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C₂(omega): A Countable Second-Order Inner Model

Updated 9 July 2026
  • C₂(omega) is an inner model defined using a fragment of second-order logic with quantifiers restricted to countable subsets, enhancing definability beyond that of L.
  • It employs a truth-folded construction in L²_ω that ensures the model satisfies ZF and AC while embedding complex large-cardinal features like inner models with finitely many Woodin cardinals.
  • Under strong large-cardinal hypotheses, C₂(omega) exhibits generic absoluteness, club determinacy, and bounded power set captures, positioning it between traditional L-hierarchies and full HOD.

Searching arXiv for the exact notation and primary paper. arxiv_search(query="(Magidor et al., 25 Aug 2025)", max_results=5, sort_by="submittedDate")

C2(ω)C_2(\omega) is the inner model C(Lω2)C(\mathcal{L}^2_\omega) based on a fragment of second-order logic in which second-order variables range over countable subsets of the domain. In this construction, definability is strengthened beyond first-order LL-style definability but remains weaker than full second-order definability, because the quantifiers range only over countable sets in the ambient universe VV. The resulting model is transitive, contains all ordinals, is contained in the Chang model Cω1ωC_{\omega_1\omega}, and, under strong large-cardinal hypotheses, has generic absoluteness and substantial inner large-cardinal content (Magidor et al., 25 Aug 2025).

1. Logical basis

The logic underlying C2(ω)C_2(\omega) is Lω2\mathcal{L}^2_\omega. Its first-order variables x,y,zx,y,z range over the domain DD of a structure MM, while its second-order variables C(Lω2)C(\mathcal{L}^2_\omega)0 range over countable subsets of C(Lω2)C(\mathcal{L}^2_\omega)1 or countable subsets of C(Lω2)C(\mathcal{L}^2_\omega)2. The crucial semantic feature is externality: in a structure C(Lω2)C(\mathcal{L}^2_\omega)3, the quantifiers C(Lω2)C(\mathcal{L}^2_\omega)4 and C(Lω2)C(\mathcal{L}^2_\omega)5 range over sets that are countable in C(Lω2)C(\mathcal{L}^2_\omega)6, not merely countable in C(Lω2)C(\mathcal{L}^2_\omega)7, and not necessarily elements of C(Lω2)C(\mathcal{L}^2_\omega)8 itself. Thus C(Lω2)C(\mathcal{L}^2_\omega)9 means that there is a set LL0 that is countable in LL1 such that LL2.

This makes LL3 a fragment of second-order logic with bound second-order quantification restricted to countable sets or relations. The paper describes this logic as incompact and notoriously non-axiomatizable, but still robust enough to support a LL4-style inner-model construction. Definability in LL5 is by LL6-formulas over the current stage, using parameters from that stage. Because second-order variables range over countable subsets in LL7, definability can reach out to countable pieces of the ambient universe even when those pieces are not internal to the stage under consideration (Magidor et al., 25 Aug 2025).

A basic comparison point is full second-order logic. The paper states that LL8, while the restriction to countable second-order quantification places LL9 strictly below VV0 in general. This difference is central to the model’s behavior: VV1 is intended to capture a level of definability sensitive to externally countable structure without collapsing to full ordinal definability.

2. Stage-by-stage construction

Conceptually, VV2 is obtained by replacing the definability step of Gödel’s VV3-hierarchy with definability in VV4. To ensure the Axiom of Choice, the construction uses the “truth-folded” definition of VV5: at each stage one folds in a truth predicate for VV6 over the current level.

Formally, the hierarchy VV7 is defined by double induction. One introduces truth-codes VV8 such that

VV9

where Cω1ωC_{\omega_1\omega}0 and Cω1ωC_{\omega_1\omega}1. The stages are then defined by

Cω1ωC_{\omega_1\omega}2

Cω1ωC_{\omega_1\omega}3

and

Cω1ωC_{\omega_1\omega}4

where Cω1ωC_{\omega_1\omega}5 is the rudimentary closure augmented to allow the operation Cω1ωC_{\omega_1\omega}6 and interpretations of Cω1ωC_{\omega_1\omega}7-truth at stage Cω1ωC_{\omega_1\omega}8. Finally,

Cω1ωC_{\omega_1\omega}9

The paper also states that one may define C2(ω)C_2(\omega)0 using countable sequences instead of countable subsets; the resulting model is the same. With the truth-folded construction, C2(ω)C_2(\omega)1 satisfies C2(ω)C_2(\omega)2 and also C2(ω)C_2(\omega)3. By contrast, the older definition may fail to imply C2(ω)C_2(\omega)4 for C2(ω)C_2(\omega)5, because truth in C2(ω)C_2(\omega)6 is not guaranteed to be internally adequate (Magidor et al., 25 Aug 2025).

