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Rational approximation to analytic functions with polar singular set - - PowerPoint PPT Presentation

Rational approximation to analytic functions with polar singular set and finitely many branchpoints Laurent Baratchart INRIA Sophia-Antipolis-M editerrann ee France based on joint work with Maxim Yattselev (IUPUI, Indianapolis) and


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Rational approximation to analytic functions with polar singular set and finitely many branchpoints

Laurent Baratchart

INRIA Sophia-Antipolis-M´ editerrann´ ee France based on joint work with

Maxim Yattselev (IUPUI, Indianapolis) and Herbert Stahl†

MWAA-IUPUI, October 6-8, 2017.

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The possibility of rational approximation

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The possibility of rational approximation

  • In 1885, Runge proved that holomorphic functions of one

complex variable can be approximated by rational functions, locally uniformly on their domain of holomorphy.

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The possibility of rational approximation

  • In 1885, Runge proved that holomorphic functions of one

complex variable can be approximated by rational functions, locally uniformly on their domain of holomorphy.

  • Theorem[Runge, 1885]
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The possibility of rational approximation

  • In 1885, Runge proved that holomorphic functions of one

complex variable can be approximated by rational functions, locally uniformly on their domain of holomorphy.

  • Theorem[Runge, 1885]

Let K ⊂ Ω ⊂ C with K compact and Ω open. If f ∈ Hol(Ω) and ε > 0, there is a rational function R such that |f (z) − R(z)| < ε, z ∈ K.

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SLIDE 6

The possibility of rational approximation

  • In 1885, Runge proved that holomorphic functions of one

complex variable can be approximated by rational functions, locally uniformly on their domain of holomorphy.

  • Theorem[Runge, 1885]

Let K ⊂ Ω ⊂ C with K compact and Ω open. If f ∈ Hol(Ω) and ε > 0, there is a rational function R such that |f (z) − R(z)| < ε, z ∈ K.

  • Runge’s proof rests on his “pole shifting technique”.
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SLIDE 7

The possibility of rational approximation

  • In 1885, Runge proved that holomorphic functions of one

complex variable can be approximated by rational functions, locally uniformly on their domain of holomorphy.

  • Theorem[Runge, 1885]

Let K ⊂ Ω ⊂ C with K compact and Ω open. If f ∈ Hol(Ω) and ε > 0, there is a rational function R such that |f (z) − R(z)| < ε, z ∈ K.

  • Runge’s proof rests on his “pole shifting technique”.
  • Today, it is a consequence of the duality between complex

measures and continuous functions with compact support.

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Subsequent developments

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Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity)

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SLIDE 10

Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity) approximability on noncompact sets [Roth, 1976].

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SLIDE 11

Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity) approximability on noncompact sets [Roth, 1976].

  • Characterization of smoothness from the rate of

approximation [Dolzhenko 68, Pekarskii 83, Peller 86].

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Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity) approximability on noncompact sets [Roth, 1976].

  • Characterization of smoothness from the rate of

approximation [Dolzhenko 68, Pekarskii 83, Peller 86].

  • Constructive approximation:
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Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity) approximability on noncompact sets [Roth, 1976].

  • Characterization of smoothness from the rate of

approximation [Dolzhenko 68, Pekarskii 83, Peller 86].

  • Constructive approximation:
  • in number theory to check for irrationality, transcendency,
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SLIDE 14

Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity) approximability on noncompact sets [Roth, 1976].

  • Characterization of smoothness from the rate of

approximation [Dolzhenko 68, Pekarskii 83, Peller 86].

  • Constructive approximation:
  • in number theory to check for irrationality, transcendency,
  • in modeling and control engineering (robust control)
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Subsequent developments

  • Approximability on K of continuous functions analytic in
  • K

[Bishop 60, Mergelyan 62, Vitushkin 66] (analytic capacity) approximability on noncompact sets [Roth, 1976].

  • Characterization of smoothness from the rate of

approximation [Dolzhenko 68, Pekarskii 83, Peller 86].

  • Constructive approximation:
  • in number theory to check for irrationality, transcendency,
  • in modeling and control engineering (robust control)
  • in electrical engineering, to check stability of microwave

circuits.

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A discretization viewpoint

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A discretization viewpoint

  • An analytic function is a Cauchy integral:

f (z) = dµ(t) t − z).

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A discretization viewpoint

  • An analytic function is a Cauchy integral:

f (z) = dµ(t) t − z).

  • Thus, using the identification R2 ∼ C, it becomes the

gradient of a logarithmic potential: f (z) = − ∂ ∂z

  • log

1 |t − z|dµ(t).

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SLIDE 19

A discretization viewpoint

  • An analytic function is a Cauchy integral:

f (z) = dµ(t) t − z).

  • Thus, using the identification R2 ∼ C, it becomes the

gradient of a logarithmic potential: f (z) = − ∂ ∂z

  • log

1 |t − z|dµ(t).

  • A rational function is the gradient of a discrete potential:

r(z) =

n

  • j=1

aj z − bj = ∂ ∂z

  • log

1 |t − z|dνn(t)

  • where νn = n

j=1 ajδbj.

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A discretization viewpoint

  • An analytic function is a Cauchy integral:

f (z) = dµ(t) t − z).

  • Thus, using the identification R2 ∼ C, it becomes the

gradient of a logarithmic potential: f (z) = − ∂ ∂z

  • log

1 |t − z|dµ(t).

  • A rational function is the gradient of a discrete potential:

r(z) =

n

  • j=1

aj z − bj = ∂ ∂z

  • log

1 |t − z|dνn(t)

  • where νn = n

j=1 ajδbj.

  • Hence, rational approximation may be viewed as optimal

discretization of a logarithmic potential with respect to a Sobolev norm.

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Remarks

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Remarks

  • The talk is concerned with asymptotic error rates and pole

distribution when the degree of the approximant goes large.

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Remarks

  • The talk is concerned with asymptotic error rates and pole

distribution when the degree of the approximant goes large.

  • Understanding the behaviour of poles of rational approximants

is the non-convex and difficult part of the problem.

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Remarks

  • The talk is concerned with asymptotic error rates and pole

distribution when the degree of the approximant goes large.

  • Understanding the behaviour of poles of rational approximants

is the non-convex and difficult part of the problem.

  • A fundamental feature is: we have branchpoints.
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Remarks

  • The talk is concerned with asymptotic error rates and pole

distribution when the degree of the approximant goes large.

  • Understanding the behaviour of poles of rational approximants

is the non-convex and difficult part of the problem.

  • A fundamental feature is: we have branchpoints. This will get

us an attractor for the poles:

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Remarks

  • The talk is concerned with asymptotic error rates and pole

distribution when the degree of the approximant goes large.

  • Understanding the behaviour of poles of rational approximants

is the non-convex and difficult part of the problem.

  • A fundamental feature is: we have branchpoints. This will get

us an attractor for the poles: the normalized counting measure 1 n

n

  • i=1

δξi, with ξj the poles, will converge weak-* to some probability measure as the degree of the approximant goes large

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SLIDE 27

Remarks

  • The talk is concerned with asymptotic error rates and pole

distribution when the degree of the approximant goes large.

  • Understanding the behaviour of poles of rational approximants

is the non-convex and difficult part of the problem.

  • A fundamental feature is: we have branchpoints. This will get

us an attractor for the poles: the normalized counting measure 1 n

n

  • i=1

δξi, with ξj the poles, will converge weak-* to some probability measure as the degree of the approximant goes large (dominancy of branchpoints).

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Some notation

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Some notation

  • f is holomorphic on a domain Ω ⊂ C.
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Some notation

  • f is holomorphic on a domain Ω ⊂ C.
  • K is a compact subset of Ω.
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Some notation

  • f is holomorphic on a domain Ω ⊂ C.
  • K is a compact subset of Ω.
  • Rn denotes the set of rational functions of degree n:

Rn = {pn qn ; pn, qn complex polynomials of degree at most n}.

