# Hyperreal number

In mathematics, the system of **hyperreal numbers** is a way of treating infinite and infinitesimal (infinitely small but non-zero) quantities. The hyperreals, or **nonstandard reals**, ***R**, are an extension of the real numbers **R** that contains numbers greater than anything of the form

Such numbers are infinite, and their reciprocals are infinitesimals. The term "hyper-real" was introduced by Edwin Hewitt in 1948.^{[1]}

Concerns about the soundness of arguments involving infinitesimals date back to ancient Greek mathematics, with Archimedes replacing such proofs with ones using other techniques such as the method of exhaustion.^{[2]} In the 1960s, Abraham Robinson proved that the hyperreals were logically consistent if and only if the reals were. This put to rest the fear that any proof involving infinitesimals might be unsound, provided that they were manipulated according to the logical rules that Robinson delineated.

The idea of the hyperreal system is to extend the real numbers **R** to form a system ***R** that includes infinitesimal and infinite numbers, but without changing any of the elementary axioms of algebra. Any statement of the form "for any number x..." that is true for the reals is also true for the hyperreals. For example, the axiom that states "for any number *x*, *x* + 0 = *x*" still applies. The same is true for quantification over several numbers, e.g., "for any numbers *x* and *y*, *xy* = *yx*." This ability to carry over statements from the reals to the hyperreals is called the transfer principle. However, statements of the form "for any *set* of numbers *S* ..." may not carry over. The only properties that differ between the reals and the hyperreals are those that rely on quantification over sets, or other higher-level structures such as functions and relations, which are typically constructed out of sets. Each real set, function, and relation has its natural hyperreal extension, satisfying the same first-order properties. The kinds of logical sentences that obey this restriction on quantification are referred to as statements in first-order logic.

The transfer principle, however, does not mean that **R** and ***R** have identical behavior. For instance, in ***R** there exists an element *ω* such that

but there is no such number in **R**. (In other words, ***R** is not Archimedean.) This is possible because the nonexistence of *ω* cannot be expressed as a first-order statement.

Informal notations for non-real quantities have historically appeared in calculus in two contexts: as infinitesimals, like *dx*, and as the symbol ∞, used, for example, in limits of integration of improper integrals.

As an example of the transfer principle, the statement that for any nonzero number *x*, *2x* ≠ *x*, is true for the real numbers, and it is in the form required by the transfer principle, so it is also true for the hyperreal numbers. This shows that it is not possible to use a generic symbol such as ∞ for all the infinite quantities in the hyperreal system; infinite quantities differ in magnitude from other infinite quantities, and infinitesimals from other infinitesimals.

Similarly, the casual use of 1/0 = ∞ is invalid, since the transfer principle applies to the statement that division by zero is undefined. The rigorous counterpart of such a calculation would be that if ε is a non-zero infinitesimal, then 1/ε is infinite.

For any finite hyperreal number *x*, its standard part, st(*x*), is defined as the unique real number that differs from it only infinitesimally. The derivative of a function *y*(*x*) is defined not as *dy/dx* but as the standard part of the corresponding difference quotient.

For example, to find the derivative *f′*(*x*) of the function *f*(*x*) = *x*^{2}, let *dx* be a non-zero infinitesimal. Then,

The use of the standard part in the definition of the derivative is a rigorous alternative to the traditional practice of neglecting the square^{[citation needed]} of an infinitesimal quantity. Dual numbers are a number system based on this idea. After the third line of the differentiation above, the typical method from Newton through the 19th century would have been simply to discard the *dx*^{2} term. In the hyperreal system,
*dx*^{2} ≠ 0, since *dx* is nonzero, and the transfer principle can be applied to the statement that the square of any nonzero number is nonzero. However, the quantity *dx*^{2} is infinitesimally small compared to *dx*; that is, the hyperreal system contains a hierarchy of infinitesimal quantities.

One way of defining a definite integral in the hyperreal system is as the standard part of an infinite sum on a hyperfinite lattice defined as *a*, *a* + *dx*, *a* + *2dx*, ..., *a* + *ndx*, where *dx* is infinitesimal, *n* is an infinite hypernatural, and the lower and upper bounds of integration are *a* and *b* = *a* + *n* *dx.*^{[3]}

The hyperreals ***R** form an ordered field containing the reals **R** as a subfield. Unlike the reals, the hyperreals do not form a standard metric space, but by virtue of their order they carry an order topology.

The use of the definite article *the* in the phrase *the hyperreal numbers* is somewhat misleading in that there is not a unique ordered field that is referred to in most treatments.
However, a 2003 paper by Vladimir Kanovei and Saharon Shelah^{[4]} shows that there is a definable, countably saturated (meaning ω-saturated, but not, of course, countable) elementary extension of the reals, which therefore has a good claim to the title of *the* hyperreal numbers. Furthermore, the field obtained by the ultrapower construction from the space of all real sequences, is unique up to isomorphism if one assumes the continuum hypothesis.

The condition of being a hyperreal field is a stronger one than that of being a real closed field strictly containing **R**. It is also stronger than that of being a superreal field in the sense of Dales and Woodin.^{[5]}

The hyperreals can be developed either axiomatically or by more constructively oriented methods. The essence of the axiomatic approach is to assert (1) the existence of at least one infinitesimal number, and (2) the validity of the transfer principle. In the following subsection we give a detailed outline of a more constructive approach. This method allows one to construct the hyperreals if given a set-theoretic object called an ultrafilter, but the ultrafilter itself cannot be explicitly constructed.

