[1] Zhang Y Z, Mahajan S M. On broken ballooning symmetry [J]. Phys. Lett. A, 1991, 157: 133.
[2] Connor J W, Hastie R J, Taylor J B. Shear, periodicity, and plasma ballooning modes [J]. Phys. Rev. Lett., 1978, 40: 396.
[3] Lee Y C, Van Dam J W. Kinetic theory of ballooning instabilities [M]. in proceedings of the Finite Beta Theory Workshop, Varenna Summer School of Plasma Physics, September 1977, Varenna, Italy, edited by B. Coppi and B. Sadowski (U.S. Dept. of Energy, Office of Fusion Energy, Washington DC, 1979), CONF-7709167, 93.
[4] Connor J W, Hastie R J, Taylor J B. High mode number stability of an axisymmetric toroidal plasma [J]. Proc. R. Soc. London Ser. A, 1979, 365: 1.
[5] Xie T, Zhang Y Z, Mahajan S M, et al. Ballooning theory of the second kind - two dimensional tokamak modes [J]. Phys. Plasmas, 2012, 19: 072105.
[6] Taylor J B, Connor J, Wilson H R. Structure and damping of toroidal drift waves (and their implications for anomalous transport) [J]. Plasma Phys. Contr. Fusion, 1993, 35: 1063.
[7] Connor J, Taylor J B, Wilson H R. Shear damping of drift waves in toroidal plasmas, [J]. Phys. Rev. Lett., 1993, 70: 1803.
[8] Brower D L, Peebles W A, Luhmann N C, et al. Multichannel scattering studies of the spectra and spatial distribution of tokamak microturbulence [J]. Phys. Rev. Lett., 1985, 54: 689.
[9] Zhang Y Z, Mahajan S M, Zhang X D. Two dimensional aspects of toroidal drift waves in the ballooning representation [J]. Phys. Fluids, 1992, B4, 2729. |