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Some notation

  • f is holomorphic on a domain Ω ⊂ C.
  • K is a compact subset of Ω.
  • Rn denotes the set of rational functions of degree n:

Rn = {pn qn ; pn, qn complex polynomials of degree at most n}.

  • We set

en = en(f , K) := inf

rn∈Rn

f − rnL∞(K).

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Rates in approximation

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Rates in approximation

  • Strong asymptotics are estimates of en(f , K) as n goes large,

with respect to some scale depending on n.

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Rates in approximation

  • Strong asymptotics are estimates of en(f , K) as n goes large,

with respect to some scale depending on n.

  • Strong asymptotics can usually be derived for specific

functions f only.

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Rates in approximation

  • Strong asymptotics are estimates of en(f , K) as n goes large,

with respect to some scale depending on n.

  • Strong asymptotics can usually be derived for specific

functions f only.

  • Weak or n-th root asymptotics are estimates of e1/n

n

as n goes large.

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Rates in approximation

  • Strong asymptotics are estimates of en(f , K) as n goes large,

with respect to some scale depending on n.

  • Strong asymptotics can usually be derived for specific

functions f only.

  • Weak or n-th root asymptotics are estimates of e1/n

n

as n goes large.

  • n-th root rates only estimate the geometric decay of the error.
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Rates in approximation

  • Strong asymptotics are estimates of en(f , K) as n goes large,

with respect to some scale depending on n.

  • Strong asymptotics can usually be derived for specific

functions f only.

  • Weak or n-th root asymptotics are estimates of e1/n

n

as n goes large.

  • n-th root rates only estimate the geometric decay of the error.
  • They make contact with logarithmic potential theory.
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Some potential theory

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Some potential theory

  • The logarithmic potential of a positive measure µ with

compact support in C is V µ(z) :=

  • log

1 |z − t| dµ(t)

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Some potential theory

  • The logarithmic potential of a positive measure µ with

compact support in C is V µ(z) :=

  • log

1 |z − t| dµ(t)

  • This is a superharmonic function valued in R ∪ {+∞}, the

solution to ∆u = −µ which is smallest in modulus at ∞.

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Some potential theory

  • The logarithmic potential of a positive measure µ with

compact support in C is V µ(z) :=

  • log

1 |z − t| dµ(t)

  • This is a superharmonic function valued in R ∪ {+∞}, the

solution to ∆u = −µ which is smallest in modulus at ∞.

  • The logarithmic energy of µ is

I(µ) := log 1 |z − t| dµ(t)dµ(z).

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Some potential theory

  • The logarithmic potential of a positive measure µ with

compact support in C is V µ(z) :=

  • log

1 |z − t| dµ(t)

  • This is a superharmonic function valued in R ∪ {+∞}, the

solution to ∆u = −µ which is smallest in modulus at ∞.

  • The logarithmic energy of µ is

I(µ) := log 1 |z − t| dµ(t)dµ(z).

  • The energy lies in R ∪ {+∞}.
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Potential theory cont’d

  • The logarithmic capacity of K is C(K) = e−IK where

IK := inf

µ∈PK

log 1 |z − t| dµ(t)dµ(x) and PK is the set of probability measures on K.

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Potential theory cont’d

  • The logarithmic capacity of K is C(K) = e−IK where

IK := inf

µ∈PK

log 1 |z − t| dµ(t)dµ(x) and PK is the set of probability measures on K.

  • If C(K) > 0, there is a unique measure ωK ∈ PK to meet the

above infimum. It is called the equilibrium distribution on K.

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Potential theory cont’d

  • The logarithmic capacity of K is C(K) = e−IK where

IK := inf

µ∈PK

log 1 |z − t| dµ(t)dµ(x) and PK is the set of probability measures on K.

  • If C(K) > 0, there is a unique measure ωK ∈ PK to meet the

above infimum. It is called the equilibrium distribution on K.

  • If C(K) = 0 one says K is polar. Polar sets are very small and

look very bad (totally disconnected, H1-dimension zero...).

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Potential theory cont’d

  • The logarithmic capacity of K is C(K) = e−IK where

IK := inf

µ∈PK

log 1 |z − t| dµ(t)dµ(x) and PK is the set of probability measures on K.

  • If C(K) > 0, there is a unique measure ωK ∈ PK to meet the

above infimum. It is called the equilibrium distribution on K.

  • If C(K) = 0 one says K is polar. Polar sets are very small and

look very bad (totally disconnected, H1-dimension zero...).

  • A property valid outside a polar set is said to hold

quasi-everywhere.

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Potential theory cont’d

  • The logarithmic capacity of K is C(K) = e−IK where

IK := inf

µ∈PK

log 1 |z − t| dµ(t)dµ(x) and PK is the set of probability measures on K.

  • If C(K) > 0, there is a unique measure ωK ∈ PK to meet the

above infimum. It is called the equilibrium distribution on K.

  • If C(K) = 0 one says K is polar. Polar sets are very small and

look very bad (totally disconnected, H1-dimension zero...).

  • A property valid outside a polar set is said to hold

quasi-everywhere.

  • ωK is characterized by V ωK being constant q.e. on K

(Frostman theorem).

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Potential theory cont’d

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SLIDE 50

Potential theory cont’d

  • Capacity is a measure of size.
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Potential theory cont’d

  • Capacity is a measure of size.
  • Example 1: the capacity of a disk is its radius and the

equilibrium distribution is normalized arclength on the circumference.

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Potential theory cont’d

  • Capacity is a measure of size.
  • Example 1: the capacity of a disk is its radius and the

equilibrium distribution is normalized arclength on the circumference.

  • Example 2: the capacity of a segment is C[a,b] = (b − a)/4

and the equilibrium distribution is dt π

  • (t − a)(b − t)

.

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Potential theory cont’d

  • Capacity is a measure of size.
  • Example 1: the capacity of a disk is its radius and the

equilibrium distribution is normalized arclength on the circumference.

  • Example 2: the capacity of a segment is C[a,b] = (b − a)/4

and the equilibrium distribution is dt π

  • (t − a)(b − t)

.

  • The equilibrium distribution is always supported on the outer

boundary of K.

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Potential theory cont’d

  • Capacity is a measure of size.
  • Example 1: the capacity of a disk is its radius and the

equilibrium distribution is normalized arclength on the circumference.

  • Example 2: the capacity of a segment is C[a,b] = (b − a)/4

and the equilibrium distribution is dt π

  • (t − a)(b − t)

.

  • The equilibrium distribution is always supported on the outer

boundary of K.

  • The capacity of a set E is the supremum of CK over all

compact K ⊂ E.

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SLIDE 55

Potential theory cont’d

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SLIDE 56

Potential theory cont’d

  • The weighted capacity of a non polar compact set K in the

field ψ, assumed to be lower semi-continuous and finite q.e.

  • n K, is Cψ(K) = e−Iψ where

Iψ := inf

µ∈PK

log 1 |z − t|dµ(t)dµ(z) + 2

  • ψ(t)dµ(t).
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Potential theory cont’d

  • The weighted capacity of a non polar compact set K in the

field ψ, assumed to be lower semi-continuous and finite q.e.

  • n K, is Cψ(K) = e−Iψ where

Iψ := inf

µ∈PK

log 1 |z − t|dµ(t)dµ(z) + 2

  • ψ(t)dµ(t).
  • There is a unique measure ωK,ψ ∈ PK to meet the infimum; it

is called the weighted equilibrium distribution on K (w.r.t.ψ).

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Potential theory cont’d

  • The weighted capacity of a non polar compact set K in the

field ψ, assumed to be lower semi-continuous and finite q.e.

