The Pohozaev identity for the fractional Laplacian

Σχετικά έγγραφα
Example Sheet 3 Solutions

Uniform Convergence of Fourier Series Michael Taylor

Solutions to Exercise Sheet 5

Areas and Lengths in Polar Coordinates

Homework 3 Solutions

Areas and Lengths in Polar Coordinates

2 Composition. Invertible Mappings

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Other Test Constructions: Likelihood Ratio & Bayes Tests

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

Math221: HW# 1 solutions

Arithmetical applications of lagrangian interpolation. Tanguy Rivoal. Institut Fourier CNRS and Université de Grenoble 1

Lecture 26: Circular domains

Congruence Classes of Invertible Matrices of Order 3 over F 2

C.S. 430 Assignment 6, Sample Solutions

Statistical Inference I Locally most powerful tests

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Section 8.3 Trigonometric Equations

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

Problem Set 3: Solutions

Finite Field Problems: Solutions

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Fractional Colorings and Zykov Products of graphs

ST5224: Advanced Statistical Theory II

Lecture 2. Soundness and completeness of propositional logic

Every set of first-order formulas is equivalent to an independent set

Section 9.2 Polar Equations and Graphs

Partial Differential Equations in Biology The boundary element method. March 26, 2013

5. Choice under Uncertainty

Heisenberg Uniqueness pairs

derivation of the Laplacian from rectangular to spherical coordinates

The challenges of non-stable predicates

MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Section 7.6 Double and Half Angle Formulas

Solvability of Brinkman-Forchheimer equations of flow in double-diffusive convection

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2

Approximation of distance between locations on earth given by latitude and longitude

. (1) 2c Bahri- Bahri-Coron u = u 4/(N 2) u

If we restrict the domain of y = sin x to [ π 2, π 2

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

1 String with massive end-points

Integrals in cylindrical, spherical coordinates (Sect. 15.7)

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Trigonometric Formula Sheet

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

AREAS AND LENGTHS IN POLAR COORDINATES. 25. Find the area inside the larger loop and outside the smaller loop

Reminders: linear functions

Global nonlinear stability of steady solutions of the 3-D incompressible Euler equations with helical symmetry and with no swirl

CRASH COURSE IN PRECALCULUS

EE512: Error Control Coding

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

Exercises to Statistics of Material Fatigue No. 5

Parametrized Surfaces

Second Order RLC Filters

Variational Wavefunction for the Helium Atom

Inverse trigonometric functions & General Solution of Trigonometric Equations

A Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

D Alembert s Solution to the Wave Equation

= λ 1 1 e. = λ 1 =12. has the properties e 1. e 3,V(Y

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)

Srednicki Chapter 55

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

Bounding Nonsplitting Enumeration Degrees

4.6 Autoregressive Moving Average Model ARMA(1,1)

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Iterated trilinear fourier integrals with arbitrary symbols

Homework for 1/27 Due 2/5

MA 342N Assignment 1 Due 24 February 2016

Μηχανική Μάθηση Hypothesis Testing

Tridiagonal matrices. Gérard MEURANT. October, 2008

Eigenvalues and eigenfunctions of a non-local boundary value problem of Sturm Liouville differential equation

The Simply Typed Lambda Calculus

ECE598: Information-theoretic methods in high-dimensional statistics Spring 2016

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

Homework 8 Model Solution Section

Lecture 21: Properties and robustness of LSE

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint

Sequent Calculi for the Modal µ-calculus over S5. Luca Alberucci, University of Berne. Logic Colloquium Berne, July 4th 2008

Geodesic Equations for the Wormhole Metric

Concrete Mathematics Exercises from 30 September 2016

Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.

The semiclassical Garding inequality

Space-Time Symmetries

Oscillatory integrals

Divergence for log concave functions

Section 8.2 Graphs of Polar Equations

ENGR 691/692 Section 66 (Fall 06): Machine Learning Assigned: August 30 Homework 1: Bayesian Decision Theory (solutions) Due: September 13

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

Matrices and Determinants

Answer sheet: Third Midterm for Math 2339

MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS

ON A BIHARMONIC EQUATION INVOLVING NEARLY CRITICAL EXPONENT

Transcript:

The Pohozaev identity for the fractional Laplacian Xavier Ros-Oton Departament Matemàtica Aplicada I, Universitat Politècnica de Catalunya (joint work with Joaquim Serra) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 1 / 18

Outline of the talk The classical Pohozaev identity; applications The Dirichlet semilinear problem for the fractional Laplacian The Pohozaev identity for the fractional Laplacian Applications Sketch of the proof Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 / 18

The classical Pohozaev identity bounded Lipschitz domain, u = f (u) in u = 0 on, (1) Theorem (Pohozaev) ( n) u f (u)dx + n F (u)dx = u (x ν)dσ Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 3 / 18

Applications of the classical Pohozaev identity ( n) u f (u)dx + n F (u)dx = u (x ν)dσ Nonexistence of solutions: critical exponent u = u n+ n Ground states in R n : monotonicity formulas, estimates Radial symmetry: proof of P.-L. Lions combining the Pohozaev identity with the isoperimetric inequality Stable solutions: uniqueness, H 1 interior regularity etc. Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 4 / 18

