Continuous dependence estimates for the ergodic problem with an application to homogenization
|
|
- Esmond Armstrong
- 5 years ago
- Views:
Transcription
1 Continuous dependence estimates for the ergodic problem with an application to homogenization Claudio Marchi Bayreuth, September 12 th, 2013 C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 1 / 21
2 Outline 1 Continuous dependence estimates for the ergodic problem The ergodic problem Motivations Known properties Main result 2 Rate of convergence for the homogenization problem The homogenization problem Motivations literature Main result C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 2 / 21
3 Continuous dependence estimates for the ergodic problem The ergodic problem The ergodic problem For the Hamilton-Jacobi-Bellman operator H(x, p, X) = max { tr (a(x, α)x) f (x, α) p l(x, α)}, (1) α A consider the ergodic problem: seek a pair (v, U) C(R n ) R s.t. H(x, Dv, D 2 v) = U in R n, v(0) = 0. (2) Aim: establish continuous dependence estimates for v; i.e. estimate of v 1 v 2 (in some cases, of v 1 v 2 C 2), where v 1 and v 2 are solutions to two equations (2) with different coefficients. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 3 / 21
4 Continuous dependence estimates for the ergodic problem The ergodic problem The ergodic problem For the Hamilton-Jacobi-Bellman operator H(x, p, X) = max { tr (a(x, α)x) f (x, α) p l(x, α)}, (1) α A consider the ergodic problem: seek a pair (v, U) C(R n ) R s.t. H(x, Dv, D 2 v) = U in R n, v(0) = 0. (2) Aim: establish continuous dependence estimates for v; i.e. estimate of v 1 v 2 (in some cases, of v 1 v 2 C 2), where v 1 and v 2 are solutions to two equations (2) with different coefficients. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 3 / 21
5 Continuous dependence estimates for the ergodic problem Motivations Motivations 1 dynamical systems in a torus [Cornfeld et al. 82], 2 the principal eigenvalue [Bensoussan-Frehse 92], 3 strong maximum principle [Alvarez-Bardi 10]. In Optimal Control theory 1 long-time behaviour of solution to parabolic equations, 2 homogenization or singular perturbation problems. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 4 / 21
6 Continuous dependence estimates for the ergodic problem Motivations Motivations 1 dynamical systems in a torus [Cornfeld et al. 82], 2 the principal eigenvalue [Bensoussan-Frehse 92], 3 strong maximum principle [Alvarez-Bardi 10]. In Optimal Control theory 1 long-time behaviour of solution to parabolic equations, 2 homogenization or singular perturbation problems. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 4 / 21
7 Continuous dependence estimates for the ergodic problem Known properties Properties of the ergodic problem Assume (A1) A is a compact metric space; (A2) uniform ellipticity: for ν > 0, a(x, α) νi, (x, α) R n A; (A3) periodicity: a, f and l are Z n -periodic in x; (A4) regularity: a, f and l are bdd, UC and Lipschitz in x uniformly in α: ϕ(x, α) K ϕ, ϕ(x, α) ϕ(y, α) K ϕ x y for every x, y R n, α A, for ϕ = a, f, l. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 5 / 21
8 Continuous dependence estimates for the ergodic problem Known properties Introduce the stationary approximated problem for λ (0, 1) λv λ + H(x, Dv λ, D 2 v λ ) = 0 in R n, (3) and the evolutionary approximated problem t V +H(x, DV, D 2 V ) = 0 in (0, + ) R n, V (0, x) = 0 on R n. (4) Theorem 1 [Arisawa-Lions, 98] (i)!(v, U), with v periodic, s.t. the ergodic problem (2) is fulfilled; (ii) λ (0, 1),! periodic solution v λ C 2,θ (R n ) to (3); (iii)! x-periodic solution V to (4); (iv) as λ 0 +, λv λ and v λ v λ (0) uniformly converge to U and respectively to v; (v) as t +, V (t, x)/t and V (t, x) Ut uniformly converge to U and respectively to v + c 0 (for some c 0 R). C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 6 / 21
