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Course Outline
Complex Analysis
Math Spring Berkeley CA
C McMullen
Texts
Nehari Conformal Mapping
Ahlfors Lectures on Quasiconformal Mappings
Also recommended
Ahlfors Complex Analysis
Conway Functions of One Complex Variable
Lehto Univalent Functions and Teichmuller Theory
Background in real analysis and basic dierential topology such as
covering spaces and dierential forms is a prerequisite
Relations of complex analysis to other elds include algebraic geome
try complex manifolds several complex variables Lie groups and ho
mogeneous spaces C H
b
C geometry Platonic solids hyperbolic ge
ometry in dimensions two and three Teichmuller theory elliptic curves
and algebraic number theory s and prime numbers dynamics iter
ated rational maps
Algebraic origins of complex analysis solving cubic equations x
ax
b by Tchirnhaus transformation to make a This is done by
introducing a new variable y cx
d such that
P
y
i
P
y
i
even
when a and b are real it may be necessary to choose c complex the
discriminant of the equation for c is b
a
It is negative when
the cubic has only one real root this can be checked by looking at the
product of the values of the cubic at its max and min
Elements of complex analysis C Ri z and related examples for
Q
p
Geometry of multiplication why is it conformal Because
jabj jajjbj so triangles are mapped to similar triangles Visualizing
e
z
lim zn
n
A pie slice centered at n and with angle n is
mapped to the upper semicircle in the limit we nd expi
Denition fz is analytic if f
z exists Note we do not require
continuity of f
Cauchys theorem
R
fzdz Plausibility
R
z
n
dz
R
b
a
t
n
tdt
R
b
a
t
n
n
dt
Proof fzdz is a closed form when f is holomorphic assuming
fz is smooth Discussion f is holomorphic i idfdx dfdy from
this dfdz Moreover dfdx dfdz where ddz ddx
iddy We have f analytic if and only if dfdz Then df
dfdzdz dfdzdz and we see dfdz i dfdz i f is
holomorphic
Proof Goursat assuming only complex dierentiability
Analyticity and power series The fundamental integral
R
dzz The
fundamental power series z
P
z
n
Put these together with
Cauchys theorem
fz
i
Z
fd
z
to get a power series
Theorem fz
P
a
n
z
n
has a singularity where it cannot be analyti
cally continued on its circle of convergence jzj R lim sup ja
n
j
n
Innite products
Q
a
n
converges if
P
ja
n
j The proof is in
two steps rst show that when
Q
ja
n
j converges the dierences in
successive partial products bound the dierences for
Q
a
n
Then
show
P
ja
n
j
Q
ja
n
j exp
P
ja
n
j
Example evaluation of
Q
p
where p ranges over
the primes converges to
Cauchys bound jf
n
j nMRR
n
Liouvilles theorem algebraic
completeness of C Compactness of bounded functions in the uniform
topology Parsevals inequality which implies Cauchys
X
ja
n
j
R
Z
jZjR
jfzj
d MR
Moreras theorem converse to Cauchys theorem Denition of logz
R
z
d Analytic continuation natural boundaries
P
a
n
z
n
Laurent
series fz
P
a
n
z
n
where a
n
i
R
C
fzz
n
dz Classi
cation of isolated singularities removability of singularities of bounded
functions Behavior near an essential singularity WeierstrassCasorati
fU C
Generating functions and
P
F
n
z
n
F
n
the nth Fibonacci number A
power series represents a rational function i its coecients satisy a
recurrence relation Pisot numbers the golden ratio and why are
and such pleasant times
Kroneckers theorem one need only check that the determinants of the
matrices a
iij
i j n are zero for all n suciently large
Residue theorem and evaluation of denite integrals Three types
R
Rcos sin d
R
Rxdx and
R
x
a
Rxdx a R a
rational function
Hardys paper on
R
sinxx dx
The argument principle number of zeros number of poles is equal to
i
Z
f
f
d
Similary the weighted sum of gz over the zeros and poles is given by
multiplying the integrand by g
Winding numbers of the topological nature of the argument principle
if a continuous f C has nonzero winding number on the circle
then f has a zero in the disk
Rouches theorem if jgj jf j on then f g and g have the same
number of zerospoles in Example z
z has all zeros of
modulus less than but only one of modulus less than
Open mapping theorem if f is nonconstant then it sends open sets to
open sets Cor the maximum principle jf j achieves its maximum on
the boundary
Invertibility a If f U V is injective and analytic then f
is analytic b If f
z then f is locally injective at z Formal
inversion of power series
Phragmen Lindelof type results if f is bounded in a strip fa
Imz bg and f is continuous on the boundary then the sup on