  • n K, is Cψ(K) = e−Iψ where

Iψ := inf

µ∈PK

log 1 |z − t|dµ(t)dµ(z) + 2

  • ψ(t)dµ(t).
  • There is a unique measure ωK,ψ ∈ PK to meet the infimum; it

is called the weighted equilibrium distribution on K (w.r.t.ψ).

  • ωK,ψ is characterized by the fact that V ωK,ψ + ψ is constant

q.e. on supp(ωK,ψ) and at least as large as this constant q.e.

  • n K.
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SLIDE 59

Potential theory cont’d

  • The weighted capacity of a non polar compact set K in the

field ψ, assumed to be lower semi-continuous and finite q.e.

  • n K, is Cψ(K) = e−Iψ where

Iψ := inf

µ∈PK

log 1 |z − t|dµ(t)dµ(z) + 2

  • ψ(t)dµ(t).
  • There is a unique measure ωK,ψ ∈ PK to meet the infimum; it

is called the weighted equilibrium distribution on K (w.r.t.ψ).

  • ωK,ψ is characterized by the fact that V ωK,ψ + ψ is constant

q.e. on supp(ωK,ψ) and at least as large as this constant q.e.

  • n K.
  • Physically, it is the equilibrium distribution on a conductor K
  • f a unit electric charge in the electric field ψ.
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SLIDE 60

Potential theory cont’d

  • The weighted capacity of a non polar compact set K in the

field ψ, assumed to be lower semi-continuous and finite q.e.

  • n K, is Cψ(K) = e−Iψ where

Iψ := inf

µ∈PK

log 1 |z − t|dµ(t)dµ(z) + 2

  • ψ(t)dµ(t).
  • There is a unique measure ωK,ψ ∈ PK to meet the infimum; it

is called the weighted equilibrium distribution on K (w.r.t.ψ).

  • ωK,ψ is characterized by the fact that V ωK,ψ + ψ is constant

q.e. on supp(ωK,ψ) and at least as large as this constant q.e.

  • n K.
  • Physically, it is the equilibrium distribution on a conductor K
  • f a unit electric charge in the electric field ψ.
  • When ψ ≡ 0 one recovers the usual capacity.
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Green functions

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SLIDE 62

Green functions

  • Let Ω open have non-polar boundary ∂Ω.
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SLIDE 63

Green functions

  • Let Ω open have non-polar boundary ∂Ω.
  • The Green function of Ω with pole at z ∈ Ω is the function

GΩ(z, .) such that

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SLIDE 64

Green functions

  • Let Ω open have non-polar boundary ∂Ω.
  • The Green function of Ω with pole at z ∈ Ω is the function

GΩ(z, .) such that

  • t → GΩ(z, t) + log |z − t| is bounded and harmonic in Ω,
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SLIDE 65

Green functions

  • Let Ω open have non-polar boundary ∂Ω.
  • The Green function of Ω with pole at z ∈ Ω is the function

GΩ(z, .) such that

  • t → GΩ(z, t) + log |z − t| is bounded and harmonic in Ω,
  • lim

t→ξ GΩ(z, t) = 0,

q.e. ξ ∈ ∂Ω.

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SLIDE 66

Green functions

  • Let Ω open have non-polar boundary ∂Ω.
  • The Green function of Ω with pole at z ∈ Ω is the function

GΩ(z, .) such that

  • t → GΩ(z, t) + log |z − t| is bounded and harmonic in Ω,
  • lim

t→ξ GΩ(z, t) = 0,

q.e. ξ ∈ ∂Ω.

  • Equivalently, GΩ(z, .) is the smallest positive solution to

∆u = −δz in Ω.

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SLIDE 67

Green functions

  • Let Ω open have non-polar boundary ∂Ω.
  • The Green function of Ω with pole at z ∈ Ω is the function

GΩ(z, .) such that

  • t → GΩ(z, t) + log |z − t| is bounded and harmonic in Ω,
  • lim

t→ξ GΩ(z, t) = 0,

q.e. ξ ∈ ∂Ω.

  • Equivalently, GΩ(z, .) is the smallest positive solution to

∆u = −δz in Ω.

  • Example: if D is the unit disk, then

GD(z, t) = log

  • 1 − z¯

t z − t

  • .
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SLIDE 68

Potential theory cont’d

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SLIDE 69

Potential theory cont’d

  • Let ∂Ω be non-polar.
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SLIDE 70

Potential theory cont’d

  • Let ∂Ω be non-polar.
  • The Green potential of a positive measure µ with compact

support in Ω is V µ

Ω(z) :=

  • GΩ(z, t) dµ(t).
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SLIDE 71

Potential theory cont’d

  • Let ∂Ω be non-polar.
  • The Green potential of a positive measure µ with compact

support in Ω is V µ

Ω(z) :=

  • GΩ(z, t) dµ(t).
  • It is the smallest positive solution to ∆u = −µ in Ω.
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SLIDE 72

Potential theory cont’d

  • Let ∂Ω be non-polar.
  • The Green potential of a positive measure µ with compact

support in Ω is V µ

Ω(z) :=

  • GΩ(z, t) dµ(t).
  • It is the smallest positive solution to ∆u = −µ in Ω.
  • The Green energy of µ is

I G(µ) := GΩ(z, t) dµ(t)dµ(z).

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SLIDE 73

Potential theory cont’d

  • Let ∂Ω be non-polar.
  • The Green potential of a positive measure µ with compact

support in Ω is V µ

Ω(z) :=

  • GΩ(z, t) dµ(t).
  • It is the smallest positive solution to ∆u = −µ in Ω.
  • The Green energy of µ is

I G(µ) := GΩ(z, t) dµ(t)dµ(z).

  • = ∇V µ

Ω2 L2(Ω) in smooth cases

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SLIDE 74

Potential theory cont’d

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SLIDE 75

Potential theory cont’d

  • The Green capacity of K is C(K, Ω) = 1/IK where

IK := inf

µ∈PK IG(µ) = inf µ∈PK

GΩ(z, t) dµ(t)dµ(z).

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SLIDE 76

Potential theory cont’d

  • The Green capacity of K is C(K, Ω) = 1/IK where

IK := inf

µ∈PK IG(µ) = inf µ∈PK

GΩ(z, t) dµ(t)dµ(z).

  • If K, is non polar, there is a unique measure ωG

K,Ω ∈ PK to

meet the above infimum. It is called the Green equilibrium distribution of K in Ω.

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SLIDE 77

Potential theory cont’d

  • The Green capacity of K is C(K, Ω) = 1/IK where

IK := inf

µ∈PK IG(µ) = inf µ∈PK

GΩ(z, t) dµ(t)dµ(z).

  • If K, is non polar, there is a unique measure ωG

K,Ω ∈ PK to

meet the above infimum. It is called the Green equilibrium distribution of K in Ω.

  • ωG

K,Ω is characterized by the fact that V ωG

K,Ω

G

is constant q.e.

  • n K.
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SLIDE 78

Potential theory cont’d

  • The Green capacity of K is C(K, Ω) = 1/IK where

IK := inf

µ∈PK IG(µ) = inf µ∈PK

GΩ(z, t) dµ(t)dµ(z).

  • If K, is non polar, there is a unique measure ωG

K,Ω ∈ PK to

meet the above infimum. It is called the Green equilibrium distribution of K in Ω.

  • ωG

K,Ω is characterized by the fact that V ωG

K,Ω

G

is constant q.e.

  • n K.
  • Green capacities and Green equilibrium distributions are

conformally invariant.

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SLIDE 79

Potential theory cont’d

  • The Green capacity of K is C(K, Ω) = 1/IK where

IK := inf

µ∈PK IG(µ) = inf µ∈PK

GΩ(z, t) dµ(t)dµ(z).

  • If K, is non polar, there is a unique measure ωG

K,Ω ∈ PK to

meet the above infimum. It is called the Green equilibrium distribution of K in Ω.

