Abstract
Operating just once the naive Foldy-Wouthuysen-Tani transformation on the Schrödinger equation for bound states described by a Hamiltonian, we systematically develop a perturbation theory in 1/mQ which enables one to solve the Schrödinger equation to obtain masses and wave functions of the bound states in any order of 1/mQ. There also appear negative components of the wave function in our formulation which contribute also to higher order corrections to masses.
All Related Versions

This publication has 0 references indexed in Scilit: