HARMONIC HOMEOMORPHISMS: EXISTENCE AND NONEXISTENCE LEONID V. KOVALEV Abstract. These notes were prepared for International Workshop on Harmonic and Quasiconformal Mappings in Chennai, August 2010. They are based on several papers written jointly with Tadeusz Iwaniec, Jani Onninen, and Ngin-Tee Koh. The source papers are available from www.arxiv.org

Contents 1. Harmonic Mapping Problem and affine invariants 2. The Rad´o-Kneser-Choquet Theorem and approximation of homeomorphisms 3. The Nitsche conjecture and beyond References

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1. Harmonic Mapping Problem and affine invariants We study mappings f = u + iv : Ω → C defined in a domain Ω of the complex plane C = {z = x + iy : x, y ∈ R}. The partial differentiation in Ω will be expressed by the Wirtinger operators µ ¶ µ ¶ ∂ 1 ∂ ∂ ∂ 1 ∂ ∂ (1) = −i and = +i . ∂z 2 ∂x ∂y ∂ z¯ 2 ∂x ∂y Accordingly, we shall abbreviate the complex derivatives of f to µ ¶ µ ¶ ∂f 1 ∂f ∂f ∂f 1 ∂f ∂f (2) fz = = −i and fz¯ = = +i . ∂z 2 ∂x ∂y ∂ z¯ 2 ∂x ∂y For the derivative matrix ¸ · ux vx (3) Df (z) = u y vy we compute the operator norm and the Hilbert-Schmidt norm (4)

kDf k = |fz | + |fz¯|,

|Df |2 = 2(|fz |2 + |fz¯|2 ) = u2x + vx2 + u2y + vy2

Support from the National Science Foundation is gratefully acknowledged. 1

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LEONID V. KOVALEV

and the Jacobian determinant (5)

Jf (z) = det Df (z) = ux vy − uy vx = |fz |2 − |fz¯|2 .

We have Jf > 0 if the mapping is sense-preserving, which will usually be the case from now on. The condition of harmonicity reads as (6)

∆u = ∆v = 0,

or, equivalently, fz z¯ = 0

Thus, for any harmonic mapping f the functions fz and fz¯ are holomorphic. Taking (5) into account, we can write (7)

fz¯ = νfz ,

where ν is a holomorphic function, |ν| < 1 if f is sense-preserving. This is the Beltrami equation of second kind. The coefficient ν is invariant under conformal changes of variable z. The Harmonic Mapping Problem asks when there exists a harmonic bijective mapping between two given domains Ω and Ω∗ (one can ask the same question about two manifolds, or metric spaces, but here we restrict the consideration to domains in the complex plane C). Since a conformal mapping is harmonic, the case of simply connected domains is almost covered by the Riemann mapping theorem. Indeed, if neither of the domains is the entire plane C, then there is a conformal mapping, which is of course a harmonic bijection. A word of caution: the inverse of a harmonic mapping is generally not harmonic. Thus the mapping problem must take the order of the pair (Ω, Ω∗ ) into account. The studies of the Harmonic Mapping Problem began with Rad´o’s theonto orem (1927) which states that there is no harmonic bijection f : Ω −→ C for any proper domain Ω C. There is no harmonic bijection f : C → Ω either, which can be proved as follows. Suppose such f exists. Recall the function ν from (7) (the second Beltrami coefficient). Being bounded and holomorphic in C, it must be constant by Liouville’s theorem. It follows that f is an affine mapping; that is, f (z) = az + b¯ z + c with |a|2 − |b|2 6= 0. But then, of course, f (C) = C. Harmonic Mapping Problem for doubly connected domains originated from the work of Johannes C. C. Nitsche on minimal surfaces. In 1962 he conjectured [25] a precise condition that allows one circular annulus to be mapped onto another by a harmonic bijection. This conjecture will be the subject of the third lecture.

