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As is well known, the plasma velocity exceeds the bulk He gas flow velocity. Plasma diffusion to the walls of the flow tube results in the plasma residing more toward the axis, where the peak of the parabolic radial velocity distribution of the buffer gas occurs. See
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As is well known, the plasma velocity exceeds the bulk He gas flow velocity. Plasma diffusion to the walls of the flow tube results in the plasma residing more toward the axis, where the peak of the parabolic radial velocity distribution of the buffer gas occurs. See. Ferguson E.E., Fehsenfeld F.C., and Schmeltekopf A.L. Adv. At. Mol. Phys. 5 (1969) 1
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-1.) In an earlier FALP experiment, the plasma velocity was measured with radially-movable probes and found to be independent of radial position, showing directly that radial diffusion averaged the plasma velocity across a diameter of the flow tube. See
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-1.) In an earlier FALP experiment, the plasma velocity was measured with radially-movable probes and found to be independent of radial position, showing directly that radial diffusion averaged the plasma velocity across a diameter of the flow tube. See. Adams N.G., Church M.J., and Smith D. J. Phys. D 8 (1975) 1409
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