Abstract

Proton emission is described using a model which has previously given good results in the description of $\alpha$ and cluster radioactivity. The simple phenomenological formalism, based on the Gamow theory for alpha decay, is now extended by including the centrifugal term. The model contains only one parameter: the effective nuclear radius constant. Its value was once found for alpha and cluster emitters. A good agreement with the experimental half-lives for proton radioactivity is achieved without any additional fitting procedures to the data for proton emission.

Highlights

  • The decay of 53Co from its isomeric state was the first experimental observation of proton radioactivity [1, 2]

  • Analogous to alpha and cluster radioactivity, proton emission might be understood in terms of the quantummechanical tunneling of the emitted particle through

  • The best accuracy in proton emission half-lives data reproduction is obtaineed for nuclear radius constant r0 = 1.20 fm

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Summary

Introduction

The decay of 53Co from its isomeric state was the first experimental observation of proton radioactivity [1, 2]. The proton emission from the ground state of mother nuclei with masses in the range 110 ≤ A ≤ 150 was measured in the early 1980s [3]. This decay mode is typical for the odd-Z emitters beyond the proton drip line. The correlations between proton emission half-lives and the deformation of the mother nucleus were widely discussed in refs. The main aim of this paper is to show that using a very simple, uniform formalism, one can evaluate half-lives for the three different decay modes: alpha, cluster and proton radioactivity. Analogous to alpha and cluster radioactivity, proton emission might be understood in terms of the quantummechanical tunneling of the emitted particle through

Rout r
Nucleus l
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