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Involutive left-continuous t-norms arising from completion of - - PowerPoint PPT Presentation

Involutive left-continuous t-norms arising from completion of MV-chains Stefano Aguzzoli (1) , Anna Rita Ferraioli (2) , Brunella Gerla (2) (1) Dipartimento di Informatica, Universit` a di Milano, Italy aguzzoli@di.unimi.it (2) Dipartimento di


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Involutive left-continuous t-norms arising from completion of MV-chains

Stefano Aguzzoli(1), Anna Rita Ferraioli(2), Brunella Gerla(2)

(1)Dipartimento di Informatica, Universit`

a di Milano, Italy aguzzoli@di.unimi.it

(2)Dipartimento di Scienze Teoriche e Applicate, Universit`

a dell’Insubria, Varese {annarita.ferraioli, brunella.gerla}@uninsubria.it

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Chang’s MV-algebra

Linearly ordered MV-algebras (MV-chains) can be simple or non-simple: simple MV-chains are subalgebras of the standard MV-algebra [0, 1]. The basic example of a non simple MV-chain is Chang’s MV-algebra.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Chang’s MV-algebra

Linearly ordered MV-algebras (MV-chains) can be simple or non-simple: simple MV-chains are subalgebras of the standard MV-algebra [0, 1]. The basic example of a non simple MV-chain is Chang’s MV-algebra. It can be defined as C = Γ(Z lex Z, (1, 0)) , where Z lex Z is the abelian ℓ-group obtained as the lexicographic product

  • f two copies of the ℓ-group Z of the integer numbers, and Γ is Mundici’s

functor, which implements a categorical equivalence between abelian ℓ-groups with a distinguished strong unit and MV-algebras.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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DLMV

DLMV is the variety generated by the Chang’s MV-algebra C. The variety DLMV is axiomatized from the variety of MV-algebras adding the axiom (2x)2 = 2x2 .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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DLMV

DLMV is the variety generated by the Chang’s MV-algebra C. The variety DLMV is axiomatized from the variety of MV-algebras adding the axiom (2x)2 = 2x2 . The variety DLMV is not standard complete, i.e., there is no MV-algebra generating DLMV that has [0, 1] as support.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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DLMV

DLMV is the variety generated by the Chang’s MV-algebra C. The variety DLMV is axiomatized from the variety of MV-algebras adding the axiom (2x)2 = 2x2 . The variety DLMV is not standard complete, i.e., there is no MV-algebra generating DLMV that has [0, 1] as support. C is a subalgebra of Γ(Z lex R, (1, 0)). Γ(Z lex R, (1, 0)) also generates DLMV.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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The MV-algebra [0, 1](1/2)

We can represent Γ(Z lex R, (1, 0)) isomorphically as an MV-algebra [0, 1](1/2) = ([0, 1/2) ∪ (1/2, 1], ⊙, ¬, 0) which is clearly not a subalgebra of the standard MV-algebra [0, 1], nor it is complete as a lattice.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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The MV-algebra [0, 1](1/2)

We can represent Γ(Z lex R, (1, 0)) isomorphically as an MV-algebra [0, 1](1/2) = ([0, 1/2) ∪ (1/2, 1], ⊙, ¬, 0) which is clearly not a subalgebra of the standard MV-algebra [0, 1], nor it is complete as a lattice. The monoidal operation ⊙ is given by x ⊙y =      1 − x − y + 2xy if x, y ∈ (1/2, 1]

x+y−1 2y−1

if x ∈ [0, 1/2), y ∈ (1/2, 1] and x + y > 1

  • therwise

.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Cancellative hoops

Definition

A cancellative hoop is a hoop (H, ∗, →, 1) such that x ∗ y ≤ z ∗ y implies x ≤ z for each x, y, z ∈ H.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Cancellative hoops

Definition

A cancellative hoop is a hoop (H, ∗, →, 1) such that x ∗ y ≤ z ∗ y implies x ≤ z for each x, y, z ∈ H. The main example of cancellative hoop is ((0, 1], ·, →·, 1) where · is the usual product of real numbers and x →· y = 1 if x ≤ y y/x

  • therwise.
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Cancellative hoops

Definition

A cancellative hoop is a hoop (H, ∗, →, 1) such that x ∗ y ≤ z ∗ y implies x ≤ z for each x, y, z ∈ H. The main example of cancellative hoop is ((0, 1], ·, →·, 1) where · is the usual product of real numbers and x →· y = 1 if x ≤ y y/x

  • therwise.