Proof of the classical Pohozaev identity First note that (x u) = u + x ( u). Then, integrating by parts twice and using that u 0 on, we obtain (x u) u = u u + u x ( u) + (x u)( u ν)dσ = ( n) u u (x u) u + u (x ν)dσ We have used that u ν = u on. Finally, since u = f (u), then (x u) u = x F (u) = n F (u), and the identity follows. Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 5 / 18

The Dirichlet semilinear problem with ( ) s bounded C 1,1 domain, δ(x) := dist (x, ), f C 1 ( ) s u = f (u) in u = 0 in R n \, ( ) s u = g Theorem (X.R., J. Serra) (i) u C s (R n ) (ii) u/δ s C α () (iii) [u] C β (B ρ/ ) Cρs β u 0 B ρ B ρ/ (iv) [ u/δ s] C β (B ρ/ ) Cρα β Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 6 / 18

The Pohozaev identity for the fractional Laplacian bounded C 1,1 domain, ( ) s u = f (u) in u = 0 in R n \, Theorem (X. R., J. Serra) Denote δ(x) := dist (x, ). Then u/δ s C α () and ( u ) (s n) uf (u)dx + n F (u)dx = Γ(1 + s) (x ν)dσ, δ s where Γ is the gamma function. Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 7 / 18

Corollary: nonexistence results bounded C 1,1 domain, ( ) s u = f (u) in u = 0 in R n \, Corollary Assume that is star-shaped and F (t) < n s n t f (t) for all t. Then the problem admits no nontrivial solution. For example, for f (u) = u p we obtain nonexistence for p n+s n s. For positive solutions, this was done by [Fall-Weth, 1] with moving planes. Existence for subcritical p by [Servadei-Valdinoci, 1]. Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 8 / 18

Pohozaev identity with ( ) s Proposition (X. R., J. Serra) Assume 1 bounded C 1,1 domain u C s (R n ), u 0 outside, u/δ s C α () 3 Interior C β estimates for u and u/δ s, β < 1 + s 4 ( ) s u is bounded in Then (x u)( ) s u = s n u( ) s u Γ(1 + s) ( u δ s ) (x ν) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 9 / 18

Main consequences Changing the origin in our identity, we deduce the following Theorem (X. R., J. Serra) Under the same hypotheses of the Proposition, ( ) s u v xi = u xi ( ) s v + Γ(1 + s) u v δ s δ s ν i It has a local boundary term! Note the contrast with the nonlocal flux in the formula for f (x, u) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 10 / 18

Sketch of the Proof (Star-shaped domains) 1 u λ (x) = u(λx) (x u)( ) s u = d dλ u λ ( ) s u star-shaped u λ vanishes outside for λ > 1 u λ ( ) s u = ( ) s uλ ( ) s u R n Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 11 / 18

R n ( ) s uλ ( ) s u = λ s where w = ( ) s u. Therefore, R n ( ( ) s u ) (λx)( ) s u(x) dx = λ R s w(λx)w(x) dx n = λ s n w(λ 1 y)w(λ 1 y) dy R n (x u)( ) s u = s n w + 1 d R dλ n R n w λ w 1/λ where w λ (x) = w(λx). Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 1 / 18

R n ( ) s uλ ( ) s u = λ s where w = ( ) s u. Therefore, (x u)( ) s u = s n where w λ (x) = w(λx). R n ( ( ) s u ) (λx)( ) s u(x) dx = λ R s w(λx)w(x) dx n = λ s n w(λ 1 y)w(λ 1 y) dy R n u( ) s u + 1 d dλ R n w λ w 1/λ Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 1 / 18

What about d dλ λ=1 + R n w λ w 1/λ? Important properties: I(ϕ) = d dλ ϕ(λx)ϕ(x/λ) dx R n 1 I(ϕ) 0 since ( ) 1 ( ) 1 ϕ(λx)ϕ(x/λ)dx ϕ (λx)dx ϕ (x/λ)dx = ϕ R n R n Rn R n ψ smooth I(ψ) = 0 3 If I(ψ) = 0 I(ϕ + ψ) = I(ϕ) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 13 / 18

What about d dλ λ=1 + R n w λ w 1/λ? Important properties: I(ϕ) = d dλ ϕ(λx)ϕ(x/λ) dx R n 1 I(ϕ) 0 since ( ) 1 ( ) 1 ϕ(λx)ϕ(x/λ)dx ϕ (λx)dx ϕ (x/λ)dx = ϕ R n R n Rn R n ψ smooth I(ψ) = 0 3 If I(ψ) = 0 I(ϕ + ψ) = I(ϕ) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 13 / 18

What about d dλ λ=1 + R n w λ w 1/λ? Important properties: I(ϕ) = d dλ ϕ(λx)ϕ(x/λ) dx R n 1 I(ϕ) 0 since ( ) 1 ( ) 1 ϕ(λx)ϕ(x/λ)dx ϕ (λx)dx ϕ (x/λ)dx = ϕ R n R n Rn R n ψ smooth I(ψ) = 0 3 If I(ψ) = 0 I(ϕ + ψ) = I(ϕ) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 13 / 18

