A3.15

Symmetries and Groups in Physics | Part II, 2004

(i) Show that the character of an SU(2)S U(2) transformation in the 2l+12 l+1 dimensional irreducible representation dld_{l} is given by

χl(θ)=sin⁡[(l+1/2)θ]sin⁡[θ/2]\chi_{l}(\theta)=\frac{\sin [(l+1 / 2) \theta]}{\sin [\theta / 2]}

What are the characters of irreducible SO(3)S O(3) representations?

(ii) The isospin representation of two-particle states of pions and nucleons is spanned by the basis T={∣π+p⟩,∣π+n⟩,∣π0p⟩,∣π0n⟩,∣π−p⟩,∣π−n⟩}T=\left\{\left|\pi^{+} p\right\rangle,\left|\pi^{+} n\right\rangle,\left|\pi^{0} p\right\rangle,\left|\pi^{0} n\right\rangle,\left|\pi^{-} p\right\rangle,\left|\pi^{-} n\right\rangle\right\}.

Pions form an isospin triplet with π+=∣1,1⟩,π0=∣1,0⟩,π−=∣1,−1⟩\pi^{+}=|1,1\rangle, \pi^{0}=|1,0\rangle, \pi^{-}=|1,-1\rangle; and nucleons form an isospin doublet with p=∣1/2,1/2⟩,n=∣1/2,−1/2⟩p=|1 / 2,1 / 2\rangle, n=|1 / 2,-1 / 2\rangle. Find the values of the isospin for the irreducible representations into which TT will decompose.

Using I−∣j,m⟩=(j−m+1)(j+m)∣j,m−1⟩I_{-}|j, m\rangle=\sqrt{(j-m+1)(j+m)}|j, m-1\rangle, write the states of the basis TT in terms of isospin states.

Consider the transitions

π+p→π+pπ−p→π−pπ−p→π0n\begin{array}{ll} \pi^{+} p & \rightarrow \pi^{+} p \\ \pi^{-} p & \rightarrow \pi^{-} p \\ \pi^{-} p & \rightarrow \pi^{0} n \end{array}

and show that their amplitudes satisfy a linear relation.

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