“…For simplicity, we shall write, for instance, N(τ ) instead of N(τ, u) if that will not result in ambiguities. Relativistic nonholonomic phase spacetimes can be enabled with necessary types double nonholonomic (2+2)+(2+2) and (3+1)+(3+1) splitting[35,36,37,28,17]. Local (3+1)+(3+1) coordinates are labeled in the form u = { u α = u αs = (x i 1 , y a 2 ; pa 3 , pa 4 ) = (xì, u 4 = y 4 = t; pà, p8 = E)} for i1, j1, k1, ... = 1, 2; a1, b1, c1, ... = 3, 4; a2, b2, c2, ... = 5, 6; a3, b3, c3, ... = 7, 8.…”