“…Another extreme is to view diquarks as a type of "Voodoo few-body 3 ". In this empirical approach to fewbody physics, to estimate the energy and wave function of, say, (a 1 a 2 a 3 ), with masses m i and interaction v i j (r), one first solves for (a 1 a 2 ) with v 12 alone, with energy η 12 , then estimates the bound state of a point-like (a 1 a 2 ) of mass m 1 + m 2 , or perhaps m 1 + m 2 + ε 2 in some variants, located at R 12 , interacting with a 3 through the potential v 13 12 ), resulting in binding energy η 12,3 , and the whole energy is given by η 12 + η 12,3 . For a 4-body system, the (a 1 a 2 ) and (a 3 a 4 ) systems are estimated first, and then a third two-body equation is solved for (a 1 a 2 ) interacting with (a 3 a 4 ) via a potential v i j (R 12 − R 34 ), where Σ denotes i = 1, 2 and j = 3, 4 throughout this paper, in particular in Sec.…”