A simple technique employed almost three decades ago to manufacture partial
ly solvable quantum many-body problems is revisited. [A quantum problem is
"partially solvable" if (only) some of its eigenvalues and eigenfunctions c
an be exhibited]. The models thereby generated are characterized by Hamilto
nians of normal form, i.e., standard kinetic plus momentum-independent pote
ntial energy; in most cases the latter features three-body, in addition to
two-body and one-body, interactions. The setting refers to D-dimensional sp
ace; the examples focus on D=1, D=2, and D greater than or equal to 2, and
include generalizations of, and additional results on, cases recently discu
ssed in the literature, as well as new models. (C) 1999 American Institute
of Physics. [S0022-2488(99)02409-3].