# Phase semantics

m (→Soundness: \hdots not recoginzed by texvc) |
m (→Completeness: typo) |
||

Line 242: | Line 242: | ||

{{Definition|The '''syntactic assignation''' is the assignation that sends any variable <math>\alpha</math> to the fact <math>\{\alpha\}\orth</math>.}} |
{{Definition|The '''syntactic assignation''' is the assignation that sends any variable <math>\alpha</math> to the fact <math>\{\alpha\}\orth</math>.}} |
||

− | We instantiate the pole as <math>\Bot</math><math> := \{\Gamma \mid \vdash\Gamma\}</math>. |
+ | We instantiate the pole as <math>\Bot := \{\Gamma \mid \vdash\Gamma\}</math>. |

{{Theorem|If <math>\Gamma\in\sem{\Gamma}\orth</math>, then <math>\vdash\Gamma</math>.}} |
{{Theorem|If <math>\Gamma\in\sem{\Gamma}\orth</math>, then <math>\vdash\Gamma</math>.}} |

## Revision as of 15:05, 22 October 2011

## Contents |

## Introduction

The semantics given by phase spaces is a kind of "formula and provability semantics", and is thus quite different in spirit from the more usual denotational semantics of linear logic. (Those are rather some "formulas and *proofs* semantics".)

--- probably a whole lot more of blabla to put here... ---

## Preliminaries: relation and closure operators

Part of the structure obtained from phase semantics works in a very general framework and relies solely on the notion of relation between two sets.

### Relations and operators on subsets

The starting point of phase semantics is the notion of *duality*. The structure needed to talk about duality is very simple: one just needs a relation *R* between two sets *X* and *Y*. Using standard mathematical practice, we can write either or to say that and are related.

**Definition**

If is a relation, we write for the converse relation: iff .

Such a relation yields three interesting operators sending subsets of *X* to subsets of *Y*:

**Definition**

Let be a relation, define the operators , [*R*] and _^{R} taking subsets of *X* to subsets of *Y* as follows:

- iff
- iff
- iff

The operator is usually called the *direct image* of the relation, [*R*] is sometimes called the *universal image* of the relation.

It is trivial to check that and [*R*] are covariant (increasing for the relation) while _^{R} is contravariant (decreasing for the relation). More interesting:

**Lemma** (Galois Connections)

- is right-adjoint to [
*R*^{˜}]: for any and , we have iff - we have iff

This implies directly that commutes with arbitrary unions and [*R*] commutes with arbitrary intersections. (And in fact, any operator commuting with arbitrary unions (resp. intersections) is of the form (resp. [*R*]).

*Remark:* the operator _^{R} sends unions to intersections because is right adjoint to ...

### Closure operators

**Definition**

A closure operator on is a monotonic operator *P* on the subsets of *X* which satisfies:

- for all , we have
- for all , we have

Closure operators are quite common in mathematics and computer science. They correspond exactly to the notion of *monad* on a preorder...

It follows directly from the definition that for any closure operator *P*, the image *P*(*x*) is a fixed point of *P*. Moreover:

**Lemma**

*P*(*x*) is the smallest fixed point of *P* containing *x*.

One other important property is the following:

**Lemma**

Write for the collection of fixed points of a closure operator *P*. We have that is a complete inf-lattice.

*Remark:*
A closure operator is in fact determined by its set of fixed points: we have

Since any complete inf-lattice is automatically a complete sup-lattice, is also a complete sup-lattice. However, the sup operation isn't given by plain union:

**Lemma**

If *P* is a closure operator on , and if is a (possibly infinite) family of subsets of *X*, we write .

We have is a complete lattice.

*Proof.*
easy.

A rather direct consequence of the Galois connections of the previous section is:

**Lemma**

The operator and and the operator are closures.

A last trivial lemma:

**Lemma**

We have .

As a consequence, a subset is in iff it is of the form .

*Remark:* everything gets a little simpler when *R* is a symmetric relation on *X*.

