P-bot has decided that this is likely welldefined: (Note : the whole of the LaTeX may not be visible)
\begin{eqnarray*}C_{0,m}(\alpha) = \{0,\Omega\} \\ C_{,m}(\alpha)=\bigcup_{n<\omega}(C_{n,m}(\alpha))\\ C_{n+1,m+1}(\alpha)=\{\gamma+\delta,\gamma\delta,\gamma^\delta,\phi_\gamma(\delta),(\psi_{0,m+1}(η))| \gamma,\delta,\eta\in(C_{n,m+1}(\alpha));\eta<\alpha\}\bigcup\\\{(\psi_{1,o}(\gamma)),(\psi_{0,o}(\gamma)),\Omega_\gamma| \gamma\in(C_{n,m+1}(\alpha));o<(m+1)\}\\ C_{n+1,0}(\alpha)=\{\gamma+\delta,\gamma\delta,\gamma^\delta,\phi_\gamma(\delta),(\psi_{0,0}(\eta)),\Omega_\gamma|\gamma,\delta,\eta\in(C_{n,0}(\alpha));\eta<\alpha\}\\ \psi_{0,m}(\alpha)=min\{\beta\in\Omega|\beta\notin(C_{,m}(\alpha))\}\\ \psi_{1,m}(\alpha)=sup((C_{,m}(\alpha)))\\ \\\end{eqnarray*}
Just posting this so that I can stop cluttering my old OCF post.
In plain text:
C_0,0(α)={0,Ω}
C_n+1,0(α)={γ+δ,γδ,γ^δ,φ_γ(δ),(ψ_0,0(η)),w_γ|γ,δ,η∈(C_n,0(α));η<α}
C,0(α)=⋃(n<ω)C_n,0(α)
ψ_0,0(α)=min{β∈Ω|β∉C,0(α)}
ψ_1,0(α)=sup(C,0(α))
C_0,m(α)={0,Ω}
C_n+1,m+1(α)={γ+δ,γδ,γ^δ,φ_γ(δ),(ψ_0,m+1(η)),(ψ_1,o(γ)),(ψ_0,o(γ)),w_γ| γ,δ,η∈(C_n,m+1(α));η<α,o<(m+1)}
C,m(α)=⋃(n<ω)(C_n,m(α))
ψ_0,m(α)=min{β∈Ω|β∉(C,m(α))}
ψ_1,m(α)=sup((C,m(α)))
Basically, it's a system of OCFs where each one can access the prior ones. This is why I thought it was welldefined. (And it is).
EDIT: another related one: \begin{eqnarray*}C_{0,m}(\alpha) = \{0,\Omega\} \\
C_{,m}(\alpha)=\bigcup_{n<\omega}(C_{n,m}(\alpha))\\
C_{n+1,m+1}(\alpha)=\{\gamma+\delta,\gamma\delta,\gamma^\delta,\phi_\gamma(\delta),(\psi_{0,m+1}(η))| \gamma,\delta,\eta\in(C_{n,m+1}(\alpha));\eta<\alpha\}\bigcup\\\{(\psi_{2,o}(\gamma)),(\psi_{1,o}(\gamma)),(\psi_{0,o}(\gamma)),\Omega_\gamma| \gamma\in(C_{n,m+1}(\alpha));o<(m+1)\}\\
C_{n+1,0}(\alpha)=\{\gamma+\delta,\gamma\delta,\gamma^\delta,\phi_\gamma(\delta),(\psi_{0,0}(\eta)),\Omega_\gamma|\gamma,\delta,\eta\in(C_{n,0}(\alpha));\eta<\alpha\}\\
\psi_{0,m}(\alpha)=min\{\beta\in\Omega|\beta\notin(C_{,m}(\alpha))\}\\
\psi_{1,m}(\alpha)=min(\beta>\Omega|\beta\notin(C_{,m}(\alpha)))\\
\psi_{2,m}(\alpha)=sup((C_{,m}(\alpha)))\\
\\\end{eqnarray*}
This one has a third function which finds the minimum ordinal \(\beta\) that is larger than \(\Omega\) and not in the set. This makes it somewhat stronger than the previous.