Reversed shear Alfvén eigenmodes (RSAEs) are typically thought of as being localized near the minima in the magnetic safety factor profile, however, their spatial coupling to global toroidal Alfvén eigenmodes (TAEs) has been observed in DIII-D discharges. For a decreasing minimum magnetic safety factor, the RSAE frequency chirps up through that of stable and unstable TAEs. Coupling creates a small gap at the frequency degeneracy point forming two distinct global modes. The core-localized RSAE mode structure changes and becomes temporarily global. Similarly, near the mode frequency crossing point, the global TAE extends deeper into the plasma core. The frequency splitting and spatial structure of the two modes throughout the various coupling stages, as measured by an array of internal fluctuation diagnostics, are in close agreement with linear ideal MHD calculations using the NOVA code. The implications of this coupling for eigenmode stability is also investigated and marked changes are noted throughout the coupling process.
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May 2007
Research Article|
March 23 2007
Coupling of global toroidal Alfvén eigenmodes and reversed shear Alfvén eigenmodes in DIII-Da) Available to Purchase
M. A. Van Zeeland;
M. A. Van Zeeland
c)
1
General Atomics
, P.O. Box 85608, San Diego, California 92186-5608
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M. E. Austin;
M. E. Austin
2Fusion Research Center,
University of Texas
, 1 University Station, Austin, Texas 78712-0263
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N. N. Gorelenkov;
N. N. Gorelenkov
3
Princeton Plasma Physics Laboratory
, P.O. Box 451, Princeton, New Jersey 08543
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W. W. Heidbrink;
W. W. Heidbrink
4
University of California
, Irvine, California 92697
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G. J. Kramer;
G. J. Kramer
3
Princeton Plasma Physics Laboratory
, P.O. Box 451, Princeton, New Jersey 08543
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M. A. Makowski;
M. A. Makowski
5
Lawrence Livermore National Laboratory
, Livermore, California 94550
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G. R. McKee;
G. R. McKee
6
University of Wisconsin
, 1500 Engineering Drive, Madison, Wisconsin 53706
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R. Nazikian;
R. Nazikian
3
Princeton Plasma Physics Laboratory
, P.O. Box 451, Princeton, New Jersey 08543
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E. Ruskov;
E. Ruskov
7
University of California
, Irvine, California 92697
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A. D. Turnbull
A. D. Turnbull
1
General Atomics
, P.O. Box 85608, San Diego, California 92186-5608
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M. A. Van Zeeland
1,c)
M. E. Austin
2
N. N. Gorelenkov
3
W. W. Heidbrink
4
G. J. Kramer
3
M. A. Makowski
5
G. R. McKee
6
R. Nazikian
3
E. Ruskov
7
A. D. Turnbull
1
1
General Atomics
, P.O. Box 85608, San Diego, California 92186-5608
2Fusion Research Center,
University of Texas
, 1 University Station, Austin, Texas 78712-0263
3
Princeton Plasma Physics Laboratory
, P.O. Box 451, Princeton, New Jersey 08543
4
University of California
, Irvine, California 92697
5
Lawrence Livermore National Laboratory
, Livermore, California 94550
6
University of Wisconsin
, 1500 Engineering Drive, Madison, Wisconsin 53706
7
University of California
, Irvine, California 92697Phys. Plasmas 14, 056102 (2007)
Article history
Received:
October 27 2006
Accepted:
December 14 2006
Citation
M. A. Van Zeeland, M. E. Austin, N. N. Gorelenkov, W. W. Heidbrink, G. J. Kramer, M. A. Makowski, G. R. McKee, R. Nazikian, E. Ruskov, A. D. Turnbull; Coupling of global toroidal Alfvén eigenmodes and reversed shear Alfvén eigenmodes in DIII-D. Phys. Plasmas 1 May 2007; 14 (5): 056102. https://doi.org/10.1063/1.2436489
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