The heliospheric current sheet

The heliospheric current sheet (HCS) is the boundary between open oppositely directed magnetic field lines which commonly originate as the outward extension of the solar magnetic dipole. The dipole tilt, the rotation of the Sun, and the outward propagation of the solar wind cause peaks and valleys in the current sheet which spiral outward. The HCS extends throughout the heliosphere to the greatest distances reached by Pioneer and Voyager. It serves as a magnetic equator, and solar wind parameters including speed, temperature, density, and composition vary with distance from the HCS. Extrapolated back to the Sun, especially near solar minimum, the HCS corresponds to the low-latitude streamer belt. Both features are closely related to a neutral line obtained by extrapolating photospheric magnetic fields to a source surface at several solar radii. The current sheet and sector structure persist throughout the solar cycle including solar maximum. At 1 AU the width of the HCS is approximately 10,000 km while a surrounding plasma sheet is thicker by a factor of ∼30. The field inside the HCS does not simply decrease to a null and then reappear with the opposite sense. Instead, the field rotates at nearly constant magnitude from one polarity to the other. In spite of theoretical expectations that fields on opposite sides of the HCS will merge or reconnect, there is little evidence that such is occurring. Many scientific questions remain unanswered. What are the global properties of the HCS near solar maximum, and how faithfully are they reproduced by source surface models? Are multiple HCS crossings caused by waves on the current sheet or by multiple current sheets? What is the effect of coronal mass ejections on the HCS and vice versa?

[1]  J. Kóta,et al.  Evidence of a North-South Asymmetry in the Heliosphere Associated with a Southward Displacement of the Heliospheric Current Sheet , 2000 .

[2]  J. Lean,et al.  The long‐term variation of the Sun's open magnetic flux , 2000 .

[3]  N. Rich,et al.  Evolution of coronal streamer structure during the rising phase of solar cycle 23 , 2000 .

[4]  P. Lamy,et al.  Origin of Streamer Material in the Outer Corona , 1998 .

[5]  J. Gosling,et al.  Magnetic clouds at sector boundaries , 1998 .

[6]  T. Sanderson,et al.  The Ulysses north polar pass: Latitudinal gradients of anomalous cosmic ray O, N And Ne , 1997 .

[7]  S. Suess,et al.  Latitudinal dependence of the radial IMF component: Coronal imprint , 1996 .

[8]  S. Bame,et al.  A Solar Polar North-South Asymmetry for Cosmic-Ray Propagation in the Heliosphere: The Ulysses Pole-to-Pole Rapid Transit , 1996 .

[9]  Eugene N. Parker,et al.  The alternative paradigm for magnetospheric physics , 1996 .

[10]  Xuepu Zhao,et al.  Effect of coronal mass ejections on the structure of the heliospheric current sheet , 1996 .

[11]  J. Phillips,et al.  Heliospheric plasma sheets as small‐scale transients , 1996 .

[12]  Y.-M. Wang Nonradial Coronal Streamers , 1996 .

[13]  B. Heber,et al.  Spatial variation of >40 MeV/n nuclei fluxes observed during the Ulysses rapid latitude scan , 1996 .

[14]  A. Balogh,et al.  Ulysses observations of the radial magnetic field , 1995 .

[15]  I. Daglis,et al.  Tailward flowing energetic oxygen ion bursts associated with multiple flux ropes in the distant magnetotail: GEOTAil observations , 1995 .

[16]  Y.-M. Wang,et al.  Solar Implications of Ulysses Interplanetary Field Measurements , 1995 .

[17]  N. Murphy,et al.  Heliomagnetic latitude dependence of the heliospheric magnetic field , 1995 .

[18]  Edward J. Smith,et al.  The heliospheric plasma sheet , 1994 .

[19]  V. Pizzo Global, quasi‐steady dynamics of the distant solar wind: 2. Deformation of the Heliospheric Current Sheet , 1994 .

[20]  G. Siscoe,et al.  A test of source‐surface model predictions of heliospheric current sheet inclination , 1994 .

[21]  L. Burlaga,et al.  Large‐scale distant heliospheric magnetic field: Voyager 1 and 2 observations from 1986 through 1989 , 1993 .