The map h : x ∈ (0, 1] → (x + 1)/2 ∈ (1/2, 1] is a bijection and, so, h induces on (1/2, 1] a structure of cancellative hoop.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Disconnected rotation

Definition

Let (H, ·, →, 1) be a hoop and H− be a set disjoint from H, and let − be a bijection from H onto H−. We denote by DR(H) the structure whose domain is H ∪ H−, whose constants are 1 and 0 = 1− and whose

  • perations ◦, ⇒ and ¬ are defined, for all x, y ∈ H by the following

clauses: x ◦ y =        x · y, if x, y ∈ H (x → y−)− if x ∈ H, y ∈ H− (y → x−)− if x ∈ H−, y ∈ H

  • therwise.

x ⇒ y =        x → y, if x, y ∈ H (x · y−)− if x ∈ H, y ∈ H− 1 if x ∈ H−, y ∈ H y− → x− if x, y ∈ H− This construction is called disconnected rotation.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Starting from cancellative hoops

The MV-algebra [0, 1](1/2) is, up to isomorphisms, the disconnected rotation of the standard cancellative hoop ((0, 1], ·, →, 1).

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Starting from cancellative hoops

The MV-algebra [0, 1](1/2) is, up to isomorphisms, the disconnected rotation of the standard cancellative hoop ((0, 1], ·, →, 1). In the paper [CigTor] a very general construction is given, that has as a particular case the construction of the algebras in the variety DLMV from cancellative hoops.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Starting from cancellative hoops

The MV-algebra [0, 1](1/2) is, up to isomorphisms, the disconnected rotation of the standard cancellative hoop ((0, 1], ·, →, 1). In the paper [CigTor] a very general construction is given, that has as a particular case the construction of the algebras in the variety DLMV from cancellative hoops. Another case of the same construction permits to obtain product algebras from cancellative hoops: Product standard algebra is given by the t-norm of product and its associated residuum x →· y = 1 if x ≤ y y/x

  • therwise.
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Starting from cancellative hoops

The MV-algebra [0, 1](1/2) is, up to isomorphisms, the disconnected rotation of the standard cancellative hoop ((0, 1], ·, →, 1). In the paper [CigTor] a very general construction is given, that has as a particular case the construction of the algebras in the variety DLMV from cancellative hoops. Another case of the same construction permits to obtain product algebras from cancellative hoops: Product standard algebra is given by the t-norm of product and its associated residuum x →· y = 1 if x ≤ y y/x

  • therwise.

It is easy to see that the product algebra ([0, 1], ·, →·, 0) can be obtained from the cancellative hoop ((0, 1], ·, →·, 1) by adding a bottom element and properly extending the operations.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free algebras

In this section we give an explicit functional description of the free algebra in the variety DLMV. It is know that

Theorem (CigTor)

Fn

DLMV ≃ 2n

  • i=1

DR(Fn

CH)

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free algebras

In this section we give an explicit functional description of the free algebra in the variety DLMV. It is know that

Theorem (CigTor)

Fn

DLMV ≃ 2n

  • i=1

DR(Fn

CH)

In order to give a [0, 1]-functional representation of Fn

DLMV, we are going

to use the fact that DLMV is generated by a disconnected rotation of the cancellative hoop (0, 1], together with resizing functions: β0 : x ∈ [0, 1/2) → 1 − 2x ∈ (0, 1], β1 : x ∈ (1/2, 1] → 2x − 1 ∈ (0, 1].

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free cancellative hoops

Definition

A monomial n-variate function on D ⊆ R is a function f : Dn → D such that f (x1, . . . , xn) = 1 ∧ (xm1

1

· . . . · xmn

n ) where mi ∈ Z, for each

i = 1, . . . , n. A piece-wise monomial function f on D ⊆ R is a continuous function f such that there exists a family {fm}m∈M of monomial functions and f =

p

  • q fpq.
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free cancellative hoops

Definition

A monomial n-variate function on D ⊆ R is a function f : Dn → D such that f (x1, . . . , xn) = 1 ∧ (xm1

1

· . . . · xmn

n ) where mi ∈ Z, for each

i = 1, . . . , n. A piece-wise monomial function f on D ⊆ R is a continuous function f such that there exists a family {fm}m∈M of monomial functions and f =

p

  • q fpq.

