On the logarithm of the minimizing integrand for certain variational problems in two dimensions

Similar documents
figuresection σ FINITENESS OF A CERTAIN BOREL MEASURE ASSOCIATED WITH A POSITIVE WEAK SOLUTION TO A QUASILINEAR ELLIPTIC PDE IN SPACE

NECESSARY CONDITIONS FOR WEIGHTED POINTWISE HARDY INEQUALITIES

HIGHER INTEGRABILITY WITH WEIGHTS

MAT 578 FUNCTIONAL ANALYSIS EXERCISES

Hardy inequalities and thickness conditions

THE L 2 -HODGE THEORY AND REPRESENTATION ON R n

Follow links Class Use and other Permissions. For more information, send to:

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction

Growth estimates through scaling for quasilinear partial differential equations

Ahmed Mohammed. Harnack Inequality for Non-divergence Structure Semi-linear Elliptic Equations

Mathematical Research Letters 4, (1997) HARDY S INEQUALITIES FOR SOBOLEV FUNCTIONS. Juha Kinnunen and Olli Martio

PROBLEMS. (b) (Polarization Identity) Show that in any inner product space

Shock Reflection-Diffraction, Nonlinear Conservation Laws of Mixed Type, and von Neumann s Conjectures 1

PACKING-DIMENSION PROFILES AND FRACTIONAL BROWNIAN MOTION

TD M1 EDP 2018 no 2 Elliptic equations: regularity, maximum principle

WELL-POSEDNESS OF A RIEMANN HILBERT

INTEGRABILITY OF SUPERHARMONIC FUNCTIONS IN A JOHN DOMAIN. Hiroaki Aikawa

2.4 Hilbert Spaces. Outline

STABILITY FOR DEGENERATE PARABOLIC EQUATIONS. 1. Introduction We consider stability of weak solutions to. div( u p 2 u) = u

Mapping problems and harmonic univalent mappings

Packing-Dimension Profiles and Fractional Brownian Motion

New Identities for Weak KAM Theory

THE BRUNN-MINKOWSKI INEQUALITY AND A MINKOWSKI PROBLEM FOR NONLINEAR CAPACITY

PROPERTIES OF CAPACITIES IN VARIABLE EXPONENT SOBOLEV SPACES

HOMEOMORPHISMS OF BOUNDED VARIATION

MODULUS AND CONTINUOUS CAPACITY

COMPOSITION SEMIGROUPS ON BMOA AND H AUSTIN ANDERSON, MIRJANA JOVOVIC, AND WAYNE SMITH

Splitting methods with boundary corrections

Everywhere differentiability of infinity harmonic functions

Applied Analysis (APPM 5440): Final exam 1:30pm 4:00pm, Dec. 14, Closed books.

Continuity of weakly monotone Sobolev functions of variable exponent

ON BOUNDEDNESS OF MAXIMAL FUNCTIONS IN SOBOLEV SPACES

ON A MAXIMAL OPERATOR IN REARRANGEMENT INVARIANT BANACH FUNCTION SPACES ON METRIC SPACES

Partial Differential Equations, 2nd Edition, L.C.Evans The Calculus of Variations

Problem Set 5: Solutions Math 201A: Fall 2016

MATH 263: PROBLEM SET 1: BUNDLES, SHEAVES AND HODGE THEORY

Second Order Elliptic PDE

Complex Analysis, Stein and Shakarchi Meromorphic Functions and the Logarithm

A NOTE ON CORRELATION AND LOCAL DIMENSIONS

Murat Akman. The Brunn-Minkowski Inequality and a Minkowski Problem for Nonlinear Capacities. March 10

Lecture No 1 Introduction to Diffusion equations The heat equat

Computations of Critical Groups at a Degenerate Critical Point for Strongly Indefinite Functionals

Sharp Sobolev Strichartz estimates for the free Schrödinger propagator

1 Math 241A-B Homework Problem List for F2015 and W2016

Conjugate Harmonic Functions and Clifford Algebras

ON A CERTAIN GENERALIZATION OF THE KRASNOSEL SKII THEOREM

SYMMETRY OF POSITIVE SOLUTIONS OF SOME NONLINEAR EQUATIONS. M. Grossi S. Kesavan F. Pacella M. Ramaswamy. 1. Introduction

APPROXIMATION BY LIPSCHITZ FUNCTIONS IN ABSTRACT SOBOLEV SPACES ON METRIC SPACES

EQUADIFF 1. Rudolf Výborný On a certain extension of the maximum principle. Terms of use:

Minimal Surface equations non-solvability strongly convex functional further regularity Consider minimal surface equation.