9 Continuous dependence estimates for the ergodic problem Known properties Introduce the stationary approximated problem for λ (0, 1) λv λ + H(x, Dv λ, D 2 v λ ) = 0 in R n, (3) and the evolutionary approximated problem t V +H(x, DV, D 2 V ) = 0 in (0, + ) R n, V (0, x) = 0 on R n. (4) Theorem 1 [Arisawa-Lions, 98] (i)!(v, U), with v periodic, s.t. the ergodic problem (2) is fulfilled; (ii) λ (0, 1),! periodic solution v λ C 2,θ (R n ) to (3); (iii)! x-periodic solution V to (4); (iv) as λ 0 +, λv λ and v λ v λ (0) uniformly converge to U and respectively to v; (v) as t +, V (t, x)/t and V (t, x) Ut uniformly converge to U and respectively to v + c 0 (for some c 0 R). C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 6 / 21
10 Continuous dependence estimates for the ergodic problem Known properties Introduce the stationary approximated problem for λ (0, 1) λv λ + H(x, Dv λ, D 2 v λ ) = 0 in R n, (3) and the evolutionary approximated problem t V +H(x, DV, D 2 V ) = 0 in (0, + ) R n, V (0, x) = 0 on R n. (4) Theorem 1 [Arisawa-Lions, 98] (i)!(v, U), with v periodic, s.t. the ergodic problem (2) is fulfilled; (ii) λ (0, 1),! periodic solution v λ C 2,θ (R n ) to (3); (iii)! x-periodic solution V to (4); (iv) as λ 0 +, λv λ and v λ v λ (0) uniformly converge to U and respectively to v; (v) as t +, V (t, x)/t and V (t, x) Ut uniformly converge to U and respectively to v + c 0 (for some c 0 R). C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 6 / 21
11 Continuous dependence estimates for the ergodic problem Known properties Introduce the stationary approximated problem for λ (0, 1) λv λ + H(x, Dv λ, D 2 v λ ) = 0 in R n, (3) and the evolutionary approximated problem t V +H(x, DV, D 2 V ) = 0 in (0, + ) R n, V (0, x) = 0 on R n. (4) Theorem 1 [Arisawa-Lions, 98] (i)!(v, U), with v periodic, s.t. the ergodic problem (2) is fulfilled; (ii) λ (0, 1),! periodic solution v λ C 2,θ (R n ) to (3); (iii)! x-periodic solution V to (4); (iv) as λ 0 +, λv λ and v λ v λ (0) uniformly converge to U and respectively to v; (v) as t +, V (t, x)/t and V (t, x) Ut uniformly converge to U and respectively to v + c 0 (for some c 0 R). C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 6 / 21
12 Continuous dependence estimates for the ergodic problem Optimal control interpretation Known properties Consider the control system for s > 0 dx s = f (x s, α s )ds + 2σ(x s, α s )dw s, x 0 = x where (Ω, F, P) is a probability space endowed with a right continuous filtration (F t ) 0 t<+ and a p-dimensional Brownian motion W t. The control α is chosen in the set A of progressively measurable processes with value in A for minimizing one of the costs (E x denotes the expectation). + P(x, α) := E x l(x s, α s )e λs ds, t P(t, x, α) := E x l(x s, α s )ds 0 0 C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 7 / 21
13 Continuous dependence estimates for the ergodic problem Known properties Then, for a = σσ T, we have We deduce that (for some c 0 R) v λ (x) = inf P(x, α) α A V (t, x) = inf P(t, x, α). α A U = lim λ 0 + λ inf α A E x 1 = lim t + t [ v = lim λ 0 + λ = lim t + [ inf α A E x inf α A inf α A + 0 t P(t, x, α) Ut l(x s, α s )e λs ds l(x s, α s )ds 0 ] P(x, α) inf P(0, α) α A ] + c 0. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 8 / 21
14 Continuous dependence estimates for the ergodic problem Main result Continuous dependence for the ergodic solution - 1 For i = 1, 2, consider { ) } tr (a i D 2 v i f i Dv i l i = U i in R n, v i (0) = 0. (Ei) max α A Theorem 2 [M., ppt] Under assumptions (A1)-(A4), we have v 1 v 2 CC l (max x,α a 1 a 2 + max x,α f 1 f 2 where C l := 1 + K l1 K l2 and C is independent of K li. ) + C max x,α l 1 l 2 C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 9 / 21
15 Continuous dependence estimates for the ergodic problem Main result Sketch of the proof Set w λ i := v λ i v λ i (0). By Theorem 1-(iv), it suffices to establish w λ 1 w λ 2 CC l (max x,α a 1 a 2 + max x,α f 1 f 2 ) + C max x,α l 1 l 2 (5) for every λ (0, 1). In order to prove this relation: (α) by the comparison principle, we get λ w λ 1 w λ 2 C 1 C l (max x,α a 1 a 2 +max x,α f 1 f 2 )+C max x,α l 1 l 2 ; (β) we proceed by contradiction; (γ) by the regularity of v λ i, we obtain a periodic function w, s.t. w = 1, w(0) = 0, H (Dw, D 2 w) 0 for some elliptic operator H with H (0, 0) = 0. (δ) contradiction to maximum principle. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 10 / 21
