field from a collisionless cylindrical plasma is given by Es(r,t)=p_0√π/2 e(3/4)πj k^4/√klp(ι+ρ) e j(ωτ-κι-κρ) s_0^∞ n(ρ') J_0 (2κρ' sinθ/2)ρ'dρ'e_z, where (ι, π, 0) and (ρ, θ, 0) are the cylindrical coordinates of the source and the observing point, respectively, η(ρ') is ωρ^2/ω^2 with the plasma frequency ωρ and here only the term lowest in 1/κι and 1/κι is retained.
- 社団法人日本物理学会の論文
- 1961-07-05
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