When Newton and (more explicitly) Leibniz introduced differentials, they used infinitesimals and these were still regarded as useful by later mathematicians such as Euler and Cauchy. Nonetheless these concepts were from the beginning seen as suspect, notably by George Berkeley. Berkeley's criticism centered on a perceived shift in hypothesis in the definition of the derivative in terms of infinitesimals (or fluxions), where *dx* is assumed to be nonzero at the beginning of the calculation, and to vanish at its conclusion (see Ghosts of departed quantities for details). When in the 1800s calculus was put on a firm footing through the development of the (ε, δ)-definition of limit by Bolzano, Cauchy, Weierstrass, and others, infinitesimals were largely abandoned, though research in non-Archimedean fields continued (Ehrlich 2006).

However, in the 1960s Abraham Robinson showed how infinitely large and infinitesimal numbers can be rigorously defined and used to develop the field of nonstandard analysis.^{[6]} Robinson developed his theory nonconstructively, using model theory; however it is possible to proceed using only algebra and topology, and proving the transfer principle as a consequence of the definitions. In other words hyperreal numbers *per se*, aside from their use in nonstandard analysis, have no necessary relationship to model theory or first order logic, although they were discovered by the application of model theoretic techniques from logic. Hyper-real fields were in fact originally introduced by Hewitt (1948) by purely algebraic techniques, using an ultrapower construction.

We are going to construct a hyperreal field via sequences of reals.^{[7]} In fact we can add and multiply sequences componentwise; for example:

Comparing sequences is thus a delicate matter. We could, for example, try to define a relation between sequences in a componentwise fashion:

This is a total preorder and it turns into a total order if we agree not to distinguish between two sequences *a* and *b* if *a* ≤ *b* and *b* ≤ *a*. With this identification, the ordered field ***R** of hyperreals is constructed. From an algebraic point of view, *U* allows us to define a corresponding maximal ideal **I** in the commutative ring **A** (namely, the set of the sequences that vanish in some element of *U*), and then to define ***R** as **A**/**I**; as the quotient of a commutative ring by a maximal ideal, ***R** is a field. This is also notated **A**/*U*, directly in terms of the free ultrafilter *U*; the two are equivalent. The maximality of **I** follows from the possibility of, given a sequence *a*, constructing a sequence *b* inverting the non-null elements of *a* and not altering its null entries. If the set on which *a* vanishes is not in *U*, the product *ab* is identified with the number 1, and any ideal containing 1 must be *A*. In the resulting field, these *a* and *b* are inverses.

The field **A**/*U* is an ultrapower of **R**.
Since this field contains **R** it has cardinality at least that of the continuum. Since **A** has cardinality

One question we might ask is whether, if we had chosen a different free ultrafilter *V*, the quotient field **A**/*U* would be isomorphic as an ordered field to **A**/*V*. This question turns out to be equivalent to the continuum hypothesis; in ZFC with the continuum hypothesis we can prove this field is unique up to order isomorphism, and in ZFC with the negation of continuum hypothesis we can prove that there are non-order-isomorphic pairs of fields that are both countably indexed ultrapowers of the reals.

For more information about this method of construction, see ultraproduct.

The following is an intuitive way of understanding the hyperreal numbers. The approach taken here is very close to the one in the book by Goldblatt.^{[8]} Recall that the sequences converging to zero are sometimes called infinitely small. These are almost the infinitesimals in a sense; the true infinitesimals include certain classes of sequences that contain a sequence converging to zero.

Let us see where these classes come from. Consider first the sequences of real numbers. They form a ring, that is, one can multiply, add and subtract them, but not necessarily divide by a non-zero element. The real numbers are considered as the constant sequences, the sequence is zero if it is identically zero, that is, *a*_{n} = 0 for all *n*.

Any family of sets that satisfies (2–4) is called a filter (an example: the complements to the finite sets, it is called the Fréchet filter and it is used in the usual limit theory). If (1) also holds, U is called an ultrafilter (because you can add no more sets to it without breaking it). The only explicitly known example of an ultrafilter is the family of sets containing a given element (in our case, say, the number 10). Such ultrafilters are called trivial, and if we use it in our construction, we come back to the ordinary real numbers. Any ultrafilter containing a finite set is trivial. It is known that any filter can be extended to an ultrafilter, but the proof uses the axiom of choice. The existence of a nontrivial ultrafilter (the ultrafilter lemma) can be added as an extra axiom, as it is weaker than the axiom of choice.

Now if we take a nontrivial ultrafilter (which is an extension of the Fréchet filter) and do our construction, we get the hyperreal numbers as a result.

The map st is continuous with respect to the order topology on the finite hyperreals; in fact it is locally constant.

Suppose *X* is a Tychonoff space, also called a T_{3.5} space, and C(*X*) is the algebra of continuous real-valued functions on *X*. Suppose *M* is a maximal ideal in C(*X*). Then the factor algebra *A* = C(*X*)/*M* is a totally ordered field *F* containing the reals. If *F* strictly contains **R** then *M* is called a **hyperreal ideal** (terminology due to Hewitt (1948)) and *F* a **hyperreal field**. Note that no assumption is being made that the cardinality of *F* is greater than **R**; it can in fact have the same cardinality.

An important special case is where the topology on *X* is the discrete topology; in this case *X* can be identified with a cardinal number κ and C(*X*) with the real algebra **R**^{κ} of functions from κ to **R**. The hyperreal fields we obtain in this case are called ultrapowers of **R** and are identical to the ultrapowers constructed via free ultrafilters in model theory.