Liouville's theorem (complex analysis) explained
for which there exists a positive number
such that
for all
is constant. Equivalently, non-constant holomorphic functions on
have unbounded images.
The theorem is considerably improved by Picard's little theorem, which says that every entire function whose image omits two or more complex numbers must be constant.
Proof
This important theorem has several proofs.
A standard analytical proof uses the fact that holomorphic functions are analytic.
Another proof uses the mean value property of harmonic functions.
The proof can be adapted to the case where the harmonic function
is merely bounded above or below. See Harmonic function#Liouville's theorem.
Corollaries
Fundamental theorem of algebra
There is a short proof of the fundamental theorem of algebra based upon Liouville's theorem.[1]
No entire function dominates another entire function
A consequence of the theorem is that "genuinely different" entire functions cannot dominate each other, i.e. if
and
are entire, and
everywhere, then
for some complex number
. Consider that for
the theorem is trivial so we assume
. Consider the function
. It is enough to prove that
can be extended to an entire function, in which case the result follows by Liouville's theorem. The holomorphy of
is clear except at points in
. But since
is bounded and all the zeroes of
are isolated, any singularities must be removable. Thus
can be extended to an entire bounded function which by Liouville's theorem implies it is constant.
If f is less than or equal to a scalar times its input, then it is linear
Suppose that
is entire and
, for
. We can apply Cauchy's integral formula; we have that
d\zeta\right|\leq
| |f(\zeta)| |
\left|(\zeta-z)2\right| |
|d\zeta|\leq
| M|\zeta| | \left|d\zeta\right|= |
\left|(\zeta-z)2\right| |
where
is the value of the remaining integral. This shows that
is bounded and entire, so it must be constant, by Liouville's theorem. Integrating then shows that
is
affine and then, by referring back to the original inequality, we have that the constant term is zero.
Non-constant elliptic functions cannot be defined on the complex plane
cannot be
. Suppose it was. Then, if
and
are two periods of
such that
is not real, consider the
parallelogram
whose
vertices are 0,
,
, and
. Then the image of
is equal to
. Since
is
continuous and
is
compact,
is also compact and, therefore, it is bounded. So,
is constant.
cannot be
is what Liouville actually proved, in 1847, using the theory of elliptic functions. In fact, it was
Cauchy who proved Liouville's theorem.
Entire functions have dense images
If
is a non-constant entire function, then its image is
dense in
. This might seem to be a much stronger result than Liouville's theorem, but it is actually an easy corollary. If the image of
is not dense, then there is a complex number
and a real number
such that the open disk centered at
with radius
has no element of the image of
. Define
Then
is a bounded entire function, since for all
,
So,
is constant, and therefore
is constant.
On compact Riemann surfaces
Any holomorphic function on a compact Riemann surface is necessarily constant.[2]
Let
be holomorphic on a compact Riemann surface
. By compactness, there is a point
where
attains its maximum. Then we can find a chart from a neighborhood of
to the unit disk
such that
is holomorphic on the unit disk and has a maximum at
, so it is constant, by the
maximum modulus principle.
Remarks
Let
be the one-point compactification of the complex plane
. In place of holomorphic functions defined on regions in
, one can consider regions in
. Viewed this way, the only possible singularity for entire functions, defined on
\Complex\subset\Complex\cup\{infty\}
, is the point
. If an entire function
is bounded in a neighborhood of
, then
is a
removable singularity of
, i.e.
cannot blow up or behave erratically at
. In light of the
power series expansion, it is not surprising that Liouville's theorem holds.
Similarly, if an entire function has a pole of order
at
- that is, it grows in magnitude comparably to
in some neighborhood of
- then
is a polynomial. This extended version of Liouville's theorem can be more precisely stated: if
for
sufficiently large, then
is a polynomial of degree at most
. This can be proved as follows. Again take the Taylor series representation of
,
The argument used during the proof using Cauchy estimates shows that for all
,
So, if
, then
|ak|\leq\limr\toinftyMrn-k=0.
Therefore,
.
Liouville's theorem does not extend to the generalizations of complex numbers known as double numbers and dual numbers.[3]
See also
References
- Book: Benjamin Fine. Gerhard Rosenberger. The Fundamental Theorem of Algebra. 1997. Springer Science & Business Media. 978-0-387-94657-3. 70–71.
- a concise course in complex analysis and Riemann surfaces, Wilhelm Schlag, corollary 4.8, p.77 http://www.math.uchicago.edu/~schlag/bookweb.pdf
- Liouville theorems in the Dual and Double Planes. Rose-Hulman Undergraduate Mathematics Journal. 15 January 2017. 12. 2. Denhartigh. Kyle. Flim. Rachel.