REMOVABLE SINGULARITIES FOR BOUNDED p-harmonic AND QUASI(SUPER)HARMONIC FUNCTIONS ON METRIC SPACES

PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS

Probability and Measure

Math 410 Homework 6 Due Monday, October 26

A CONNECTION BETWEEN A GENERAL CLASS OF SUPERPARABOLIC FUNCTIONS AND SUPERSOLUTIONS

Bounded point derivations on R p (X) and approximate derivatives

Geometry and the Kato square root problem

On harmonic and QC maps

LECTURE # 0 BASIC NOTATIONS AND CONCEPTS IN THE THEORY OF PARTIAL DIFFERENTIAL EQUATIONS (PDES)

Positive eigenfunctions for the p-laplace operator revisited

Analytic families of multilinear operators

Theory of PDE Homework 2

Estimates in surfaces with positive constant Gauss curvature

AN ASYMPTOTIC MEAN VALUE CHARACTERIZATION FOR p-harmonic FUNCTIONS. To the memory of our friend and colleague Fuensanta Andreu

A lower bound for the Bloch radius of K-quasiregular mappings

Chain Rule for planar bi Sobolev maps

The Dirichlet s P rinciple. In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation:

A LOCALIZATION PROPERTY AT THE BOUNDARY FOR MONGE-AMPERE EQUATION

Weights, inequalities and a local HÖlder norm for solutions to ( / t-l)(u)=divf on bounded domains

arxiv: v1 [math.sp] 11 Jun 2010

HOPF S LEMMA FOR A CLASS OF SINGULAR/DEGENERATE PDE-S

b i (µ, x, s) ei ϕ(x) µ s (dx) ds (2) i=1

David E. Barrett and Jeffrey Diller University of Michigan Indiana University

COINCIDENCE SETS IN THE OBSTACLE PROBLEM FOR THE p-harmonic OPERATOR

Regularity and nonexistence results for anisotropic quasilinear elliptic equations in convex domains

Iteration of analytic self-maps of the disk: an overview 1 2

A PHYSICAL SPACE PROOF OF THE BILINEAR STRICHARTZ AND LOCAL SMOOTHING ESTIMATES FOR THE SCHRÖDINGER EQUATION

FIXED POINT METHODS IN NONLINEAR ANALYSIS

Minimal Surfaces: Nonparametric Theory. Andrejs Treibergs. January, 2016

Sobolev Spaces. Chapter Hölder spaces

Estimates for Bergman polynomials in domains with corners

Citation Osaka Journal of Mathematics. 41(4)

ABELIAN COVERINGS, POINCARÉ EXPONENT OF CONVERGENCE AND HOLOMORPHIC DEFORMATIONS

Nonlinear aspects of Calderón-Zygmund theory

Measure and Integration: Solutions of CW2

CRITICAL POINT METHODS IN DEGENERATE ANISOTROPIC PROBLEMS WITH VARIABLE EXPONENT. We are interested in discussing the problem:

A capacity approach to the Poincaré inequality and Sobolev imbeddings in variable exponent Sobolev spaces

On John type ellipsoids

MATH 126 FINAL EXAM. Name:

Math The Laplacian. 1 Green s Identities, Fundamental Solution

Geometry and the Kato square root problem

arxiv: v1 [math.mg] 25 May 2008

EXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE. Leszek Gasiński

Holder regularity for hypoelliptic kinetic equations

SUBELLIPTIC CORDES ESTIMATES

Stability for parabolic quasiminimizers. Y. Fujishima, J. Habermann, J. Kinnunen and M. Masson

NULL SETS FOR DOUBLING AND DYADIC DOUBLING MEASURES

ALUR DUAL RENORMINGS OF BANACH SPACES SEBASTIÁN LAJARA

Quasiconformal and Lipschitz harmonic mappings of the unit disk onto bounded convex domains

SOLUTIONS TO SOME PROBLEMS

Transcription:

On the logarithm of the minimizing integrand for certain variational problems in two dimensions University of Kentucky John L. Lewis University of Kentucky Andrew Vogel Syracuse University 2012 Spring Central Section Meeting University of Kansas, Lawrence, KS March 31, 2012