What about d dλ λ=1 + R n w λ w 1/λ? Important properties: I(ϕ) = d dλ ϕ(λx)ϕ(x/λ) dx R n 1 I(ϕ) 0 since ( ) 1 ( ) 1 ϕ(λx)ϕ(x/λ)dx ϕ (λx)dx ϕ (x/λ)dx = ϕ R n R n Rn R n ψ smooth I(ψ) = 0 3 If I(ψ) = 0 I(ϕ + ψ) = I(ϕ) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 13 / 18

What about d dλ λ=1 + R n w λ w 1/λ? We want to compute: I(w) = d dλ w λ w 1/λ R n Reduce to a 1 D calculation Use star-shaped (t, z)-coordinates (/3, z) z (1/3, z) 0 (1/, z) z x = tz, z, t > 0 d dλ w λ w 1/λ = R n d dλ (z ν)dσ(z) 0 t n 1 w(λtz)w ( tz λ ) dt Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 14 / 18

What about d dλ λ=1 + R n w λ w 1/λ? We want to compute: I(w) = d dλ w λ w 1/λ R n Reduce to a 1 D calculation Use star-shaped (t, z)-coordinates (/3, z) z (1/3, z) 0 (1/, z) z x = tz, z, t > 0 d dλ w λ w 1/λ = R n (z ν)dσ(z) d dλ 0 t n 1 w(λtz)w ( tz λ ) dt Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 14 / 18

What do we know about w = ( ) s/ u? Proposition (X. R., J. Serra) Fix z. Then, where w(tz) = ( ) s/ { u(tz) = c 1 log t 1 + c χ (0,1) (t) } u (z) + h(t) δs d dλ 0 ( t t n 1 h(λt)h dt = 0 λ) c 1 = Γ(1 + s) sin ( ) πs, and c = π π tan ( πs ) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 15 / 18

Summarising... { w(tz) = c 1 log t 1 + c χ (0,1) (t) } u (z) + h(t) δs d dλ w λ w 1/λ = (z ν)dσ(z) d ( tz ) R n dλ t n 1 w(λtz)w dt 0 λ = (z ν)dσ(z) d ( u ) ( t ) dλ δ s (z) t n 1 φ s (λt)φ s dt 0 λ u ) = (z ν)dσ(z)( δ s (z) C(s) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 16 / 18

Summarising... w(tz) = φ s (t) u (z) + h(t) δs { where φ s (t) = c 1 log t 1 + c χ (0,1) (t) } d dλ w λ w 1/λ = (z ν)dσ(z) d ( tz ) R n dλ t n 1 w(λtz)w dt 0 λ = (z ν)dσ(z) d ( u ) ( t ) dλ δ s (z) t n 1 φ s (λt)φ s dt 0 λ u ) = (z ν)dσ(z)( δ s (z) C(s) Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 16 / 18

And if the domain is not star-shaped... Key observations: 1 Pohozaev identity is quadratic in u and it comes from a bilinear identity (x u)( )s u = s n u( )s u Γ(1+s) (x u)( )s v + (x v)( )s u = u( )s v + s n v( )s u Γ(1 + s) s n every C 1,1 domain is locally star-shaped ( u δ s ) (x ν) u δ s v δ s (x ν) 3 the bilinear identity holds easily when u and v have disjoint support Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 17 / 18

And if the domain is not star-shaped... Key observations: 1 Pohozaev identity is quadratic in u and it comes from a bilinear identity (x u)( )s u = s n u( )s u Γ(1+s) (x u)( )s v + (x v)( )s u = u( )s v + s n v( )s u Γ(1 + s) s n every C 1,1 domain is locally star-shaped ( u δ s ) (x ν) u δ s v δ s (x ν) 3 the bilinear identity holds easily when u and v have disjoint support Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 17 / 18

And if the domain is not star-shaped... Key observations: 1 Pohozaev identity is quadratic in u and it comes from a bilinear identity (x u)( )s u = s n u( )s u Γ(1+s) (x u)( )s v + (x v)( )s u = u( )s v + s n v( )s u Γ(1 + s) s n every C 1,1 domain is locally star-shaped ( u δ s ) (x ν) u δ s v δ s (x ν) 3 the bilinear identity holds easily when u and v have disjoint support Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 17 / 18

And if the domain is not star-shaped... Key observations: 1 Pohozaev identity is quadratic in u and it comes from a bilinear identity (x u)( )s u = s n u( )s u Γ(1+s) (x u)( )s v + (x v)( )s u = u( )s v + s n v( )s u Γ(1 + s) s n every C 1,1 domain is locally star-shaped ( u δ s ) (x ν) u δ s v δ s (x ν) 3 the bilinear identity holds easily when u and v have disjoint support Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 17 / 18

The end Thank you! Xavier Ros-Oton (UPC) The Pohozaev identity for the fractional Laplacian BCAM, Bilbao, February 013 18 / 18