Journal of Modern Classical Physics & Quantum Neuroscience

Abstract

In nuclear magnetic resonance we obtain that[H,FZ] = 0 and thus the Hamiltonian H and Z 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 estimated 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.