Standard part function

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In non-standard analysis, the standard part function is a function from the limited (finite) hyperreal numbers to the real numbers. Briefly, the standard part function "rounds off" a finite hyperreal to the nearest real. It associates to every such hyperreal x, the unique real x_0 infinitely close to it, i.e. x-x_0 is infinitesimal. As such, it is a mathematical implementation of the historical concept of adequality introduced by Pierre de Fermat,[1] as well as Leibniz's Transcendental law of homogeneity.

It can also be thought of as a mathematical implementation of Leibniz's Transcendental Law of Homogeneity. The standard part function was first defined by Abraham Robinson who used the notation {}^{\circ}x for the standard part of a hyperreal x (see Robinson 1974). This concept plays a key role in defining the concepts of the calculus, such as the derivative and the integral, in non-standard analysis. The latter theory is a rigorous formalisation of calculations with infinitesimals. The standard part of x is sometimes referred to as its shadow.

Definition[edit]

The standard part function "rounds off" a finite hyperreal to the nearest real number. The "infinitesimal microscope" is used to view an infinitesimal neighborhood of a standard real.

Nonstandard analysis deals primarily with the pair \mathbb{R}\subset{}^{\ast}\mathbb{R}, where the hyperreals {}^{\ast}\mathbb{R} are an ordered field extension of the reals \mathbb{R}, and contain infinitesimals, in addition to the reals. In the hyperreal line every real number has a collection of numbers (called a monad, or halo) of hyperreals infinitely close to it. The standard part function associates to a finite hyperreal x, the unique standard real number x0 which is infinitely close to it. The relationship is expressed symbolically by writing

\,\mathrm{st}(x)=x_0.

The standard part of any infinitesimal is 0. Thus if N is an infinite hypernatural, then 1/N is infinitesimal, and st(1/N) = 0.

If a hyperreal u is represented by a Cauchy sequence \langle u_n:n\in\mathbb{N} \rangle in the ultrapower construction, then

\text{st}(u)=\lim_{n\to\infty}u_n.

Not internal[edit]

The standard part function "st" is not defined by an internal set. There are several ways of explaining this. Perhaps the simplest is that its domain L, which is the collection of limited (i.e. finite) hyperreals, is not an internal set. Namely, since L is bounded (by any infinite hypernatural, for instance), L would have to have a least upper bound if L were internal, but L doesn't have a least upper bound. Alternatively, the range of "st" is \mathbb{R}\subset {}^*\mathbb{R} which is not internal; in fact every internal set in {}^\ast\mathbb{R} which is a subset of \mathbb{R} is necessarily finite, see (Goldblatt, 1998).

Applications[edit]

The standard part function is used to define the derivative of a function f. If f is a real function, and h is infinitesimal, and if f′(x) exists, then

f'(x) = \operatorname{st}\left(\frac {f(x+h)-f(x)}h\right).

Alternatively, if y=f(x), one takes an infinitesimal increment \Delta x, and computes the corresponding \Delta y=f(x+\Delta x)-f(x). One forms the ratio \frac{\Delta y}{\Delta x}. The derivative is then defined as the standard part of the ratio:

\frac{dy}{dx}=\text{st}\left( \frac{\Delta y}{\Delta x}  \right).

See also[edit]

Notes[edit]

  1. ^ Karin Usadi Katz and Mikhail G. Katz (2011) A Burgessian Critique of Nominalistic Tendencies in Contemporary Mathematics and its Historiography. Foundations of Science. doi:10.1007/s10699-011-9223-1 [1] See arxiv. The authors refer to the Fermat-Robinson standard part.

References[edit]