Abstract

In nuclear magnetic resonance we have that [H, Fz] = 0 and thus H and Fz have a common set of orthonormalized eigenfunctions that employ the use of Clebsch-_Gordan coefficients that we use in the present paper. We have calculated the Clebsch_Gordan coefficients with the value j1xj2 =1/2x1/2 and we estimated the energy levels and the transition energies of this system under the nuclear magnetic resonance. The generalities of the A2, AB; AX, and three spin system are studied.

DOI: doi.org/10.63721/25JPQN0103

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