## Phase Semantics

### Phase spaces

**Definition** (monoid)

A monoid is simply a set *X* equipped with a binary operation s.t.:

- the operation is associative
- there is a neutral element

The monoid is *commutative* when the binary operation is commutative.

**Definition** (Phase space)

A phase space is given by:

- a commutative monoid ,
- together with a subset .

The elements of *X* are called *phases*.

We write for the relation . This relation is symmetric.

A *fact* in a phase space is simply a fixed point for the closure operator .

Thanks to the preliminary work, we have:

**Corollary**

The set of facts of a phase space is a complete lattice where:

- is simply ,
- is .

### Additive connectives

The previous corollary makes the following definition correct:

**Definition** (additive connectives)

If is a phase space, we define the following facts and operations on facts:

Once again, the next lemma follows from previous observations:

**Lemma** (additive de Morgan laws)

We have

### Multiplicative connectives

In order to define the multiplicative connectives, we actually need to use the monoid structure of our phase space. One interpretation that is reminiscent in phase semantics is that our spaces are collections of *tests* / programs / proofs / *strategies* that can interact with each other. The result of the interaction between *a* and *b* is simply .

The set can be thought of as the set of "good" things, and we thus have iff "*a* interacts correctly with all the elements of *x*".

**Definition**

If *x* and *y* are two subsets of a phase space, we write for the set .

Thus contains all the possible interactions between one element of *x* and one element of *y*.

The tensor connective of linear logic is now defined as:

**Definition** (multiplicative connectives)

If *x* and *y* are facts in a phase space, we define

- ;
- ;
- the tensor to be the fact ;
- the par connective is the de Morgan dual of the tensor: ;
- the linear arrow is just .

Note that by unfolding the definition of , we have the following, "intuitive" definition of :

**Lemma**

If *x* and *y* are facts, we have iff

*Proof.*
easy exercise.

Readers familiar with realisability will appreciate...

*Remark:*
Some people say that this idea of orthogonality was implicitly present in Tait's proof of strong normalisation. More recently, Jean-Louis Krivine and Alexandre Miquel have used the idea explicitly to do realisability...

### Properties

All the expected properties hold:

**Lemma**

- The operations , , and are commutative and associative,
- They have respectively , , and for neutral element,
- is absorbant for ,
- is absorbant for ,
- distributes over ,
- distributes over .

### Exponentials

**Definition** (Exponentials)

Write *I* for the set of idempotents of a phase space: . We put:

- ,
- .

This definition captures precisely the intuition behind the exponentials:

- we need to have contraction, hence we restrict to indempotents in
*x*, - and weakening, hence we restrict to .

Since *I* isn't necessarily a fact, we then take the biorthogonal to get a fact...

## Soundness

**Definition**

Let be a commutative monoid.

Given a formula *A* of linear logic and an assignation ρ that associate a fact to any variable, we can inductively define the interpretation of *A* in *X* as one would expect. Interpretation is lifted to sequents as .

**Theorem**

Let Γ be a provable sequent in linear logic. Then .

*Proof.* By induction on .

## Completeness

Phase semantics is complete w.r.t. linear logic. In order to prove this, we need to build a particular commutative monoid.

**Definition**

We define the **syntactic monoid** as follows:

- Its elements are sequents Γ quotiented by the equivalence relation generated by the rules:
- if Γ is a permutation of Δ

- Product is concatenation:

- Neutral element is the empty sequent: .

The equivalence relation intuitively means that we do not care about the multiplicity of -formulae.

**Lemma**

The syntactic monoid is indeed a commutative monoid.

**Definition**

The **syntactic assignation** is the assignation that sends any variable α to the fact .

We instantiate the pole as .

**Theorem**

If , then .

*Proof.* By induction on Γ.

## Cut elimination

Actually, the completeness result is stronger, as the proof does not use the cut-rule in the reconstruction of . By refining the pole as the set of *cut-free* provable formulae, we get:

**Theorem**

If , then Γ is cut-free provable.

From soundness, one can retrieve the cut-elimination theorem.

**Corollary**

Linear logic enjoys the cut-elimination property.