Measurement and interpretation of the velocity space correlation of a laboratory plasma fluctuation with laser induced fluorescence
A technique for probing velocity space correlations has been developed using laserinduced fluorescence. In this paper, a description of the experimental setup is given, with results to follow in a later publication. The experiment consists of a cylindrical plasma column 3m long and radius ~ 0.25 cm,...
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Published in | Journal of instrumentation Vol. 8; no. 11; p. C11015 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
01.11.2013
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Online Access | Get full text |
ISSN | 1748-0221 1748-0221 |
DOI | 10.1088/1748-0221/8/11/C11015 |
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Abstract | A technique for probing velocity space correlations has been developed using laserinduced fluorescence. In this paper, a description of the experimental setup is given, with results to follow in a later publication. The experiment consists of a cylindrical plasma column 3m long and radius ~ 0.25 cm, holding singly-charged argon ions (Ar II) with density n ~ 10 super(9) cm super(-3), T sub(e) ~ 5 eV, T sub(i,) ~ .06 eV, and a 1 kG axial magnetic field. Two separate metastable lines are excited by single frequency lasers at 611 nm and 668 nm. These lasers may tune with a precision of .01 pm. The separate lasers are used to measure independent slices of the velocity distribution function. To confirm the velocity distribution and magnetic field, the Doppler-broadened, sigma-polarized Zeeman line for each transition is measured. With this, the absolute parallel component of ion velocity subject to LIF can be determined. The two separate lasers then give us a signal as a function of two separate parallel ion velocities. Two point correlation is used to reduce the noise floor on the plasma fluctuation. This fluctuation is then investigated as a function of the difference in velocity. |
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AbstractList | A technique for probing velocity space correlations has been developed using laserinduced fluorescence. In this paper, a description of the experimental setup is given, with results to follow in a later publication. The experiment consists of a cylindrical plasma column 3m long and radius ~ 0.25 cm, holding singly-charged argon ions (Ar II) with density n ~ 10 super(9) cm super(-3), T sub(e) ~ 5 eV, T sub(i,) ~ .06 eV, and a 1 kG axial magnetic field. Two separate metastable lines are excited by single frequency lasers at 611 nm and 668 nm. These lasers may tune with a precision of .01 pm. The separate lasers are used to measure independent slices of the velocity distribution function. To confirm the velocity distribution and magnetic field, the Doppler-broadened, sigma-polarized Zeeman line for each transition is measured. With this, the absolute parallel component of ion velocity subject to LIF can be determined. The two separate lasers then give us a signal as a function of two separate parallel ion velocities. Two point correlation is used to reduce the noise floor on the plasma fluctuation. This fluctuation is then investigated as a function of the difference in velocity. |
Author | Mattingly, S W Skiff, F Berumen, J Chu, F Hood, R |
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Cites_doi | 10.1093/comjnl/7.4.308 10.1016/j.cnsns.2007.04.005 10.1103/PhysRevLett.34.1548 10.1175/1520-0469(2004)061<1630:ACMATV>2.0.CO;2 10.1063/1.2122527 10.1063/1.2179056 |
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References | 1 2 3 E.U. Condon (5) 1959 A. Diallo (4) 2005 8 9 A.V. Oppenheim (7) 2010 A. Kramida (6) 2013 10 |
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SubjectTerms | Correlation Density Fluctuation Instrumentation Ion velocity Laser induced fluorescence Lasers Magnetic fields Velocity distribution |
Title | Measurement and interpretation of the velocity space correlation of a laboratory plasma fluctuation with laser induced fluorescence |
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