  • ωG

K,Ω is characterized by the fact that V ωG

K,Ω

G

is constant q.e.

  • n K.
  • Green capacities and Green equilibrium distributions are

conformally invariant. This allows to speak of the Green capacity of a closed set, possibly containing ∞, in an open set

  • f the Riemann sphere.
slide-80
SLIDE 80

n-th root estimates: upper bound

slide-81
SLIDE 81

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s.

slide-82
SLIDE 82

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s. He proved the following:

slide-83
SLIDE 83

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s. He proved the following:

  • Theorem[Walsh]

Let f be holomorphic on a domain Ω and K ⊂ Ω be compact;

slide-84
SLIDE 84

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s. He proved the following:

  • Theorem[Walsh]

Let f be holomorphic on a domain Ω and K ⊂ Ω be compact; Put en = infrn∈Rnf − pn/qnL∞(K).

slide-85
SLIDE 85

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s. He proved the following:

  • Theorem[Walsh]

Let f be holomorphic on a domain Ω and K ⊂ Ω be compact; Put en = infrn∈Rnf − pn/qnL∞(K). Then lim sup

n→∞ e1/n n

≤ exp

1 C(K, Ω)

  • .
slide-86
SLIDE 86

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s. He proved the following:

  • Theorem[Walsh]

Let f be holomorphic on a domain Ω and K ⊂ Ω be compact; Put en = infrn∈Rnf − pn/qnL∞(K). Then lim sup

n→∞ e1/n n

≤ exp

1 C(K, Ω)

  • .
  • It is obtained by interpolating the function.
slide-87
SLIDE 87

n-th root estimates: upper bound

  • J.L. Walsh was perhaps first to connect weak asymptotics in

rational approximation with Green potentials in the late 40’s. He proved the following:

  • Theorem[Walsh]

Let f be holomorphic on a domain Ω and K ⊂ Ω be compact; Put en = infrn∈Rnf − pn/qnL∞(K). Then lim sup

n→∞ e1/n n

≤ exp

1 C(K, Ω)

  • .
  • It is obtained by interpolating the function. There are

functions for which this bound is sharp (Tikhomirov).

slide-88
SLIDE 88

A proof on the disk

slide-89
SLIDE 89

A proof on the disk

  • By outer continuity of the Green capacity, we may assume

that f is bounded on D, say f H∞(D) = 1.

slide-90
SLIDE 90

A proof on the disk

  • By outer continuity of the Green capacity, we may assume

that f is bounded on D, say f H∞(D) = 1.

  • For Bn a Blaschke product with zeros at z1, · · · , zn ∈ K,

projection of f onto H2 ⊖ BH2 yields rn ∈ Rn interpolating f at those points, rnH2 ≤ 1. By a Bernstein-type estimate r′

nH∞ ≤ cn [Baranov-Zarouf, 2014] so that rnH∞ ≤ Cn.

slide-91
SLIDE 91

A proof on the disk

  • By outer continuity of the Green capacity, we may assume

that f is bounded on D, say f H∞(D) = 1.

  • For Bn a Blaschke product with zeros at z1, · · · , zn ∈ K,

projection of f onto H2 ⊖ BH2 yields rn ∈ Rn interpolating f at those points, rnH2 ≤ 1. By a Bernstein-type estimate r′

nH∞ ≤ cn [Baranov-Zarouf, 2014] so that rnH∞ ≤ Cn.

  • |f (z) − rn(z)| ≤ C ′n Πn

j=1

  • z − zj

1 − z ¯ zj

slide-92
SLIDE 92

A proof on the disk

  • By outer continuity of the Green capacity, we may assume

that f is bounded on D, say f H∞(D) = 1.

  • For Bn a Blaschke product with zeros at z1, · · · , zn ∈ K,

projection of f onto H2 ⊖ BH2 yields rn ∈ Rn interpolating f at those points, rnH2 ≤ 1. By a Bernstein-type estimate r′

nH∞ ≤ cn [Baranov-Zarouf, 2014] so that rnH∞ ≤ Cn.

  • |f (z) − rn(z)| ≤ C ′n Πn

j=1

  • z − zj

1 − z ¯ zj

  • Equivalently, with νn = 1

n

n

j=1 δzj,

|f (z) − rn(z)| ≤ C ′n exp

  • −n
  • GD(z, t)dνn(t)
slide-93
SLIDE 93

A proof on the disk

  • By outer continuity of the Green capacity, we may assume

that f is bounded on D, say f H∞(D) = 1.

  • For Bn a Blaschke product with zeros at z1, · · · , zn ∈ K,

projection of f onto H2 ⊖ BH2 yields rn ∈ Rn interpolating f at those points, rnH2 ≤ 1. By a Bernstein-type estimate r′

nH∞ ≤ cn [Baranov-Zarouf, 2014] so that rnH∞ ≤ Cn.

  • |f (z) − rn(z)| ≤ C ′n Πn

j=1

  • z − zj

1 − z ¯ zj

  • Equivalently, with νn = 1

n

n

j=1 δzj,

|f (z) − rn(z)| ≤ C ′n exp

  • −n
  • GD(z, t)dνn(t)
  • Taking n-th root while choosing the zj so that νn converges

weak* to ωG

K,D and letting n → ∞ gives the desired bound.

slide-94
SLIDE 94

A proof on the disk

  • By outer continuity of the Green capacity, we may assume

that f is bounded on D, say f H∞(D) = 1.

  • For Bn a Blaschke product with zeros at z1, · · · , zn ∈ K,

projection of f onto H2 ⊖ BH2 yields rn ∈ Rn interpolating f at those points, rnH2 ≤ 1. By a Bernstein-type estimate r′

nH∞ ≤ cn [Baranov-Zarouf, 2014] so that rnH∞ ≤ Cn.

  • |f (z) − rn(z)| ≤ C ′n Πn

j=1

  • z − zj

1 − z ¯ zj

  • Equivalently, with νn = 1

n

n

j=1 δzj,

|f (z) − rn(z)| ≤ C ′n exp

  • −n
  • GD(z, t)dνn(t)
  • Taking n-th root while choosing the zj so that νn converges

weak* to ωG

K,D and letting n → ∞ gives the desired bound.

slide-95
SLIDE 95

The Gonchar conjecture

slide-96
SLIDE 96

The Gonchar conjecture

  • A. A. Gonchar conjectured in 1978 that

lim inf

n→∞ e1/n n

≤ exp

2 C(K, Ω)

  • .

(1)

slide-97
SLIDE 97

The Gonchar conjecture

  • A. A. Gonchar conjectured in 1978 that

lim inf

n→∞ e1/n n

≤ exp

2 C(K, Ω)

  • .

(1)

  • Gonchar’s conjecture means that using rational approximants

instead of polynomials improves convergence like a Newton scheme improves a steepest descent algorithm: it squares the error, at least for a subsequence.

slide-98
SLIDE 98

The Gonchar conjecture

  • A. A. Gonchar conjectured in 1978 that

lim inf

n→∞ e1/n n

≤ exp

2 C(K, Ω)

  • .

(1)

  • Gonchar’s conjecture means that using rational approximants

instead of polynomials improves convergence like a Newton scheme improves a steepest descent algorithm: it squares the error, at least for a subsequence.

  • Gonchar and Rakhmanov substantiated the conjecture by

constructing classes of functions for which (1) is both an equality and a true limit.

slide-99
SLIDE 99

The Gonchar conjecture

  • A. A. Gonchar conjectured in 1978 that

lim inf

n→∞ e1/n n

≤ exp

2 C(K, Ω)

  • .

(1)

  • Gonchar’s conjecture means that using rational approximants

instead of polynomials improves convergence like a Newton scheme improves a steepest descent algorithm: it squares the error, at least for a subsequence.