HARMONIC HOMEOMORPHISMS: EXISTENCE AND NONEXISTENCE

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Let A = A(r, R) := {z ∈ C : r < |z| < R} be a circular annulus in the complex plane (we allow 0 6 r < R 6 ∞). It is convenient to introduce the quantity Mod A := log Rr called the conformal modulus of an annulus. This notion extends to other doubly connected domains as follows: Mod Ω = Mod A if there is a conformal mapping of Ω onto A. (Any doubly connected domains can be conformally mapped onto some circular annulus.) The reason why Mod Ω is relevant to the Harmonic Mapping Problem is that harmonic functions remain harmonic upon conformal change of the independent variable z ∈ Ω. The harmonicity of a mapping f : Ω → Ω∗ is also preserved under affine transformations of the target Ω∗ . Thus it is natural to investigate necessary and sufficient conditions for the existence of f in terms of the conformal modulus of Ω and of some affine invariant of the target Ω∗ . This leads us to the concept of affine modulus. Definition 1. The affine modulus of a doubly connected domain Ω ⊂ C is defined by (8)

Mod@ Ω = sup{Mod φ(Ω) :

onto

φ : C −→ C affine}.

Obviously Mod@ Ω > Mod Ω. Exercise 2. (a) Find a doubly connected domain Ω for which Mod Ω < ∞ but Mod@ Ω = ∞. (b) Find a doubly connected domain Ω for which Mod@ Ω < ∞ but the supremum in (8) is not attained. (c) Find a doubly connected domain Ω for which Mod@ Ω = Mod Ω < ∞ (and prove this). In terms of Mod Ω and Mod@ Ω we can give both a necessary condition (Theorem 5 below) and a sufficient condition (Theorem 3) for the existence onto of a harmonic bijection f : Ω −→ Ω∗ . Theorem 3. Let Ω and Ω∗ be doubly connected domains in C such that (9)

Mod@ Ω∗ > Mod Ω.

Then there exists a harmonic homeomorphism f : Ω → Ω∗ unless C \ Ω∗ is bounded. In the latter case there is no such f . Problem 4. Does equality in (9) (with both sides finite) suffice for the existence of f ?

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LEONID V. KOVALEV

Theorem 5. If f : Ω → Ω∗ is a harmonic bijection between doubly connected domains, and Mod Ω < ∞, then (10)

Mod@ Ω∗ > Mod Ω · Φ(Mod Ω)

where Φ : (0, ∞) → (0, 1) is an increasing function such that Φ(τ ) → 1 as τ → ∞. One can take µ ¶ π2 log t − log(1 + log t) (11) Φ(τ ) = λ coth , where λ(t) = , t > 1. 2τ 2 + log t When Mod Ω → ∞, the comparison of inequalities (9) and (10) shows that both are asymptotically sharp. However, our function Φ can certainly be improved. Its best possible form is unknown. Conjecture 6. Suppose that f : Ω → Ω∗ is a harmonic bijection between doubly connected domains. Then (12)

Mod@ Ω∗ > log cosh Mod Ω.

The inequality (12) would be sharp, if true. ∼ Let us write Ω1 ,→ Ω2 when Ω1 is contained in Ω2 in such a way that Ω1 separates the boundary components of Ω2 . The monotonicity of modulus ∼ can be expressed by saying that Ω1 ,→ Ω2 implies Mod Ω1 6 Mod Ω2 and Mod@ Ω1 6 Mod@ Ω2 . Observe that both conditions (9) and (10) are preserved if Ω is replaced by a domain with a smaller conformal modulus, or Ω∗ is replaced by a domain with a greater affine modulus. Theorems 3 and 5 suggest the formulation of the following conjectural comparison principles. Problem 7. (Domain Comparison Principle) Let Ω and Ω∗ be doubly connected domains such that Mod Ω < ∞ and there exists a harmonic ∼ onto bijection f : Ω −→ Ω∗ . If Ω◦ ,→ Ω, then there exists a harmonic bijection onto f◦ : Ω◦ −→ Ω∗ . Problem 8. (Target Comparison Principle) Let Ω and Ω∗ be doubly onto connected domains such that there exists a harmonic bijection f : Ω −→ ∼ Ω∗ . If Mod Ω∗◦ < ∞ and Ω∗ ,→ Ω∗◦ , then there exists a harmonic bijection onto h◦ : Ω −→ Ω∗◦ . Let us now examine the properties of the affine modulus in more detail. The equality Mod@ Ω = Mod Ω is attained, for example, if Ω is the Teichm¨ uller ring (13)