[22]  A. Hundhausen,et al.  Sizes and locations of coronal mass ejections - SMM observations from 1980 and 1984-1989 , 1993 .

[23]  J. Gosling,et al.  Multiple heliospheric current sheets and coronal streamer belt dynamics , 1993 .

[24]  K. Ogilvie,et al.  Heat flux dropouts in the solar wind and Coulomb scattering effects , 1992 .

[25]  N. Omidi Rotational discontinuities in anisotropic plasmas , 1992 .

[26]  N. R. Sheeley,et al.  On potential field models of the solar corona , 1992 .

[27]  J. Hoeksema LARGE-SCALE STRUCTURE OF THE HELIOSPHERIC MAGNETIC FIELD: 1976-1991 , 1992 .

[28]  V. Pizzo The evolution of corotating stream fronts near the ecliptic plane in the inner solar system: 2. Three‐dimensional tilted‐dipole fronts , 1991 .

[29]  C. Goodrich,et al.  An investigation of the structure of rotational discontinuities , 1991 .

[30]  E. Smith The heliospheric current sheet and modulation of galactic cosmic rays , 1990 .

[31]  A. Hundhausen,et al.  Solar wind and coronal structure near sunspot minimum: Pioneer and SMM observations from 1985–1987 , 1990 .

[32]  Lou‐Chuang Lee,et al.  On the stability of rotational discontinuities and intermediate shocks , 1989 .

[33]  J. E. Smith Interplanetary magnetic field over two solar cycles and out to 20 AU , 1989 .

[34]  J. Gosling,et al.  Interplanetary magnetic field draping about fast coronal mass ejecta in the outer heliosphere , 1988 .

[35]  R. Wolfson A coronal magnetic field model with volume and sheet currents , 1985 .

[36]  A. Hundhausen,et al.  Organization of solar wind plasma properties in a tilted, heliomagnetic coordinate system , 1981 .

[37]  W. Feldman,et al.  Solar wind helium and hydrogen structure near the heliospheric current sheet: A signal of coronal streamers at 1 AU , 1981 .

[38]  J. R. Jokipii,et al.  Effects of drift on the transport of cosmic rays IV. Modulation by a wavy interplanetary current sheet , 1981 .

[39]  J. T. Gosling,et al.  Coronal streamers in the solar wind at 1 AU , 1980 .

[40]  B. Tsurutani,et al.  Observations of the interplanetary sector structure up to heliographic latitudes of 16°: Pioneer 11 , 1978 .

[41]  E. Gustafson,et al.  The mean magnetic field of the Sun: Observations at Stanford , 1977 .

[42]  H. Alfvén Electric currents in cosmic plasmas , 1977 .

[43]  W. Hubbard,et al.  Effects of particle drift on cosmic-ray transport. I. General properties, application to solar modulation , 1977 .

[44]  J. Wilcox,et al.  Structure of the extended solar magnetic field and the sunspot cycle variation in cosmic ray intensity , 1976, Nature.

[45]  E. Levy The interplanetary magnetic field structure , 1976, Nature.

[46]  J. Wilcox,et al.  The sun's magnetic sector structure , 1975 .

[47]  L. Svalgaard On the use of Godhavn H-component as an indicator of the interplanetary sector polarity , 1974 .

[48]  R. Howard,et al.  Observation of sectored structure in the outer solar corona: Correlation with interplanetary magnetic field , 1974 .

[49]  M. Schulz Interplanetary sector structure and the helliomagnetic equator , 1973 .

[50]  J. Wilcox,et al.  Annual and solar-magnetic-cycle variations in the interplanetary magnetic field, 1926-1971. , 1972 .

[51]  L. Davis The interplanetary magnetic field , 1972 .

[52]  K. Schatten Current sheet magnetic model for the solar corona , 1971 .

[53]  P. Coleman,et al.  Heliographic latitude dependence of the dominant polarity of the interplanetary magnetic field , 1969 .

[54]  J. Wilcox,et al.  A model of interplanetary and coronal magnetic fields , 1969 .

[55]  M. Altschuler,et al.  Magnetic fields and the structure of the solar corona , 1969 .

[56]  J. Wilcox,et al.  Quasi‐stationary corotating structure in the interplanetary medium , 1965 .