The low-momentum-transfer expansion of a charge form factor,

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Nuclear Physics · The nuclear force and nuclear models

The Nucleus Resolved, Ch The deuteron and what two nucleons do to each other

Problem

The low-momentum-transfer expansion of a charge form factor, F(q2)≈1−q2⟨r2⟩/6F(q^2)\approx 1-q^2\langle r^2\rangle/6, determines a mean square radius, and a purely spherically symmetric (L=0L=0) distribution has no preferred axis and so no quadrupole moment; that rule (an L=0L=0 state has zero electric quadrupole moment) was established for single-particle states. The deuteron, Jπ=1+J^\pi=1^+, has a measured spectroscopic quadrupole moment Qsp=+0.286 fm2Q_{sp}=+0.286\,\mathrm{fm^2}. ((a)) Using two-nucleon antisymmetry, (−1)L+S+T=−1(-1)^{L+S+T}=-1, and the deuteron's T=0T=0 (forced by its even LL and S=1S=1 through the antisymmetry rule), list every term symbol 2S+1LJ^{2S+1}L_J with S=1S=1, T=0T=0 that is consistent with J=1J=1. ((b)) Explain, using the L=0⇒L=0\Rightarrow zero-quadrupole-moment rule, why an admixture beyond the lowest term symbol you found is required by the measured QspQ_{sp}, and identify the operator in the nucleon-nucleon force responsible for connecting the two term symbols while conserving JJ and parity.

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