Weight function

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A weight function is a mathematical device used when performing a sum, integral, or average in order to give some elements more of a "weight" than others. They occur frequently in statistics and analysis, and are closely related to the concept of a measure. Weight functions can be constructed in both discrete and continuous settings.

Discrete weights

In the discrete setting, a weight function w: A \to {\Bbb R}^+ is a positive function defined on a discrete set A, which is typically finite or countable. The weight function w(a): = 1 corresponds to the unweighted situation in which all elements have equal weight. One can then use apply this weight to various concepts.

If

f: A \to {\Bbb R}

is a real-valued function, then the unweighted sum of f on A is

\sum_{a \in A} f(a);

but for a weight function

w: A \to {\Bbb R}^+,

the weighted sum is

\sum_{a \in A} f(a) w(a).

One common application of weighted sums arises in numerical integration.

If B is a finite subset of A, one can replace the unweighted cardinality |B| of B by the weighted cardinality

\sum_{a \in B} w(a).

If A is a finite non-empty set, one can replace the unweighted mean or average

\frac{1}{|A|} \sum_{a \in A} f(a)

by the weighted mean or weighted average

 \frac{\sum_{a \in A} f(a) w(a)}{\sum_{a \in A} w(a)}..

In this case only the relative weights are relevant. Weighted means are commonly used in statistics to compensate for the presence of bias.

The terminology weight function arises from mechanics: if one has a collection of n objects on a lever, with weights

w_1, \ldots, w_n

(where weight is now interpreted in the physical sense) and locations

x_1,\ldots,x_n,

then the lever will be in balance if the fulcrum of the lever is at the center of mass

\frac{\sum_{i=1}^n w_i x_i}{\sum_{i=1}^n w_i},

which is also the weighted average of the positions xi.

Continuous weights

In the continuous setting, a weight is a positive measure such as w(x) dx on some domain Ω, which is typically a subset of an Euclidean space {\Bbb R}^n, for instance Ω could be an interval [a,b]. Here dx is Lebesgue measure and w: \Omega \to \R^+ is a non-negative measurable function. In this context, the weight function w(x) is sometimes referred to as a density.

  1. If f: \Omega \to {\Bbb R} is a real-valued function, then the unweighted integral \int_\Omega f(x)\ dx can be generalized to the weighted integral \int_\Omega f(x)\ w(x) dx. Note that one may need to require f to be absolutely integrable with respect to the weight w(x) dx in order for this integral to be finite.
  2. If E is a subset of Ω, then the volume vol(E) of E can be generalized to the weighted volume  \int_E w(x)\ dx.
  3. If Ω has finite non-zero weighted volume, then we can replace the unweighted average \frac{1}{vol(\Omega)} \int_\Omega f(x)\ dx by the weighted average  \frac{\int_\Omega f(x)\ w(x) dx}{\int_\Omega w(x)\ dx}.
  4. If f: \Omega \to {\Bbb R} and g: \Omega \to {\Bbb R} are two functions, one can generalize the unweighted inner product \langle f, g \rangle := \int_\Omega f(x) g(x)\ dx to a weighted inner product \langle f, g \rangle := \int_\Omega f(x) g(x)\ w(x) dx. See the entry on Orthogonality for more details.
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