Abstract
Starting from the semirelativistic Hamiltonian for a doubly heavy baryon system () with Coulomb and linear confining scalar potentials, and operating the naive Foldy-Wouthuysen-Tani transformation on two heavy quarks, I construct a formulation how to calculate mass spectra and wave functions of doubly heavy baryons. Based on our formulation, their masses and wave functions are expanded in with a heavy quark mass and the mode lowest-order equation is examined carefully to obtain a complete set of eigenfunctions. I claim that the mode wave function should be given by other nonrelativistic methods, e.g., the Godfrey-Isgur model to give a complete wave function for a doubly heavy baryon.
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