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Complex Anal

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Complex Anal

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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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