Equational Theories

3 Infinite models

In this chapter we consider non-implications which are refuted only on infinite models, as those are more challenging to prove—they can’t be proved by directly giving an operation table and checking which laws it satisfies.

The singleton or empty magma obeys all equational laws. One can ask whether an equational law admits nontrivial finite or infinite models. An Austin law is a law which admits infinite models, but no nontrivial finite models. Austin [ 1 ] established the first such law, namely the order 9 law

(((11)1)0)(((11)((11)1))2)0.

A shorter Austin law of order 6 was established in [ 6 ] :

Theorem 3.1 Kisielewicz’s first Austin law

Definition 2.56 is an Austin law.

Proof

An even shorter law (order 5) was obtained by the same author in a follow-up paper [ 5 ] :

Theorem 3.2 Kisielewicz’s second Austin law

Definition 2.54 is an Austin law.

Proof

In that paper a computer search was also used to show that no law of order four or less is an Austin law.

An open question is whether Definition 2.52 is an Austin law. We have the following partial result from [ 5 ] :

Theorem 3.3 Equation 5093 has no non-trivial finite models

Definition 2.52 has no non-trivial finite models.

Proof

We also have such a non-implication involving two laws of order 4:

Theorem 3.4 3994 implies 3588 for finite models

All finite magmas which satisfy Definition 2.44 also satisfy Definition 2.41.

Proof
Theorem 3.5 3994 does not imply 3588 for infinite models

There exists a magma which satisfies Definition 2.44 and not Definition 2.41.

Proof

The following result was established in [ 2 ] :

Theorem 3.6 Austin’s finite model theorem
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Any law with at most two variables has a non-trivial finite model.

Proof

Many implications for finite magmas rely on the fact that if f,g:XX are functions on a finite set X, then fg=I if and only if gf=I. Two more complicated variants of this are as follows.

Lemma 3.7
#

Let X be finite, and let f,g:XX be such that f=ffg. Then f=fgf.

Proof
Lemma 3.8
#

Let X be finite, and let f,g:XX be such that f=gff. Then f=fgf.

Proof

This can be used to obtain a few positive finite magma implications, for instance by setting f,g to be left and right multiplication operators. Another useful lemma is

Lemma 3.9 Eventual period

Let X be finite and f:XX. Then there exists n1 such that f2n=fn.

Proof

As a sample application, we have

On a finite magma M, equation 3342, xy=y(x(xx)), implies equation 3522, xy=x((yy)y), as well as equation 4118, xy=((xx)x)y.

Proof
Proposition 3.11 1167 implies 1096

For finite magmas, Equation 1167,

x=y((z(yy))x)

implies Equation 1096,

x=y((x(zy))x).
Proof
Proposition 3.12 1133 implies 1167

For finite magmas, Equation 1133,

x=y((y(zy))x)

implies Equation 1167,

x=y((z(yy))x).
Proof
Proposition 3.13 1441 implies 4067, 1443 implies 3055

For finite magmas, Equation 1441,

x=(xy)(x(xx))

implies Equation 4067,

xx=((xx)y)x,

and equation 1443,

x=(xy)(x(xz))

implies Equation 3055,

x=(((xx)y)x)x.
Proof
Proposition 3.14 1681 implies 3877, 1701 implies 1035

For finite magmas, Equation 1681,

x=(yx)((xx)x)

implies Equation 3877,

xx=(y(xx))x,

and Equation 1701,

x=(yx)((zx)x)

implies Equation 1035,

x=x((y(xx))x).
Proof