09:28
@MaliceVidrine Not sure what is "ternary veblen", but the large veblen ordinal hierarchy can be understood by some prototypical examples. First the terms are 0 and φ(m,x) where x is a term and m is a finite list of pairs of terms where each pair (i,k) represents that the i-th parameter of φ is k. φ([[0,k]],x) represents the binary φ function; the Feferman-Schutte ordinal is Γ = sup { 0 , φ([[0,0]],0) , φ([[0,φ([[0,0]],0)]],0) , ... }.
If i<ω in each pair (i,k) in m, then the small veblen ordinal is sup { φ([[n,1]],0) : n<ω }.
The large veblen ordinal is sup { 0 , φ([[0,1]],0) , φ([[φ([[0,1]],0),1]],0) , ... }.
φ([[0,1]],0) = { 0 | φ([],~) }, meaning sup { 0 , φ([],0) , φ([],φ([],0)) , ... }
φ([[0,1]],1) = { φ([[0,1]],0)+1 | φ([],~) }, meaning sup { x , φ([],x) , φ([],φ([],x)) , ... } where x = φ([[0,1]],0)+1.
φ([[0,1]],2) = { φ([[0,1]],1)+1 | φ([],~) }.
φ([[0,1]],x) = sup { { φ([[0,1]],y)+1 | φ([],~) } : y<x }.
φ([[0,2]],0) = { 0 | φ([[0,1]],~) }.
φ([[0,2]],x) = sup { { φ([[0,2]],y)+1 | φ([],~) } : y<x }.
φ([[0,k]],0) = sup { { 0 | φ([[0,k']],~) } : k'<k }.
φ([[0,k]],x) = sup { { φ([[0,k]],y)+1 | φ([],~) } : y<x }.
By the way, φ(m,x) ignores any pairs in m of the form [i,0]. So φ([[0,0]],x) = φ([],x).
φ([[1,1]],0) = { 0 | φ([[0,~]],0) } = Γ.
φ([[1,1]],1) = { φ([[1,1]],0)+1 | φ([[0,~]],0) }.
φ([[1,1]],2) = { φ([[1,1]],1)+1 | φ([[0,~]],0) }.
φ([[1,1]],x) = sup { { φ([[1,1]],y)+1 | φ([[0,~]],0) } : y<x }.
φ([[1,1],[0,1]],0) = { 0 | φ([[1,1]],~) }.
φ([[1,1],[0,1]],x) = sup { { φ([[1,1],[0,1]],y)+1 | φ([[1,1]],~) } : y<x }.
Just to compare with the simpler multivariable φ function, φ([[1,j],[0,k]],x) represents φ[j,k](x).
φ([[2,1]],0) = { 0 | φ([[1,~]],0) }.
φ([[ω,1]],0) = sup { { 0 | φ([[i,~]],0) } : i<ω } = small veblen ordinal.
φ([[ω+1,1]],0) = { 0 | φ([[ω,~]],0) }.
Note that ω = φ([],1) so these are actually terms! For example φ([[ω+1,1]],0) = φ([[φ([],1)+1,1]],0).
And this should give an idea of how it can grow extremely fast, because we are diagonalizing within the parameters of φ themselves, where the index of each parameter is itself given by a term!
In general, the rules for non-trivial m (not all parameters are zero) are:
◇ φ(t+[[i,0]],0) = φ(t,0).