16 Continuous dependence estimates for the ergodic problem Main result Continuous dependence for the ergodic solution - 2 For i = 1, 2, consider H i (x, Dv i, D 2 v i ) = U i in R n, v i (0) = 0. Theorem 3 [M., ppt] Assume (A1)-(A4) and that, for some θ (0, 1), H i C 1,θ loc. Then, for some C R and K R n R n S n ( ) v 1 v 2 C 2 (R n ) C max a 1 a 2 + max f 1 f 2 + max l 1 l 2 x,α x,α x,α +[H 1 H 2 ] 1,K where [H 1 H 2 ] 1,K is the Lipschitz constant of (H 1 H 2 ) on the set K. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 11 / 21
17 Rate of convergence for the homogenization problem RATE OF CONVERGENCE IN HOMOGENIZATION PROBLEM C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 12 / 21
18 Rate of convergence for the homogenization problem The homogenization problem The homogenization problem We consider the homogenization problem ( u ε + H x, x ε, Duε, D 2 u ε) = 0 in R n (6) where H(x, y, p, X) = max { tr (a(x, y, α)x) f (x, y, α) p l(x, y, α)}. α A Aim Investigate how fast, as ε 0, u ε converges to the solution u to the effective equation (which needs to be suitably defined) ( ) u + H x, Du, D 2 u = 0 in R n. (7) C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 13 / 21
19 Rate of convergence for the homogenization problem The homogenization problem The homogenization problem We consider the homogenization problem ( u ε + H x, x ε, Duε, D 2 u ε) = 0 in R n (6) where H(x, y, p, X) = max { tr (a(x, y, α)x) f (x, y, α) p l(x, y, α)}. α A Aim Investigate how fast, as ε 0, u ε converges to the solution u to the effective equation (which needs to be suitably defined) ( ) u + H x, Du, D 2 u = 0 in R n. (7) C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 13 / 21
20 Rate of convergence for the homogenization problem The homogenization problem Assume (A1) A is a compact metric space; (A2) uniform ellipticity: for ν > 0, a(x, y, α) νi, (x, y, α); (A3) periodicity: a, f and l are Z n -periodic in y; (A4) regularity: a, f and l are bdd, UC and Lipschitz in (x, y) uniformly in α: for ϕ = a, f, l, there holds ϕ K and ϕ(x 1, y 1, α) ϕ(x 2, y 2, α) K ( x 1 x 2 + y 1 y 2 ) for every x 1, x 2, y 1, y 2 R n, α A. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 14 / 21
21 Rate of convergence for the homogenization problem Motivations Motivation: a stochastic optimal control problem Consider the dynamics in a medium with microscopic heterogeneities ( dx s = f x s, x ) s ε, α s ds + ( 2σ x s, x ) s ε, α s dw s, x 0 = x (s > 0) where (Ω, F, P) is a probability space endowed with a right continuous filtration (F t ) 0 t<+ and a p-dimensional Brownian motion W t. The control α is chosen in the set A of progressively measurable processes with value in A for minimizing the cost P(x, α) = E x + 0 ( l x s, x ) s ε, α s e s ds. (E x denotes the expectation). The value function u ε (x) := inf α A P(x, α) solves (6) with a = σσ T. The purpose of homogenization is to investigate what happens when the size of heterogeneities becomes smaller and smaller. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 15 / 21
22 Rate of convergence for the homogenization problem literature Literature Evans, 89-92; Alvarez-Bardi, 01 H(x, p, X) is the ergodic constant for H(x,, p, X + ) i.e.:! a y-periodic sol v = v(y; x, p, X) to the cell problem H(x, y, p, X + D 2 yyv) = H(x, p, X) in R n, v(0; x, p, X) = 0; u C 2,θ, for some θ (0, 1]; u ε converges to u locally uniformly in R n. This feature is formally motivated by the expansion u ε (x) = u(x) + εu 1 (x, x/ε) + ε 2 u 2 (x, x/ε) (8) C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 16 / 21
23 Rate of convergence for the homogenization problem literature Literature Evans, 89-92; Alvarez-Bardi, 01 H(x, p, X) is the ergodic constant for H(x,, p, X + ) i.e.:! a y-periodic sol v = v(y; x, p, X) to the cell problem H(x, y, p, X + D 2 yyv) = H(x, p, X) in R n, v(0; x, p, X) = 0; u C 2,θ, for some θ (0, 1]; u ε converges to u locally uniformly in R n. This feature is formally motivated by the expansion u ε (x) = u(x) + εu 1 (x, x/ε) + ε 2 u 2 (x, x/ε) (8) C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 16 / 21