T (s) := C \ ([−1, 0] ∪ [s, +∞)),

s>0

HARMONIC HOMEOMORPHISMS: EXISTENCE AND NONEXISTENCE

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Indeed, for any affine automorphism φ : C → C there is a C-affine automorphism ψ(z) = αz + β that agrees with φ on R. Since φ(T (s)) = ψ(T (s)) and ψ is conformal, it follows that Mod φ(T (s)) = Mod T (s). It is desirable to have an upper estimate for Mod@ Ω in terms of some geometric properties of Ω. Recall that the width of a compact set E ⊂ C, denoted w(E), is the smallest distance between two parallel lines that enclose the set. For connected sets this is also the length of the shortest 1-dimensional projection. Proposition 9. Let Ω be a doubly connected domain such that Mod Ω < ∞. Denote by d the distance between its boundary component, and by w the width of the inner boundary component. If w > 0, then (14)

Mod@ Ω 6 Mod T (d/w).

Proof. Let φ : C → C be an affine automorphism. Denote its Lipschitz constant by L := |φz | + |φz¯|. For the annulus φ(Ω) the distance between boundary components is at most Ld and the diameter of the inner component is at least Lw. Now the inequality (14) follows from the extremal property of the Teichm¨ uller ring: it has the greatest conformal modulus among all domains with given diameter of the bounded component and given distance between components [1]. ¤ Another canonical example of a doubly connected domain is the Gr¨ otzsch ring (15)

G(s) = {z ∈ C : |z| > 1} \ [s, +∞),

We claim that (16)

Mod@ G(s) = Mod T

s > 1.

¡ s−1 ¢ 2

Proposition 9 implies one half of (16). To obtain the reverse inequality, consider the images of G(s) under mappings of the form z + k¯ z , k % 1. They converge to the domain C \ ([−2, 2] ∪ [2s, ∞)) which is a rescaled copy ¢ ¡ of T s−1 2 . The identity (16) somewhat resembles the well-known relation between conformal moduli of the Gr¨otzsch and Teichm¨ uller rings [1], 1 (17) Mod G(s) = Mod T (s2 − 1). 2 Remark 10. Since equality holds in (16), Proposition 9 is sharp. The pair ¡ ¢ of domains Ω = T s−1 and Ω∗ = G(s) can serve as a test case for whether 2 equality in (9) implies the existence of a harmonic bijection.

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LEONID V. KOVALEV

´ -Kneser-Choquet Theorem and approximation of 2. The Rado homeomorphisms Let U ⊂ C be a bounded simply connected domain. For any continuous function f : ∂U → C there exists a unique continuous function PU f : U → C, called the Poisson modification of f , such that PU f is harmonic in U and agrees with f on ∂U . This is classical [10, 27]. The Rad´o-Kneser-Choquet theorem [8] is a simple and effective tool for construction of harmonic homeomorphism. Here is a strengthened version of it. Theorem 11. Let U and D be bounded simply connected domains in C with D convex. Suppose that f : ∂U → ∂D is a mapping that can be continuously extended to a homeomorphism of U onto D. Then PU f is a harmonic homeomorphism of U onto D. In other words, if there is some homeomorphic extension of f , then there is a harmonic homeomorphism extension (necessarily unique). The difference between Theorem 11 and the versions of the Rad´o-Kneser-Choquet theorem commonly found in the literature (e.g., [8]) is that U is not assumed to be a Jordan domain. Let us derive Theorem 11 from the Jordan case. onto

Proof. Let F : U −→ D be some homeomorphism that extends f . Denote g = PU f . It is not difficult to show that g(U ) = D; the issue is the injectivity of g. Let {Dn } be an exhaustion of D by convex domains. Define Un = −1 F (Dn ) and note that Un is a Jordan domain. By the Rad´o-KneserChoquet Theorem the mapping gn := PUn F is harmonic homeomorphism of Un onto Dn . As n → ∞, gn → PU f uniformly on compact subsets of U . This can be seen by harmonic measure estimates, or directly from the Wiener solution of the Dirichlet problem presented in [10]. The convergence of harmonic functions implies the convergence of their derivatives. Therefore Jgn → Jg pointwise, in particular Jg > 0. This means that the holomorphic functions gz and gz¯ satisfy the inequality |gz¯| 6 |gz |. The latter is only possible when either |gz¯| < |gz | in U or |gz¯| ≡ |gz | in U . The second case cannot occur, for it would yield Jg ≡ 0, contradicting g(U ) = D. Therefore Jh > 0, so the mapping g is locally invertible. But it is also a uniform limit of homeomorphisms gn (locally), which implies that h is injective in U . ¤

