Extension by definitions explained

In mathematical logic, more specifically in the proof theory of first-order theories, extensions by definitions formalize the introduction of new symbols by means of a definition. For example, it is common in naive set theory to introduce a symbol

\emptyset

for the set that has no member. In the formal setting of first-order theories, this can be done by adding to the theory a new constant

\emptyset

and the new axiom

\forallx(x\notin\emptyset)

, meaning "for all x, x is not a member of

\emptyset

". It can then be proved that doing so adds essentially nothing to the old theory, as should be expected from a definition. More precisely, the new theory is a conservative extension of the old one.

Definition of relation symbols

Let

T

be a first-order theory and

\phi(x1,...,xn)

a formula of

T

such that

x1

, ...,

xn

are distinct and include the variables free in

\phi(x1,...,xn)

. Form a new first-order theory

T'

from

T

by adding a new

n

-ary relation symbol

R

, the logical axioms featuring the symbol

R

and the new axiom

\forallx1...\forallxn(R(x1,...,xn)\leftrightarrow\phi(x1,...,xn))

,called the defining axiom of

R

.

If

\psi

is a formula of

T'

, let

\psi\ast

be the formula of

T

obtained from

\psi

by replacing any occurrence of

R(t1,...,tn)

by

\phi(t1,...,tn)

(changing the bound variables in

\phi

if necessary so that the variables occurring in the

ti

are not bound in

\phi(t1,...,tn)

). Then the following hold:

\psi\leftrightarrow\psi\ast

is provable in

T'

, and

T'

is a conservative extension of

T

.

The fact that

T'

is a conservative extension of

T

shows that the defining axiom of

R

cannot be used to prove new theorems. The formula

\psi\ast

is called a translation of

\psi

into

T

. Semantically, the formula

\psi\ast

has the same meaning as

\psi

, but the defined symbol

R

has been eliminated.

Definition of function symbols

Let

T

be a first-order theory (with equality) and

\phi(y,x1,...,xn)

a formula of

T

such that

y

,

x1

, ...,

xn

are distinct and include the variables free in

\phi(y,x1,...,xn)

. Assume that we can prove

\forallx1...\forallxn\exists!y\phi(y,x1,...,xn)

in

T

, i.e. for all

x1

, ...,

xn

, there exists a unique y such that

\phi(y,x1,...,xn)

. Form a new first-order theory

T'

from

T

by adding a new

n

-ary function symbol

f

, the logical axioms featuring the symbol

f

and the new axiom

\forallx1...\forallxn\phi(f(x1,...,xn),x1,...,xn)

,called the defining axiom of

f

.

Let

\psi

be any atomic formula of

T'

. We define formula

\psi\ast

of

T

recursively as follows. If the new symbol

f

does not occur in

\psi

, let

\psi\ast

be

\psi

. Otherwise, choose an occurrence of

f(t1,...,tn)

in

\psi

such that

f

does not occur in the terms

ti

, and let

\chi

be obtained from

\psi

by replacing that occurrence by a new variable

z

. Then since

f

occurs in

\chi

one less time than in

\psi

, the formula

\chi\ast

has already been defined, and we let

\psi\ast

be

\forallz(\phi(z,t1,...,t

\ast)
n)\chi
(changing the bound variables in

\phi

if necessary so that the variables occurring in the

ti

are not bound in

\phi(z,t1,...,tn)

). For a general formula

\psi

, the formula

\psi\ast

is formed by replacing every occurrence of an atomic subformula

\chi

by

\chi\ast

. Then the following hold:

\psi\leftrightarrow\psi\ast

is provable in

T'

, and

T'

is a conservative extension of

T

.

The formula

\psi\ast

is called a translation of

\psi

into

T

. As in the case of relation symbols, the formula

\psi\ast

has the same meaning as

\psi

, but the new symbol

f

has been eliminated.

The construction of this paragraph also works for constants, which can be viewed as 0-ary function symbols.

Extensions by definitions

A first-order theory

T'

obtained from

T

by successive introductions of relation symbols and function symbols as above is called an extension by definitions of

T

. Then

T'

is a conservative extension of

T

, and for any formula

\psi

of

T'

we can form a formula

\psi\ast

of

T

, called a translation of

\psi

into

T

, such that

\psi\leftrightarrow\psi\ast

is provable in

T'

. Such a formula is not unique, but any two of them can be proved to be equivalent in T.

In practice, an extension by definitions

T'

of T is not distinguished from the original theory T. In fact, the formulas of

T'

can be thought of as abbreviating their translations into T. The manipulation of these abbreviations as actual formulas is then justified by the fact that extensions by definitions are conservative.

Examples

=

(equality) and

\in

(membership) as its only primitive relation symbols, and no function symbols. In everyday mathematics, however, many other symbols are used such as the binary relation symbol

\subseteq

, the constant

\emptyset

, the unary function symbol P (the power set operation), etc. All of these symbols belong in fact to extensions by definitions of ZF.

T

be a first-order theory for groups in which the only primitive symbol is the binary product ×. In T, we can prove that there exists a unique element y such that x×y = y×x = x for every x. Therefore we can add to T a new constant e and the axiom

\forallx(x x e=xande x x=x)

,

and what we obtain is an extension by definitions

T'

of

T

. Then in

T'

we can prove that for every x, there exists a unique y such that x×y=y×x=e. Consequently, the first-order theory

T''

obtained from

T'

by adding a unary function symbol

f

and the axiom

\forallx(x x f(x)=eandf(x) x x=e)

is an extension by definitions of

T

. Usually,

f(x)

is denoted

x-1

.

See also

Bibliography