Theorem

The free cancellative hoop Fn

CH over n generators is the algebra of

functions from (0, 1]n → (0, 1] that are piecewise monomial.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free DLMV -algebras

Definition

For every b = (b1, . . . , bn) ∈ {0, 1}n consider Bb

i =

[0, 1/2) if bi = 0 (1/2, 1] if bi = 1 and let Db = Bb

1 × . . . × Bb n .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free DLMV -algebras

Definition

For every b = (b1, . . . , bn) ∈ {0, 1}n consider Bb

i =

[0, 1/2) if bi = 0 (1/2, 1] if bi = 1 and let Db = Bb

1 × . . . × Bb n .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Let β(Db) =

n

  • i=1

βi(Bb

i ) ⊆ (0, 1]n .

Theorem

Fn

DLMV is isomorphic to the MV-algebra of functions

f : [0, 1](1/2)

n → [0, 1](1/2)

such that, for every b ∈ {0, 1}n, there exists a piecewise monomial function pb : (0, 1]n → (0, 1] such that either f ↾ Db = β−1

  • pb ◦ β or

f ↾ Db = β−1

1

  • pb ◦ β,
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Let β(Db) =

n

  • i=1

βi(Bb

i ) ⊆ (0, 1]n .

Theorem

Fn

DLMV is isomorphic to the MV-algebra of functions

f : [0, 1](1/2)

n → [0, 1](1/2)

such that, for every b ∈ {0, 1}n, there exists a piecewise monomial function pb : (0, 1]n → (0, 1] such that either f ↾ Db = β−1

  • pb ◦ β or

f ↾ Db = β−1

1

  • pb ◦ β,

with operations defined pointwisely.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Example

This is an example for n = 1:

0.0 0.2 0.4 0.6 0.8 1.0 0.2 0.4 0.6 0.8 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Example

This is an example for n = 1:

0.0 0.2 0.4 0.6 0.8 1.0 0.2 0.4 0.6 0.8 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Adding 1/2 to [0, 1] \ {1/2}

We want now to extend the operation ⊙ to the operation ⊙JΠ defined on the whole interval [0, 1]: x ⊙JΠ y =            x ⊙y if x, y / ∈ S3 x ⊙3 y if x, y ∈ S3 x ⊙3 ⌈y⌉2 if x ∈ S3 \ {1}, y / ∈ S3 ⌈x⌉2 ⊙3 y if x / ∈ S3, y ∈ S3 \ {1} where ⊙ is the conjunction of [0, 1](1/2), S3 is the MV-chain {0, 1/2, 1}, ⊙3 is the conjunction in S3 and for each x ∈ [0, 1], ⌈x⌉2 =      if x = 0 1/2 if 0 < x ≤ 1/2 1 if 1/2 < x ≤ 1

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Rotation of product t-norm

Definition

Let T be a left continuous t-norm without zero divisors and T1 the linear trasformation of T into [1/2, 1]. Define TJ : [0, 1]2 → [0, 1] by TJ(x, y) =            T1(x, y) if x, y > 1/2 ¬IT1(x, ¬y) if x > 1/2, y ≤ 1/2 ¬IT1(y, ¬x) if x ≤ 1/2, y > 1/2 if x, y ≤ 1/2 , where IT1(x, y) = sup{s ∈ [1/2, 1] | T1(x, s) ≤ y}. We call TJ the connected rotation of T.

Proposition

⊙JΠ is a left-continuous t-norm. In particular it is the connected rotation

  • f the product t-norm.
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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We can then consider the MTL-algebra [0, 1]JΠ = ([0, 1], ⊙JΠ, →JΠ, ∧, 0) (that actually is an IMTL-algebra). Note that [0, 1]JΠ is not an MV-algebra.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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We can then consider the MTL-algebra [0, 1]JΠ = ([0, 1], ⊙JΠ, →JΠ, ∧, 0) (that actually is an IMTL-algebra). Note that [0, 1]JΠ is not an MV-algebra. We further have [0, 1]JΠ is the connected rotation of the cancellative hoop ((0, 1], ·, →·, 1).

Definition

Let JΠ denote the variety of IMTL-algebras generated by ([0, 1], ⊙JΠ, →JΠ, ∧, 0).