HARMONIC HOMEOMORPHISMS: EXISTENCE AND NONEXISTENCE

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Exercise 12. Show that Theorem 11 fails in the following situations. (a) U is a bounded Jordan domain, D is an unbounded convex domain. (b) U and D are bounded doubly connected domains, the boundary of D consists of two convex Jordan curves. The Rad´o-Kneser-Choquet Theorem was recently applied to the approximation problem for Sobolev homeomorphisms [15]. Let Ω be a bounded domain in C, 1 6 p < ∞. For a continuously differentiable function f : Ω → C the Sobolev W 1,p norm is defined by Z Z p p (18) kf k1,p = |f | + |Df |p . Ω



By definition, a function f ∈ Lp (Ω) belongs to the Sobolev space W 1,p (Ω) if it is the limit of a sequence of smooth functions fj that form a Cauchy sequence with respect to the norm k·k1,p . (There are more elegant definitions, but this one suffices for our purposes.) Problem 13. Suppose that f ∈ W 1,p (Ω) is a homeomorphism of Ω onto another domain Ω∗ . Can we choose an approximating sequence {fj } so that each fj is a diffeomorphism of Ω onto Ω∗ ? A different (but logically equivalent in dimensions n 6 3) version of the above problem asks for fj to be piecewise affine invertible mappings. In this form the approximation problem was put forward by J. M. Ball [3] who attributed it to L.C. Evans. The paper [15] gives the affirmative solution of the Ball-Evans problem in the case p = n = 2 (that is, W 1,2 in a planar domain). The construction of an approximating diffeomorphism involves five consecutive modifications of f . Steps 1, 2, and 4 are Poisson modifications based on the Rad´o-KneserChoquet Theorem, while the other steps are an explicit smoothing procedure adopted from J. Munkres [24]. The condition p = 2 comes into play because the Poisson modification does not increase the integral of |Df |2 . To make the proof work for p 6= 2, one needs a p-harmonic version of the Rad´oKneser-Choquet Theorem. Question 14. Is there a version of the Rad´o-Kneser-Choquet theorem for p-harmonic mappings, p 6= 2? That is, given two Jordan domains U, D ⊂ C onto with D convex, does the p-harmonic extension of a homeomorphism ∂U −→ onto ∂D yield a homeomorphism U −→ D?

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LEONID V. KOVALEV

It may be the case that additional geometric assumptions on D are needed for Question 14 to have an affirmative answer. In higher dimensions the Ball-Evans problem presents additional challenges, for example, the Rad´oKneser-Choquet theorem fails in dimensions n > 3 even when U and D are the unit ball [21]. 3. The Nitsche conjecture and beyond Let A = A(r, R) := {z ∈ C : r < |z| < R} be a circular annulus in the complex plane. Schottky’s theorem (1877) asserts that A(r, R) can be mapped conformally onto another annulus A∗ = A(r∗ , R∗ ) if and only if (19)

R R∗ , = r r∗

this is why the conformal modulus Mod Ω of a doubly connected domain Ω is well-defined. Since harmonic mappings are more flexible than conformal ones, one may ask: When does there exist a bijective harmonic mapping of A(r, R) onto A(r∗ , R∗ )? In 1962 Johannes C. C. Nitsche conjectured that such a mapping exists if and only if µ ¶ R∗ 1 R r (20) > + r∗ 2 r R How did he come up with this conjecture? He tried radial mappings, that onto is, f : A −→ A∗ of the form (21)

f (ρeiθ ) = g(ρ)eiθ

for some strictly monotone function g. From Laplace’s equation ∆f = 0 one sees that g must be of the form g(ρ) = Aρ + Bρ−1 . Since g must also be monotone, the coefficients A and B satisfy a certain inequality, and this is where (20) comes from. But of course, harmonic mappings between annuli do not have to be radial. Even explicit non-radial examples may be given. It is convenient to scale both annuli so that the inner radius of each is 1; that is, r = r∗ = 1. Define z+a (22) f (z) = + c log|z|, z∈A 1+a ¯z where a, c ∈ C and |a| < 1. Clearly, f maps the unit circle onto itself. The outer boundary of A is also mapped onto a circle, and we can choose c so that it will be centered at 0. (This value of c depends on a and R.) We

