Knowledge of the total gamma ray production rate per H atom from the decay of pion(0) produced in interstellar cosmic ray interactions is essential for determining the possible amount of interstellar H2. This production rate is recalculated using the latest accelerator data on pion(0) production in pp interactions up to approximately 300 GeV. A simple but accurate approximation resolves the past disagreement over the magnitude of this rate. An upper limit is obtained of (1.51 + or - 0.23) x 10 to the minus 25th power/sec. consistent with the observed upper limit of 1.6 x 10 to the minus 25th power/sec
Four Arde conospheroid metallic diaphragms were tested at NASA to evaluate their capability for use ...
Broad band photometer experiments in the 1200 to 3000 A have been operating on Nimbus 3 and 4 since ...
Using observed data for wide-band type IV solar radio bursts, the onset time differences between the...
The flux of secondary protons below 100 MeV in interstellar space is calculated using detailed cross...
The theory of gamma ray line emission from solar flares is reviewed and revised. It is shown that th...
A balloon borne measurement of the cosmic ray electron spectrum from 10 to 200 GeV is reported in wh...
It is argued that it is appropriate to consider two correlation lengths for interplanetary magnetic ...
Maps of electron fluxes 10,000, 1 million, and 10 million particles/sq cm/sec are presented for a...
The performance is discussed of 10-micron mercury-cadmiumtelluride and lead-tin-telluride photodiode...
Numerical calculations of the generation and propagation of the two important fundamental symmetric ...
The charge composition of solar cosmic rays were measured during two flares occurring in April and S...
The problem of deriving a kinetic equation for the cosmic ray distribution function in a random magn...
Results are made of a numerical calculation of the ultrahigh energy photon spectrum. After assuming ...
The theory of multiphoton ionization for an atomic system of arbitrary complexity is developed using...
Frequency comparisons were made among five NASA hydrogen masers in 1969 and again in 1972 to a preci...
Four Arde conospheroid metallic diaphragms were tested at NASA to evaluate their capability for use ...
Broad band photometer experiments in the 1200 to 3000 A have been operating on Nimbus 3 and 4 since ...
Using observed data for wide-band type IV solar radio bursts, the onset time differences between the...
The flux of secondary protons below 100 MeV in interstellar space is calculated using detailed cross...
The theory of gamma ray line emission from solar flares is reviewed and revised. It is shown that th...
A balloon borne measurement of the cosmic ray electron spectrum from 10 to 200 GeV is reported in wh...
It is argued that it is appropriate to consider two correlation lengths for interplanetary magnetic ...
Maps of electron fluxes 10,000, 1 million, and 10 million particles/sq cm/sec are presented for a...
The performance is discussed of 10-micron mercury-cadmiumtelluride and lead-tin-telluride photodiode...
Numerical calculations of the generation and propagation of the two important fundamental symmetric ...
The charge composition of solar cosmic rays were measured during two flares occurring in April and S...
The problem of deriving a kinetic equation for the cosmic ray distribution function in a random magn...
Results are made of a numerical calculation of the ultrahigh energy photon spectrum. After assuming ...
The theory of multiphoton ionization for an atomic system of arbitrary complexity is developed using...
Frequency comparisons were made among five NASA hydrogen masers in 1969 and again in 1972 to a preci...
Four Arde conospheroid metallic diaphragms were tested at NASA to evaluate their capability for use ...
Broad band photometer experiments in the 1200 to 3000 A have been operating on Nimbus 3 and 4 since ...
Using observed data for wide-band type IV solar radio bursts, the onset time differences between the...