Outline 1 Introduction 2 Main Result 3 Inspired Results 4 Future Work

Outline 1 Introduction 2 Main Result 3 Inspired Results 4 Future Work

Notations and Definitions Let Ω denote a bounded region in the complex plane C. Given p, 1 < p <, let z = x 1 + ix 2 denote points in C and let W 1,p (Ω) denote equivalence classes of functions h : C R with distributional gradient h = h x1 + ih x2 and Sobolev norm h W 1,p (Ω) = ( ( h p + h p )da) 1/p < Ω where da denotes two dimensional Lebesgue measure.

Notations and Definitions Let Ω denote a bounded region in the complex plane C. Given p, 1 < p <, let z = x 1 + ix 2 denote points in C and let W 1,p (Ω) denote equivalence classes of functions h : C R with distributional gradient h = h x1 + ih x2 and Sobolev norm h W 1,p (Ω) = ( ( h p + h p )da) 1/p < Ω where da denotes two dimensional Lebesgue measure. Let C0 (Ω) denote infinitely differentiable functions with compact support in Ω and let W 1,p 0 (Ω) denote the closure of C0 (Ω) in the norm of W 1,p (Ω).

Notations and Definitions Let Ω denote a bounded region in the complex plane C. Given p, 1 < p <, let z = x 1 + ix 2 denote points in C and let W 1,p (Ω) denote equivalence classes of functions h : C R with distributional gradient h = h x1 + ih x2 and Sobolev norm h W 1,p (Ω) = ( ( h p + h p )da) 1/p < Ω where da denotes two dimensional Lebesgue measure. Let C0 (Ω) denote infinitely differentiable functions with compact support in Ω and let W 1,p 0 (Ω) denote the closure of C0 (Ω) in the norm of W 1,p (Ω). Let f : C \ {0} (0, ) be homogeneous of degree p on C \ {0}. That is, f (η) = η p f ( η ) > 0 when η C \ {0}. η

Notations and Definitions Let Ω denote a bounded region in the complex plane C. Given p, 1 < p <, let z = x 1 + ix 2 denote points in C and let W 1,p (Ω) denote equivalence classes of functions h : C R with distributional gradient h = h x1 + ih x2 and Sobolev norm h W 1,p (Ω) = ( ( h p + h p )da) 1/p < Ω where da denotes two dimensional Lebesgue measure. Let C0 (Ω) denote infinitely differentiable functions with compact support in Ω and let W 1,p 0 (Ω) denote the closure of C0 (Ω) in the norm of W 1,p (Ω). Let f : C \ {0} (0, ) be homogeneous of degree p on C \ {0}. That is, f (η) = η p f ( η ) > 0 when η C \ {0}. η Assume also that f is strictly convex in C \ {0}.

Euler Equation Given h W 1,p (Ω), let E = {h + φ : φ W 1,p 0 (Ω)}. It is well known (see Heinonen, Kilpelainen, Martio, Nonlinear Potential Theory of Degenerate Elliptic Equations, Chapter 5, Dover Publications, 2006) that Euler equation has unique minimizer u E, i.e inf w E Ω f ( w)da = Ω f ( u)da for some u E.

Euler Equation Given h W 1,p (Ω), let E = {h + φ : φ W 1,p 0 (Ω)}. It is well known (see Heinonen, Kilpelainen, Martio, Nonlinear Potential Theory of Degenerate Elliptic Equations, Chapter 5, Dover Publications, 2006) that Euler equation has unique minimizer u E, i.e inf w E Ω f ( w)da = Ω f ( u)da for some u E. Moreover, u is a weak solution at z Ω to the Euler equation 0 = ( f ( u(z))) = f ηk η j ( u(z)) u xk x j (z). (1) k,j=1

Euler Equation Given h W 1,p (Ω), let E = {h + φ : φ W 1,p 0 (Ω)}. It is well known (see Heinonen, Kilpelainen, Martio, Nonlinear Potential Theory of Degenerate Elliptic Equations, Chapter 5, Dover Publications, 2006) that Euler equation has unique minimizer u E, i.e inf w E Ω f ( w)da = Ω f ( u)da for some u E. Moreover, u is a weak solution at z Ω to the Euler equation That is, 0 = ( f ( u(z))) = Ω f ηk η j ( u(z)) u xk x j (z). (1) k,j=1 f ( u(z)), θ(z) da = 0 whenever θ W 1,p 0 (Ω).

