Measuring Direct and Return Albedo Proton Fluxes in the PAMELA Experiment

2021 ◽  
Vol 85 (4) ◽  
pp. 350-352
Author(s):  
O. A. Golub ◽  
A. G. Mayorov
2018 ◽  
Vol 854 (1) ◽  
pp. L2 ◽  
Author(s):  
M. Martucci ◽  
R. Munini ◽  
M. Boezio ◽  
V. Di Felice ◽  
O. Adriani ◽  
...  

2015 ◽  
Vol 799 (1) ◽  
pp. L4 ◽  
Author(s):  
O. Adriani ◽  
G. C. Barbarino ◽  
G. A. Bazilevskaya ◽  
R. Bellotti ◽  
M. Boezio ◽  
...  

2015 ◽  
Vol 120 (5) ◽  
pp. 3728-3738 ◽  
Author(s):  
O. Adriani ◽  
G. C. Barbarino ◽  
G. A. Bazilevskaya ◽  
R. Bellotti ◽  
M. Boezio ◽  
...  

2004 ◽  
Vol 42 (3) ◽  
pp. 203-209 ◽  
Author(s):  
N. V. Kuznetsov ◽  
R. A. Nymmik ◽  
M. I. Panasyuk ◽  
E. N. Sosnovets ◽  
M. V. Teltsov

1966 ◽  
Vol 19 (3) ◽  
pp. 309 ◽  

Height distributions are presented for the atmospheric ionization rate and Balmer radiation resulting from precipitation of auroral protons. These results have been computed assuming proton fluxes with several different energy spectra and pitch-angle distributions about the magnetic field, the total proton energy range being restricted to 1-1000 keY.


1965 ◽  
Vol 18 (1) ◽  
pp. 59 ◽  
Author(s):  
KKM Wu ◽  
BSK Chow

Proton fluxes at atmospheric depths between 10 and 50 g/cm2 have been measured using nuclear emulsions during a series of balloon flights over Melbourne (A = 47� S. geomagnetic) in the period November 1961-April 1962. The proton flux J(x) decreases with increasing depth within this region. It can be represented by the relation log J(x) = (3�05�0�02)-(2�36�0�66)xlO-3x and, when extrapolated, gives the flux at the top of the atmosphere to be 1120�50 protons m-2 steradian-1 S-l.


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