the boundary is the sup on the interior
Hadamards circles theorem if f is analytic in an annulus then
logMr is a convex function of log r where Mr is the sup of jf j over
jzj r Proof a function s of one real variable is convex if and only
if s ar satises the maximum principle for any constant a This
holds for logMexps
by considering fzz
a
locally
The concept of a Riemann surface the notion of isomorphism the three
simplyconnected Riemann surface C
b
C and H
A nonconstant map between compact surfaces is surjective by the open
mapping theorem
Theorem AutC faz bg
The complex plane C The notion of metric zjdzj The automor
phism group is solvable Inducing a metric jdzjjzj on C
The cone
metric jdzjj
p
zj giving the quotient by z
The Riemann sphere
b
C and its automorphisms Theorem Aut
b
C
PSL
C A particularly nice realization of this action is as the pro
jectivization of the linear action on C
Mobius transformations invertible form a group act by automor
phisms of
b
C triplytransitive sends circles to circles Proof of last a
circle x
y
Ax By C is also given by r
rA cos
B sin C and it is easy to transform the latter under z z
which replaces r by and by
Classication of Mobius transformations and their trace squared a
identity b parabolic a single xed point c elliptic two xed
points derivative of modulus one
d hyperbolic two xed
points one attracting and one repelling C
Stereographic projection preserves circles and angles Proof for angles
given an angle on the sphere construct a pair of circles through the
north pole meeting at that angle These circles meet in the same angle
at the pole on the other hand each circle is the intersection of the
sphere with a plane These planes meet C in the same angle they meet
a plane tangent to the sphere at the north pole QED
Four views of
b
C the extended complex plane the Riemann sphere the
Riemann surface obtained by gluing together two disks with z z
the projective plane for C
The spherical metric jdzj jzj
Derive from the fact Riemann
circle! and the map x tan and conformality of stereographic
projection
Some topology of projective spaces RP
is the union of a disk and a
Mobius band the Hopf map S
S
GaussBonnet for spherical triangles area equals angle defect Prove
by looking at the three lunes of area for the three angles of a
triangle General form X
R
X
K
R
X
k
Theorem AutH PSL
R Schwarz Lemma and automorphisms
of the disk The hyperbolic metric jdzj Imz on H and its equivalence
to jdzj jzj
on
Classication of automorphisms of H
according to translation dis
tance
Hyperbolic geometry geodesics are circles perpendicular to the circle
at innity Euclids fth postulate given a line and a point not on the
line there is a unique parallel through the point Here two lines are
parallel if they are disjoint
GaussBonnet in hyperbolic geometry a Area of an ideal triangle is
R
R
p
x
y
dydx b Area A of a triangle with two ideal
vertices and one external angle is additive A AA
as a diagram shows Thus A c Finally one can extend
the edges of a general triangle T in a spiral fashion to obtain an ideal
triangle containing T and other triangles each with ideal vertices
Harmonic functions A realvalue function uz is harmonic i u is
locally the real part of an analytic function indeed harmonic means
ddu and v
R
du Harmonic functions are preserved under
analytic mappings Examples electric potential "uid "ow around a
cylinder
The meanvalue principle u average over the circle follows from
Cauchys formula as does the Poisson integral formula up visual
average of u
The Schwarz re"ection principle if U U
and f is analytic on UH
continuous and real on the boundary then fz extends f to all of U
This is easy from Moreras theorem A better version only requires
that Imf at the real axis and can be formulated in terms of
harmonic functions cf Ahlfors
If v is harmonic on U H and vanishes on the real axis then vz
vz extends v to a harmonic function on U For the proof use the
Poisson integral to replace v with a harmonic function on any disk
centered on the real axis the result coincides with v on the boundary
of the disk and on the diameter where it vanishes by symmetry so
by the maximum principle it is v
Re"ection gives another proof that all automorphisms of the disk ex
tend to the sphere
Normal families any bounded family of analytic functions is normal
by ArzelaAscoli
Riemann mapping theorem given a simplyconnected region U C
U C and a basepoint u U there is a unique conformal homeo
morphism f U u such that f
