Abstract

In nuclear magnetic resonance we obtain that,[H,FZ ] = 0 and thus the Hamiltonian H and FZ have a common set of orthonormalized eigenfunctions that require the use of Clebsch-Gordan coefficients used in the present paper. We have calculated such Clebsch-Gordan coefficients with the value j₁xj₂=1/2x1/2 and we have esti mated the energy levels and the transition energies of this system under the nuclear magnetic resonance. The generalities of the A2, AB; AX, and the three-spin system are studied. On the four-spin system we give the generalities of such a system

DOI: doi.org/10.63721/25JPQN0113

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