Galactic effects of the cosmic-ray gas
Cosmic ray gas galactic effects, discussing galactic magnetic field, hydromagnetic wave propagation, etc
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Cosmic ray gas galactic effects, discussing galactic magnetic field, hydromagnetic wave propagation, etc
Cosmic ray electrons during propagation in interstellar space analyzed for energy spectrum modulation
Solar cosmic rays satellite observation, considering flare associated, recurrent and storm particle events and active center associated energetic particles
Cosmic ray particles diffusion with simultaneous energy transport, using leakage lifetime approximation
Galactic cosmic rays solar modulation effects on fast neutron flux in atmosphere
Cosmic ray intensity mean diurnal variation, taking into account angle between solar corotational velocity and earth equatorial plane
Cosmic ray electron intensity and energy spectrum from nuclear emulsion-spark chamber combination detector triggered by scintillation and Cerenkov counters on high altitude balloon
Cosmic ray diffusion from discrete sources in random galactic location, studying chemical constituents anisotropy and age with scattering model
Galactic cosmic ray transport equation numerical solution for interplanetary region, considering modulation, diffusion, convection and energy loss effects
Solar cosmic ray data, discussing multicharged nuclei relative abundances in photosphere and propagation models
Cosmic ray spectra and solar electron data in the 10 to 200 MeV range, as measured by experiment E-09 on OGO-5, are reported.
Cosmic ray electron measurements and radio background data are analyzed to obtain bounds on the galactic magnetic fields. It is shown that the magnetic field required to explain the radio flux must be greater than 2 micro Gauss. The difference in the steepening of the radio spectra towards the Anticenter and the Halo Minimum provides evidence that the magnetic field decreases with the height above the galactic plane. The calculations of Bulanov and Dogiel (1975) are applied to the radio and electron observations. It is shown that the most plausible interpretation of these results requires that the electron injection spectrum has an intrinsic flattening below a few GeV. The observed steepening of radio and electron data is apparently a combined effect of the injection spectrum and the first break due to continuous energy loss of electrons in space.
Ultraheavy cosmic rays have been measured by both passive and electronic detectors. These detectors are reviewed, and the requirements are given for the next major step in detector design.
Deuterium and helium 3 produced by nuclear interactions of cosmic rays with interstellar gas
The cosmic ray division participation in the cooperative agreement was activated in the second year. The scientific goals will be analysis of cosmic ray data from the Japanese-American Cooperative Emulsion Experiments (JACEE). Measurements of primary cosmic rays in the JACEE emulsion chambers will be made to derive for each detected particle the deposited energy in the chamber and the primary charge (atomic number). The data will be corrected to the primary flux above the atmosphere, and the composition and energy spectra will be derived. The spectra of the individual elements will be interpreted in context with the supernova shock and other models of cosmic ray acceleration. Additional information is contained in the original extended abstract.
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The radial distribution is derived of gamma ray emissivity and the cosmic ray intensity in the Galaxy using the final SAS-2 results, the recently corrected COS-B results, and recent CO surveys of the Northern and Southern Galactic Hemispheres. In addition to the 5 kpc ring of enhanced emission, there is evidence for spiral features. A strong increase in the cosmic ray flux is found in the inner Galaxy, particularly in the 5 kpc region, in both halves of the plane.
The gamma ray line intensities due to cosmic ray spallation reactions in clouds, the galactic disk and accreting binary pulsars are calculated. With the most favorable plausible assumptions, only a few lines may be detectable to the level of 0.0000001 per sq. cm per sec. The intensities are compared with those generated in nuclear excitation reactions.