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free algebras in JΠ

Theorem

Fn

JΠ ∼

= DR(Fn

CH)2n × n−1

  • j=1

(CR(Fi

CH))2i(n

i)

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Free algebras in JΠ

Theorem

Fn

JΠ ∼

= DR(Fn

CH)2n × n−1

  • j=1

(CR(Fi

CH))2i(n

i)

Definition

For every b = (b1, . . . , bn) ∈ {0, 1/2, 1}n consider Bb

i =

   [0, 1/2) if bj = 0 (1/2, 1] if bj = 1 {1/2} if bj = 1/2 and let Db = Bb

1 × . . . × Bb n .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Functional description of Fn

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Functional description of Fn

We define β(Db) =

  • i∈Ib

βi(Bb

i ) ⊆ (0, 1]nb

where Ib = {i | bi = 1/2} and nb = |Ib|.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Let FJΠn be the set of functions f : [0, 1]n → [0, 1] such that, for every b ∈ {0, 1/2, 1}n, there exists a piecewise monomial function pb : (0, 1]nb → (0, 1] such that either f ↾ Db = β−1

  • pb ◦ β or

f ↾ Db = β−1

1

  • pb ◦ β or

(just in case nb < n) f ↾ Db = 1/2. The set FJΠn can be equipped with a structure of IMTL-algebra by extending componentwise the operations of [0, 1]JΠ.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Let FJΠn be the set of functions f : [0, 1]n → [0, 1] such that, for every b ∈ {0, 1/2, 1}n, there exists a piecewise monomial function pb : (0, 1]nb → (0, 1] such that either f ↾ Db = β−1

  • pb ◦ β or

f ↾ Db = β−1

1

  • pb ◦ β or

(just in case nb < n) f ↾ Db = 1/2. The set FJΠn can be equipped with a structure of IMTL-algebra by extending componentwise the operations of [0, 1]JΠ.

Theorem

Fn

JΠ is isomorphic to FJΠn.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Example

Example for n = 1:

0.0 0.2 0.4 0.6 0.8 1.0 0.2 0.4 0.6 0.8 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Example

Example for n = 2:

0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Example

Example for n = 2:

0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

Let B = [0, 1](1/2) C = {0, 1/2, 1} D = [0, 1]JΠ and note that B and C are MV-algebras, while D is not (we fix a common IMTL-language).

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

Let B = [0, 1](1/2) C = {0, 1/2, 1} D = [0, 1]JΠ and note that B and C are MV-algebras, while D is not (we fix a common IMTL-language). Then, from a direct inspection of the functions involved, we have the following result F1(V(B, C)) ∼ = F1(V(D)) . As a consequence, the two varieties cannot be distinguished by equations with one variable.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

Let B = [0, 1](1/2) C = {0, 1/2, 1} D = [0, 1]JΠ and note that B and C are MV-algebras, while D is not (we fix a common IMTL-language). Then, from a direct inspection of the functions involved, we have the following result F1(V(B, C)) ∼ = F1(V(D)) . As a consequence, the two varieties cannot be distinguished by equations with one variable. Hence, all one-variable equations holding for MV-algebras must also hold in D.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

Theorem

The variety of MV-algebras admits no one-variable axiomatisation from the variety of MTL-algebras.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

Theorem

The variety of MV-algebras admits no one-variable axiomatisation from the variety of MTL-algebras.

Corollary

The variety of BL-algebras admits no one-variable axiomatisation from the variety of MTL-algebras.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Axiomatising MV from IMTL

Theorem

The variety of MV-algebras admits no one-variable axiomatisation from the variety of MTL-algebras.

Corollary

The variety of BL-algebras admits no one-variable axiomatisation from the variety of MTL-algebras. The variety V(B, C) can be axiomatized with one-variable equations from the axioms defining MV-algebras; hence:

Proposition

MV ∩ V(D) = V(B, C) .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Categorical equivalences

Let us consider the categories Π, DLMV, JΠ and CH and their full subcategories of directly indecomposable objects.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Categorical equivalences

Let us consider the categories Π, DLMV, JΠ and CH and their full subcategories of directly indecomposable objects. Directly indecomposable algebras in Π are exactly cancellative hoops with an added bottom.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Categorical equivalences