u, and u xi are both solution Lζ Here denotes divergence in the z = x 1 + ix 2 variable and, denotes the standard inner product on C.

u, and u xi are both solution Lζ Here denotes divergence in the z = x 1 + ix 2 variable and, denotes the standard inner product on C. Moreover, if f is sufficiently smooth, it follows from either Schauder theory or the fact that u is a quasiregular mapping of C that u has continuous third derivatives in a neighborhood of z whenever u(z) 0.

u, and u xi are both solution Lζ Here denotes divergence in the z = x 1 + ix 2 variable and, denotes the standard inner product on C. Moreover, if f is sufficiently smooth, it follows from either Schauder theory or the fact that u is a quasiregular mapping of C that u has continuous third derivatives in a neighborhood of z whenever u(z) 0. In this case, (1) holds pointwise and we can differentiate this equation with respect to x l, l = 1, 2 to get 0 = ( x l ( f ( u(z))) ) = k,j=1 x k ( 2 f η k η j ( u(z)) u xj x l )

u, and u xi are both solution Lζ Here denotes divergence in the z = x 1 + ix 2 variable and, denotes the standard inner product on C. Moreover, if f is sufficiently smooth, it follows from either Schauder theory or the fact that u is a quasiregular mapping of C that u has continuous third derivatives in a neighborhood of z whenever u(z) 0. In this case, (1) holds pointwise and we can differentiate this equation with respect to x l, l = 1, 2 to get 0 = ( x l ( f ( u(z))) ) = k,j=1 x k ( 2 f η k η j ( u(z)) u xj x l From this display we see that if u(z) 0, and u, f are sufficiently smooth, then ζ = u xl satisfies ( Lζ = b kj (z) ζ ) = 0 (2) x k x j k,j=1 where b kj (z) = f ηk η j ( u(z)) when 1 k, j 2. )

u, and u xi are both solution Lζ Using the homogeneity of f and Euler s formula for k = 1, 2 and if η 0, then η j f ηk η j (η) = (p 1)f ηk (η) and j=1 η k f ηk (η) = pf (η). (3) k=1

u, and u xi are both solution Lζ Using the homogeneity of f and Euler s formula for k = 1, 2 and if η 0, then η j f ηk η j (η) = (p 1)f ηk (η) and j=1 η k f ηk (η) = pf (η). (3) k=1 Putting u in for ζ in (2) and using (3) and (1), it follows that Lu = k,j=1 x k ( f ηk η j ( u(z)) u ) x j = (p 1) k=1 x k (f ηk ( u(z))) = 0.

u, and u xi are both solution Lζ Using the homogeneity of f and Euler s formula for k = 1, 2 and if η 0, then η j f ηk η j (η) = (p 1)f ηk (η) and j=1 η k f ηk (η) = pf (η). (3) k=1 Putting u in for ζ in (2) and using (3) and (1), it follows that Lu = k,j=1 x k ( f ηk η j ( u(z)) u ) x j = (p 1) k=1 x k (f ηk ( u(z))) = 0. Hence, ζ = u is also solution to Lζ = 0 in a neighborhood of z.

Outline 1 Introduction 2 Main Result 3 Inspired Results 4 Future Work

Theorem Using Lζ = k,j=1 x k for ζ = u xl, l = 1, 2 and ζ = u ( b kj (z) ζ ) = 0 x j

Theorem Using Lζ = k,j=1 x k for ζ = u xl, l = 1, 2 and ζ = u we prove Theorem (Akman, Lewis, Vogel) ( b kj (z) ζ ) = 0 x j In a neighborhood of z and under the above assumptions, log f ( u)) is a sub solution, solution, or super solution to L when p > 2, p = 2, p < 2, respectively.

Possible Applications of the Theorem Let B(z, r) = {w C : w z < r} whenever z C and r > 0. Let d(e, F ) denote the distance between the sets E, F C.