3. Structural properties

Several basic structural properties are established. C2(ω)C_2(\omega)7 is transitive, contains all ordinals, and is definable as a subclass of C2(ω)C_2(\omega)8. It is also contained in the Chang model C2(ω)C_2(\omega)9, and repeating the construction inside Lω2\mathcal{L}^2_\omega0 yields the same Lω2\mathcal{L}^2_\omega1. This containment is important because it identifies Lω2\mathcal{L}^2_\omega2 as an inner model built from countable information but still strictly controlled by a canonical closure condition.

A cardinality bound is proved: for every Lω2\mathcal{L}^2_\omega3,

Lω2\mathcal{L}^2_\omega4

The proof described in the paper uses a chain of Lω2\mathcal{L}^2_\omega5-elementary submodels of Lω2\mathcal{L}^2_\omega6 together with a collapse argument. This places a strong restriction on how much of the power set of a cardinal can be captured by Lω2\mathcal{L}^2_\omega7.

The model is compatible with the failure of the Continuum Hypothesis. The paper proves

Lω2\mathcal{L}^2_\omega8

The argument uses Harrington’s long projective well-ordering to produce a model of Lω2\mathcal{L}^2_\omega9 with a projective well-order x,y,zx,y,z0 and then shows that x,y,zx,y,z1 contains all reals of the ambient universe in that setting. This demonstrates that x,y,zx,y,z2 is not tied to the combinatorics of x,y,zx,y,z3 and can accommodate non-x,y,zx,y,z4 behavior (Magidor et al., 25 Aug 2025).

4. Comparison with x,y,zx,y,z5 and x,y,zx,y,z6

A central theme of the paper is the comparison between x,y,zx,y,z7 and the stationary-logic inner model x,y,zx,y,z8. In stationary logic, the generalized quantifier x,y,zx,y,z9 binds variables over DD0, and the statement DD1 means that DD2 is a club subset of DD3. The hybrid model DD4 is obtained by combining DD5 with the DD6-quantifier in the same truth-folded style.

The paper records the trivial inclusions

DD7

and

DD8

Beyond these inclusions, the relationship between DD9 and MM0 is delicate. In ZFC alone, one cannot prove that MM1 is “bigger” than MM2 in any absolute sense. Indeed, the paper gives a consistency result showing

MM3

The proof starts from MM4, adds a Cohen real by homogeneous c.c.c. forcing so that MM5 remains MM6, and then codes that real into a stationary pattern on MM7 without adding countable sets; in the final model the coded real belongs to MM8, so MM9.

At the same time, under stronger large-cardinal assumptions the comparison shifts. Assuming a proper class of Woodin cardinals, the paper states that C(Lω2)C(\mathcal{L}^2_\omega)00 and that for every C(Lω2)C(\mathcal{L}^2_\omega)01, C(Lω2)C(\mathcal{L}^2_\omega)02 contains an inner model with C(Lω2)C(\mathcal{L}^2_\omega)03 Woodin cardinals, whereas under the same assumption C(Lω2)C(\mathcal{L}^2_\omega)04 contains no inner model with a Woodin cardinal. It also proves that all reals of C(Lω2)C(\mathcal{L}^2_\omega)05 are in C(Lω2)C(\mathcal{L}^2_\omega)06 under a proper class of Woodin cardinals, and under a stronger hypothesis denoted “C(Lω2)C(\mathcal{L}^2_\omega)07” every subset of C(Lω2)C(\mathcal{L}^2_\omega)08 in C(Lω2)C(\mathcal{L}^2_\omega)09 is in C(Lω2)C(\mathcal{L}^2_\omega)10 (Magidor et al., 25 Aug 2025).

5. Large cardinals inside and around C(Lω2)C(\mathcal{L}^2_\omega)11

The large-cardinal behavior of C(Lω2)C(\mathcal{L}^2_\omega)12 is one of the paper’s main results. Assuming a proper class of Woodin cardinals, C(Lω2)C(\mathcal{L}^2_\omega)13 contains, for every finite C(Lω2)C(\mathcal{L}^2_\omega)14, an inner model with C(Lω2)C(\mathcal{L}^2_\omega)15 Woodin cardinals. The argument uses the fact that for each C(Lω2)C(\mathcal{L}^2_\omega)16, C(Lω2)C(\mathcal{L}^2_\omega)17 is a C(Lω2)C(\mathcal{L}^2_\omega)18-singleton and is therefore definable in C(Lω2)C(\mathcal{L}^2_\omega)19; iterating the top measure inside C(Lω2)C(\mathcal{L}^2_\omega)20 then yields the desired inner models.