HARMONIC HOMEOMORPHISMS: EXISTENCE AND NONEXISTENCE

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also want the mapping f to be injective in A. After consideration of the boundary values of f it remains to check that its Jacobian determinant ¯ ¯2 ¯ ¯2 ¯ ∂f ¯ ¯ ∂f ¯ (23) Jf := ¯¯ ¯¯ − ¯¯ ¯¯ ∂z ∂ z¯ is positive in A. This leads to an upper bound on |a| which depends on R. Eventually one finds that the mappings (22) do not give a counterexample to the Nitsche conjecture: all this work was for nought. Exercise 15. Find a harmonic bijection between circular annuli that is not of the form (21) or (22). The Nitsche conjecture was proved in [11, 12]. The proof is far too long to discuss here in detail, but I will indicate some of the ideas. Under the normalization r = r∗ = 1 we prove the integral inequality µ ¶ Z 1 2 1 2 (24) U (ρ) := − |f | > ρ+ , 1<ρ e (fat domain). To understand the difference, consider the representation X (25) f (z) = fn (z) n∈Z

zn

/¯ zn

where fn (z) = an + bn for n 6= 0; also f0 (z) = a0 log|z| + b0 . This representation is orthogonal on every circle Tρ , which links it directly to the quantity U (ρ): XZ (26) U (ρ) := − |fn |2 . n∈Z Tρ

For example, the initial value conditions U (1) = 1 and U 0 (1) > 0 translate into inequalities involving the coefficients of fn . The most difficult term to handle is f0 , as it grows slowly and lacks the convexity properties shared by fn for n 6= 0. When ρ is small, the logarithmic term is somewhat comparable to the powers of ρ, and the contribution of f0 to (26) is still usable. But when ρ is large, |f0 | contributes a negligible amount to (26) while its effect on

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LEONID V. KOVALEV

U (1) and U 0 (1) can still be substantial. This is the main cause of difficulties. (Indeed, the special case b0 = 0 admits a relatively short proof [11].) We successfully solved the “fat domain” case after careful consideration of harmonic bijections of the unit disk D = {z ∈ C : |z| < 1} onto itself. The following area contraction result came as a follow-up to this investigation. Let Dr = {z : |z| < r}; the area of a set E will be denoted by |E|. onto

Theorem 16. [20] Let f : D −→ D be a bijective harmonic mapping. Then (27)

|f (Dr )| 6 |Dr |,

0 < r < 1.

The area contraction inequality (27) is also true for any holomorphic mapping f : D → D (Exercise: prove this.) However, the following problem remains open. Problem 17. Does (27) hold for injective harmonic mappings f : D → D? Or even for arbitrary harmonic mappings f : D → D? Let us now take another look at mappings between annuli, from the viewpoint of quasiconformality. Recall the distortion theorems of H. Gr¨otzsch (1928) which presaged the development of the theory of quasiconformal mappings [1]. onto

Theorem 18. If f : A(r, R) −→ A(r∗ , R∗ ) is a K-quasiconformal mapping, then µ ¶1/K µ ¶K R R R∗ (28) 6 6 . r r∗ r Equalities are attained, uniquely modulo conformal automorphisms of A, 1 for the multiples of the mappings f (z) = |z| K −1 z and h(z) = |z|K−1 z, respectively. We notice at once that the extremal mappings in Theorem 18 fail to be harmonic except for K = 1. This naturally leads one to expect a better inequality for harmonic quasiconformal mappings. And indeed, we have the following sharp result. onto

Theorem 19. [13] If f : A(r, R) −→ A(r∗ , R∗ ) is a K-quasiconformal harmonic mapping, then R∗ K +1R K −1 r (29) > + . r∗ 2K r 2K R Equality is attained, uniquely modulo conformal automorphisms of A, for K +1z K −1r (30) f (z) = + . 2K r 2K z¯

