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
A shorter Austin law of order \(6\) was established in [ 5 ] :
Definition 2.56 is an Austin law.
First we show that every finite model of Definition 2.56 is trivial. Write \(y^2 := y \diamond y\) and \(y^3 := y^2 \diamond y\). For any \(y,z\), introduce the functions \({f_y: x \mapsto y^3 \diamond x}\) and \({g_{yz}: x \mapsto x \diamond (y^2 \diamond z)}\). Definition 2.56 says that \(g_{yz}(f_y(x))=x\), hence by finiteness \(g_{yz}=f_y^{-1}\), showing that \(g_{yz}\) does not depend on the value of \(z\). Since
it follows that \(f_y(y^2 \diamond z)=f_y(y^3)\) which by injectivity of \(f_y\) implies that \(z\mapsto y^2 \diamond z\) is a constant function (with \(y\) fixed). Substituting \(y^2\) for \(y\) shows that the same is true for \(z\mapsto (y^2 \diamond y^2) \diamond z\), and since
we conclude that \(f_y\) is also a constant function. But this function is already known to be injective, thus there do not exist distinct elements in its domain, showing that the model must be trivial.
To construct an infinite model, consider the magma of positive integers \(\mathbb {Z}^+\) with the operation \(x \diamond y\) defined by
Then \(y \diamond y = 2^y\) and \((y \diamond y) \diamond y = 1\) for all \(y\). If \(x\neq 1\) we have that
and since \((y \diamond y) \diamond z\) is a power of two for all \(y, z\) it follows that
The case \(x=1\) requires a further argument: observe that \(w = (y \diamond y) \diamond z\) evaluates to one unless \(z = 2^y\), in which case it evaluates to \(2^{2^y}\) (which is greater than or equal to four). In particular, \(w\) never takes the value two. Thus
concluding our proof that this magma is a model of Definition 2.56
An even shorter law (order \(5\)) was obtained by the same author in a follow-up paper [ 4 ] :
Definition 2.54 is an Austin law.
Using the \(y^2\) and \(y^3\) notation as before, the law reads
In particular, for any \(y\), the map \(T_y \colon x \mapsto y^3 \diamond x\) is injective, hence bijective in a finite model \(G\). In particular we can find a function \(f : G \to G\) such that \(T_y f(y) = y^3\) for all \(y\) Applying Equation 5 with \(x = f(y)\), we conclude
and thus \(y \diamond z\) is independent of \(z\) by injectivity of \(T_y\). Thus, the left-hand side of Equation 5 does not depend on \(x\), and so the model is trivial. This shows there are no non-trivial finite models.
To establish an infinite model, use \(\mathbb {N}\) with \(x \diamond y\) defined by requiring
and
for \(x \neq 3^y\), and
for \(z \neq 3^y 5^x\). Finally set
for \(z \neq 3^y, 2^{3^y}\). All other assignments of \(\diamond \) may be made arbitrarily. It is then a routine matter to establish Equation 5.
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 [ 4 ] :
Definition 2.52 has no non-trivial finite models.
From Definition 2.52 we see that the map \(w \mapsto y \diamond w\) is onto, hence injective in a finite model. Using this injectivity four times in Definition 2.52, we see that \(z \diamond y\) does not depend on \(z\), hence the expression \(x \diamond (z \diamond y)\) does not depend on \(x\). By Definition 2.52 again, this means that \(x\) does not depend on \(x\), which is absurd in a non-trivial model.
We also have such a non-implication involving two laws of order \(4\):
All finite magmas which satisfy Definition 2.44 also satisfy Definition 2.41.
For a finite magma \(M\), consider the set \(S = \{ x \diamond y | x, y \in M\} \). Now \(f_z : x \mapsto z \diamond x\) and \(g_z : x \mapsto x \diamond z\). They both map \(S\) to \(S\), and due to the hypothesis \(g_z \diamond f_z\) is the identity on \(S\), so because \(S\) is finite \(f_z\) and \(g_z\) must be inverse bijections on it, and therefore they commute.
There exists a magma which satisfies Definition 2.44 and not Definition 2.41.
Consider \(\mathbb {N}\), with \(x \diamond y\) defined as \(x \oplus y\) (bitwise XOR) if \(x\) and \(y\) are even, \(y+2\) if only \(y\) is even, \(x \dot- 2\) if only \(x\) is even, and \(0\) if both are odd. Note that the range of the operation is the set of even naturals. Definition 2.44 is satisfied, because for even \(z\) we get \(z \oplus (x \diamond y) \oplus z = x \diamond y\) and for odd \(z\) we get \((x \diamond y) + 2 \dot- 2 = x \diamond y\). Setting \(x = y = z = 1\), Definition 2.41 isn’t satisfied.
The following result was established in [ 2 ] :
Any law with at most two variables has a non-trivial finite model.
If neither side of the law is a single variable then the zero law \(x \diamond y = 0\) will work, so one can assume the law takes the form \(x = f(x,y)\). Consider a finite field \(F\) with the operation \(x \diamond y := ax+by\) for some coefficients \(a,b \in F\). Then the law becomes a pair of equations \(P(a,b)=0\), \(Q(a,b)=1\) in the coefficients for some polynomials \(P,Q\) with integer coefficients, which one can verify to not divide each other (they have the same degree, and do not have the same set of non-zero monomials). From Bezout’s theorem, this equation has a solution in some field, and hence by the Lefschetz principle it has a solution in a finite field.
Many implications for finite magmas rely on the fact that if \(f, g:X \to X\) are functions on a finite set \(X\), then \(f \circ g = I\) if and only if \(g \circ f = I\). Two more complicated variants of this are as follows.
Let \(X\) be finite, and let \(f, g: X \to X\) be such that \(f = f \circ f \circ g\). Then \(f = f \circ g \circ f\).
Call a point \(x \in X\) periodic if \(f^n(x) = x\) for some \(n{\gt}0\). Because the forward orbit \(x, f(x), f^2(x), \dots \) in a finite space \(X\) must repeat, we see that for each \(x\) there exists an \(n\) such that \(f^n(x)\) is periodic. Let \(n_x\) be the first \(n\) for which this occurs. If \(n_x {\gt} 1\), then \(g(x), f(g(x)), f(f(g(x))\) cannot be periodic (as this would imply \(f(x)\) periodic), and then we can see that \(n_{g(x)} = n_x + 1\). Hence the maximal value of \(n_x\) is at most \(1\), which implies that \(f(x)\) is periodic for every \(x\). Thus there is an \(n {\gt} 1\) such that \(f^n = f\). Since \(f = f^2 \circ g\), we have \(f^n = f^{n-2} \circ f \circ f = f^{n-2} \circ (f^2 \circ g) \circ f = f^n \circ g \circ f = f \circ g \circ f\), as desired.
Let \(X\) be finite, and let \(f, g: X \to X\) be such that \(f = g \circ f \circ f\). Then \(f = f \circ g \circ f\).
By hypothesis, \(f^2(x)\) uniquely determines \(f(x)\). This prevents \(n_x = 2\) for any \(x\) (because if \(n{\gt}2\) is such that \(f^{n+2}(x) = f^2(x)\), then \(f^{n+1}(x) \neq f(x)\)), and hence also prevents \(n_x {\gt} 2\) for any \(x\). So again we have \(f(x)\) periodic for all \(x\), so \(f^n = f\) for some \(n{\gt}1\). Then \(f = f^n = f \circ (g \circ f^2) \circ f^{n-2} = f \circ g \circ f^n = f \circ g \circ f\) as required.
This can be used to obtain a few positive finite magma implications.