Tearing instability, flux ropes, and the kinetic current sheet kink instability in the Earth`s magnetotail: A three-dimensional perspective from particle simulations
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[1] D. Baker,et al. Observations of Energetic Electrons (E 200 keV) in the Earth's Magnetotail' Plasma Sheet and Fireball Observations , 1977 .
[2] B. Tsurutani,et al. The relationship between the IMF B(y) and the distant tail (150-238 Re) lobe and plasmasheet B(y) fields , 1984 .
[3] N. T. Gladd,et al. Lower-hybrid-drift instability in field reversed plasmas , 1980 .
[4] N. T. Gladd,et al. Lower-hybrid-drift wave turbulence in the distant magnetotail. Interim report , 1978 .
[5] R. Winglee,et al. Electron beam injection during active experiments: 1. Electromagnetic wave emissions , 1990 .
[6] H. Karimabadi,et al. Collisionless reconnection in a quasi‐neutral sheet near marginal stability , 1989 .
[7] C. Russell,et al. Current carriers in the near-earth cross-tail current sheet during substorm growth phase , 1990 .
[8] Motohiko Tanaka,et al. Simulations on lower hybrid drift instability and anomalous resistivity in the magnetic neutral sheet , 1981 .
[9] W. Hughes,et al. Observations of earthward and tailward propagating flux rope plasmoids: Expanding the plasmoid model of geomagnetic substorms , 1994 .
[10] W. Zwingmann,et al. Particle simulation of magnetic reconnection in the magnetotail configuration , 1990 .
[11] G. Parks,et al. Particle orbits in model current sheets with a nonzero By component , 1993 .
[12] P. Pritchett,et al. does ion tearing exist , 1991 .
[13] D. Winske. Current‐driven microinstabilities in a neutral sheet , 1981 .
[14] Ashis Bhattacharjee,et al. Collisionless tearing instability in magnetotail plasmas , 1990 .
[15] P. Pritchett,et al. Convection and the formation of thin current sheets in the near‐Earth plasma sheet , 1994 .
[16] F. Coroniti. On the tearing mode in quasi‐neutral sheets , 1980 .
[17] A. Nishida. Magnetospheric plasma physics. , 1982 .
[18] J. Slavin,et al. The distant magnetotail's response to a strong interplanetary magnetic field By - Twisting, flattening, and field line bending , 1985 .
[19] E. W. Hones,et al. Three‐dimensional computer modeling of dynamic reconnection in the geomagnetic tail , 1981 .
[20] Kunihiko Watanabe,et al. Formation of field-twisting flux tubes on the magnetopause and solar wind particle entry into the magnetosphere , 1986 .
[21] P. Palmadesso,et al. Tearing instability in an anisotropic neutral sheet , 1983 .
[22] Lev M. Zelenyi,et al. Regular and chaotic charged particle motion in magnetotaillike field reversals: 1. Basic theory of trapped motion , 1989 .
[23] S. Antiochos,et al. Secondary instability in three-dimensional magnetic reconnection , 1992 .
[24] K. Schindler,et al. A theory of the substorm mechanism , 1974 .
[25] E. G. Harris. On a plasma sheath separating regions of oppositely directed magnetic field , 1962 .
[26] R. Morse,et al. NUMERICAL SIMULATION OF THE WEIBEL INSTABILITY IN ONE AND TWO DIMENSIONS. , 1971 .
[27] L. Zelenyi,et al. Tearing instability in plasma configurations , 1976 .
[28] B. Coppi,et al. Dynamics of the Geomagnetic Tail , 1966 .
[29] Dan Winske,et al. A cross‐field current instability for substorm expansions , 1991 .
[30] J. Birn. Computer studies of the dynamic evolution of the geomagnetic tail , 1980 .
[31] R. Walker,et al. A magnetohydrodynamic simulation of the formation of magnetic flux tubes at the earth's dayside magnetopause , 1989 .
[32] A. Roux. Generation of field-aligned current structures at substorm onsets , 1985 .
[33] R. Walker,et al. Magnetic flux ropes in 3-dimensional MHD simulations , 1990 .
[34] E. W. Hones,et al. The possible role of ionospheric oxygen in the initiation and development of plasma sheet instabilities , 1982 .
[35] C. W. Allen,et al. Interaction of the plasma sheet with the lobes of the Earth's magnetotail , 1987 .
[36] K. Papadopoulos,et al. A current disruption mechanism in the neutral sheet: A possible trigger for substorm expansions , 1990 .
[37] C. Russell,et al. ISEE‐1 and 2 observations of magnetic flux ropes in the magnetotail: FTE's in the plasma sheet? , 1986 .
[38] R. Winglee,et al. Energy storage and dissipation in the magnetotail during substorms 1. Particle simulations , 1993 .
[39] J. Kan. Developing a global model of magnetospheric substorms , 1990 .
[40] P. Pritchett. Effect of electron dynamics on collisionless reconnection in two-dimensional magnetotail equilibria , 1994 .
[41] F. Coroniti. Explosive tail reconnection: The growth and expansion phases of magnetospheric substorms , 1985 .
[42] T. Engelder,et al. Correction [to “An experimental study of permeability and fluid chemistry in an artificially jointed marble” by Chris Marone, James Rubenstone, and Terry Engelder] , 1989 .
[43] R. Elphic,et al. Current sheet thickness in the near-earth plasma sheet during substorm growth phase , 1990 .
[44] René Pellat,et al. Stability of a thick two‐dimensional quasineutral sheet , 1982 .
[45] N. T. Gladd,et al. On the role of the lower hybrid drift instability in substorm dynamics , 1981 .
[46] Lev M. Zelenyi,et al. Chaotization of the electron motion as the cause of an internal magnetotail instability and substorm onset , 1987 .
[47] G. Paschmann,et al. Average plasma properties in the central plasma sheet , 1989 .
[48] Robert L. McPherron,et al. Satellite studies of magnetospheric substorms on August 15, 1968. IX - Phenomenological model for substorms. , 1973 .
[49] A. Langdon,et al. Electromagnetic and Relativistic Plasma Simulation Models , 1976 .
[50] Lou‐Chuang Lee,et al. Streaming sausage, kink and tearing instabilities in a current sheet with applications to the earth's magnetotail , 1988 .