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The $\Lambda^{0}$ baryon has two possible decays, the first is $\Lambda^{0} \to \pi^{0} + n^{0}$ and the second $\Lambda^{0} \to \pi^{-} + p^{+}$.

I've been asked to determine the ratio of protons to neutrons observed in the decay.

Properties: $$ \begin{array}{cccc} \text{Particle} & \text{Spin} & \text{Charge} & \text{total isospin} \\\hline \Lambda^0 & \frac12 & 0 & 0 \\ \rm n^0 & \frac12 & 0 & \frac12 \\ \rm p^+ & \frac12 & +1 & \frac12 \\ \pi^- & 0 & -1 & 1 \\ \pi^0 & 0 & 0 & 1 \\ \end{array} $$

Charge and angular momentum are conserved in the decay, but the total isospin changes by $\frac{1}{2}$. I'm supposed to ignore all relativistic effects.

How do I even begin with this question? I don't understand how these conservations lead to the number of particles observed in the decay...

Qmechanic
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1 Answers1

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A hint, since we discourage complete answers to homework questions and homework-like questions:

Isospin gets its name because the isospin of a composite system is related to its components using the same rules as for combining spin angular momenta. The strong force is, to good approximation, blind to the $z$-component of isospin (a.k.a. electric charge); your two final states are the components of a composite state whose isospin is well-defined. (You even say what it is.) What are its Clebsch-Gordan coefficients?

rob
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