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Iterated structures are not modally definable

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Iterated structures are not modally definable

Philippe Balbiani, Levan Uridia

To cite this version:

Philippe Balbiani, Levan Uridia. Iterated structures are not modally definable. TbiLLC 2019

-Thirteenth International Tbilisi Symposium on Language, Logic and Computation, Sep 2019, Batoumi,

Georgia. �hal-02411269�

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Iterated structures are not modally definable

P. Balbiani and L. Uridia

1

Universit´e de Toulouse, Philippe.Balbiani@irit.fr

2

TSU A. Razmadze Mathematical Institute l.uridia@freeuni.edu.ge

1

Introduction

Iterated structures are bi-relational Kripke frames where each relation is a strict partial order and additionally second relation is the greatest fixed point of the first relation under monotone operator on the lattice of all partial orders included in the first relation. The study of these structures closely relates to the modal logic study of Cantor Bendixon rank. The details about this connection as well as important results around this study could be found in [2]

In this work we touch the issue of modal definability of iterated strict partial orders. The modal logic of iterated strict partial orders is studied in [2] where we present the complete axiomatisation of the logic. The logic is axiomatised by the following modal formulas 2φ → 22φ, 2?φ →2?2?φ,2φ → 2?φ,2?φ → 22?φ, 2?φ →2?2φ, 22?φ →2?φ. Moreover we

prove that the class of iterated structures is not first order definable and that the modality2∗ interpreted on the second relation is not modally definable. In this paper we prove that the class of iterated structures is not modally definable either.

2

Preliminaries

A strict partial order on X is a binary relation R on X such that: (i) for all x ∈ X, x 6∈ R(x), (ii) for all x ∈ X, R(R(x)) ⊆ R(x), where R(x) = {y | xRy}. Let ≤ be the binary relation between strict partial orders on X defined by R ≤ R0 iff R ⊆ R0. Given a strict partial order R on X, let LR be the set of all strict partial orders R0 on X such that R0 ≤ R. We point

out that the least element of LR is the strict partial order ∅ and the greatest element of LR

is R. Moreover, the least upper bound of a family {R0

i: i ∈ I} in LR is the transitive closure

of S{R0

i: i ∈ I} and the greatest lower bound of a family {R0i: i ∈ I} in LR is T{R0i: i ∈ I}.

Hence, (LR, ≤) is a complete lattice.

For a given a strict partial order R on X, let θRbe the function θR: LR→ LRsuch that for

all R0∈ LR, θR(R0) = R ◦ R0, i.e. θR(R0) is the binary relation on X such that for all x, y ∈ X,

xθR(R0)y iff there exists z ∈ X such that xRz and zR0y. It is straightforward to check that

the function θR is monotone. Since (LR, ≤) is a complete lattice, the function θR has a least

fixpoint lfp(θR) and a greatest fixpoint gfp(θR). Obviously, lfp(θR) = ∅ while gfp(θR) is the

least upper bound of the family {R0: R0≤ θR(R0)} in LR[1]. Equally gfp(θR) can be obtained

by iteration of θR. For all ordinals α, we inductively define θR↓α as follows:

• θR↓0 is R,

• for all successor ordinals α, θR↓α is θR(θR↓(α − 1)),

• for all limit ordinals α, θR↓α is the greatest lower bound of the family {θR↓β: β ∈ α} in

LR.

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Iterated structures are not modally definable

Fact 1. (i) for all ordinals α, gfp(θR) ≤ θR↓α,

(ii) there exists an ordinal α such that gfp(θR) = θR↓α.

The least ordinal α such that θR↓α = gfp(θR) is called the Cantor-Bendixson rank of R.

3

A modal logic

In this section, we present a modal logic with modal operators 2 and 2?. We define the

relational semantics where 2 and 2? are respectively interpreted by strict partial orders and

the greatest fixpoints of the θ-like functions they define. The language of the modal logic is defined using a countable set of propositional variables. We inductively define the set of formulas as follows: φ ::= p | ⊥ | ¬φ | (φ ∨ ψ) |2φ | 2?φ. The other connectives are defined as

usual. We obtain the formulas3φ and 3?φ as abbreviations: 3φ ::= ¬2¬φ, 3?φ ::= ¬2?¬φ.

Relational semantics of the modal logic is based on the iterated structures which are bire-lational strict partial orders with certain interconnection between the two relations.

Definition 2. An iterated structure is a structure of the form F = (X, R, S) such that (i) X is a nonempty set, (ii) R is a strict partial order on X, (iii) S is the greatest fixpoint of the function θR in LR.

The second relation i.e. the greatest fixpoint S of θRin the iterated structure F = (X, R, S)

can be represented in more intuitive way. The following proposition gives the desired represen-tation. This representation plays an important role in the proof of the main theorem.

Proposition 3. For a given iterated structure F = (X, R, S) and two points x, y ∈ X we have: xSy iff there exists an infinitely ascending chain a1, a2, ... such that x = a1 and for each i the

member of chain ai is a predecessor of y i.e. aiRy.

x |= ♦∗φ y |= φ a1 a2 ... ak ...

On the figure we see an iterated structure (X, R, S) where the root x satisfies the for-mula ♦∗φ. The left arrow represents the relation S while small arrows represent the relation R.

Figure 1:

4

Modal Definability

In this section we touch the main issue of our study and prove the main theorem that the class of iterated structures is not definable in modal language. In [2] we prove that the class 2

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Iterated structures are not modally definable

of iterated structures is not first order definable. Besides we show that the2∗ modality is not definable in simpler language which only contains2. Here we present the more intuitive proof of this fact and additionally show that the property of S to be the greatest fixpoint of R in the bi relational frame (X, R, S) with R being strict partial order, is not definable in modal language with two modalities.

Fact 4. [2] The modality2∗ is not definable in a simpler language which only contains 2 and Boolean connectives. Which means that there is no formula φ in the language with one 2 such that 2∗p ↔ φ.

Theorem 5. The class of iterated structures is not modally definable.

Sketch. We construct the two structures (X, R, S = ∅) and (X0, R0, S0 = ∅) as depicted on the picture (ignore the rounded arrows of the frame on the rigth). The first is an iterated structure and (X0, R0, S0) is a p-morphic image of (X, R, S) while the later is not the iterated structure. This follows from the Proposition 3. p-morphism f is established by the following clauses f (ai) = a0i and f (bi) = a0ω. a00 a0ω a01 a02 ... a0k ... a0 b1 a1 a2 b2 ... ak bk ...

On the figure we see an iterated structure (X, R, S) on the left and bi relational frame (X0, R0, S0) on the right. For (X0, R0, S0) to be an iterated structure S0 should contain all pairs connected by rounded arrows

Figure 2:

References

[1] Tarski, A., A lattice-theoretical fixpoint theorem and its applications. Pacific Journal of Mathe-matics 5 (1955) 285-309.

[2] P. Balbiani and L. Uridiaia, Completeness and Definability of a Modal Logic Interpreted over Iterated Strict Partial Orders. Advances in Modal Logic 2012: 71-88.

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