The mu-meson spectrum for energies from 10 super 11 to 10 super 13 eV at sea level
Muon energy spectrum at sea level determined from large ionization burst spectrum
SEARCH · Engineering Papers
Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.
Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.
Muon energy spectrum at sea level determined from large ionization burst spectrum
Nuclear structure effects in muon-meson atomic spectral analyses
Nuclear charge distribution model for muon-meson atomic calculations
Muon-meson atomic spectral analyses of spherical and nearly spherical nuclei
Muon-meson X-ray spectra and charge distribution in deformed nuclei
Muon-meson atomic spectral analyses of spherical nuclei
Muon-meson X-ray spectral analysis of deformed isotopic tungsten, uranium, and samarium nuclei
Neutron monitor modifications and muon telescope design for cosmic ray studies
Equivalence principle for unstable elementary particles established on basis of calculation showing muon coupling to gravitation
Dark noise component produced by Cerenkov pulses in photomultipliers due to cosmic ray muons, discussing spectrophotometry of faint astronomical sources
Validity of Lorentz invariance, discussing nuclear magnetic resonance test on torque for spin of electrons, muons and neutrons
Nucleon-meson transport code NMTC to compute transport of nucleons below 3.5 GeV and muons and charged pions below 2.5 GeV
Cross section for electron and muon neutrino- antineutrino pair production by photons, using intermediate boson theory
Calculations have been made using the nucleon-meson transport code NMTC to estimate the absorbed dose and dose equivalent distributions in astronauts inside space vehicles bombarded by solar flare and Van Allen protons. A spherical shell shield of specific radius and thickness with a 30-cm-diam. tissue ball at the geometric center was used to simulate the spacecraft-astronaut configuration. The absorbed dose and the dose equivalent from primary protons, secondary protons, heavy nuclei, charged pions, muons, photons, and positrons and electrons are given as a function of depth in the tissue phantom. Results are given for solar flare protons with a characteristic rigidity of 100 MV and for Van Allen protons in a 240-nautical-mile circular orbit at 30 degree inclination angle incident on both 20-g/sq cm-thick aluminum and polyethylene spherical shell shields.
An analytical theory of atmospheric cosmic-ray propagation is developed based on a phenomenological model of hadron-nucleus collisions. This model correctly predicts the sea level cosmic-ray nucleon, pion and muon spectra, the cosmic-ray ionization profile in the atmosphere, and neutron flux and density profiles in the atmosphere. It is concluded that the large scale properties of atmospheric cosmic-rays can be accurately predicted on the basis of a nucleonic cascade with all secondaries mediated by pion production. Implications for energy independence of cross sections, the recent 70 GeV results from Serpukhov, and nucleonic relaxation rates in the atmosphere are discussed.
The origin of high-energy cosmic electrons is considered. It is found that electrons of energies below 1000 GeV could have been produced by local supernovae associated with known radio remnants. At higher energies, observations of muon-poor air showers indicate the existence of electrons at 1,000,000 GeV which may have originated entirely from the supernova Vela X.
A method is proposed for obtaining the energies of high-energy hadrons incident upon a glass-scintillator ionization spectrometer. The description of the apparatus and of its calibration with cosmic ray muons is followed by a demonstration of the processing of the data obtained.
The survey of negative pion absorption reactions on light and medium nuclei was continued. Muon spin precession was studied using an iron target. An impulse approximation model of the pion absorption process implied that the ion will absorb almost exclusively on nucleon pairs, single nucleon absorption being suppressed by energy and momentum conservation requirements. For measurements on both paramagnetic and ferromagnetic iron, the external magnetic field was supplied by a large C-type electromagnet carrying a current of about 100 amperes.