  • Gonchar and Rakhmanov substantiated the conjecture by

constructing classes of functions for which (1) is both an equality and a true limit.

  • For this they used interpolation again.
slide-100
SLIDE 100

Pad´ e interpolants and N.H. orthogonal polynomials

slide-101
SLIDE 101

Pad´ e interpolants and N.H. orthogonal polynomials

  • Let f (z) =

dµ(ξ)

z−ξ where µ is a complex measure supported

  • n E compact. W. r. t. previous notation, Ω = C \ E.
slide-102
SLIDE 102

Pad´ e interpolants and N.H. orthogonal polynomials

  • Let f (z) =

dµ(ξ)

z−ξ where µ is a complex measure supported

  • n E compact. W. r. t. previous notation, Ω = C \ E.
  • If pn−1/qn interpolates f in {ξ(n)

1 , · · · , ξ(n) 2n , ∞} ⊂ Ω and if

w2n(z) = Πj(1 − z/ξ(n)

j

), then

  • qn(ξ)

w2n(ξ)ξkdµ(ξ) = 0, k ∈ {0, 1, . . . , n − 1}. (2)

slide-103
SLIDE 103

Pad´ e interpolants and N.H. orthogonal polynomials

  • Let f (z) =

dµ(ξ)

z−ξ where µ is a complex measure supported

  • n E compact. W. r. t. previous notation, Ω = C \ E.
  • If pn−1/qn interpolates f in {ξ(n)

1 , · · · , ξ(n) 2n , ∞} ⊂ Ω and if

w2n(z) = Πj(1 − z/ξ(n)

j

), then

  • qn(ξ)

w2n(ξ)ξkdµ(ξ) = 0, k ∈ {0, 1, . . . , n − 1}. (2)

  • Note that orthogonality is non Hermitian.
slide-104
SLIDE 104

Pad´ e interpolants and N.H. orthogonal polynomials

  • Let f (z) =

dµ(ξ)

z−ξ where µ is a complex measure supported

  • n E compact. W. r. t. previous notation, Ω = C \ E.
  • If pn−1/qn interpolates f in {ξ(n)

1 , · · · , ξ(n) 2n , ∞} ⊂ Ω and if

w2n(z) = Πj(1 − z/ξ(n)

j

), then

  • qn(ξ)

w2n(ξ)ξkdµ(ξ) = 0, k ∈ {0, 1, . . . , n − 1}. (2)

  • Note that orthogonality is non Hermitian.
  • To assess the asymptotic behavior of qn, it was realized that

E should have special properties. of the normalized counting measures of the ξ(n)

j

: 1 2n

2n

  • ℓ=1

δξ(n)

w∗

− → ν.

slide-105
SLIDE 105

Symmetric contours

slide-106
SLIDE 106

Symmetric contours

  • A weighted S-contour in the field ψ is a compact set E which

is an analytic arc in the neighborhood of q.e. point, and such that at every such point ∂ (V ωE,ψ + ψ) /∂n+ = ∂ (V ωE,ψ + ψ) /∂n− where ∂±n indicates normal derivatives from each side.

slide-107
SLIDE 107

Symmetric contours

  • A weighted S-contour in the field ψ is a compact set E which

is an analytic arc in the neighborhood of q.e. point, and such that at every such point ∂ (V ωE,ψ + ψ) /∂n+ = ∂ (V ωE,ψ + ψ) /∂n− where ∂±n indicates normal derivatives from each side.

  • The notion was introduced in nuce by [Nutall, 70’s] and

expounded by [Stahl, 1985] in the unweighted case, suitable to study classical Pad´ e aproximants.

slide-108
SLIDE 108

Symmetric contours

  • A weighted S-contour in the field ψ is a compact set E which

is an analytic arc in the neighborhood of q.e. point, and such that at every such point ∂ (V ωE,ψ + ψ) /∂n+ = ∂ (V ωE,ψ + ψ) /∂n− where ∂±n indicates normal derivatives from each side.

  • The notion was introduced in nuce by [Nutall, 70’s] and

expounded by [Stahl, 1985] in the unweighted case, suitable to study classical Pad´ e aproximants. He showed that when ψ = 0 then the zeros ζ{n}

1

, · · · , ζ{n}

n

  • f qn satisfy

µn := 1 n

n

  • ℓ=1

δζ{n}

w∗

− → ωE.

slide-109
SLIDE 109

Symmetric contours

  • A weighted S-contour in the field ψ is a compact set E which

is an analytic arc in the neighborhood of q.e. point, and such that at every such point ∂ (V ωE,ψ + ψ) /∂n+ = ∂ (V ωE,ψ + ψ) /∂n− where ∂±n indicates normal derivatives from each side.

  • The notion was introduced in nuce by [Nutall, 70’s] and

expounded by [Stahl, 1985] in the unweighted case, suitable to study classical Pad´ e aproximants. He showed that when ψ = 0 then the zeros ζ{n}

1

, · · · , ζ{n}

n

  • f qn satisfy

µn := 1 n

n

  • ℓ=1

δζ{n}

w∗

− → ωE. Like in classical case on a segment.

slide-110
SLIDE 110

Symmetric contours

  • A weighted S-contour in the field ψ is a compact set E which

is an analytic arc in the neighborhood of q.e. point, and such that at every such point ∂ (V ωE,ψ + ψ) /∂n+ = ∂ (V ωE,ψ + ψ) /∂n− where ∂±n indicates normal derivatives from each side.

  • The notion was introduced in nuce by [Nutall, 70’s] and

expounded by [Stahl, 1985] in the unweighted case, suitable to study classical Pad´ e aproximants. He showed that when ψ = 0 then the zeros ζ{n}

1

, · · · , ζ{n}

n

  • f qn satisfy

µn := 1 n

n

  • ℓ=1

δζ{n}

w∗

− → ωE. Like in classical case on a segment.

  • Dwelling on his work, Gonchar and Rakhmanov generalized

the result to the multipoint case as follows.

slide-111
SLIDE 111

The Gonchar-Rakhmanov theorem

slide-112
SLIDE 112

The Gonchar-Rakhmanov theorem

Theorem [Gonchar-Rachmanov,87] If f is (essentially) a Cauchy integral on a weighted S-contour E in the field −V ν, with q.e. continuous nonzero density on E, and if the interpolation points ξ(n)

1 , · · · , ξ(n) 2n are picked with asymptotic density ν on K:

νn := 1 2n

2n

  • ℓ=1

δξ(n)

w∗ −

→ ν, supp ν ⊂ K,

slide-113
SLIDE 113

The Gonchar-Rakhmanov theorem

Theorem [Gonchar-Rachmanov,87] If f is (essentially) a Cauchy integral on a weighted S-contour E in the field −V ν, with q.e. continuous nonzero density on E, and if the interpolation points ξ(n)

1 , · · · , ξ(n) 2n are picked with asymptotic density ν on K:

νn := 1 2n

2n

  • ℓ=1

δξ(n)

w∗ −

→ ν, supp ν ⊂ K, then the Pad´ e interpolants pn−1/qn in the points ξ(n)

converge in capacity to f in the complement of E: lim

n→∞ cap{z /

∈ E : |f (z) − pn−1(z)/qn(z)|1/n > ε} = 0.

slide-114
SLIDE 114

The Gonchar-Rakhmanov theorem

Theorem [Gonchar-Rachmanov,87] If f is (essentially) a Cauchy integral on a weighted S-contour E in the field −V ν, with q.e. continuous nonzero density on E, and if the interpolation points ξ(n)

1 , · · · , ξ(n) 2n are picked with asymptotic density ν on K:

νn := 1 2n

2n

  • ℓ=1

δξ(n)

w∗ −

→ ν, supp ν ⊂ K, then the Pad´ e interpolants pn−1/qn in the points ξ(n)

converge in capacity to f in the complement of E: lim

n→∞ cap{z /

∈ E : |f (z) − pn−1(z)/qn(z)|1/n > ε} = 0. and the normalized counting measure of their poles converges towards ωE,−Uν.

slide-115
SLIDE 115

Consequences

slide-116
SLIDE 116

Consequences

  • If f has finitely many branchpoints contained in K c, an open

set Ω exists to minimize C(K, Ω) with f analytic on Ω.

slide-117
SLIDE 117

Consequences

  • If f has finitely many branchpoints contained in K c, an open

set Ω exists to minimize C(K, Ω) with f analytic on Ω. Then E = Ωc is a weighted S-contour in the field −V ωG

K,Ω [Stahl

1989].

slide-118
SLIDE 118

Consequences

  • If f has finitely many branchpoints contained in K c, an open

set Ω exists to minimize C(K, Ω) with f analytic on Ω. Then E = Ωc is a weighted S-contour in the field −V ωG

K,Ω [Stahl

1989].

