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After approximate replacing of Maxwellian distribution exponent with therational polynomial fraction we have obtained precise analytical expression forand calculated the principal value of logarithmically divergent integral in theelectron wave dispersion equation. At the same time our calculations have shownthe presence of strong collisionless damping of the electromagneticlow-velocity (electron) wave in plasmas with Maxwellian-like electron velocitydistribution function at some small, of the order of several per cents,differences from Maxwellian distribution in the main region of large electrondensities, however due to the differences in the distribution tail, whereelectron density itself is negligibly small.

Strong collisionless damping of the low-velocity branch of  electromagnetic wave in plasmas with Maxwellian-like electron velocity  distribution function