u Proof let F be the
family of univalent maps U u Using a squareroot and an
inversion show F is nonempty Also F is closed under limits By the
Schwarz Lemma jf
uj has a nite maximum over all f F Let f
be a maximizing function If f is not surjective to the disk then we
can apply a suitable composition of a squareroot and two automor
phisms of the disk to get a g F with jg
uj jf
uj again using
the Schwarz Lemma QED
Uniformization of annuli any doublyconnected region in the sphere is
conformal isomorphic to C
or AR fz jzj Rg The
map from H to AR is z z
where logRi The deck
transformation is given by z z where
logR
The class S of univalent maps f C such that f and
f
Compactness of S The Bieberbach Conjecturede Brange
Theorem fz
P
a
n
z
n
with ja
n
j n
The area theorem if fz z
P
b
n
z
n
is univalent on fz jzj
g then
P
njb
n
j
The proof is by integrating fdf over the unit
circle and observing that the result is proportional to the area of the
complement of the image of f
Proof that ja
j rst apply the area theorem to conclude ja
a
j
Then consider
q
fz
for f S
The Koebe Theorem if f S then f Proof if
w is omitted from the image then fz fzw S now apply
ja
j
Riemann surfaces and holomorphic forms The naturality of the
residue and of df
The Residue Theorem the sum of the residues of a meromorphic
form on a compact Riemann surface is zero Application to dff and
thereby to the degree of a meromorphic function
Remarks on forms a holomorphic form on the sphere is zero be
cause it integrates to a global analytic function Moreover a meromor
phic form on the sphere always has more poles than zeros
The SchwarzChristoel formula Let f H U be the Riemann
mapping to a polygon with vertices p
i
i n and exterior angles
i
Then
fz
Z
d
Q
n
q
i
i
d
where fq
i
p
i
Proof compute the nonlinearity Nf f
zf
zdz By Schwarz
re"ection it extends to a meromorphic form on the sphere with simple
poles at the q
i
Using the fact that z
i
straightens out the ith vertex
of U one nds that Nf has residue
i
at q
i
Since a form is
determined by its singularities we have
Nf
X
i
dz
z q
i
and the formula results by integration
Examples of SchwarzChristoel logz
R
d maps to a bigon
with external angles of
sin
z
R
d
p
maps to a triangle
with external angles and
The lengtharea method Let f Ra b Q be a conformal map of a
rectangle to a Jordan region Q C where Ra b a b C
Then there is a horizontal line a fyg whose image has length
L
ab areaQ Similarly for vertical lines
Corollary given any quadrilateral Q the product of the minimum
distances between opposite sides is a lower bound for areaQ
Theorem The Riemann map to a Jordan domain extends to a home
omorphism on the closed disk Proof given a point z map
to an innite strip sending z to one end Then there is a sequence of
disjoint squares in the strip tending towards that end The images of
these squares have areas tending to zero so there are crosscuts whose
lengths tend to zero as well by the lengtharea inequality This gives
continuity at z Injectivity is by contradiction if the map is not in
jective then it is constant on some interval along the boundary of the
disk
WeierstrassHadamard factorization theory A good reference for this
material is Titchmarsh Theory of Functions We will examine the
extent to which an entire function is determined by its zeros We
beginning by showing that any discrete set in C arises as the zeros of
an entire function
Weierstrass factor Inspired by the fact that z exp log z
and that log z z z
z
we set
E
p
z z exp
z
z
z
p
p
By convention E
z z
Theorem For jzj we have jE
p
z j jzj
p
Proof Writing E
p
z
P
a
k
z
k
one may check by computing
E
p
z
that all a
k
P
ja
k
j and a
a
a
p
Then
jE
p
z j j
P
a
k
z
k
j jzj
p
P
ja
k
j jzj
p
QED
Theorem If
P
rja
n
j
p
n
for all r then fz
Q
E
p
n
za
n
converges to an entire function with zeros exactly at the a
n
Cor Since p
n
n works for any a
n
we have shown any discrete
set arises as the zeros of an entire function
Blaschke products Let f be a proper map of degree d Then
fz e
i
d
Y
z a
i
a
i
z
where the a
i
enumerate the zeros of f
Jensens formula Let fz be holomorphic on the disk of radius R
about the origin Then the average of log jfzj over the circle of radius
R is given by
log jfj
X
fz jzjR
log
R
jzj
Proof Suces to assume R Clear if f has no zeros because
log jfzj is harmonic Clear for a Blaschke factor zaaz But
the formula is true for fg if it is true for f and g so we are done
Cor Let nr be the number of zeros of f inside the circle of radius r
Then
Z
R
nr
dr
r
Z
log jfRe
i
jd log jfj
