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Subatomic Physics

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5.7. Decays 99<br />

Figure 5.15: Exponential decay.<br />

Figure 5.16: Real part of the<br />

wave function of a decaying state.<br />

It is assumed that the decaying<br />

state is formed at t =0.<br />

Figure 5.15 shows log N(t) plotted against t. Half life and mean life are indicated.<br />

In one half life, one half of all atoms present decay. The mean life is the average<br />

time a particle exists before it decays; it is connected to λ and t 1/2 by<br />

τ = 1<br />

λ = t 1/2<br />

ln 2 ∼ = 1.44t 1/2. (5.34)<br />

To relate the exponential decay to properties of the decaying state, the time dependence<br />

of the wave function of a particle at rest (p = 0) is shown explicitly<br />

as<br />

�<br />

ψ(t) =ψ(0) exp − iEt<br />

�<br />

. (5.35)<br />

�<br />

If the energy E of this state is real, the probability of finding the particle is not a<br />

function of time because<br />

|ψ(t)| 2 = |ψ(0)| 2 .<br />

A particle described as a wave function of the type of Eq. (5.35) with real E does<br />

not decay. To introduce an exponential decay of a state described by ψ(t), a small<br />

imaginary part is added to the energy,<br />

where E0 and Γ are real and where the factor 1<br />

2<br />

Eq. (5.36), the probability becomes<br />

E = E0 − 1<br />

2iΓ, (5.36)<br />

|ψ(t)| 2 = |ψ(0)| 2 exp<br />

� −Γt<br />

is chosen for convenience. With<br />

�<br />

�<br />

. (5.37)

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