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Physics LibreTexts

4.6: Radioactive decay and imaginary potentials

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If the number of particles in a given state is reduced in time, then the total intensity of that state is reduced. Consider a particle moving in a region of imaginary potential V(r)=iV0. The TDSE is:

it|Φ,t=[H0iV0]|Φ,t

Assume that the time independent part of the state is an combination of eigenstates of the real part of the Hamiltonian:

|Φ,t=ncn(t) exp(iEnt/)|Φn; where H0|Φn=En|Φn

Following the same analysis as for TDSE, premultiplying by m|, and for constant V0, Vmn=δmnV0 we obtain:

i˙cm=iV0cm|cm(t)|2=|cm(0)|2e2V0t/

Thus the probability amplitude of the state decreases in time. An imaginary potential can be used to represent destruction of particles, either by absorption (in a scattering process, perhaps) or by radioactive decay. Obviously the ket is not a full description of the system, since that should include information about the decay products. The lifetime of the state is τ=/2V0.

Notice that iV0 is not a Hermitian operator, and so it is not possible to perform a single measurement of half life.


This page titled 4.6: Radioactive decay and imaginary potentials is shared under a CC BY 4.0 license and was authored, remixed, and/or curated by Graeme Ackland via source content that was edited to the style and standards of the LibreTexts platform.

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