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==== Beyond the Feferman-Schütte ordinal ====
We have <math>\psi(\Omega^{\Omega+\alpha}) = \phi_{\Gamma_0+\alpha}(0)</math> for all <math>\alpha\leq\Gamma_1</math> where <math>\Gamma_1</math> is the next fixed point of <math>\alpha \mapsto \phi_\alpha(0)</math>. So, if <math>\alpha\mapsto\Gamma_\alpha</math> enumerates the fixed points in question. (which can also be noted <math>\phi(\alpha+1,0,0)</math> using the many-valued Veblen functions) we have <math>\psi(\Omega^{\Omega(
* <math>\psi(\Omega^{\Omega^2})</math> is the [[Ackermann ordinal]] (the range of the notation <math>\phi(\alpha,\beta,\gamma)</math> defined predicatively),
* <math>\psi(\Omega^{\Omega^\omega})</math> is the [[small Veblen ordinal|“small” Veblen ordinal]] (the range of the notations <math>\phi(\ldots)</math> predicatively using finitely many variables),
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