Nonlinear low-frequency wave aspect of foreshock density holes

Recent observations have uncovered short-duration density holes in the Earth's foreshock region. There is evidence that the formation of density holes involves non-linear growth of fluctuations in the magnetic field and plasma density, which results in shock-like boundaries followed by a decrease in both density and magnetic field. In this study we examine in detail a few such events focusing on their low frequency wave characteristics. The propagation properties of the waves are studied using Cluster's four point observations. We found that while these density hole-structures were convected with the solar wind, in the plasma rest frame they propagated obliquely and mostly sunward. The wave amplitude grows non-linearly in the process, and the waves are circularly or elliptically polarized in the left hand sense. The phase velocities calculated from four spacecraft timing analysis are compared with the velocity estimated from δ E /δ B . Their agreement justifies the plane electromagnetic wave nature of the structures. Plasma conditions are found to favor firehose instabilities. Oblique Alfven firehose instability is suggested as a possible energy source for the wave growth. Resonant interaction between ions at certain energy and the waves could reduce the ion temperature anisotropy and thus the free energy, thereby playing a stabilizing role.

[1]  G. Parks,et al.  Foreshock density holes in the context of known upstream plasma structures , 2008 .

[2]  P. Canu,et al.  Density holes in the upstream solar wind , 2007 .

[3]  F. Mozer,et al.  Larmor radius size density holes discovered in the solar wind upstream of Earth's bow shock , 2006 .

[4]  A. Lazarus,et al.  Solar wind proton temperature anisotropy: Linear theory and WIND/SWE observations , 2006 .

[5]  P. Hellinger,et al.  Parallel and oblique proton fire hose instabilities in the presence of alpha/proton drift : Hybrid simulations , 2006 .

[6]  T. Horbury,et al.  Cluster observations of hot flow anomalies , 2004 .

[7]  B. Lavraud,et al.  Properties of fast magnetosonic shocklets at the bow shock , 2003 .

[8]  W. Wilkinson The earth's quasi-parallel bow-shock: review of observations and perspectives for Cluster , 2003 .

[9]  J. Eastwood,et al.  On the existence of Alfvén waves in the terrestrial foreshock , 2003 .

[10]  A. Vaivads,et al.  Multi‐point electric field measurements of Short Large‐Amplitude Magnetic Structures (SLAMS) at the Earth's quasi‐parallel bow shock , 2003 .

[11]  M. Dunlop,et al.  Cluster magnetic field observations at a quasi-parallel bow shock , 2002 .

[12]  T. Horbury,et al.  Cluster observations of fast magnetosonic waves in the terrestrial foreshock , 2002 .

[13]  A. Szabo,et al.  Wind observations of foreshock cavities: A case study , 2002 .

[14]  Alan J. Lazarus,et al.  Wind/SWE observations of firehose constraint on solar wind proton temperature anisotropy , 2002 .

[15]  T. Carozzi,et al.  First results of electric field and density observations by Cluster EFW based on initial months of operation , 2001 .

[16]  H. Matsumoto,et al.  Nonlinear competition between the whistler and Alfvén fire hoses , 2001 .

[17]  H. Matsumoto,et al.  New kinetic instability: Oblique Alfvén fire hose , 2000 .

[18]  S. Gary,et al.  Electromagnetic proton/proton instabilities in the solar wind: Simulations , 1999 .

[19]  William Daughton,et al.  Electromagnetic proton/proton instabilities in the solar wind , 1998 .

[20]  Dan Winske,et al.  Proton resonant firehose instability: Temperature anisotropy and fluctuating field constraints , 1998 .

[21]  J. Sauvaud,et al.  Gross deformation of the dayside magnetopause , 1998 .

[22]  S. Schwartz Shock and Discontinuity Normals, Mach Numbers, and Related Parameters , 1998 .

[23]  Mario H. Acuna,et al.  THE CLUSTER MAGNETIC FIELD INVESTIGATION , 1997 .

[24]  Rudolf A. Treumann,et al.  Advanced space plasma physics , 1997 .

[25]  D. Burgess What do we really know about upstream waves , 1997 .

[26]  J. Rouzaud,et al.  THE CLUSTER ION SPECTROMETRY (CIS) EXPERIMENT , 1997 .

[27]  G. Le,et al.  ULF waves in the foreshock , 1995 .

[28]  Hermann Lühr,et al.  Observations of short large-amplitude magnetic structures at a quasi-parallel shock , 1992 .

[29]  Steven J. Schwartz,et al.  Quasi-parallel shocks: A patchwork of three-dimensional structures , 1991 .

[30]  J. Gosling,et al.  Observational test of a hot flow anomaly formation mechanism. [high temperature plasma observed in solar wind and magnetosheath] , 1990 .

[31]  C. Russell,et al.  Magnetic pulsations at the quasi-parallel shock , 1990 .

[32]  P. Yoon Electromagnetic fire-hose instability in a fully relativistic bi-Maxwellian plasma , 1989 .

[33]  C. Russell,et al.  Hot, diamagnetic cavities upstream from the Earth's bow shock , 1986 .

[34]  S. Schwartz,et al.  An active current sheet in the solar wind , 1985, Nature.

[35]  C. Russell,et al.  Upstream waves and particles , 1983 .

[36]  D. Sentman,et al.  Instabilities of low frequency, parallel propagating electromagnetic waves in the Earth's foreshock region , 1981 .

[37]  E. Parker Dynamical Instability in an Anisotropic Ionized Gas of Low Density , 1958 .