The notion of integration is one of fundamental importance in advanced analysis. The idea of integration is expanded so as to be applicable to sets more general than subsets of
. Interested readers may refer to the Wikibook Measure Theory. Here however, we will discuss two important generalizations of integration which are still applicable only to real valued functions.
Riemann-Stieltjes integral
The Riemann-Stieltjes integral (or Stieltjes integral) can be seen as an extention of the idea behind the Darboux integral
Upper and Lower sum
Let
Let
such that
is strictly increasing over
Let
be a partition over
, and let
The Upper Sum of
with respect to
and
is given by

where
is given as in the previous chapter.
The Lower Sum of
with respect to
and
is given by

where
is given as in the previous chapter.
Definition
Let
Let
such that
is strictly increasing over
We say that
is Riemann-Stieltjes integrable on
with respect to
if and only if

where the supremum and the infimum have been taken over the set of all partitions.
is said to be the integral of
on
with respect to
and is denoted as
or as
Observe that putting
, we get the Darboux integral, and hence, the Darboux integral is a special case of the Riemann-Stieltjes integral.
Henstock Kurtzweil integral
While calculating the Riemann integral, the "fineness" of a partition was measured by it norm. However, it turns out that the norm is a very crude measure for a partition. Thus, by introducing the clever notion of gauges, we can extend the idea of the Riemann integral to a larger class of functions. In fact, it turns out that this integral, called the Henstock-Kurtzweil integral (after Ralph Henstock and Jaroslav Kurzweil) or Generalised Riemann integral is more general than the Riemann-Stieltjes integral and several other integrals on real intervals.
Gauges
A Gauge is said to be a function
, that is, the range of
includes only positive reals.
A tagged partition
is said to be δ-fine for a gauge
if and only if for all
,
![{\displaystyle [x_{k-1},x_{k}]\subseteq {\big (}t_{k}-\delta (t_{k}),t_{k}+\delta (t_{k}){\big )}}](../_assets_/eb734a37dd21ce173a46342d1cc64c92/0b49a653383e1e166de2b48d14846c5db71ce7f6.svg)
Definition
Let
Let
Then,
is said to be Henstock-Kurtzweil integrable on
if and only if, for every
there exists a gauge
such that if
is a δ-fine partition of
, then