Remark We have used the mean value property of harmonic functions
This holds for any harmonic function u on the disk by writing u
Ref f holomorphic and then applying Cauchys integral formula for
f
The physical idea of Jensens formula is that log jf j is the potential for
a set of unit point charges at the zeros of f
Entire functions of nite order An entire function f C C is of
nite order if there is an A such that jfzj Oexp jzj
A
The
least such A is the order of f
Examples Polynomials have order sinz cosz expz have order
cos
p
z has order expexpz
has innite order
Number of zeros By Jensens formula if f has order then nr
Or
where nr is the zero counting function for f Corollary
P
ja
i
j
where a
i
enumerates the zeros of f other than zero
itself
In other words a
i
f where a
i
is the exponent of convergence
of the zeros of f ie the least such that
P
ja
i
j
Denition a canonical product is an entire function of the form
fz z
m
Y
E
p
za
i
where p is the least integer such that
P
jza
i
j
p
for all z
Hadamards Factorization Theorem Let f be an entire function of
order Then fz P z expQz where P is a canonical product
with the same zeros as f and Q is a polynomial of degree less than or
equal to
To prove Hadamards theorem we develop two estimates First we
show a canonical product P z is an entire function of order a
i
This is the least order possible for the given zeros by Jensens theorem
Second we show a canonical product has mr expjzj
for most
radii r where mr is the minimum of jfzj on the circle of radius r
More precisely for any this lower bound holds for all r outside
a set of nite total length In particular it holds for r arbitrarily large
Given these facts we observe that fzP z is an entire function of
order with no zeros Thus Qz log fz is an entire function
satisfying ReQz O jzj
This implies Q is a polynomial
Indeed for any entire function fz
P
a
n
z
n
we have ja
n
jr
n
maxAr Ref
where Ar maxRe fz over the cir
cle of radius r
Example
sinz z
Y
n
z
n
Indeed the right hand side is a canonical product and sinz has
order one so the formula is correct up to a factor expQz where Qz
has degree one But since sinz is odd we conclude Q has degree
zero and by checking the derivative at z of both sides we get
Q
Little Picard Theorem A nonconstant entire function omits at most
one value in the complex plane This is sharp as shown by the example
of expz
Great Picard Theorem Near an essential singularity a meromorphic
function assumes all values on
b
C with at most two exceptions
Proof of Little Picard The key fact is that the universal cover of
C f g can be identied with the upper halfplane This can be seen
by constructing a Riemann mapping from the upper halfplane to an
ideal hyperbolic triangle sending and to the vertices and then
developing both the domain and range by Schwarz re"ection Indeed
with suitable normalizations we have that C f g is isomorphic to
H # where # PSL
Z is the group of matrices congruent to
the identity modulo This is a free group on two generators
Given this fact we lift an entire function f C C f g to a map
e
f C H which is constant by Liouvilles theorem because H
Proof of Great Picard Let f
C be a holomorphic
function omitting three values on the sphere normalized to be zero
one and innity Consider a loop around the puncture of the disk If
f sends to a contractible loop on the triplypunctured sphere then f
lifts to a map into the universal cover H which implies by Riemanns
removability theorem that f extends holomorphically over the origin
Otherwise by the Schwarz lemma f is a homotopy class that can
be represented by an arbitrarily short loop Thus it corresponds to a
puncture which we can normalize to be z rather than or
It follows that f is bounded near z so again the singularity is not
essential
The Gamma Function
#z
expz
z
Y
z
n
expzn
Note that this expression contains the reciprocal of the canonical prod
uct associated to the nonpositive integers The constant is chosen
so that # it can be given by
lim
n
X
k logn
This expression is the error in an approximation to
R
n
dxx by the
area of n rectangles of base one lying over the graph
Gausss formula
#z lim
n
nn
z
zz z n
The functional equation
#z z#z
Corollary #n n
The integral representation for Rez
#z
Z
e
t
t
z
dt
t
In other words #z is the Mellin transform of the function e
t
on R
The Mellin transform is an integral against characters R
C
given by t t
z
and as such it can be compared to the Fourier
transform for the group R under addition and to Gauss sums Indeed
the Gauss sum