Possible Applications of the Theorem Let B(z, r) = {w C : w z < r} whenever z C and r > 0. Let d(e, F ) denote the distance between the sets E, F C. Let λ > 0 be a positive function on (0, r 0 ) with lim λ(r) = 0. r 0 Define H λ Hausdorff measure on C as follows: For fixed 0 < δ < r 0 and E C, let L(δ) = {B(z i, r i )} be such that E B(z i, r i ) and 0 < r i < δ, i = 1, 2,... Set φ λ δ (E) = inf λ(ri ). L(δ)

Possible Applications of the Theorem Let B(z, r) = {w C : w z < r} whenever z C and r > 0. Let d(e, F ) denote the distance between the sets E, F C. Let λ > 0 be a positive function on (0, r 0 ) with lim λ(r) = 0. r 0 Define H λ Hausdorff measure on C as follows: For fixed 0 < δ < r 0 and E C, let L(δ) = {B(z i, r i )} be such that E B(z i, r i ) and 0 < r i < δ, i = 1, 2,... Set Then φ λ δ (E) = inf λ(ri ). L(δ) H λ (E) = lim δ 0 φ λ δ (E). In case λ(r) = r α we write H α for H λ.

Possible Applications of the Theorem Next, suppose D C is a bounded simply connected domain, z o D, Ω = D \ B(z 0, 1 2 d(z 0, D)), and u is minimizer for variational problem in Ω inf f ( w)da = f ( u)da Ω with boundary values u = 1 on B(z 0, 1 2 d(z 0, D)) and u = 0 on D in the W 1,p (Ω) sense. Put u 0 outside of D. Ω u = 0 u = 1 ( f ( u) = 0 z 0. D

Possible Applications of the Theorem Then it follows from (see Heinonen, Kilpelainen, Martio, Nonlinear Potential Theory of Degenerate Elliptic Equations, Chapter 21, Dover Publications, 2006) that there exists a unique finite positive Borel measure µ with support on D satisfying f ( u(z)), θ(z) da = θdµ ( ) C whenever θ C 0 (C \ B(z 0, 1 2 d(z 0, D))).

Possible Applications of the Theorem Then it follows from (see Heinonen, Kilpelainen, Martio, Nonlinear Potential Theory of Degenerate Elliptic Equations, Chapter 21, Dover Publications, 2006) that there exists a unique finite positive Borel measure µ with support on D satisfying f ( u(z)), θ(z) da = θdµ ( ) C whenever θ C0 (C \ B(z 0, 1 2 d(z 0, D))). Define the Hausdorff dimension of µ denoted H-dim µ, by H-dim µ = inf{α : E Borel Ω with H α (E) = 0 and µ(e) = µ( Ω)}.

Outline 1 Introduction 2 Main Result 3 Inspired Results 4 Future Work

If f ( u) = u 2, i.e, when u is harmonic, and µ = ω is harmonic measure with respect to a point in D. In [M], Makarov proved that Theorem (Makarov) a) µ is concentrated on a set of σ finite H 1 measure. b) There exists 0 < A <, such that µ is absolutely continuous with respect to Hausdorff measure defined relative to λ where λ(r) = r exp[a log 1 r log log log 1 r ], 0 < r < 10 6.

If f ( u) = u 2, i.e, when u is harmonic, and µ = ω is harmonic measure with respect to a point in D. In [M], Makarov proved that Theorem (Makarov) a) µ is concentrated on a set of σ finite H 1 measure. b) There exists 0 < A <, such that µ is absolutely continuous with respect to Hausdorff measure defined relative to λ where λ(r) = r exp[a log 1 r log log log 1 r ], 0 < r < 10 6. In [BL], Bennewitz and Lewis have attempted to generalize this result for µ defined as in ( ) relative to f ( u) = u p. Theorem (Bennewitz, Lewis) If Ω is a quasicircle, then H-dim µ 1 for 2 < p < while H-dim µ 1 for 1 < p < 2. Moreover, if Ω is the von Koch snowflake then strict inequality holds for H-dim µ.

In [LNP], Lewis, Nyström, and Poggi-Corradini proved that Theorem (Lewis, Nyström, Poggi-Corradini) Let D C be a bounded simply connected domain and 1 < p <, p 2. Put Then λ(r) = r exp[a log 1 r log log 1 r ], 0 < r < 10 6. a) If p > 2, there exists A = A(p) 1 such that µ is concentrated on a set of σ finite H λ measure. b) If 1 < p < 2, there exists A = A(p) 1, such that µ is absolutely continuous with respect to H λ.

