Modulation of low-rigidity cosmic rays and the power spectrum of the interplanetary magnetic field in 1962 and 1965.
Low rigidity cosmic ray modulation and interplanetary medium at solar minimum and at other phases of solar cycle
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Low rigidity cosmic ray modulation and interplanetary medium at solar minimum and at other phases of solar cycle
OGO 3 search coil magnetometer data correlated with magnetopause crossing by ATS 1 satellite, discussing OGO 3 crossing of outer magnetosphere into interplanetary medium
Simultaneous magnetic field measurements in interplanetary medium in front of earth and in magnetosheath at various earth radii, using satellites
Interplanetary magnetic field sectors evolution /1964-1965/, discussing solar active region development leading to magnetic loops in interplanetary medium
Diffusion models for solar proton propagation in interplanetary medium
Pioneer F/G mission to Jupiter by NASA for exploring interplanetary medium, asteroid belt, planet and environment
Inverse velocity dispersion of relativistic electron intensity in interplanetary medium after solar flare
Detecting fluxes of energetic neutral hydrogen atoms in interplanetary medium by auroral rocket flights
Analyzing data from Explorer 33 and 35 on energetic solar particles in interplanetary medium and terrestrial particle fluxes in magnetopause bow shock regions
Satellite detection of energetic particles in outer space and interpretive analysis of relationships to planetary fields and interplanetary medium
Galactic cosmic ray solar modulation in interplanetary medium, discussing spherically symmetric model
Superthermal electrons continuous stream release into interplanetary medium during hectometric solar noise storm activities
Proton flares in McMath Region 8461 /August- September 1966/, describing solar wind plasma ejection and helium enriched interplanetary medium
Observations of the scatter-free electron events from solar active region McMath No. 8905 are presented. The measurements were made on Explorer 33 satellite. The data show that more than 80% of the electrons from these events undergo no or little scattering and that these electrons travel only approximately 1.5 a.u. between the sun and the earth. The duration of these events cannot be accounted fully by velocity dispersion alone. It is suggested that these electrons could be continuously injected into interplanetary medium for a time interval of approximately 2 to 3 minutes. Energy spectra of these electrons are discussed.
Solar continuum emission was detected in the hectometric range for the first time by RAE-1 satellite. Hectometric continuum is quite similar to decametric continuum, showing that the phenomenon extends out in the corona to at least 50 solar radii, or 36.4 gigameters(0.25 AU). An interesting point is that the amplitude distribution and the bandwidth of type 3 bursts associated with hectometric continuum are the same as those of type 1 bursts associated with the metric noise storm. It is believed that the storm radiation all the way from metric through hectometric can be accounted for by plasma wave radiation. This means that streams of superthermal electrons are continuously coming out of active regions and as they travel outward through the interplanetary medium, they produce plasma waves that result in metric, decametric, hectrometric, and probably kilometric storms.
The rotational properties in the photospheric and solar wind plasma and magnetic fields are considered. In both the photosphere and the interplanetary medium near the earth, there is a tendency for the field patterns to rotate a few percent faster than the plasma patterns. The fields and plasmas show variability in their rotational properties on time scales of days or months, but averages over a few years tend to be less variable, as shown by the results for long-lived sunspots, and by the rotating solar magnetic dipole.
Spectra of modulated galactic cosmic rays are expressed in terms of the Compton-Getting coefficient C. This parameter can reveal the energy range over which the force field approximation is valid, and the range where convection effects dominate those of diffusion. A value of C near zero over an extended low energy range implies that the radial gradient at low energies can not be large. This small gradient may imply that the diffusion coefficient increases beyond 1 AU less rapidly than proportionally to heliocentric radial distance, and/or there is essentially no scattering for a sizeable distance from the Sun to earth. The behavior of C with rigidity (or energy) is discussed in terms of the omnidirectional distribution function f sub zero. Contours of constant f sub zero in the heliocentric distance vs rigidity plane are useful for illustrating the mean rigidity loss experienced by cosmic rays in the interplanetary medium.
A method by which energetic cosmic ray particles in the interplanetary medium can diffuse in solar longitude. The method consists of particle motion occurring along current sheets separating discontinuous field structures in the corona. These sheets can serve as pathways along which energetic particles drift at nearly their propagation speed. A model of the coronal magnetic field and the large scale field behavior are analyzed. A mechanism by which particles can travel across the coronal magnetic field and arrive at the earth is suggested.