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Cross-Polarization Scattering Principle
§ Second term: induced current in the ~
opposite polarization ~ Bq
−∇×∇×E +$ωi'2$1− σ 'E=−iμ∂J(i)
( s)&%c)(&%iεω)(s o∂t 0i
iεω2 ñ ω + ! - J(i)= 0 pe E+ i σσE×B/B
kI
kSkθ
ω n i εω2 , i . ie ope
ωI,kI § C-2W: Trajectories of launched X-mode ζ
and back-scattered O-mode nearly overlap (wpe >> wce)
Polarizer
§ O-mode component can be easily separated X-Mode and detected via dedicated receive antenna DBS
HTPD Conference 2020 Presenter: Lothar Schmitz
O-Mode CPS receive ωs=ωi-kθvExB
Launch/ ks=ki-kθ Receive
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