Influence of the lower hybrid drift instability on the onset of magnetic reconnection

Two-dimensional and three-dimensional kinetic simulation results reveal the importance of the lower-hybrid drift instability (LHDI) to the onset of magnetic reconnection. Both explicit and implicit kinetic simulations show that the LHDI heats electrons anisotropically and increases the peak current density. Linear theory predicts these modifications can increase the growth rate of the tearing instability by almost two orders of magnitude and shift the fastest growing modes to significantly shorter wavelengths. These predictions are confirmed by nonlinear kinetic simulations in which the growth and coalescence of small scale magnetic islands leads to a rapid onset of large scale reconnection.

[1]  J. Brackbill,et al.  The unexpected role of the lower hybrid drift instability in magnetic reconnection in three dimensions , 2002 .

[2]  J. Brackbill,et al.  Nonlinear evolution of the lower hybrid drift instability: Current sheet thinning and kinking , 2002 .

[3]  J. Drake,et al.  Kinetic theory of tearing instabilities , 1977 .

[4]  Giovanni Lapenta,et al.  3D reconnection due to oblique modes: a simulation of Harris current sheets , 2000 .

[5]  James F. Drake,et al.  Alfvénic collisionless magnetic reconnection and the Hall term , 2001 .

[6]  H. Karimabadi,et al.  Consequences of particle conservation along a flux surface for magnetotail tearing , 1996 .

[7]  William Daughton,et al.  Electromagnetic properties of the lower-hybrid drift instability in a thin current sheet , 2003 .

[8]  P. Pritchett Effect of electron dynamics on collisionless reconnection in two-dimensional magnetotail equilibria , 1994 .

[9]  Paolo Ricci,et al.  GEM reconnection challenge: Implicit kinetic simulations with the physical mass ratio , 2002 .

[10]  A. Sharma,et al.  Reconnection onset in the tail of Earth's magnetosphere , 2002 .

[11]  E. W. Herold,et al.  Controlled fusion , 1959, IRE Transactions on Electron Devices.

[12]  Louis J. Lanzerotti,et al.  Solar system plasma physics , 1979 .

[13]  P. Pritchett,et al.  does ion tearing exist , 1991 .

[14]  R. Morse,et al.  NUMERICAL SIMULATION OF THE WEIBEL INSTABILITY IN ONE AND TWO DIMENSIONS. , 1971 .

[15]  B. Coppi Magnetic reconnection driven by velocity space instabilities , 1983 .

[16]  J. Chen,et al.  Collisionless tearing instability in a non‐Maxwellian neutral sheet: An integrodifferential formulation , 1985 .

[17]  Michael Hesse,et al.  Geospace Environmental Modeling (GEM) magnetic reconnection challenge , 2001 .

[18]  M. Romanova,et al.  Magnetic field, reconnection, and particle acceleration in extragalactic jets , 1992 .

[19]  M. Kuznetsova,et al.  Nonlinear evolution of magnetic island in a sheared magnetic field with uniform plasma background , 1990 .

[20]  E. Blackman Reconnecting Magnetic Flux Tubes as a Source of In Situ Acceleration in Extragalactic Radio Sources , 1995, astro-ph/9512007.

[21]  H. Ji,et al.  Measurement of lower-hybrid drift turbulence in a reconnecting current sheet. , 2001, Physical review letters.

[22]  Manfred Scholer,et al.  Onset of collisionless magnetic reconnection in thin current sheets : Three-dimensional particle simulations , 2003 .

[23]  W. Daughton Nonlinear dynamics of thin current sheets , 2002 .

[24]  James F. Drake,et al.  The role of electron dissipation on the rate of collisionless magnetic reconnection , 1998 .

[25]  Paolo Ricci,et al.  Collisionless magnetic reconnection in the presence of a guide field , 2004 .

[26]  N. T. Gladd,et al.  Effects of Finite Plasma Beta on the Lower-Hybrid-Drift Instability, , 1977 .

