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actually we are now back to \(\zeta_0\) even though as you know our analysis has reached \(\psi(\Omega_2^\Omega)\), this analysis is very important because we will build the foundation again and now we know how to get to a high level, we have to update it from the beginning to support the above, this is a big revision
(|2) = psi(Ω^2)
(1|2) = psi(Ω^2)+1
(2|2) = psi(Ω^2)+2
(3|2) = psi(Ω^2)+3
((|1)|2) = psi(Ω^2)+psi(Ω)
((|2)|2) = psi(Ω^2)+psi(Ω^2)
((|2)(|2)|2) = psi(Ω^2)+psi(Ω^2)+psi(Ω^2)
((|2)!^(|0)|2) = psi(Ω^2)w
((|2)!^((|0)|0)|2) = psi(Ω^2)w^w
((|2)!^(((|0)|0)|0)|2) = psi(Ω^2)w^w^w
((|2)!^((((|0)|0)|0)|0)|2) = psi(Ω^2)w^w^w^w
((|2)!^(|1)|2) = psi(Ω^2)psi(Ω)
((|2)!^(|2)|2) = psi(Ω^2)psi(Ω^2)
((|2)!^(|2)|2) = psi(Ω^2+2)
((|2)!^((|2)!^(|2)|2)|2) = psi(Ω^2+3)
((|2)!^(((|2)!^(|2)|2)!^(|2)|2)|2) = psi(Ω^2+4)
((|2)!^((((|2)!^(|2)|2)!^(|2)|2)!^(|2)|2)|2) = psi(Ω^2+5)
((1|2)|2) = psi(Ω^2+w)
((2|2)|2) = psi(Ω^2+w+1)
((3|2)|2) = psi(Ω^2+w+2)
(((|0)|2)|2) = psi(Ω^2+w2)
((((|0)|0)|2)|2) = psi(Ω^2+w^2)
(((((|0)|0)|0)|2)|2) = psi(Ω^2+w^w^w)
((|1)|2)|2) = psi(Ω^2+psi(Ω))
((|2)|2)|2) = psi(Ω^2+psi(Ω^2))
(((|2)|2)|2)|2) = psi(Ω^2+psi(Ω^2+psi(Ω^2)))
((((|2)|2)|2)|2)|2) = psi(Ω^2+psi(Ω^2+psi(Ω^2+psi(Ω^2))))
(((((|2)|2)|2)|2)|2)|2) = psi(Ω^2+psi(Ω^2+psi(Ω^2+psi(Ω^2+psi(Ω^2)))))
(<|1>|2) = psi(Ω^2+Ω)
(<|1>|2) = psi(Ω^2+Ω)
(1 <|1>|2) = psi(Ω^2+Ω)+1
((|1) <|1>|2) = psi(Ω^2+Ω)+psi(Ω)
((|2) <|1>|2) = psi(Ω^2+Ω)+psi(Ω^2)
((|2) <|1>|2) = psi(Ω^2+Ω)+psi(Ω^2)
(((|2)|2) <|1>|2) = psi(Ω^2+Ω)+psi(Ω^2+psi(Ω^2))
((((|2)|2)|2) <|1>|2) = psi(Ω^2+Ω)+psi(Ω^2+psi(Ω^2+psi(Ω^2)))
((<|1>|2)<|1>|2) = psi(Ω^2+Ω+psi(Ω^2+Ω))
(((<|1>|2)<|1>|2)<|1>|2) = psi(Ω^2+Ω+psi(Ω^2+Ω+psi(Ω^2+Ω)))
((((<|1>|2)<|1>|2)<|1>|2)<|1>|2) = psi(Ω^2+Ω+psi(Ω^2+Ω+psi(Ω^2+Ω+psi(Ω^2+Ω))))
( <1|1>|2) = psi(Ω^2+Ω2)
( <2|1>|2) = psi(Ω^2+Ω3)
( <3|1>|2) = psi(Ω^2+Ω4)
( <(|0)|1>|2) = psi(Ω^2+Ωw)
( <((|0)|0)|1>|2) = psi(Ω^2+Ωw^w)
( <(((|0)|0)|0)|1>|2) = psi(Ω^2+Ωw^w^w)
( <(|1)|1>|2) = psi(Ω^2+Ωpsi(Ω))
( <( <|1>|2)|1>|2) = psi(Ω^2+Ωpsi(Ω^2+Ω))
( <( <( <|1>|2)|1>|2)|1>|2) = psi(Ω^2+Ωpsi(Ω^2+Ωpsi(Ω^2+Ω)))
( {1} |2) = psi(Ω^2*2)
( {2} |2) = psi(Ω^2*3)
( {3} |2) = psi(Ω^2*4)
( {4} |2) = psi(Ω^2*5)
( {(|0)} |2) = psi(Ω^2*w)
( {((|0)|0)} |2) = psi(Ω^2*w^w)
( {(((|0)|0)|0)} |2) = psi(Ω^2*w^w^w)
( {((((|0)|0)|0)|0)} |2) = psi(Ω^2*w^w^w^w)
( {(|1)} |2) = psi(Ω^2*psi(Ω))
( {(|2)} |2) = psi(Ω^2*psi(Ω^2))
( {(|2)} |2) = psi(Ω^2*psi(Ω^2))
( {( {(|2)} |2)} |2) = psi(Ω^2*psi(Ω^2)*psi(Ω^2))
( {( {( {(|2)} |2)} |2)} |2) = psi(Ω^2*psi(Ω^2)*psi(Ω^2*psi(Ω^2)))
( {( {( {( {(|2)} |2)} |2)} |2)} |2) = psi(Ω^2*psi(Ω^2)*psi(Ω^2*psi(Ω^2*psi(Ω^2))))