The paper also proves a reflection result for C(Lω2)C(\mathcal{L}^2_\omega)21. Assuming a Woodin limit of Woodin cardinals, C(Lω2)C(\mathcal{L}^2_\omega)22 is strongly Mahlo in C(Lω2)C(\mathcal{L}^2_\omega)23. The proof uses the countable stationary tower C(Lω2)C(\mathcal{L}^2_\omega)24 at a Woodin limit C(Lω2)C(\mathcal{L}^2_\omega)25 to obtain an embedding C(Lω2)C(\mathcal{L}^2_\omega)26 with C(Lω2)C(\mathcal{L}^2_\omega)27, then argues by elementarity that C(Lω2)C(\mathcal{L}^2_\omega)28 is inaccessible in C(Lω2)C(\mathcal{L}^2_\omega)29 and finally strongly Mahlo there.

An even stronger layer of structure appears under a proper class of Woodin limits of Woodin cardinals. The paper invokes Woodin’s principle C(Lω2)C(\mathcal{L}^2_\omega)30 and proves that C(Lω2)C(\mathcal{L}^2_\omega)31 satisfies Club Determinacy: every stage C(Lω2)C(\mathcal{L}^2_\omega)32 decides every C(Lω2)C(\mathcal{L}^2_\omega)33-formula with parameters from C(Lω2)C(\mathcal{L}^2_\omega)34 and countable parameter sequences. From Club Determinacy it deduces that every regular cardinal of C(Lω2)C(\mathcal{L}^2_\omega)35 is measurable in C(Lω2)C(\mathcal{L}^2_\omega)36. The normal ultrafilter is defined by declaring C(Lω2)C(\mathcal{L}^2_\omega)37 iff, at a sufficiently high stage, the corresponding structure satisfies that C(Lω2)C(\mathcal{L}^2_\omega)38 lies in C(Lω2)C(\mathcal{L}^2_\omega)39; Club Determinacy forces either C(Lω2)C(\mathcal{L}^2_\omega)40 or its complement into C(Lω2)C(\mathcal{L}^2_\omega)41 (Magidor et al., 25 Aug 2025).

6. Absoluteness, forcing, and surrounding inner-model context

Under a proper class of Woodin limits of Woodin cardinals, the theory of C(Lω2)C(\mathcal{L}^2_\omega)42 is generically absolute: forcing cannot change it. More precisely, for any forcing C(Lω2)C(\mathcal{L}^2_\omega)43 and any generic C(Lω2)C(\mathcal{L}^2_\omega)44, one has

C(Lω2)C(\mathcal{L}^2_\omega)45

The paper derives this from Woodin-style absoluteness, using collapse models C(Lω2)C(\mathcal{L}^2_\omega)46 at Woodin limits of Woodin cardinals together with homogeneity. This means that, under the stated hypothesis, the first-order theory of C(Lω2)C(\mathcal{L}^2_\omega)47 is fixed across forcing extensions.

The broader context includes two further inner-model comparisons. First, under C(Lω2)C(\mathcal{L}^2_\omega)48, the paper states that C(Lω2)C(\mathcal{L}^2_\omega)49, while the modified construction “C(Lω2)C(\mathcal{L}^2_\omega)50” equals C(Lω2)C(\mathcal{L}^2_\omega)51; from this it concludes that C(Lω2)C(\mathcal{L}^2_\omega)52. Second, the paper discusses C(Lω2)C(\mathcal{L}^2_\omega)53, a variant of C(Lω2)C(\mathcal{L}^2_\omega)54 arising from existential second-order definability, and states that the assertion C(Lω2)C(\mathcal{L}^2_\omega)55 is independent of C(Lω2)C(\mathcal{L}^2_\omega)56 even when one adds the existence of supercompact cardinals. One consistency direction uses a Menas model of C(Lω2)C(\mathcal{L}^2_\omega)57 with a supercompact cardinal; the other starts from C(Lω2)C(\mathcal{L}^2_\omega)58 with a supercompact cardinal and uses homogeneous Easton-support iterations and Souslin tree forcing to keep C(Lω2)C(\mathcal{L}^2_\omega)59-truth stable while changing C(Lω2)C(\mathcal{L}^2_\omega)60 (Magidor et al., 25 Aug 2025).

Taken together, these results place C(Lω2)C(\mathcal{L}^2_\omega)61 in a distinctive position among definability-based inner models. It is weaker than full second-order C(Lω2)C(\mathcal{L}^2_\omega)62, contained in the Chang model, and sensitive to externally countable structure; yet under strong large-cardinal assumptions it exhibits generic absoluteness, Club Determinacy, and inner models with finitely many Woodin cardinals. This suggests that C(Lω2)C(\mathcal{L}^2_\omega)63 functions as a bridge between C(Lω2)C(\mathcal{L}^2_\omega)64-style definability hierarchies and inner models informed by countable second-order information.

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