Let us consider the categories Π, DLMV, JΠ and CH and their full subcategories of directly indecomposable objects. Directly indecomposable algebras in Π are exactly cancellative hoops with an added bottom. Directly indecomposable algebras in DLMV are exactly disconnected rotation of cancellative hoops.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Categorical equivalences

Let us consider the categories Π, DLMV, JΠ and CH and their full subcategories of directly indecomposable objects. Directly indecomposable algebras in Π are exactly cancellative hoops with an added bottom. Directly indecomposable algebras in DLMV are exactly disconnected rotation of cancellative hoops. Directly indecomposable algebras in JΠ are either disconnected or connected rotation of cancellative hoops.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Categorical equivalences: directly indecomposable

We can hence establish a categorical equivalence among the following categories: The categories of directly indecomposable Π algebras, directly indecomposable DLMV algebras and cancellative hoops are equivalent.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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Categorical equivalences: directly indecomposable

We can hence establish a categorical equivalence among the following categories: The categories of directly indecomposable Π algebras, directly indecomposable DLMV algebras and cancellative hoops are equivalent. We can then consider a category Π♭ whose objects are pairs (P, b)

  • f a Π-algebra P and an element b in the Boolean skeleton of P, and

whose arrows (P1, b1) → (P2, b2) are product algebras homomorphisms f : P1 → P2 such that f (b1) ≤ b2. Further, let Π♭

1 be the subcategory of Π♭ in which the product algebras are

directly indecomposable. Then:

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 56

Categorical equivalences: directly indecomposable

We can hence establish a categorical equivalence among the following categories: The categories of directly indecomposable Π algebras, directly indecomposable DLMV algebras and cancellative hoops are equivalent. We can then consider a category Π♭ whose objects are pairs (P, b)

  • f a Π-algebra P and an element b in the Boolean skeleton of P, and

whose arrows (P1, b1) → (P2, b2) are product algebras homomorphisms f : P1 → P2 such that f (b1) ≤ b2. Further, let Π♭

1 be the subcategory of Π♭ in which the product algebras are

directly indecomposable. Then: The category of directly indecomposable JΠ algebras is equivalent to Π♭

1.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 57

Categorical equivalences: finitely presented

Finitely presented algebras are direct product of finitely many directly indecomposable algebras, hence we have: The category of finitely presented DLMV algebras is equivalent to the category of finitely presented Π algebras.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 58

Categorical equivalences: finitely presented

Finitely presented algebras are direct product of finitely many directly indecomposable algebras, hence we have: The category of finitely presented DLMV algebras is equivalent to the category of finitely presented Π algebras. Further, let Π♭

2 be the subcategory of Π♭ in which the product algebras are

finitely presented. The category of finitely presented JΠ algebras is equivalent to Π♭

2.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 59

Generalising

Let us fix some notation: we set Sω

n

= Γ(Z lex Z, (n − 1, 0)) , Sc

n

= Γ(Z lex R, (n − 1, 0)) , Sn = Γ(Z, n − 1) .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 60

Generalising

Let us fix some notation: we set Sω

n

= Γ(Z lex Z, (n − 1, 0)) , Sc

n

= Γ(Z lex R, (n − 1, 0)) , Sn = Γ(Z, n − 1) . Note that Sn ∼ = Ln =

  • 0,

1 n − 1, 2 n − 1 . . . , n − 2 n − 1, 1

  • .
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 61

Generalising

Let us fix some notation: we set Sω

n

= Γ(Z lex Z, (n − 1, 0)) , Sc

n

= Γ(Z lex R, (n − 1, 0)) , Sn = Γ(Z, n − 1) . Note that Sn ∼ = Ln =

  • 0,

1 n − 1, 2 n − 1 . . . , n − 2 n − 1, 1

  • .

For each integer n > 1, we can find an MV-chain Lc

n with universe

[0, 1] \ 1 n, 2 n . . . , n − 2 n

  • such that

n ⊆ Sc n ∼

= Lc

n .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 62

Left-continuous t-norms ⊙∗

n

Clearly, [0, 1] = Lc

n ∪ Ln+1.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 63

Left-continuous t-norms ⊙∗

n

Clearly, [0, 1] = Lc

n ∪ Ln+1.

