In the branch of mathematics known as integration theory, the McShane integral, created by Edward J. McShane,[1] is a modification of the Henstock-Kurzweil integral.[2] The McShane integral is equivalent to the Lebesgue integral.[3]
Given a closed interval of the real line, a free tagged partition
P
[a,b]
\{(ti,[ai-1,ai]):1\leqi\leqn\}
where
a=a0<a1<...<an=b
and each tag
ti\in[a,b]
The fact that the tags are allowed to be outside the subintervals is why the partition is called free. It's also the only difference between the definitions of the Henstock-Kurzweil integral and the McShane integral.
For a function
f:[a,b]\toR
P
S(f,P)=
n | |
\sum | |
i=1 |
f(ti)(ai-ai-1).
A positive function
\delta:[a,b]\to(0,+infty)
We say that a free tagged partition
P
\delta
i=1,2,...,n,
[ai-1,ai]\subseteq[ti-\delta(ti),ti+\delta(ti)].
Intuitively, the gauge controls the widths of the subintervals. Like with the Henstock-Kurzweil integral, this provides flexibility (especially near problematic points) not given by the Riemann integral.
The value
b | |
\int | |
a |
f
f:[a,b]\toR
\varepsilon>0
\delta
\delta
P
[a,b]
\left
bf | |
|\int | |
a |
-S(f,P)\right|<\varepsilon.
It's clear that if a function
f:[a,b]\toR
f
In order to illustrate the above definition we analyse the McShane integrability of the functions described in the following examples, which are already known as Henstock-Kurzweil integrable (see the paragraph 3 of the site of this Wikipedia "Henstock-Kurzweil integral").
Let
f:[a,b]\toR
f(a)=f(b)=0
[a,b]
(a,[x | |
ij-1 |
,x | |
ij |
])
j=1,...,λ
(b,[x | |
ik-1 |
,x | |
ik |
])
k=1,...,\mu
(t | |
ir |
,[x | |
ir-1 |
,x | |
ir |
])
r=1,...,\nu
t | |
ir |
\in]a,b[
(λ+\mu+\nu=n).
This way, we have the Riemann sum
S(f,P)=
\nu | |
\sum | |
r=1 |
\displaystyle(x | |
ir |
-x | |
ir-1 |
)
and by consequence
λ | |
|S(P,f)-(b-a)|=style\sum | |
j=1 |
\displaystyle(x | |
ij |
-x | |
ij-1 |
\mu | |
)+style\sum | |
k=1 |
\displaystyle(x | |
ik |
-x | |
ik-1 |
).
Therefore if
P
\delta
[x | |
ij-1 |
,x | |
ij |
]\subset[a-\delta(a),a+\delta(a)]
j=1,...,λ
[x | |
ik-1 |
,x | |
ik |
]\subset[b-\delta(b),b+\delta(b)]
k=1,...,\mu
Since each one of those intervals do not overlap the interior of all the remaining, we obtain
|S(P,f)-(b-a)|<2\delta(a)+2\delta(b)=
\varepsilon | + | |
2 |
\varepsilon | |
2 |
=\varepsilon.
Thus
f
b | |
\int | |
a |
f=b-a.
The next example proves the existence of a distinction between Riemann and McShane integrals.
Let
d:[a,b] → R
d(x)=\begin{cases}1,&ifxisrational,\\0,&ifxisirrational,\end{cases}
which one knows to be not Riemann integrable. We will show that
d
Denoting by
\{r1,r2,...,rn,...\}
[a,b]
\varepsilon>0
\delta(x)=\begin{cases}\varepsilon2-n-1,&ifx=rnandn=1,2,...,\\1,&ifxisirrational.\end{cases}
For any
\delta
P=\{(ti,[xi-1,xi]):i=1,...,n\}
n | |
S(P,f)=style\sum | |
i=1 |
\displaystylef(ti)(xi-xi-1)
Taking into account that
f(ti)=0
ti
P
(ti,[xi-1,xi])
ti
(rk,[x
i1-1 |
,x | |
i1 |
]),...,(rk,[x
ik-1 |
,x | |
ik |
])
[x | |
ij-1 |
,x | |
ij |
]\subset[rk-\delta(rk),rk+\delta(rk)]
j=1,...,k.
.
Thus , which proves that the Dirichlet's function is McShane integrable and that
b | |
\int | |
a |
d=0.
For real functions defined on an interval
[a,b]
f
[a,b]
f
[a,b]
f
[a,c]
[c,b]
f
[a,b]
f
[a,b]
f
[a,b]
f
[a,b]
f
[a,b]
\phi:[a,b] → [\alpha,\beta]
f:[\alpha,\beta] → R
[\alpha,\beta]
[a,b]
f
[a,b]
kf
[a,b]
k\inR
f
g
[a,b]
f+g
[a,b]
f\leqg
\left[a,b\right]
With respect to the integrals mentioned above, the proofs of these properties are identical excepting slight variations inherent to the differences of the correspondent definitions (see Washek Pfeffer[4] [Sec. 6.1]).
This way a certain parallelism between the two integrals is observed. However an imperceptible rupture occurs when other properties are analysed, such as the absolute integrability and the integrability of the derivatives of integrable differentiable functions.
On this matter the following theorems hold (see [Prop.2.2.3 e Th. 6.1.2]).
If
f:[a,b] → R
[a,b]
|f|
[a,b]
If is differentiable on
[a,b]
[a,b]
In order to illustrate these theorems we analyse the following example based upon Example 2.4.12.
Let's consider the function:
F(x)=\begin{cases}x2\cos(\pi/x2),&ifx ≠ 0,\ 0,&ifx=0.\end{cases}
F
x ≠ 0
x=0
Moreover
As the function
h(x)=\begin{cases}2x\cos(\pi/x2),&ifx ≠ 0,\ 0,&ifx=0,\end{cases}
is continuous and, by the Theorem 2, the function
F'(x)
[0,1],
But the function
is not integrable on
[0,1]
In fact, otherwise, denoting by anyone of such integrals, we should have necessarily for any positive integer
n
\int1/\sqrt{n
\geq | 1 |
2 |
| ||||
\sum | ||||
k=2 |
k | |
\int | |
k-1 |
|\sin(\pit)|dt=
1 | |
\pi |
| ||||
\sum | ||||
k=2 |
As
n
From this example we are able to conclude the following relevant consequences:
g0
g
F'
g0
g
F'
The more surprising result of the McShane integral is stated in the following theorem, already announced in the introduction.
Let
f:[a,b] → R
f
\Leftrightarrow
f
The correspondent integrals coincide.
This fact enables to conclude that with the McShane integral one formulates a kind of unification of the integration theory around Riemann sums, which, after all, constitute the origin of that theory.
So far is not known an immediate proof of such theorem.
In Washek Pfeffer [Ch. 4] it is stated through the development of the theory of McShane integral, including measure theory, in relationship with already known properties of Lebesgue integral. In Charles Swartz[5] that same equivalence is proved in Appendix 4.
Furtherly to the book by Russel Gordon [Ch. 10], on this subject we call the attention of the reader also to the works by Robert McLeod[6] [Ch. 8] and Douglas Kurtz together with Charles W. Swartz.
Another perspective of the McShane integral is that it can be looked as new formulation of the Lebesgue integral without using Measure Theory, as alternative to the courses of Frigyes Riesz and Bela Sz. Nagy[7] [Ch.II] or Serge Lang[8] [Ch.X, §4 Appendix] (see also[9]).