4.6: Radioactive decay and imaginary potentials
( \newcommand{\kernel}{\mathrm{null}\,}\)
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:
iℏ∂∂t|Φ,t⟩=[H0−iV0]|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/ℏ)|Φn⟩; where H0|Φn⟩=En|Φn⟩
Following the same analysis as for TDSE, premultiplying by ⟨m|, and for constant V0, Vmn=δmnV0 we obtain:
iℏ˙cm=−iV0cm⇒|cm(t)|2=|cm(0)|2e−2V0t/ℏ
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=ℏ/2V0.
Notice that −iV0 is not a Hermitian operator, and so it is not possible to perform a single measurement of half life.