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The law of radioactive decay.—II

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Il Nuovo Cimento B (1971-1996)

Summary

A derivation is presented of the quasi-exponential law of radioactive decay which avoids the standard «essential states» approximation (neglect of final-state interactions) and also relaxes the approximation that the density of final states be a constant (with a cut-off). It is found that the system decays as a sum of exponentials with a single term dominant at sufficiently long time. The decay constant is changed slightly from that which obtains under the essential-state approximation.

Riassunto

Si presenta una derivazione della legge quasi esponenziale del decadimento radioattivo che evita l’usuale approssimazione degli «stati essenziali» (omissione delle interazioni negli stati finali) e abbandona l’approssimazione che la densità degli stati finali sia una costante (con un taglio). Si è trovato che il sistema decade come una somma di esponenziali con un singolo termine dominante in un tempo sufficientemente lungo. La costante di decadimento è cambiata leggermente rispetto a quella che si ottiene secondo l’approssimazione degli stati essenziali.

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References

  1. M. D. Arthur, H. Brysk, S. L. Paveri-Fontana andP. F. Zweifel:Nuovo Cimento B,63, 565 (1981).

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  2. See, for example,E. Merzbacher:Quantum Mechanics, 2nd edition (New York, N.Y., 1970), Chapt. 18.

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  5. This is the same procedure followed byLandau in his treatment of plasma oscillations, except that there his cut was along the entire imaginary axis.L. D. Landau:J. Phys. USSR,10, 25 (1946).

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  6. B. W. Roos:Analytic Functions and Distributions in Physics and Engineering (New York, N.Y., 1969), subsect.4.6.

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Traduzione a cura della Redazione.

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Brysk, H., Slawny, J. & Zweifel, P.F. The law of radioactive decay.—II. Nuov Cim B 73, 213–225 (1983). https://doi.org/10.1007/BF02721790

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  • DOI: https://doi.org/10.1007/BF02721790

PACS. 03.65

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