Chapter 3
The harmonic-oscillator model

Although the aim of this review is to discuss elaborate methods for solving the three-body problem, the very simple harmonic-oscillator model deserves some presentation. First, it has played an essential role in the development of the quark model, with, in particular, the pioneering works of Dalitz [34] and Greenberg [4] and the very complete and convincing studies of the baryon spectrum by Dalitz and Horgan [35], Isgur and Karl [36], Gromes et al.[37], Cutkosky and Hendrick [38], Hey et al.[6] and many others [39]. The harmonic-oscillator model may also serve as a basis or a starting point for accurate variational methods. Its understanding is anyhow necessary for getting some insight into the three-body problem and, in particular, into the difficulties associated with the symmetrization of the wave functions.

 3.1 The linear oscillator
 3.2 The spatial oscillator
 3.3 Three-body oscillator with equal masses
 3.4 Permutation of three quarks
 3.5 Colour, spin, and isospin wave functions
 3.6 Spatial wave functions of given permutation symmetry
 3.7 Harmonic oscillator with unequal masses