Atomic Masses and Fundamental Constants 4 1972
DOI: 10.1007/978-1-4684-7876-1_21
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Measurements of Atom Masses in the Region from Titanium to Iron

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Cited by 2 publications
(2 citation statements)
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“…The most satisfactory filling was obtained at a magnetic-field intensity on the system axis of about 850 Oe. The microwave power supplied was 100 W. The microwave discharge in the residual gas in the pressure range 10~s to 10" 6 torr created a plasma with conventional parameters: n e = 10 9 -10 10 cm" 3 , T e = 5 eV, Ti <T e . Analyses show that, with these plasma parameters, we get a superbanana diffusion regime in which localized particles must make the main contribution to diffusion losses across the magnetic field.…”
Section: Plasma Generationmentioning
confidence: 99%
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“…The most satisfactory filling was obtained at a magnetic-field intensity on the system axis of about 850 Oe. The microwave power supplied was 100 W. The microwave discharge in the residual gas in the pressure range 10~s to 10" 6 torr created a plasma with conventional parameters: n e = 10 9 -10 10 cm" 3 , T e = 5 eV, Ti <T e . Analyses show that, with these plasma parameters, we get a superbanana diffusion regime in which localized particles must make the main contribution to diffusion losses across the magnetic field.…”
Section: Plasma Generationmentioning
confidence: 99%
“…To reduce superbanana plasma losses it is possible to convert trapped charged particles into circulating particles using an alternating longitudinal electric field, with an alternation frequency identical with or a multiple of the oscillation frequency of the particles trapped between local magnetic mirrors [3,4]. This possibility has been tested experimentally in the Saturn stellarator, where it was shown [5] that plasma losses in the superbanana diffusion regime can be reduced by 30-40% when an alternating electric field with a broad spectrum is excited in the plasma.…”
Section: Introductionmentioning
confidence: 99%