Alpha Decay — Question 7

Section 42-4 · Physics pages 7064–7065

Question 7 The Coulomb action leads to strong inverse-square-root energy dependence For zero orbital angular momentum, a WKB Coulomb action is G = ℏ−1 ∫b R √ 2µ(K/r −Q) dr, where b = K/Q. Use the substitution r = b sin2 ϕ. Q−1/2 ln T1/2 Schematic; labels, not drawing lengths, specify the data. (a) Derive a closed expression for G in terms of x = R/b. (b) For R/b ≪1, obtain the leading energy dependence of ln T1/2 if the decay prefactor is held fixed and P = e−2G.
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Question 7 - Solution The Coulomb action leads to strong inverse-square-root energy dependence Q−1/2 ln T1/2 (a) Method and calculation G = 2b√2µQ ℏ ∫π/2 sin−1 √x cos2 ϕ dϕ. G = K√2µ ℏ√Q [ cos−1 √x − √ x(1 −x) ] . (b) Interpretation and further calculation x →0 : G ≃πK√2µ 2ℏ√Q . ln T1/2 = constant + 2G ≃constant + πK√2µ ℏ√Q . Physical check The logarithm grows roughly with charge and inverse square root of Q. Finite radius, angular momentum and alpha preformation modify this leading approximation.

Question 7

The Coulomb action leads to strong inverse-square-root energy dependence

For zero orbital angular momentum, a WKB Coulomb action is G=ℏ−1∫Rb2μ(K/r−Q)drG=\hbar^{-1}\int_R^b\sqrt{2\mu(K/r-Q)}\,dr, where b=K/Qb=K/Q. Use the substitution r=bsin⁡2ϕr=b\sin^2\phi.

Diagram shown in the original SVG worksheet.

  1. Derive a closed expression for G in terms of x=R/bx=R/b.

  2. For R/b≪1R/b\ll1, obtain the leading energy dependence of ln⁡T1/2\ln T_{1/2} if the decay prefactor is held fixed and P=e−2GP=e^{-2G}.

Question 7 - Solution

The Coulomb action leads to strong inverse-square-root energy dependence

Diagram shown in the original SVG worksheet.

(a) Method and calculation

G=2b2μQℏ∫sin⁡−1xπ/2cos⁡2ϕdϕ.G=\frac{2b\sqrt{2\mu Q}}\hbar\int_{\sin^{-1}\sqrt x}^{\pi/2}\cos^2\phi\,d\phi.G=K2μℏQ[cos⁡−1x−x(1−x)].\boxed{G=\frac{K\sqrt{2\mu}}{\hbar\sqrt Q}\left[\cos^{-1}\sqrt x-\sqrt{x(1-x)}\right]}.

(b) Interpretation and further calculation

x→0:G≃πK2μ2ℏQ.x\to0:\quad G\simeq\frac{\pi K\sqrt{2\mu}}{2\hbar\sqrt Q}.ln⁡T1/2=constant+2G≃constant+πK2μℏQ.\boxed{\ln T_{1/2}=\text{constant}+2G\simeq\text{constant}+\frac{\pi K\sqrt{2\mu}}{\hbar\sqrt Q}}.

Physical check

The logarithm grows roughly with charge and inverse square root of Q. Finite radius, angular momentum and alpha preformation modify this leading approximation.