Final answer:
The interaction between two nucleons can be represented by the operator ˆV(1,2) = σ^(1) σ^(2). To evaluate the two-body matrix element in the coupled basis, we need to decompose the state | l1 s1 l2 s2; LS ; JMj > into the possible states allowed by the interaction.
Step-by-step explanation:
The interaction between two nucleons can be represented by the operator ˆV(1,2) = σ^(1) σ^(2), where σ^(i) are the Pauli matrices.
To evaluate the two-body matrix element in the coupled basis, we need to decompose the state | l1 s1 l2 s2; LS ; JMj > into the possible states allowed by the interaction.
As the bound state has J^π = 1^+, the only possibilities are S=1, L=0(L=2 will not yield J=1).
The operator ˆV(1,2) acts on the spin space of the nucleons, not on the coordinates l1, s1, l2, s2, L, S, J, Mj, so we can't say that the matrix element is 1 directly.