Nuclear Physics C. Nuclear Dynamics, Experimental
Nuclear Physics C. Nuclear Dynamics, Experimental
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DOI:
10.1103/revmodphys.9.245
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发表时间:
1937-07
影响因子:
44.1
通讯作者:
M. Livingston;H. Bethe
中科院分区:
文献类型:
--
作者:
M. Livingston;H. Bethe
Artificial disintegration of elements was hrst accomplished by Rutherford in 1919 using the high speed alpha-particles from Ra C'as pro-jectiles, and more than 10yearspassed before any other projectiles were considered. By 1930several laboratories were working on the development of high voltageapparatus to produce high speed ions artificially. It was expected that energies sufficient to penetrate the force fields of nuclei would be required, ie, several million volts, and the proton was considered the most likely p~ ssibility as a projectile. At this stage Gamow ('(* 7) and Condon and Gurney (C32) introduced the quantum mechanical interpretation of natural Q.-decay according to which thereexists a certain probability of penetration of a potential barrier by particles with considerably less energy than required to go over the top of the barrier. Cock-croft and Walton (C18) realized that this might make disintegrations possible with relatively low energy protons and performed the first successful experiment resulting in the disintegration of Li ((.'19). Lawrence, Livingston and White (L11) immediately checked these observations with the 1 MV protons then available with the magnetic resonance accelerator, and others soon followed, some using much lower proton energies and proving the validity of the hypothesis. At the present time the projectiles that have