Plasma waves observed in the cusp turbulent boundary layer: An analysis of high time resolution wave and particle measurements from the Polar spacecraft

The boundary layer located in the cusp and adjacent to the magnetopause is a region that is quite turbulent and abundant with waves. The Polar spacecraft's orbit and sophisticated instrumentation are ideal for studying this region of space. Our analysis of the waveform data obtained in this turbulent boundary layer shows broadband magnetic noise extending up to a few kilohertz (but less than the electron cyclotron frequency); sinusoidal bursts (a few tenths of a second) of whistler mode waves at around a few tens of hertz, a few hundreds of hertz, and just below the electron cyclotron frequency; and bipolar pulses, interpreted as electron phase-space holes. In addition, bursts of electron cyclotron harmonic waves are occasionally observed with magnetic components. We show evidence of broadband electrostatic bursts covering a range of ∼3 to ∼25 kHz (near but less than the plasma frequency) occurring in packets modulated at the frequency of some of the whistler mode waves. On the basis of high time resolution particle data from the Polar HYDRA instrument, we show that these bursts are consistent with generation by the resistive medium instability. The most likely source of the whistler mode waves is the magnetic reconnection site closest to the spacecraft, since the waves are observed propagating both toward and away from the Earth, are bursty, which is often the case with reconnection, and do not fit on the theoretical cold plasma dispersion relation curve.

[1]  F. Mozer,et al.  DEBYE-SCALE PLASMA STRUCTURES ASSOCIATED WITH MAGNETIC-FIELD-ALIGNED ELECTRIC FIELDS , 1998 .

[2]  D. Gurnett,et al.  Electrostatic electron cyclotron waves observed by the plasma wave instrument on board Polar , 2001 .

[3]  R. Elphic,et al.  FAST satellite observations of electric field structures in the auroral zone , 1998 .

[4]  New Features of Time Domain Electric-Field Structures in the Auroral Acceleration Region , 1997 .

[5]  D. Gurnett,et al.  Polar spacecraft observations of the turbulent outer cusp/magnetopause boundary layer of Earth , 1999 .

[6]  D. Gurnett Auroral plasma waves , 1989 .

[7]  C. Russell,et al.  The polar cusp location and its dependence on dipole tilt , 1999 .

[8]  P. Kintner,et al.  The measurement of wavelength in space plasmas , 1989 .

[9]  J. Šimůnek,et al.  ULF-ELF-VLF-HF plasma wave observations in the polar cusp onboard high and low altitude satellites , 1998 .

[10]  W. H. Mish,et al.  The Global Geospace Science Program and its investigations , 1995 .

[11]  J. R. Franz A study of electron phase-space holes in the polar magnetosphere , 2000 .

[12]  M. Oppenheim,et al.  Nonlinear two‐stream instabilities as an explanation for auroral bipolar wave structures , 1999 .

[13]  D. Gurnett,et al.  Polar cap boundary layer waves: An auroral zone phenomenon , 2001 .

[14]  E. Budnik,et al.  The cusp/magnetosheath interface on May 29, 1996: Interball‐1 and Polar observations , 1998 .

[15]  A. Galeev,et al.  Plasma waves using the BUDVAR complex for combined wave diagnostics (Prognoz-10-Interkosmos) , 1986 .

[16]  P. Kintner,et al.  On the perpendicular scale of electron phase‐space holes , 2000 .

[17]  D. Gurnett,et al.  Plasma waves in the polar cusp: observations from Hawkeye 1. Progress report , 1977 .

[18]  D. Gurnett,et al.  Plasma waves in the dayside polar cap boundary layer: Bipolar and monopolar electric pulses and whistler mode waves , 1998 .

[19]  J. R. Phillips,et al.  The Polar plasma wave instrument , 1995 .

[20]  C. Russell,et al.  Comparisons of Polar satellite observations of solitary wave velocities in the plasma sheet boundary and the high altitude cusp to those in the auroral zone , 1999 .

[21]  R. Ergun,et al.  Analysis and simulation of BGK electron holes , 1999 .

[22]  James F. Drake,et al.  Transition to whistler mediated magnetic reconnection , 1994 .

[23]  H. Rosenbauer,et al.  Wave and particle measurements at the polar cusp , 1974 .

[24]  P. Kintner,et al.  POLAR observations of coherent electric field structures , 1998 .

[25]  B. Tsurutani,et al.  Some basic concepts of wave‐particle interactions in collisionless plasmas , 1997 .

[26]  L. J. Cahill,et al.  Magnetopause structure and attitude from Explorer 12 observations. , 1967 .

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

[28]  C. Russell,et al.  Plasma waves observed during cusp energetic particle events and their correlation with Polar and akebono satellite and ground data , 1999 .

[29]  David Klumpar,et al.  FAST satellite observations of large‐amplitude solitary structures , 1998 .

[30]  C. Russell,et al.  Plasma Wave Turbulence at the Magnetopause: Observations From ISEE 1 and 2 (Paper 9A0742) , 1979 .

[31]  B. Kadomtsev,et al.  Magnetic field line reconnection , 1987 .

[32]  B. Tsurutani,et al.  The generation mechanism for magnetosheath lion roars , 1981, Nature.

[33]  D. Gurnett,et al.  Electron acceleration by Landau resonance with whistler mode wave packets. Progress report , 1983 .

[34]  R. Treumann,et al.  Plasma waves at the dayside magnetopause , 1988 .

[35]  J. Holtet,et al.  The polar cusp , 1985 .

[36]  W. Gekelman,et al.  Magnetic field line reconnection experiments: 6. Magnetic turbulence , 1984 .

[37]  T. Eastman,et al.  Electrostatic bursts generated by electrons in Landau Resonance with whistler mode chorus , 1983 .

[38]  R. Ergun,et al.  Phase‐space electron holes along magnetic field lines , 1999 .

[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]  T. H. Stix Waves in plasmas , 1992 .

[41]  J. Sauvaud,et al.  Interball tail probe measurements in outer cusp and boundary layers , 2013 .

[42]  Edward J. Smith,et al.  Magnetosheath lion roars , 1976 .