Outline 1 Introduction 2 Main Result 3 Inspired Results 4 Future Work

Plausible Theorem 1 Makarov s result corresponds to f (η) = η 2, which is homogeneous of degree 2. In the future, we want to generalize this result for f which is homogeneous of degree 2 on C \ {0} and strictly convex on C \ {0} and the measure µ relative to f defined as f ( u(z)), θ(z) da = θdµ. ( ) C

Plausible Theorem 1 Makarov s result corresponds to f (η) = η 2, which is homogeneous of degree 2. In the future, we want to generalize this result for f which is homogeneous of degree 2 on C \ {0} and strictly convex on C \ {0} and the measure µ relative to f defined as f ( u(z)), θ(z) da = θdµ. ( ) C Plausible Theorem 1 a) µ is concentrated on a set of σ finite H 1 measure. b) There exists a universal constant 0 < C <, for any Jordan domain Ω, the measure µ is absolutely continuous with respect to the Hausdorff measure defined relative to λ where λ(r) = r exp{c log 1 r log log log 1 }, 0 < t < 10 6 r

Plausible Theorem 2 The result obtained by Bennewitz and Lewis and Lewis, Nyström, and Poggi-Corradini corresponds to f (η) = η p, which is homogeneous of degree p. We want to obtain similar result for general f, where f is homogeneous of degree p on C \ {0} and strictly convex on C \ {0}; Plausible Theorem 2 Let D C be bounded simply connected domain and 1 < p <, p 2. Define λ(r) = r exp{a log 1 r log log 1 }, 0 < r < 10 6 r Then a) If p > 2, there exists A such that µ defined as in ( ) is concentrated on a set of σ finite H λ measure. b) If 1 < p < 2, there exists A such that µ defined as in ( ) is absolutely continuous with respect to H λ.

Main Steps Let v(z) = log f ( u(z)). For k = 1, 2 we have at z b kj v xj = 1 f ( u) f ηn ( u)b kj u xnxj. n=1 Summing this over k, j = 1, 2, and using Lζ = 0 for ζ = u xn, we get Lv = k,j=1 x k (b kj v xj ) and multiplying this by (f ( u(z))) 2 we rewrite this equation in the form; (f ( u)) 2 Lv = f ( u)t 1 T 2 where at z, T 1 = n,j,k,l=1 b nl b kj u xl x k u xj x n and T 2 = n,j,k,l=1 b kj f ηn f ηl u xl x k u xj x n

Main Steps We now use matrix notation. We write at z, ( a b (b kj (z)) = (f ηk η j ( u(z))) = b c ( ) A B (u xk x j (z)) = B C ( ux1 u x2 ) ( cos θ = u sin θ ) ) (6) Observe that if D = A B B C a b b c then T 1 = tr (D 2 ). (7)

Main Steps To simplify our calculations we choose an orthonormal matrix O such that A B A 0 O t O = B C 0 C a b a b (8) O t O =. b c b c Then, T 1 = tr D 2 = tr [(O t DO) 2 ] = (a A ) 2 +2(b ) 2 A C +(c C ) 2 (9) ( ) ( ) cos φ = O t cos θ (10) sin φ sin θ

Main Steps Then from with p = 2, we find at z, f ( u) = 1 2 u 2 [a (cos φ) 2 + 2b sin φ cos φ + c (sin φ) 2 ] Putting everything together we deduce that f ( u)t 1 = 1 2 u 2 [(a A ) 2 + 2(b ) 2 A C + (c C ) 2 ] [a (cos φ) 2 + 2b sin φ cos φ + c (sin φ) 2 ]. If we consider T 2, and follow similar procedure we obtain, f ( u)t 1 = T 2. So we have shown that Lv = 0 at z when p = 2. The proof of that Lv 0 for p > 2 and Lv 0 for 1 < p < 2 is essentially same only in these cases we use the fact that f is homogeneous of degree p.

References B. Bennewitz and John L. Lewis. On the dimension of p-harmonic measure. Ann. Acad. Sci. Fenn. Math,, 30:459 505, 2005. John L. Lewis, Kaj Nyström, and Pietro Poggi-Corradini. P harmonic measure in simply connected domains. Annales de l institut Fourier, 61:689 715, 2011. N. Makarov. Distortion of boundary sets under conformal mapping. Proc. London Math. Soc., 51:369 384, 1985.