We can define for each integer n > 1 the operation ⊙∗

n setting, for every

x, y ∈ [0, 1]: x ⊙∗

n y =

           x ⊙c

n y

if x, y / ∈ Ln+1 x ⊙n+1 y if x, y ∈ Ln+1 x ⊙n+1 ⌈y⌉n+1 if x ∈ Ln+1, y / ∈ Ln+1 ⌈x⌉n+1 ⊙n+1 y if x / ∈ Ln+1, y ∈ Ln+1 where ⊙c

n is the monoidal conjunction of Lc n, ⊙n+1 is the monoidal

conjunction of Ln+1 and for each x ∈ [0, 1], ⌈x⌉n+1 is the smallest element

  • f Ln+1 greater or equal to x.
  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 64

Left-continuous t-norms ⊙∗

n

Clearly, [0, 1] = Lc

n ∪ Ln+1.

We can define for each integer n > 1 the operation ⊙∗

n setting, for every

x, y ∈ [0, 1]: x ⊙∗

n y =

           x ⊙c

n y

if x, y / ∈ Ln+1 x ⊙n+1 y if x, y ∈ Ln+1 x ⊙n+1 ⌈y⌉n+1 if x ∈ Ln+1, y / ∈ Ln+1 ⌈x⌉n+1 ⊙n+1 y if x / ∈ Ln+1, y ∈ Ln+1 where ⊙c

n is the monoidal conjunction of Lc n, ⊙n+1 is the monoidal

conjunction of Ln+1 and for each x ∈ [0, 1], ⌈x⌉n+1 is the smallest element

  • f Ln+1 greater or equal to x.

⊙∗

n is a left-continuous t-norm.

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 65

This is an example for n = 3:

0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 66

This is an example for n = 4:

0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 67

This is an example for n = 5:

0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 68

This is an example for n = 20:

0.0 0.5 1.0 0.0 0.5 1.0 0.0 0.5 1.0

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 69

We obtain an IMTL-algebra ([0, 1], ⊙c

n, →c n, ∧, 0).

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 70

We obtain an IMTL-algebra ([0, 1], ⊙c

n, →c n, ∧, 0).

Note that, for each n > 1, F1(V([0, 1], ⊙c

n, →c n, ∧, 0)) ∼

= F1(V(Sω

n , Sn+1)),

and MV ∩ V([0, 1], ⊙c

n, →c n, ∧, 0)) = V(Sω n , Sn+1) .

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 71

We obtain an IMTL-algebra ([0, 1], ⊙c

n, →c n, ∧, 0).

Note that, for each n > 1, F1(V([0, 1], ⊙c

n, →c n, ∧, 0)) ∼

= F1(V(Sω

n , Sn+1)),

and MV ∩ V([0, 1], ⊙c

n, →c n, ∧, 0)) = V(Sω n , Sn+1) .

Theorem

Given a subvariety of MV-algebras V, if there exists a standard IMTL-algebra L such that: F1(V) ∼ = F1(V(L)) then either V = MV (and the L is the standard MV-algebra) or there is n such that V = V(Sω

n , Sn+1).

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains

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SLIDE 72

References

  • S. Aguzzoli, S. Bova, B. Gerla: Free Algebras and Functional Representation for

Fuzzy Logics, Chapter IX of Handbook of Mathematical Fuzzy Logic - Volume 2.

  • P. Cintula, P. H´

ajek, C. Noguera Eds., Studies in Logic, vol. 38, College Publications, London, pp. 713-791, 2011.

  • S. Aguzzoli, A.R. Ferraioli, B. Gerla: A note on minimal axiomatisations of some

extensions of MTL, Fuzzy Sets and Systems, to appear.

  • R. Cignoli, A. Torrens: Free Algebras in Varieties of Glivenko MTL-algebras

Satisfying the Equation 2(x2) = (2x)2. Studia Logica 83(1-3): 157-181 (2006)

  • S. Jenei: Structure of left-continuous triangular norms with strong induced
  • negations. (III) Construction and decomposition, Fuzzy Sets and Systems, 128

(2002) 197-208.

  • C. Noguera: Algebraic study of axiomatic extensions of triangular norm based fuzzy

logics, Monografies de l’Institut d’Investigaci en Intelligncia Artificial vol. 27, Barcelona, 2007.

  • G. Panti: Varieties of MV-algebras. Journal of Applied Non-Classical Logics 9(1):

141-157 (1999)

  • B. Gerla (DiSTA)

Involutive left-continuous t-norms arising from completion of MV-chains