Interaction of the bow shock with a tangential discontinuity and solar wind density decrease: Observations of predicted fast mode waves and magnetosheath merging

[1] Shortly after 0600 UT on 7 April 2000 a tangential discontinuity (TD) in the solar wind passed the Advanced Composition Explorer satellite (ACE). It was characterized by a rotation of the interplanetary magnetic field (IMF) by ∼145° and more than a factor-of-2 decrease in the plasma density. About 50 min later, Polar encountered more complex manifestations of the discontinuity near noon in the magnetosheath outside the Northern Hemisphere cusp. On the basis of Polar observations, theoretical modeling, and MHD simulations we interpret the event as demonstrating that (1) a fast mode rarefaction wave was generated during the TD-bow shock interaction, (2) the fast wave carried a significant fraction of the density change to the magnetopause while the remainder stayed with the transmitted discontinuity, and (3) magnetic merging occurred between IMF field lines within the magnetosheath on opposite sides of the discontinuity's surface as it approached the magnetopause. Before the discontinuity passed the spacecraft, Polar detected ions accelerated antiparallel to B in the fast wave and perpendicular to B in a weak slow mode structure located adjacent to and just downstream of the fast wave. The antiparallel accelerated ions in the fast wave had no measurable ion-velocity dispersion signature, placing their source a few RE equatorward of Polar. Simulation results, a Walen test, detections of wave Poynting flux parallel to B, bidirectional electron heat flux, and ion velocity enhancements all indicate that the three ion bursts associated with the passage of the discontinuity were signatures of time-dependent, magnetic merging events within the magnetosheath.

[1]  Louis J. Lanzerotti,et al.  Characteristics of merging at the magnetopause inferred from dayside 557.7-nm all-sky images: IMF drivers of poleward moving auroral forms , 2006 .

[2]  J. K. Chao,et al.  Magnetospheric response to solar wind dynamic pressure variations: Interaction of interplanetary tangential discontinuities with the bow shock , 1993 .

[3]  Michelle F. Thomsen,et al.  Observations of the density profile in the magnetosheath near the stagnation streamline , 1990 .

[4]  Lou‐Chuang Lee,et al.  Increase of ion kinetic temperature across a collisionless shock: I. A new mechanism , 1986 .

[5]  Christopher T. Russell,et al.  Fingerprints of collisionless reconnection at the separator, I, Ambipolar‐Hall signatures , 2002 .

[6]  David G. Sibeck,et al.  Comprehensive study of the magnetospheric response to a hot flow anomaly , 1999 .

[7]  G. Paschmann,et al.  ISEE plasma observations near the subsolar magnetopause , 1978 .

[8]  I. Papamastorakis,et al.  Evidence for magnetic field reconnection at the Earth's magnetopause , 1981 .

[9]  David J. McComas,et al.  Direct evidence for magnetic reconnection in the solar wind near 1 AU , 2004 .

[10]  G. Siscoe,et al.  Predictions of magnetosheath merging between IMF field lines of opposite polarity , 2002 .

[11]  K. Hain The partial donor cell method , 1978 .

[12]  R. P. Lepping,et al.  Magnetic field directional discontinuities: Characteristics between 0.46 and 1.0 AU , 1980 .

[13]  Hideaki Kawano,et al.  On the Determination of a Moving MHD Structure: Minimization of the Residue of Integrated Faraday's Equation , 1996 .

[14]  John Ambrosiano,et al.  Acceleration of charged particles in magnetic reconnection: Solar flares, the magnetosphere, and solar wind , 1986 .

[15]  Nancy U. Crooker,et al.  Dayside merging and cusp geometry , 1979 .

[16]  Michelle F. Thomsen,et al.  The electron edge of low latitude boundary layer during accelerated flow events , 1990 .

[17]  William J. Burke,et al.  Observed and simulated depletion layers with southward IMF , 2004 .

[18]  David J. Southwood,et al.  Magnetosheath flow near the subsolar magnetopause: Zwan‐Wolf and Southwood‐Kivelson theories reconciled , 1995 .

[19]  F. Mariani,et al.  Variations of the occurrence rate of discontinuities in the interplanetary magnetic field , 1973 .

[20]  G. Paschmann,et al.  ISEE plasma observations near the subsolar magnetopause , 1978 .

[21]  N. C. Maynard Correction to “Responses of the open‐closed field line boundary in the evening sector to IMF changes: A source mechanism for Sun‐aligned arcs” by N. C. Maynard et al. , 2003 .

[22]  Christopher T. Russell,et al.  Electron signatures of active merging sites on the magnetopause , 2005 .