HARMONIC HOMEOMORPHISMS: EXISTENCE AND NONEXISTENCE

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In contrast to (28), the inequality (29) is one-sided: it only gives the lower bound for the modulus of the image. There is a natural conjecture for the upper bound, but it remains open. onto

Conjecture 20. If f : A(r, R) −→ A(r∗ , R∗ ) is a K-quasiconformal harmonic mapping, then (31)

K +1R K −1 r R∗ 6 − . r∗ 2 r 2 R

Equality is attained, uniquely modulo conformal automorphisms of A, for z K−1 r f (z) = K+1 2 r − 2 z¯ . Theorem 19 and Conjecture 20 impose more constraints on f than the original Nitsche conjecture did. In the opposite direction, one can try to remove as many assumptions as possible. For instance, circular shapes and invertibility of f are not imposed in the following conjecture. Conjecture 21. (Reverse Harnack Inequality) Let Ω ⊂ C be a doubly connected domain. Suppose that f : Ω → C◦ = C \ {0} is a harmonic mapping that is not homotopic to a constant within the class of continuous mappings from Ω to C◦ . Then µ ¶ supΩ |h| 1 (32) > cosh Mod Ω inf Ω |h| 2 If h is in addition injective, then the factor 1/2 can be omitted. The mapping h(z) = z + z1¯ and the domain Ω = A(1/R, R) turn (32) into an equality. The mapping h also provides an injective example when restricted to the annulus A(1, R). The theorems and conjectures stated above have implications for the theory of minimal surfaces, which we do not pursue here. See [12, 13]. References 1. L. V. Ahlfors, Lectures on quasiconformal mappings, 2nd ed. University Lecture Series, 38. American Mathematical Society, Providence, RI, 2006. 2. K. Astala, T. Iwaniec, and G. J. Martin, Elliptic partial differential equations and quasiconformal mappings in the plane, Princeton University Press, 2009. 3. J. M. Ball, Singularities and computation of minimizers for variational problems, Foundations of computational mathematics (Oxford, 1999), 1–20, London Math. Soc. Lecture Note Ser., 284, Cambridge Univ. Press, Cambridge, 2001. older continuous homeomor4. J. C. Bellido and C. Mora-Corral, Approximation of H¨ phisms by piecewise affine homeomorphisms, Houston J. Math., to appear. 5. D. Bshouty and W. Hengartner, Univalent solutions of the Dirichlet problem for ring domains, Complex Variables Theory Appl. 21 (1993), no. 3–4, 159–169.