  • Pick ν = ωG

K,Ω; a computation shows that

(f − pn−1 qn )(z) = w2n q2

n

(z) 1 2iπ

  • E

fqn w2n (ξ) dξ z − ξ .

slide-119
SLIDE 119

Consequences

  • If f has finitely many branchpoints contained in K c, an open

set Ω exists to minimize C(K, Ω) with f analytic on Ω. Then E = Ωc is a weighted S-contour in the field −V ωG

K,Ω [Stahl

1989].

  • Pick ν = ωG

K,Ω; a computation shows that

(f − pn−1 qn )(z) = w2n q2

n

(z) 1 2iπ

  • E

fqn w2n (ξ) dξ z − ξ .

  • Taking moduli and 2n-th root, the surviving term is
  • w2n

q2

n

(z)

  • 1/2n

= exp log |w2n(z)| 2n − log |qn(z)| n

  • = exp {−V νn + V µn} → exp
  • V

ωG

K,Ec

G

(z)

  • . =

1 C(K, E) on K.

slide-120
SLIDE 120

Best H2-rational approximation

slide-121
SLIDE 121

Best H2-rational approximation

  • Gonchar-Rakhmanov theorem shows there are rational

interpolants with best n-th root approximation rate on K to functions with finitely many bnnranchpoints off K.

slide-122
SLIDE 122

Best H2-rational approximation

  • Gonchar-Rakhmanov theorem shows there are rational

interpolants with best n-th root approximation rate on K to functions with finitely many bnnranchpoints off K.

  • Moreover, when the degree goes large, the normalized

counting measure of the poles of these approximants converges to the Green equilibrium distribution on the cut of minimal Green capacity in K c outside f which f is single-valued.

slide-123
SLIDE 123

Best H2-rational approximation

  • Gonchar-Rakhmanov theorem shows there are rational

interpolants with best n-th root approximation rate on K to functions with finitely many bnnranchpoints off K.

  • Moreover, when the degree goes large, the normalized

counting measure of the poles of these approximants converges to the Green equilibrium distribution on the cut of minimal Green capacity in K c outside f which f is single-valued.

  • Is this also the behaviour of best approximants?
slide-124
SLIDE 124

Best H2 rational approximation and interpolation

slide-125
SLIDE 125

Best H2 rational approximation and interpolation

Let H2 be the familar Hardy space of the disk.

slide-126
SLIDE 126

Best H2 rational approximation and interpolation

Let H2 be the familar Hardy space of the disk. If f ∈ H2 and pn/qn is a rational function in H2 to minimize f − pn qn 2

2 := 1

  • T
  • f (ξ) − pn

qn (ξ)

  • 2

|dξ| with T the unit circle, then pn/qn interpolates f at 1/ξj with order 2 for each zero ξj of qn, and also at 0 [Levin, 76], [Della-Dora, 72].

slide-127
SLIDE 127

Best H2 rational approximation and interpolation

Let H2 be the familar Hardy space of the disk. If f ∈ H2 and pn/qn is a rational function in H2 to minimize f − pn qn 2

2 := 1

  • T
  • f (ξ) − pn

qn (ξ)

  • 2

|dξ| with T the unit circle, then pn/qn interpolates f at 1/ξj with order 2 for each zero ξj of qn, and also at 0 [Levin, 76], [Della-Dora, 72]. So, it is a particular case of multipoint Pad´ e interpolant (with unknown interpolation points).

slide-128
SLIDE 128

Asymptotics of H2 approximants

Theorem (H. Stahl, M. Yattselev, L.B., 2013)

Let f be analytic except for finitely many branchpoint off the closed unit disk, and pn/qn a best rational approximant of degree n in H2. The counting measure of the poles of pn/qn converges weak-* when n → ∞ to the equilibrium measure of the set KG of minimal Green capacity in C \ D outside of which f is single-valued.

slide-129
SLIDE 129

Asymptotics of H2 approximants

Theorem (H. Stahl, M. Yattselev, L.B., 2013)

Let f be analytic except for finitely many branchpoint off the closed unit disk, and pn/qn a best rational approximant of degree n in H2. The counting measure of the poles of pn/qn converges weak-* when n → ∞ to the equilibrium measure of the set KG of minimal Green capacity in C \ D outside of which f is single-valued. Moreover it holds that lim

n→∞ f − pn−1/qn1/2n L2(T) = e−1/Cap(T,KG ),

lim

n→∞ f − pn−1/qn1/2n L∞(T) = e−1/Cap(T,KG )

slide-130
SLIDE 130

Asymptotics of H2 approximants

Theorem (H. Stahl, M. Yattselev, L.B., 2013)

Let f be analytic except for finitely many branchpoint off the closed unit disk, and pn/qn a best rational approximant of degree n in H2. The counting measure of the poles of pn/qn converges weak-* when n → ∞ to the equilibrium measure of the set KG of minimal Green capacity in C \ D outside of which f is single-valued. Moreover it holds that lim

n→∞ f − pn−1/qn1/2n L2(T) = e−1/Cap(T,KG ),

lim

n→∞ f − pn−1/qn1/2n L∞(T) = e−1/Cap(T,KG )

The result is not a direct consequence of the Gonchar Rakhmanov theorem, for one needs to establish that there exists a S-contour in the field −V ν, where ν is the asymptotic distribution of the reciprocal of the poles of pn−1/qn (the interpolation points).

slide-131
SLIDE 131

The Parfenov-Prokhorov theorem

slide-132
SLIDE 132

The Parfenov-Prokhorov theorem

  • When the complement of K is connected, O.G. Parfenov

proved Gonchar’s conjecture in1986.

slide-133
SLIDE 133

The Parfenov-Prokhorov theorem

  • When the complement of K is connected, O.G. Parfenov

proved Gonchar’s conjecture in1986.

  • In 1994 the result was extended to the finitely connected case

by V. A. Prokhorov.

slide-134
SLIDE 134

The Parfenov-Prokhorov theorem

  • When the complement of K is connected, O.G. Parfenov

proved Gonchar’s conjecture in1986.

  • In 1994 the result was extended to the finitely connected case

by V. A. Prokhorov.

  • Whereas Gonchar-Rakhmanov did approach the conjecture

trying to construct approximants (interpolants), Parfenov’s proof is non-constructive and relies on the Adamjan-Arov-Krein theory of best meromorphic approximation, along with the observation that n-th root asymptotics in rational and meromorphic approximation are equivalent.

slide-135
SLIDE 135

The Parfenov-Prokhorov theorem

  • When the complement of K is connected, O.G. Parfenov

proved Gonchar’s conjecture in1986.

  • In 1994 the result was extended to the finitely connected case

by V. A. Prokhorov.