[23]  D. Hunten,et al.  Depletion of solar wind plasma near a planetary boundary , 1976 .

[24]  David Klumpar,et al.  Mass density and pressure changes across the dayside magnetopause , 1993 .

[25]  B. Thidé,et al.  Slow magnetosonic solitons detected by the cluster spacecraft. , 2003, Physical review letters.

[26]  M. Acuna,et al.  The ACE Magnetic Fields Experiment , 1998 .

[27]  J. W. Griffee,et al.  Solar Wind Electron Proton Alpha Monitor (SWEPAM) for the Advanced Composition Explorer , 1998 .

[28]  G. Paschmann,et al.  Low‐latitude dayside magnetopause and boundary layer for high magnetic shear: 2. Occurrence of magnetic reconnection , 1996 .

[29]  K. Stasiewicz,et al.  Theory and observations of slow-mode solitons in space plasmas. , 2004, Physical review letters.

[30]  Michelle F. Thomsen,et al.  Slow mode transition in the frontside magnetosheath , 1992 .

[31]  Michelle F. Thomsen,et al.  Ion and electron heating at collisionless shocks near the critical Mach number , 1985 .

[32]  George L. Siscoe,et al.  Responses of the open–closed field line boundary in the evening sector to IMF changes: A source mechanism for Sun‐aligned arcs , 2003 .

[33]  G. Paschmann,et al.  Structure of the Dayside Magnetopause for Low Magnetic Shear , 1993 .

[34]  John R Wygant,et al.  The electric field instrument on the polar satellite , 1995 .

[35]  Lou‐Chuang Lee,et al.  Increase of ion kinetic temperature across a collisionless shock: 2. A simulation study , 1987 .

[36]  M. W. Dunlop,et al.  Polar, Cluster and SuperDARN Evidence for High-Latitude Merging during Southward IMF: Temporal/Spatial Evolution , 2003 .

[37]  I. Papamastorakis,et al.  Plasma acceleration at the Earth's magnetopause: evidence for reconnection , 1979, Nature.

[38]  George L. Siscoe,et al.  Response of ionospheric convection to changes in the interplanetary magnetic field: Lessons from a MHD simulation , 2001 .

[39]  T. Zawistowski,et al.  Hydra — A 3-dimensional electron and ion hot plasma instrument for the POLAR spacecraft of the GGS mission , 1995 .

[40]  F. Mozer,et al.  Photoemission current-spacecraft voltage relation: Key to routine, quantitative low-energy plasma measurements , 2000 .

[41]  B. Sonnerup,et al.  Magnetopause reconnection rate , 1974 .

[42]  N. Maynard,et al.  Electric field measurements at the magnetopause: 1. Observation of large convective velocities at rotational magnetopause discontinuities , 1983 .

[43]  G. Paschmann,et al.  The magnetosheath region adjacent to the dayside magnetopause: AMPTE/IRM observations , 1994 .

[44]  S. F. Fung,et al.  Configuration of high-latitude and high-altitude boundary layers , 2000 .

[45]  William J. Burke,et al.  Variable time delays in the propagation of the interplanetary magnetic field , 2002 .

[46]  Christopher T. Russell,et al.  Generalized Walén tests through Alfvén waves and rotational discontinuities using electron flow velocities , 1999 .

[47]  Heinrich J. Völk,et al.  Motions of the bow shock induced by interplanetary disturbances , 1974 .

[48]  D. Pierce,et al.  The GGS/POLAR magnetic fields investigation , 1995 .

[49]  Christopher T. Russell,et al.  Temporal-spatial structure of magnetic merging at the magnetopause inferred from 557.7-nm all-sky images , 2004 .

[50]  G. Paschmann,et al.  Evidence for magnetic reconnection initiated in the magnetosheath , 2007 .

[51]  J. Scudder,et al.  Observations of electron beams in the low-latitude boundary layer , 1984 .

[52]  J. Sakai,et al.  Ion acceleration in quasi‐perpendicular collisionless magnetosonic shock waves with subcritical Mach number , 1985 .

[53]  Y. Ohsawa,et al.  Nonlinear Magnetosonic Fast and Slow Waves in Finite β Plasmas and Associated Resonant Ion Acceleration , 1985 .

[54]  I. Papamastorakis,et al.  Magnetopause properties from AMPTE/IRM observations of the convection electric field: Method development , 1987 .

[55]  David J. Southwood,et al.  On the form of the flow in the magnetosheath , 1992 .

[56]  G. Siscoe,et al.  MHD Simulation of Magnetospheric Transport at the Mesoscale , 2013 .