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6. D. Bshouty and W. Hengartner, Univalent harmonic mappings in the plane, Ann. Univ. Mariae Curie-SkÃlodowska Sect. A 48 (1994), 12–42. ¨ 7. T. Carleman, Uber ein Minimalproblem der mathematischen Physik, Math. Z. 1 (1918), no. 2–3, 208–212. 8. P. Duren, Harmonic mappings in the plane, Cambridge University Press, Cambridge, 2004. 9. P. Duren and W. Hengartner, Harmonic mappings of multiply connected domains, Pacific J. Math. 180 (1997), no. 2, 201–220. 10. J. B. Garnett and D. E. Marshall, Harmonic measure, Cambridge Univ. Press, Cambridge, 2005. 11. T. Iwaniec, L. V. Kovalev, and J. Onninen, Harmonic mappings of an annulus, Nitsche conjecture and its generalizations, Amer. J. Math., to appear. 12. T. Iwaniec, L. V. Kovalev, and J. Onninen, The Nitsche conjecture, arXiv:0908.1253. 13. T. Iwaniec, L. V. Kovalev, and J. Onninen, Doubly connected minimal surfaces and extremal harmonic mappings, arXiv:0912.3542. 14. T. Iwaniec, L. V. Kovalev, and J. Onninen, Harmonic mapping problem and affine capacity, arXiv:1001.2124. 15. T. Iwaniec, L. V. Kovalev, and J. Onninen, Hopf differentials and smoothing Sobolev homeomorphisms, arXiv:1006.5174. 16. J. Jost, Two-dimensional geometric variational problems, John Wiley & Sons, Ltd., Chichester, 1991. 17. J. Jost and R. Schoen, On the existence of harmonic diffeomorphisms, Invent. Math. 66 (1982), no. 2, 353–359. 18. D. Kalaj, On the Nitsche conjecture for harmonic mappings in R2 and R3 . Israel J. Math. 150 (2005), 241–251. 19. D. Kalaj and M. Mateljevi´c, Quasiconformal and harmonic mappings between smooth Jordan domains, Novi Sad J. Math. 38 (2008), no. 3, 147–156. 20. N.-T. Koh and L. V. Kovalev, Area contraction for harmonic automorphisms of the disk, arXiv: 21. R. S. Laugesen, Injectivity can fail for higher-dimensional harmonic extensions, Complex Variables Theory Appl. 28 (1996), no. 4, 357–369. 22. A. Lyzzaik, The modulus of the image annuli under univalent harmonic mappings and a conjecture of J.C.C. Nitsche, J. London Math. Soc., 64 (2001), 369–384. 23. V. Markovi´c and M. Mateljevi´c, A new version of the main inequality and the uniqueness of harmonic maps, J. Analyse Math. 79 (1999), 315–334. 24. J. Munkres, Obstructions to the smoothing of piecewise-differentiable homeomorphisms, Ann. of Math. (2) 72 (1960), 521–554. 25. J. C. C. Nitsche, On the modulus of doubly connected regions under harmonic mappings, Amer. Math. Monthly, 69 (1962), 781–782. 26. R. Osserman, A survey of minimal surfaces, Van Nostrand Reinhold Co., New YorkLondon-Melbourne (1969). 27. T. Ransford, Potential theory in the complex plane, Cambridge University Press, Cambridge, 1995. 28. R. Schoen, Analytic aspects of the harmonic map problem, in “Seminar on nonlinear partial differential equations” (Berkeley, Calif., 1983), 321–358, Math. Sci. Res. Inst. Publ., 2, Springer, New York, 1984. 29. A. Weitsman, Univalent harmonic mappings of annuli and a conjecture of J.C.C. Nitsche, Israel J. Math., 124 (2001), 327–331. Department of Mathematics, Syracuse University, Syracuse, NY 13244, USA E-mail address: [email protected]

HARMONIC HOMEOMORPHISMS: EXISTENCE AND ...

F−1(Dn) and note that Un is a Jordan domain. By the Radó-Kneser-. Choquet Theorem the mapping gn := PUn F is harmonic homeomorphism of Un onto Dn. As n → ∞, gn → PU f uniformly on compact subsets of. U. This can be seen by harmonic measure estimates, or directly from the. Wiener solution of the Dirichlet ...

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is one of the most celebrated infinite series of mathematics. As a counterexam- ple, few series more clearly illustrate that the convergence of terms to zero is not sufficient to guarantee the convergence of a series. As a known series, only a handfu

Harmonic Dynamics and Transition to Chaos in a ...
the parametric electromechanical system using analytical method. We find the harmonic oscillatory states both in the nonlinear and linear cases using the ...

Boundary Element Formulation of Harmonic ... - Semantic Scholar
On a deeper level, BEM makes possible the comparison of trans- finite harmonic ... Solving a Dirichlet problem could seem a high price to pay, but the quality of the .... Euclidean space, and not just to some large yet bounded domain. This task ...

Peeter Joot [email protected] Harmonic ...
[email protected]. Harmonic oscillator and displacement coordinates. Motivation In lattice ... with a number of masses all harmonically coupled. Two body harmonic oscillator in 3D For the system illustrated in fig. .... to bring the masses into c

man-40\harmonic-oscillator-kinematics.pdf
Connect more apps... Try one of the apps below to open or edit this item. man-40\harmonic-oscillator-kinematics.pdf. man-40\harmonic-oscillator-kinematics.pdf.

The Existence and Uniqueness of Monotone Pure ... - Semantic Scholar
Jun 5, 2006 - of Athey (2001). Our contribution is to establish a simple condition that ensures both ... effect), and the strategy profile of its opponents (a strategic interaction). Our sufficient ...... Figure 1: Illustration of Theorem 1 since the

Sharp existence and uniqueness theorems for non ...
data (2.15), there is a smooth solution (φ,ψ,aj ,bj ) with φ realizing these zeros if and ..... In view of (3.7), we see that we may choose μ > 0 large enough so that.