History of Beta Decay
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Vieweg+Teubner Verlag
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http://link.springer.com/content/pdf/10.1007/978-3-663-20204-2_5
Reference95 articles.
1. Rutherford, Phil. Mag. 28, 305 (1914). In this paper he considered the continuous spectra as due to the statistical nature of energy losses in collisions between the disintegration electrons and the outer electrons of the atom.
2. Harkins, Journ. Amer. Chem. Soc. 42, 1956 (1920);
3. Meitner, Zeit. f. Phys. 4, 146 (1921);
4. Rutherford, Phil. Mag. 4, 580 (1927). They proposed that electrons do not exist in the free states in the nucleus, but α’ particles of nuclear dimensions are formed out of close combinations between two electrons and an oc particle. An α’ particle breaks up by first emitting one of its electrons and then the other. The spread of the continuous distribution is due to the difference in the energies of the stationary states occupied by the α’ particle before and after the departure of one of its electrons.
5. Von Baeyer and Hahn, Phys. Zeit. 11, 488 (1910).
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1. Das Problem der âentscheidenden Experimenteâ;Berichte zur Wissenschaftsgeschichte;1986
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