This paper presents an analysis of the penetration of an intense electromagnetic beam in an inhomogeneous plasma. It is seen that on account of the electron density gradient created by an intense transversely inhomogeneous beam a region is created in the overdense plasma where the beam can propagate. Typically a CO₂ laser beam of width r₀=100 {μ}m, power $P=15$ GW, and ω=1.7×10¹⁴ sec^-1 can penetrate to a region where ωₚ²ω²=20 in a 500-eV inhomogeneous plasma characterized by ωₚ²ω²=(ωₚ₀²ω²)(1+Bz).
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Sodha et al. (1977) studied this question.
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