  • Whereas Gonchar-Rakhmanov did approach the conjecture

trying to construct approximants (interpolants), Parfenov’s proof is non-constructive and relies on the Adamjan-Arov-Krein theory of best meromorphic approximation, along with the observation that n-th root asymptotics in rational and meromorphic approximation are equivalent.

slide-136
SLIDE 136

Meromorphic approximation

slide-137
SLIDE 137

Meromorphic approximation

  • We approximate f on ∂K by the sum of a rational function

and (the trace of) a function in H∞(K c): emn := f −gn−rnL∞(∂K) = inf

g∈H∞(K c), rn∈Rn

f −g−rnL∞(∂K).

slide-138
SLIDE 138

Meromorphic approximation

  • We approximate f on ∂K by the sum of a rational function

and (the trace of) a function in H∞(K c): emn := f −gn−rnL∞(∂K) = inf

g∈H∞(K c), rn∈Rn

f −g−rnL∞(∂K).

  • In other words, we approximate f on ∂K by the trace of a

meromorphic function with at most n poles in K c. This makes conformal invariance obvious.

slide-139
SLIDE 139

Meromorphic approximation

  • We approximate f on ∂K by the sum of a rational function

and (the trace of) a function in H∞(K c): emn := f −gn−rnL∞(∂K) = inf

g∈H∞(K c), rn∈Rn

f −g−rnL∞(∂K).

  • In other words, we approximate f on ∂K by the trace of a

meromorphic function with at most n poles in K c. This makes conformal invariance obvious.

  • By the Cauchy formula

f (z) − rn(z) = 1 2iπ

  • ∂K

(f − rn − g)(t) t − z dt for z ∈

  • K,

which implies easily that lim sup e1/nk

nk

= lim sup em1/nk

nk

, lim inf e1/nk

nk

= lim inf em1/nk

nk

along any subsequence nk.

slide-140
SLIDE 140

Parfenov’s proof

slide-141
SLIDE 141

Parfenov’s proof

  • By conformal mapping assume K = C \ D with D the unit

disk, and Ω = C \ E, with E compact lying interior to the unit circle T.

slide-142
SLIDE 142

Parfenov’s proof

  • By conformal mapping assume K = C \ D with D the unit

disk, and Ω = C \ E, with E compact lying interior to the unit circle T.

  • By outer regularity of capacity, one may further assume that

∂E is a smooth Jordan curve Γ.

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SLIDE 143

Parfenov’s proof

  • By conformal mapping assume K = C \ D with D the unit

disk, and Ω = C \ E, with E compact lying interior to the unit circle T.

  • By outer regularity of capacity, one may further assume that

∂E is a smooth Jordan curve Γ.

  • AAK theory tells that the best error in uniform approximation

to f on T by meromorphic functions with n poles is the n + 1 singular value of the Hankel operator: Af : H2(D) → H2

0(C \ D)

u → P−(fu)

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SLIDE 144

Parfenov’s proof

  • By conformal mapping assume K = C \ D with D the unit

disk, and Ω = C \ E, with E compact lying interior to the unit circle T.

  • By outer regularity of capacity, one may further assume that

∂E is a smooth Jordan curve Γ.

  • AAK theory tells that the best error in uniform approximation

to f on T by meromorphic functions with n poles is the n + 1 singular value of the Hankel operator: Af : H2(D) → H2

0(C \ D)

u → P−(fu) where P− is the projection L2(T) → H2

0(C \ D) in the

  • rthogonal decomposition:

L2(T) = H2(D) ⊕ H2

0(C \ D).

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SLIDE 145

Parfenov’s proof cont’d

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SLIDE 146

Parfenov’s proof cont’d

  • By Cauchy formula

f (z) = 1 2iπ

  • Γ

f (ξ) z − ξ dξ, z ∈ Ω.

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SLIDE 147

Parfenov’s proof cont’d

  • By Cauchy formula

f (z) = 1 2iπ

  • Γ

f (ξ) z − ξ dξ, z ∈ Ω.

  • Moreover by the residue theorem

P−(h)(z) = 1 2iπ

  • T

h(ξ) z − ξ dξ, h ∈ L2(T), z ∈ C \ D.

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SLIDE 148

Parfenov’s proof cont’d

  • By Cauchy formula

f (z) = 1 2iπ

  • Γ

f (ξ) z − ξ dξ, z ∈ Ω.

  • Moreover by the residue theorem

P−(h)(z) = 1 2iπ

  • T

h(ξ) z − ξ dξ, h ∈ L2(T), z ∈ C \ D.

  • By the above, Fubini’s theorem, and the residue formula, we

get for v ∈ H2(D): Af (v)(z) = 1 2iπ

  • Γ

v(ξ)f (ξ) (z − ξ) dζ, z ∈ C \ D.

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SLIDE 149

Parfenov’s proof cont’d

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SLIDE 150

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

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SLIDE 151

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

  • B4 : H2(D) → L2(Γ) is the embedding operator obtained by

restricting functions to Γ,

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SLIDE 152

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

  • B4 : H2(D) → L2(Γ) is the embedding operator obtained by

restricting functions to Γ,

  • B3 : L2(Γ) → L2(Γ) is the multiplication by f ,
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SLIDE 153

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

  • B4 : H2(D) → L2(Γ) is the embedding operator obtained by

restricting functions to Γ,

  • B3 : L2(Γ) → L2(Γ) is the multiplication by f ,
  • B2 : L2(Γ) → S2(Ω) is the Cauchy projection onto the

Smirnov class of Ω,

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SLIDE 154

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

  • B4 : H2(D) → L2(Γ) is the embedding operator obtained by

restricting functions to Γ,

  • B3 : L2(Γ) → L2(Γ) is the multiplication by f ,
  • B2 : L2(Γ) → S2(Ω) is the Cauchy projection onto the

Smirnov class of Ω,

  • B1 : S2(Ω) → H2(C \ D) is the embedding operator arising by

restriction.

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SLIDE 155

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

  • B4 : H2(D) → L2(Γ) is the embedding operator obtained by

restricting functions to Γ,

  • B3 : L2(Γ) → L2(Γ) is the multiplication by f ,
  • B2 : L2(Γ) → S2(Ω) is the Cauchy projection onto the

Smirnov class of Ω,

  • B1 : S2(Ω) → H2(C \ D) is the embedding operator arising by

restriction.

  • B3, B2 are bounded, and for the singular values of B1, B4 we

have [Zakharyuta-Skiba, 1976][Fischer-Micchelli, 1980]: lim

k→∞ s1/k k

(B1) = lim

k→∞ s1/k k

(B4) = exp

1 C(C \ D, Γ)

  • .
slide-156
SLIDE 156

Parfenov’s proof cont’d

Therefore Af is the composition of four elementary operators: Af = B1 B2 B3 B4,

  • B4 : H2(D) → L2(Γ) is the embedding operator obtained by

restricting functions to Γ,

  • B3 : L2(Γ) → L2(Γ) is the multiplication by f ,
  • B2 : L2(Γ) → S2(Ω) is the Cauchy projection onto the

Smirnov class of Ω,

  • B1 : S2(Ω) → H2(C \ D) is the embedding operator arising by

restriction.

