Abstract | ||
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ing on w and pairing with oe(p(c); (x)Ap(q(c); x) ! p(c)) in the first coordinateyieldshoe(p(c);(x)Ap(q(c); x) ! p(c));(w)(Ap(q(c); p(w)); (x)Ap(q(c); Ap(q(w); x)))i 2 PAR;i.e. s (c) 2 PAR.We define the operator that builds the universe (U1; T1) by puttingf(c) := s (c) +hn 1 ; (x)R 1 (x; p(c))i;for c 2 PAR, and let e := fix((c)f(c)). Hence e 2 PAR is a fixed point of f ,e = f(e). The right summand of f corresponds to the rules (2).We now interpret Type:Type. The universe ... |
Year | DOI | Venue |
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1991 | 10.2178/jsl/1183743747 | J. Symb. Log. |
DocType | Volume | Issue |
Journal | 56 | 3 |
Citations | PageRank | References |
1 | 0.43 | 3 |
Authors | ||
1 |
Name | Order | Citations | PageRank |
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Erik Palmgren | 1 | 233 | 43.17 |