Modern elementary particle physics: the fundamental by G. L. Kane Gordon L. Kane

By G. L. Kane Gordon L. Kane

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J. Cell. Comp. Physiol. 1952, 39 (suppl. 1), 75. Bohr, N. Philos. Mag. 1913, 25, 10. Bohr, N. Kgl. Dan. Vied. Selskab. -Fys. Medd. 1948, 18, 9. See, for example, Kuppermann, A. J. Chem. Ed. 1959, 36, 279. A. Ann. Physik. 1930, 5, 325; 1933, 24, 273. A. Z. Physik. 1932, 76, 293. Inokuti, M. Rev. Mod. Phys. 1971, 43, 297. L. Annu. Rev. Phys. Chem. 1961, 12, 389. Bloch, F. Ann. Physik. 1933, 16, 285. A. J. Chem. Phys. 1969, 50, 1829. L. , ed. Amsterdam: North Holland, 1967, 20. L. ; Academic Press: New York, 1962, 47.

Mod. Phys. 1992, 64, 313. ; Mozumder, A. Radiat. Res. 1993, 133, 282. D. J. Cell. Comp. Physiol. 1952, 39 (suppl. 1), 75. Bohr, N. Philos. Mag. 1913, 25, 10. Bohr, N. Kgl. Dan. Vied. Selskab. -Fys. Medd. 1948, 18, 9. See, for example, Kuppermann, A. J. Chem. Ed. 1959, 36, 279. A. Ann. Physik. 1930, 5, 325; 1933, 24, 273. A. Z. Physik. 1932, 76, 293. Inokuti, M. Rev. Mod. Phys. 1971, 43, 297. L. Annu. Rev. Phys. Chem. 1961, 12, 389. Bloch, F. Ann. Physik. 1933, 16, 285. A. J. Chem. Phys. 1969, 50, 1829.

This correction is often called the Barkas correction after his measurements determined that the range of negative pions was somewhat larger than that for positively charged pions. This correction is often simply referred to as the z3 correction because it depends on the cube of the particle charge. The last term in Eq. (4) is needed to bring agreement between the first-order theory of Bethe and a full quantum mechanical result of Bloch valid for high-energy particles. All of these additional ‘‘correction’’ factors have come about because of approximations made in the theoretical development of stopping power theory and because the ability to make accurate measurements of stopping power enables one to identify subtle differences between theory and experiment.

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