By K. Siegbahn
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Jesse and J. Sadauskis, Phys. Rev. 97 (1955) 1668. E. Rutherford, J. Chadwick and C. Ellis, Radiation from Radioactive Substances (Cambridge, 41 1930). A . H . C o m p t o n and S. K. Allison, X - R a y s in Theory and Experiment ( L o n d o n , 1936); W. Gerbes, A n n . Physik 2 3 (1935) 648. 17 INTERACTION OF ELECTRONS CH. I specific primary ionization. The total ionization is defined as the total number of ions formed by an electron and its secondary electrons, and is equal to Ni = E/w. Conversely, one can determine the kinetic energy of the primary electron by measuring the number of ions.
Kgl. D a n . Vid. Selsk. 18 N o . 8 (1948). 66 J. H. M . Brunnings, J. K. K n i p p and E. Teller, Phys. Rev. 60 (1941) 657. J. D . Jackson and H. Schiff, Phys. Rev. 89 (1953) 359. (12) 28 G. KNOP AND W. PAUL CH. I It has been found that f is mainly a function of the velocity v, as shown in Fig. 2- 1 1 9 / 1 0 Fig. 28. 3. 8 20 M e a n charge number z o f α-particles as a function o f velocity v. F r o m various authors RANGE-ENERGY RELATIONS Integration of the differential energy loss leads to a formula for the range dE R (13) dE/dx Since — dE/dx is unknown for low velocities one cannot use (13) for the total range; it is only useful for the high energy part of the range.
97 (1955) 1668. E. Rutherford, J. Chadwick and C. Ellis, Radiation from Radioactive Substances (Cambridge, 41 1930). A . H . C o m p t o n and S. K. Allison, X - R a y s in Theory and Experiment ( L o n d o n , 1936); W. Gerbes, A n n . Physik 2 3 (1935) 648. 17 INTERACTION OF ELECTRONS CH. I specific primary ionization. The total ionization is defined as the total number of ions formed by an electron and its secondary electrons, and is equal to Ni = E/w. Conversely, one can determine the kinetic energy of the primary electron by measuring the number of ions.