AMES collaborative study of cosmic ray neutrons

The results of a collaborative study to define both the neutron flux and the spectrum more precisely and to develop a dosimetry package that can be flown quickly to altitude for solar flare events are described. Instrumentation and analysis techniques were used which were developed to measure accelerator-produced radiation. The instruments were flown in the Ames Research Center high altitude aircraft. Neutron instrumentation consisted of Bonner spheres with both active and passive detector elements, threshold detectors of both prompt-counter and activation-element types, a liquid scintillation spectrometer based on pulse-shape discrimination, and a moderated /sup 3/BF counter neutron monitor. In addition, charged particles were measured with a Reuter--Stokes ionization chamber system; and dose equivalent, with another instrument. Preliminary results from the first series of flights at 12.5 km (41,000 ft) are presented, including estimates of total neutron flux intensity and spectral shape and of the variation of intensity with altitude and geomagnetic latitude. (auth)

[1]  S. A. Korff,et al.  Fast‐Neutron Detector with Discrimination against Background Radiation , 1963 .

[2]  R. M. Cameron,et al.  Design and Operation of the NASA 91.5-cm Airborne Telescope. , 1971, Applied optics.

[3]  J. W. Baum,et al.  FACTORS AFFECTING PULSE SIZE IN SEALED TISSUE-EQUIVALENT COUNTERS. , 1970 .

[4]  H. W. Patterson,et al.  The flux and spectrum of cosmic-ray produced neutrons as a function of altitude. , 1959, Health Physics.

[5]  Frank J. Lynch,et al.  Time Dependence of Scintillations and the Effect on Pulse-Shape Discrimination , 1968 .

[6]  M. Merker The contribution of galactic cosmic rays to the atmospheric neutron maximum dose equivalent as a function of neutron energy and altitude. , 1973, Health Physics.

[7]  E. Steinberg,et al.  Pulse height-energy relations for electrons and alpha particles in a liquid scintillator☆ , 1964 .

[8]  G. Boella,et al.  Measurement of the cosmic ray neutron flux at 4.6 billion volts geomagnetic cutoff rigidity , 1965 .

[9]  K. C. Chandler,et al.  Calculations of neutron flux spectra induced in the Earth's atmosphere by galactic cosmic rays , 1973 .

[10]  Serge A. Korff,et al.  Time dependent worldwide distribution of atmospheric neutrons and of their products: 1. Fast neutron observations , 1973 .

[11]  G. Boella,et al.  Measurement of the cosmic-ray neutron flux in the atmosphere , 1963 .

[12]  W. Cross,et al.  A rapid reading technique for nuclear particle damage tracks in thin foils , 1969 .

[13]  S. A. Korff,et al.  Time dependent worldwide distribution of atmospheric neutrons and of their products. I, II, III. , 1973 .

[14]  H. W. Patterson,et al.  "What quality factor"? , 1971, Health Physics.

[15]  R. S. White,et al.  Angular distribution and altitude dependence of atmospheric neutrons from 10 to 100 MeV , 1974 .

[16]  H. Beck,et al.  High pressure argon ionization chamber systems for the measurement of environmental radiation exposure rates. , 1972 .

[17]  W. R. Burrus,et al.  CALIBRATION OF AN ORGANIC SCINTILLATOR FOR NEUTRON SPECTROMETRY. , 1968 .

[18]  Alan R. Smith THRESHOLD DETECTOR APPLICATIONS TO NEUTRON SPECTROSCOPY AT THE BERKELEY ACCELERATORS , 1965 .

[19]  K. O'brien,et al.  Calculated cosmic ray neutron monitor response to solar modulation of galactic cosmic rays , 1973 .

[20]  Ronald I. Ewing,et al.  A new type of neutron spectrometer , 1960 .

[21]  W. S. Snyder,et al.  Radiobiological aspects of the supersonic transport. , 1966, Health physics.

[22]  Richard E. Lingenfelter,et al.  Cosmic‐ray neutron demography , 1961 .

[23]  R. Sherr,et al.  Pulse Shape Discrimination in Stilbene Scintillators , 1961 .

[24]  C. R. Pierce,et al.  Comparison of neutron spectra measured with three sizes of organic liquid scintillators using differentiation analysis , 1972 .

[25]  H. W. Patterson,et al.  Cosmic‐ray‐produced neutrons at ground level: Neutron production rate and flux distribution , 1966 .

[26]  J. W. Baum Nonlinear amplifier for use in mixed radiation rem responding radiation meters. , 1967, Health physics.

[27]  K. O'brien Cosmic-ray propagation in the atmosphere , 1971 .

[28]  P. W. Benjamin,et al.  A HIGH-RESOLUTION SPHERICAL PROPORTIONAL COUNTER , 1968 .

[29]  L. Penrose REPORT OF THE UNITED NATIONS SCIENTIFIC COI\IMITTEE ON THE EFFECTS OF ATOMIC RADIATION , 2006 .

[30]  K. O'brien,et al.  The radiation dose to man from galactic cosmic rays. , 1972, Health physics.

[31]  W. R. Burrus,et al.  Fast-neutron spectroscopy with thick organic scintillators , 1969 .

[32]  Wilmot N. Hess,et al.  COSMIC-RAY NEUTRON ENERGY SPECTRUM , 1959 .

[33]  V. Schönfelder,et al.  Support for Crand Theory from measurements of Earth albedo neutrons between 70 and 250 MeV , 1974 .

[34]  H. Rossi,et al.  Measurements of neutron dose as a function of linear energy transfer. , 1955, Radiation research.

[35]  J. Simpson NEUTRONS PRODUCED IN THE ATMOSPHERE BY THE COSMIC RADIATIONS , 1951 .

[36]  J. W. Baum,et al.  PORTABLE MIXED RADIATION DOSE EQUIVALENT METER. , 1972 .

[37]  Qu Liang,et al.  The United Nations Scientific Committee on the Effects of Atomic Radiation , 1965, Nature.

[38]  J. Lockwood,et al.  The energy dependence of the cosmic‐ray neutron leakage flux in the range 0.01–10 Mev , 1971 .