  • B3, B2 are bounded, and for the singular values of B1, B4 we

have [Zakharyuta-Skiba, 1976][Fischer-Micchelli, 1980]: lim

k→∞ s1/k k

(B1) = lim

k→∞ s1/k k

(B4) = exp

1 C(C \ D, Γ)

  • .
  • Spectral theoretic interpretation of “2”.
slide-157
SLIDE 157

Parfenov’s proof cont’d

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SLIDE 158

Parfenov’s proof cont’d

  • Applying now the Horn-Weyl inequalities:

Πn

k=0 sk(AB) ≤ Πn k=0 sk(A) Πn k=0 sk(B),

n ∈ N valid for any pair of bounded operators A : H1 → H2 and B : H2 → H3 between Hilbert spaces,

slide-159
SLIDE 159

Parfenov’s proof cont’d

  • Applying now the Horn-Weyl inequalities:

Πn

k=0 sk(AB) ≤ Πn k=0 sk(A) Πn k=0 sk(B),

n ∈ N valid for any pair of bounded operators A : H1 → H2 and B : H2 → H3 between Hilbert spaces,

  • we obtain

Πn

k=0 sk(Af ) ≤ |||B2|||n+1|||B3|||n+1Πn k=0 sk(B1)) Πn k=0 sk(B4),

slide-160
SLIDE 160

Parfenov’s proof cont’d

  • Applying now the Horn-Weyl inequalities:

Πn

k=0 sk(AB) ≤ Πn k=0 sk(A) Πn k=0 sk(B),

n ∈ N valid for any pair of bounded operators A : H1 → H2 and B : H2 → H3 between Hilbert spaces,

  • we obtain

Πn

k=0 sk(Af ) ≤ |||B2|||n+1|||B3|||n+1Πn k=0 sk(B1)) Πn k=0 sk(B4),

  • from which Parfenov’s theorem follows easily upon taking

1/n2-roots.

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SLIDE 161

Rational approximation to functions with polar singular set

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SLIDE 162

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints.

slide-163
SLIDE 163

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints. Let K ⊂ Ω be compact with K c connected.

slide-164
SLIDE 164

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints. Let K ⊂ Ω be compact with K c connected. Let Ω∗ maximize the Green capacity C(K, Ω∗) under the condition that f is analytic and single-valued in Ω∗.

slide-165
SLIDE 165

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints. Let K ⊂ Ω be compact with K c connected. Let Ω∗ maximize the Green capacity C(K, Ω∗) under the condition that f is analytic and single-valued in Ω∗. Then

slide-166
SLIDE 166

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints. Let K ⊂ Ω be compact with K c connected. Let Ω∗ maximize the Green capacity C(K, Ω∗) under the condition that f is analytic and single-valued in Ω∗. Then

  • limn→∞ e1/n

n

= exp

  • −2

C(K,Ω∗)

slide-167
SLIDE 167

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints. Let K ⊂ Ω be compact with K c connected. Let Ω∗ maximize the Green capacity C(K, Ω∗) under the condition that f is analytic and single-valued in Ω∗. Then

  • limn→∞ e1/n

n

= exp

  • −2

C(K,Ω∗)

  • If there is a branchpoint and K is regular, then the asymptotic

density of the poles ξ(n)

1 , · · · , ξ(n) n

  • f an asymptotically optimal

sequence rn of rational approximants of degree n is ωG

K,Ω∗:

1 nΣn

ℓ=1δξ(n)

w∗ −

→ ωG

K,Ω∗.

slide-168
SLIDE 168

Rational approximation to functions with polar singular set

Theorem (H. Stahl†, M.Yattselev, L.B.)

Let f be analytic in Ω ⊂ C and continuable indefinitely except over a polar set which has finitely many branchpoints. Let K ⊂ Ω be compact with K c connected. Let Ω∗ maximize the Green capacity C(K, Ω∗) under the condition that f is analytic and single-valued in Ω∗. Then

  • limn→∞ e1/n

n

= exp

  • −2

C(K,Ω∗)

  • If there is a branchpoint and K is regular, then the asymptotic

density of the poles ξ(n)

1 , · · · , ξ(n) n

  • f an asymptotically optimal

sequence rn of rational approximants of degree n is ωG

K,Ω∗:

1 nΣn

ℓ=1δξ(n)

w∗ −

→ ωG

K,Ω∗.

  • If there is no branchpoint convergence is faster than gometric,

but asymptotic distribution of poles is unknown.

slide-169
SLIDE 169

About the proof

slide-170
SLIDE 170

About the proof

  • We first prove the result for meromorphic approximants.
slide-171
SLIDE 171

About the proof

  • We first prove the result for meromorphic approximants.
  • Assume C(K, Ω) > 0. We know that

lim inf

n→∞ e1/n n

≤ exp

  • −2

C(KΩ)

  • (Parfenov).
slide-172
SLIDE 172

About the proof

  • We first prove the result for meromorphic approximants.
  • Assume C(K, Ω) > 0. We know that

lim inf

n→∞ e1/n n

≤ exp

  • −2

C(KΩ)

  • (Parfenov).

lim sup

n→∞ e1/n n

≤ exp

  • −1

C(K, Ω)

  • (Walsh).
slide-173
SLIDE 173

About the proof

  • We first prove the result for meromorphic approximants.
  • Assume C(K, Ω) > 0. We know that

lim inf

n→∞ e1/n n

≤ exp

  • −2

C(KΩ)

  • (Parfenov).

lim sup

n→∞ e1/n n

≤ exp

  • −1

C(K, Ω)

  • (Walsh).
  • Dwelling on Horn-Weyl inequalities for singular values of the

Hankel operator with symol f , we prove: lim sup

n→∞ e1/n n

> exp

  • −2

C(K, Ω)

  • =

⇒ lim inf

n→∞ e1/n n

< exp

  • −2

C(K, Ω)

  • .
slide-174
SLIDE 174

About the proof cont’d

slide-175
SLIDE 175

About the proof cont’d

  • In a second step, one shows that along any subsequence

lim inf e1/n

n

≥ exp

  • −2

C(K,Ω∗)

  • and that this speed of

convergence is attained only if the asymptotic density of the poles is ωG

(K,Ω∗)

slide-176
SLIDE 176

About the proof cont’d

  • In a second step, one shows that along any subsequence

lim inf e1/n

n

≥ exp

  • −2

C(K,Ω∗)

  • and that this speed of

convergence is attained only if the asymptotic density of the poles is ωG

(K,Ω∗)

  • This is done by analyzing the limit L, along a subsequence, of

(log en)/n on the Riemann surface of f . We use Bagemihl-type arguments on a maximal region containing the domain of convergence, yielding geometric interpretation of the 2.

slide-177
SLIDE 177

About the proof cont’d

  • In a second step, one shows that along any subsequence

lim inf e1/n

n

≥ exp

  • −2

C(K,Ω∗)

  • and that this speed of

convergence is attained only if the asymptotic density of the poles is ωG

(K,Ω∗)

  • This is done by analyzing the limit L, along a subsequence, of

(log en)/n on the Riemann surface of f . We use Bagemihl-type arguments on a maximal region containing the domain of convergence, yielding geometric interpretation of the 2.

  • One dificulty is that L is only finely continuous, but neither

subharmonic nor superharmonic.

slide-178
SLIDE 178

About the proof cont’d

  • In a second step, one shows that along any subsequence

lim inf e1/n

n

≥ exp

  • −2

C(K,Ω∗)

  • and that this speed of

convergence is attained only if the asymptotic density of the poles is ωG

(K,Ω∗)

  • This is done by analyzing the limit L, along a subsequence, of

(log en)/n on the Riemann surface of f . We use Bagemihl-type arguments on a maximal region containing the domain of convergence, yielding geometric interpretation of the 2.

  • One dificulty is that L is only finely continuous, but neither

subharmonic nor superharmonic.

  • In a final step we connect poles in rational approximation with

poles in meromorphic approximation. The result on the poles holds in fact for any sequence of approximant with optimal n-th root rate.

slide-179
SLIDE 179

Some experiments

−0.6 −0.4 −0.2 0.2 0.4 0.6 0.8 1 Poles [x] − Zeros [o]

slide-180
SLIDE 180

Some experiments

−0.6 −0.4 −0.2 0.2 0.4 0.6 0.8 1 Poles [x] − Zeros [o]

slide-181
SLIDE 181

A sad note

slide-182
SLIDE 182

A sad note

In memoriam Herbert Stahl, August 3, 1942–April 22, 2013.

slide-183
SLIDE 183

And most importantly Thank you!