Spin dependence in a bounded nucleon-pair model
A rotationally invariant central nucleon-pair model can include V(r)=V_c(r)+V_s(r)S_p·S_n/ħ².
Key knowledge
A rotationally invariant central nucleon-pair model can include V(r)=V_c(r)+V_s(r)S_p·S_n/ħ². For two spin-½ nucleons the spin factor is +¼ in the triplet S=1 channel and −¾ in the singlet S=0 channel, producing different radial potentials. This illustrates why a spin-independent attraction cannot describe both channels with the same fitted potential.
Values and equations
V=V_c+V_s(S_p·S_n)/ħ²; (S_p·S_n)/ħ²=½[S(S+1)−3/2]
- V,V_c,V_s
- Potential energies/coefficient J
- r
- Nucleon separation m
- S_p,S_n
- Nucleon spin operators J s
- ħ
- Reduced Planck constant J s
- S
- Coupled spin quantum number, 0 or 1
Conditions and scope
- V_c and V_s have energy units; the relative-motion nonrelativistic model omits tensor, spin–orbit, charge-symmetry breaking and many-body terms. It is an effective model, not the fundamental QCD interaction.
- The central s-wave approximation represents the deuteron's bound triplet channel and unbound singlet contrast without asserting that the real deuteron is a pure s-wave or copying fitted numerical well strengths.
Sources · 1
References
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Evidence and review
Introduction to Applied Nuclear Physics: chapter 5 (2012): Section 5.2.4, printed page 73: scalar spin coupling, coupled-spin eigenvalues and distinct triplet/singlet fitted wells. Correct ħ² normalization is retained; section 5.1's exact charge-independence and nonconservation-of-total-angular-momentum wording are not adopted.
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