Broadband plasma waves observed in the polar cap boundary layer: Polar

Polar observations indicate the presence of intense broadband plasma waves nearly all of the time (96% occurrence frequency in this study) near the apogee of the Polar trajectory (∼6–8 RE). The region of wave activity bounds the dayside (0500 to 1800 LT) polar cap magnetic fields, and we thus call these waves polar cap boundary layer (PCBL) waves. The waves are spiky signals spanning a broad frequency range from ∼101 to 2 × 104 Hz. The waves have a rough power law spectral shape. The wave magnetic component has on average a ƒ−2.7 frequency dependence and appears to have an upper frequency cutoff of ∼(6–7) × 103 Hz, which is the electron cyclotron frequency. The electric component has on average a ƒ−2.2 frequency dependence and extends up to ∼2 × 104 Hz. The frequency dependences of the waves and the amplitude ratios of B′/E′ indicate a possible mixture of obliquely propagating electromagnetic whistler mode waves plus electrostatic waves. There are no clear intensity peaks in either the magnetic or electric spectra which can identify the plasma instability responsible for the generation of the PCBL waves. The wave character (spiky nature, frequency dependence and admixture of electromagnetic and electrostatic components) and intensity are quite similar to those of the low-latitude boundary layer (LLBL) waves detected at and inside the low-latitude dayside magnetopause. Because of the location of the PCBL waves just inside the polar cap magnetic field lines, it is natural to assume that these waves are occurring on the same magnetic field lines as the LLBL waves, but at lower altitudes. Because of the similar wave intensities at both locations and the occurrence at all local times, we rule out an ionospheric source. We also find a magnetosheath origin improbable. The most likely scenario is that the waves are locally generated by field-aligned currents or current gradients. We find a strong relationship between the presence of ionospheric and magnetosheath ions and the waves near the noon sector. These waves may thus be responsible for ion heating observed near the cusp region. Antisunward convection of these freshly accelerated oxygen ions over the polar cap during intense wave events (occurring during southward Bz events) might lead to enhanced plasma sheet O+ population. For magnetic storm intervals this mechanism would lead to a natural delay between the main phase onset and the appearance of oxygen ions in the ring-current.

[1]  B. Tsurutani,et al.  Generation of Broadband Plasma Waves in the Polar Cap Boundary Layer , 1997 .

[2]  C. Russell,et al.  Correlative Magnetopause Boundary Layer Observations , 1997 .

[3]  Chio Cheng,et al.  Global structure of mirror modes in the magnetosheath , 1996 .

[4]  R. Prangé,et al.  Plasma wave characteristics of the Jovian magnetopause boundary layer: Relationship to the Jovian aurora? , 1997 .

[5]  G. Lakhina,et al.  Stochastic acceleration by lower hybrid waves in the solar corona , 1996 .

[6]  C. Russell,et al.  The relationship between ELF-VHF waves and magnetic shear at the dayside magnetopause , 1996 .

[7]  B. Tsurutani,et al.  The efficiency of “viscous interaction” between the solar wind and the magnetosphere during intense northward IMF events , 1995 .

[8]  B. A. Whalen,et al.  The Toroidal Imaging Mass-Angle Spectrograph (TIMAS) for the polar mission , 1995 .

[9]  L. Rezeau,et al.  Resonant amplification of magnetosheath MHD fluctuations at the magnetopause , 1995 .

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

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

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

[13]  Drake,et al.  Structure of thin current layers: Implications for magnetic reconnection. , 1994, Physical review letters.

[14]  J. Drake,et al.  Turbulence and transport in the magnetopause current layer , 1994 .

[15]  B. Tsurutani,et al.  A survey of low frequency waves at Jupiter: The Ulysses encounter , 1993 .

[16]  G. Lakhina,et al.  Ultralow‐frequency fluctuations at the magnetopause , 1993 .

[17]  G. Lakhina Generation of low-frequency electric field fluctuations on the auroral field lines , 1993 .

[18]  G. Crew,et al.  Ion heating by broadband low-frequency waves in the cusp/cleft , 1990 .

[19]  G. Crew,et al.  Ion cyclotron resonance heated conics: Theory and observations , 1990 .

[20]  T. Eastman,et al.  A statistical study of ELF-VLF plasma waves at the magnetopause , 1989 .

[21]  A. Roux,et al.  Characterization of Alfvenic fluctuations in the magnetopause boundary layer , 1989 .

[22]  G. Gloeckler,et al.  Ring current development during the great geomagnetic storm of February 1986 , 1988 .

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

[24]  G. Lakhina Low‐frequency electrostatic noise due to velocity shear instabilities in the regions of magnetospheric flow boundaries , 1987 .

[25]  G. Lakhina,et al.  Lower hybrid wave model for aurora , 1985 .

[26]  W.K. (Bill) Peterson Ion injection and acceleration in the polar cusp , 1985 .

[27]  D. Gurnett,et al.  Correlated low‐frequency electric and magnetic noise along the auroral field lines , 1984 .

[28]  R. Gendrin Magnetic turbulence and diffusion processes in the magnetopause boundary layer , 1983 .

[29]  B. Tsurutani,et al.  Diffusion processes in the magnetopause boundary layer , 1982 .

[30]  T. Eastman,et al.  Plasma waves near the magnetopause , 1982 .

[31]  C. Tu THE LOWER-HYBRID-DRIFT INSTABILITY IN THE MAGNETOPAUSE , 1982 .

[32]  B. Coppi,et al.  Lower hybrid acceleration and ion evolution in the suprauroral region , 1981 .

[33]  N. T. Gladd,et al.  On the role of the lower hybrid drift instability in substorm dynamics , 1981 .

[34]  C. Russell,et al.  Wave-particle interactions at the magnetopause - Contributions to the dayside aurora , 1981 .

[35]  G. Lakhina,et al.  Drift loss cone instability in the ring current and plasma sheet , 1980, Journal of Earth System Science.

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

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

[38]  D. Gurnett,et al.  A region of intense plasma wave turbulence on auroral field lines , 1977 .

[39]  Charles F. Kennel,et al.  LIMIT ON STABLY TRAPPED PARTICLE FLUXES , 1966 .

[40]  C. O. Hines,et al.  A UNIFYING THEORY OF HIGH-LATITUDE GEOPHYSICAL PHENOMENA AND GEOMAGNETIC STORMS , 1961 .