X
np
ne
inp
is the analogue of the Gamma function for the group Zp
Relation to sine function
sinz
#z# z
Proof Form the product #z#z and use the functional equation
Periodic functions If f C X has period then fz F expiz
where F C
X Example
X
z n
sin
z
From this we get
P
n
Elliptic doublyperiodic functions Such functions can be considered
as holomorphic maps f X
b
C where X C $ By general easy
results on compact Riemann surfaces An entire elliptic function is
constant The sum of the residues of f over X is zero The map f has
as many zeros as poles
More interesting is the fact that if f is nonconstant with zeros a
i
and
poles p
i
then
P
a
i
P
p
i
in the group law on X Proof integrate
zdff around a fundamental parallelogram in C
We will see that we may construct an elliptic function with given zeros
and poles subject only to this constraint
Construction of elliptic functions For n
n
z
X
z
n
denes an elliptic function of degree n For degree two we adjust the
factors in the sum so they vanish at the origin and obtain the denition
of the Weierstrass function
z
z
X
z
To see z is elliptic use the fact that z z and
z
z which implies z z A
Other ways to construct elliptic functions of degree two if $ is gener
ated by
rst sum over one period to get
f
z
X
z n
sinz
then we have
z
X
f
z n
and the convergence is rapid Similarly if we write X C
z
z then
fz
X
n
z
n
z
converges to an elliptic function of order two
Laurent expansion and dierential equation Expanding z
in
a Laurent series about z and summing we obtain
z
z
X
n z
n
G
n
where
G
n
X
n
By a straightforward calculation using the fact that an elliptic function
with no pole is constant we have
z
z
g
z g
where g
G
and g
G
Geometry of the Weierstrass map X
b
C The critical points of
are the points of order two the critical values are innity and the zeros
of the cubic equation px x
g
x g
These are distinct
The map z z
z
sends X fg to the ane cubic curve
y
px Thus uniformizes! this plane curve of genus
When $ has a rectangular fundamental domain the function can
also be constructed by taking a Riemann mapping from this rectangle
with dimensions reduced by a factor of two to the upper halfplane
and developing by Schwarz re"ection Then the dierential equation
for comes from the SchwarzChristoel formula
Function elds Given any Riemann surface X the meromorphic func
tions on X form a eld KX Then K is a contravariant functor from
category of Riemann surfaces with nonconstant maps to the category
of elds with extensions Example K
b
C C z
Theorem For X C $ KX C x yy
x
g
x g
To see that and
generate KX is easy Any even function f
X
b
C factors through fz F z
and so lies in C Any
odd function becomes even when multiplied by
and any function is
a sum of one even and one odd
To see that the eld is exactly that given is also easy It amounts
to showing that KX is of degree exactly two over C and is
transcendental over C The rst assertion is obvious and if the second
fails we would have KX C which is impossible because is
even and
is odd
An elliptic function with given poles and zeros It is natural to try to
construct an elliptic function by forming the Weierstrass product for
the lattice $
z z
Y
z
exp
z
z
Then
zz
z from which it follows that z
z expa
b
z From this it is easy to see that
z a
z a
n
z p
z p
n
denes an elliptic function whenever
P
a
i
P
p
i
and therefore this
is the only condition imposed on the zeros and poles of an elliptic
function
The moduli space of elliptic curves M
classies Riemann surfaces
of genus up to isomorphism Since any such surface is given by
X C $ and we may normalize so $ Z Z where H it is
not hard to see
M
H PSL
Z
Similarly an elliptic curve with a labelling of its points of order two is
classied by M
H #
We now present another proof that H # is naturally isomorphic to
b
C f g Given $ we get the cubic polynomial x
g
x g
xx
xx
xx
whose roots are exactly the values of z at
the points of order two Thus the crossratio x
x
x
x
depends only on the location of in M
and thus we have a map
M
b
C f g
But we can invert this map given form the degree two cover X
of
b
C
branched over f g Once we know X
is isomorphic to C $ for
some $ it is easy to show we have reconstructed up to an element of
# One might appeal to the uniformization theorem here but in fact
it is elementary to see that dx
q
xx x lifts to a nowherezero
holomorphic form on X
This one form gives a complete Euclidean
metric and so the universal cover of X
can be identied with C
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