[27]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[28]  P. Palmadesso,et al.  Tearing instability in an anisotropic neutral sheet , 1983 .

[29]  B. Coppi,et al.  Dynamics of the Geomagnetic Tail , 1966 .

[30]  J. Brackbill,et al.  Nonlinear evolution of the lower‐hybrid drift instability , 1984 .

[31]  D. Leneman,et al.  Design, construction, and properties of the large plasma research device : the LAPD at UCLA , 1991 .

[32]  Paolo Ricci,et al.  A simplified implicit maxwell solver , 2002 .

[33]  J. U. Brackbill,et al.  CELEST1D: an implicit, fully kinetic model for low-frequency, electromagnetic plasma simulation , 1992 .

[34]  A. Galeev Magnetospheric Tail Dynamics , 1982 .

[35]  H. Lesch,et al.  PARTICLE ACCELERATION BY MAGNETIC FIELD-ALIGNED ELECTRIC FIELDS IN ACTIVE GALACTIC NUCLEI , 1997 .

[36]  M. Yamada Review of controlled laboratory experiments on physics of magnetic reconnection , 1999 .

[37]  James L. Burch,et al.  Solar system plasma physics , 1989 .

[38]  Remo Guidieri Res , 1995, RES: Anthropology and Aesthetics.

[39]  T. Intrator,et al.  Reconnection scaling experiment: A new device for three-dimensional magnetic reconnection studies , 2003 .

[40]  J B Taylor,et al.  Relaxation and magnetic reconnection in plasmas , 1986 .

[41]  Paolo Ricci,et al.  Structure of the magnetotail current: Kinetic simulation and comparison with satellite observations , 2003, physics/0308034.

[42]  Lou‐Chuang Lee,et al.  Simulation of the collisionless tearing instability in an anisotropic neutral sheet , 1986 .

[43]  M. Fujimoto,et al.  Low‐frequency electromagnetic turbulence observed near the substorm onset site , 1998 .

[44]  R. Denton,et al.  Signatures of collisionless magnetic reconnection , 2003 .

[45]  T. Terasawa Hall current effect on tearing mode instability , 1983 .

[46]  J. Birn,et al.  Characteristic plasma properties during dispersionless substorm injections at geosynchronous orbit , 1997 .

[47]  J. Chen,et al.  Collisionless tearing instability of a bi‐Maxwellian neutral sheet: An integrodifferential treatment with exact particle orbits , 1989 .

[48]  Joachim Birn,et al.  Magnetic Reconnection in Plasmas , 2002 .

[49]  James Chen,et al.  A quadratic-form analysis of the collisionless tearing mode , 1988 .

[50]  H. Ji,et al.  Experimental study of lower-hybrid drift turbulence in a reconnecting current sheet , 2002 .

[51]  Y. C. Lee,et al.  Nonlinear Evolution of Collisionless and Semicollisional Tearing Modes , 1977 .

[52]  E. G. Harris On a plasma sheath separating regions of oppositely directed magnetic field , 1962 .

[53]  Christopher T. Russell,et al.  Structure of the tail plasma/current sheet at ∼11 RE and its changes in the course of a substorm , 1993 .

[54]  A. Fasoli,et al.  Dynamical plasma response during driven magnetic reconnection. , 2003, Physical review letters.

[55]  Ritoku Horiuchi,et al.  Three-dimensional particle simulation of plasma instabilities and collisionless reconnection in a current sheet , 1999 .

[56]  H. Karimabadi,et al.  Role of electron temperature anisotropy in the onset of magnetic reconnection , 2004 .

[57]  W. Daughton The unstable eigenmodes of a neutral sheet , 1999 .

[58]  R. P. Lepping,et al.  In situ detection of collisionless reconnection in the Earth's magnetotail , 2001, Nature.

[59]  Lou‐Chuang Lee,et al.  A study of tearing instability in the presence of a pressure anisotropy , 1987 .