24 Rate of convergence for the homogenization problem literature Camilli-M., 09 u ε converges to u uniformly in R n ; u ε u Cε 2θ 2+θ. Remark. The maximal rate is 2/3. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 17 / 21
25 Rate of convergence for the homogenization problem Main result An improvement for the rate of convergence Theorem [M., ppt] u ε u Cε θ. Remark. The maximal rate is 1 as 1 in the formal expansion (8), 2 in the regular case for linear problem (see: [Bensoussan-JL Lions-Papanicolaou, 78] or [Jikov-Kozlov-Oleinik, 94]). C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 18 / 21
26 Rate of convergence for the homogenization problem Sketch of the proof Main result Fix ε; for each γ > 0, introduce ϕ(x) := u ε (x) u(x) ε 2 v ( x ε ; [u](x) ) γ 2 x 2 where v(y; [u](x)) := v(y; x, Du(x), D 2 u(x)). By u C 2,θ and Theorem 2, ϕ C 0 (R n ). Let ˆx be its maximum point. For c := Cε θ, consider ( x ) ϕ(x) := u ε (x) u(x) ε 2 v ε ; [u](ˆx) γ 2 x 2 c x ˆx 2 and denote by x its maximum point in B(ˆx, ε). Main estimate u ε ( x) u(ˆx) C[ε θ + γ 1/2 ]. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 19 / 21
27 Rate of convergence for the homogenization problem Sketch of the proof Main result Fix ε; for each γ > 0, introduce ϕ(x) := u ε (x) u(x) ε 2 v ( x ε ; [u](x) ) γ 2 x 2 where v(y; [u](x)) := v(y; x, Du(x), D 2 u(x)). By u C 2,θ and Theorem 2, ϕ C 0 (R n ). Let ˆx be its maximum point. For c := Cε θ, consider ( x ) ϕ(x) := u ε (x) u(x) ε 2 v ε ; [u](ˆx) γ 2 x 2 c x ˆx 2 and denote by x its maximum point in B(ˆx, ε). Main estimate u ε ( x) u(ˆx) C[ε θ + γ 1/2 ]. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 19 / 21
28 Rate of convergence for the homogenization problem Sketch of the proof Main result Fix ε; for each γ > 0, introduce ϕ(x) := u ε (x) u(x) ε 2 v ( x ε ; [u](x) ) γ 2 x 2 where v(y; [u](x)) := v(y; x, Du(x), D 2 u(x)). By u C 2,θ and Theorem 2, ϕ C 0 (R n ). Let ˆx be its maximum point. For c := Cε θ, consider ( x ) ϕ(x) := u ε (x) u(x) ε 2 v ε ; [u](ˆx) γ 2 x 2 c x ˆx 2 and denote by x its maximum point in B(ˆx, ε). Main estimate u ε ( x) u(ˆx) C[ε θ + γ 1/2 ]. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 19 / 21
29 Rate of convergence for the homogenization problem Main result The relation ϕ( x) ϕ(ˆx) = ϕ(ˆx) ϕ(x) yields u ε (x) u(x) C[ε θ + γ 1/2 ] + γ 2 x 2. As γ 0 +, we get u ε (x) u(x) Cε θ. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 20 / 21
30 Rate of convergence for the homogenization problem Main result Example: diffusion independent of α and y Consider the homogenization problem ( u ε tr a(x)d 2 u ε) ( + F x, x ε, Duε) = 0 in R n with a C 1,1 and F(x, y, p) = max α A { f (x, y, α) p l(x, y, α)}. In this case, the effective equation is ( ) u tr a(x)d 2 u + F(x, y, Du) dy = 0 in R n. (0,1] n Corollary u ε u Cε. C. Marchi (Università di Padova) Continuous dependence Bayreuth, 12/9/13 21 / 21
Lipschitz continuity for solutions of Hamilton-Jacobi equation with Ornstein-Uhlenbeck operator
Lipschitz continuity for solutions of Hamilton-Jacobi equation with Ornstein-Uhlenbeck operator Thi Tuyen Nguyen Ph.D student of University of Rennes 1 Joint work with: Prof. E. Chasseigne(University of
More informationSingular Perturbations of Stochastic Control Problems with Unbounded Fast Variables
Singular Perturbations of Stochastic Control Problems with Unbounded Fast Variables Joao Meireles joint work with Martino Bardi and Guy Barles University of Padua, Italy Workshop "New Perspectives in Optimal
More informationMean Field Games on networks
Mean Field Games on networks Claudio Marchi Università di Padova joint works with: S. Cacace (Rome) and F. Camilli (Rome) C. Marchi (Univ. of Padova) Mean Field Games on networks Roma, June 14 th, 2017
More informationThuong Nguyen. SADCO Internal Review Metting
Asymptotic behavior of singularly perturbed control system: non-periodic setting Thuong Nguyen (Joint work with A. Siconolfi) SADCO Internal Review Metting Rome, Nov 10-12, 2014 Thuong Nguyen (Roma Sapienza)
More informationMean-Field Games with non-convex Hamiltonian
Mean-Field Games with non-convex Hamiltonian Martino Bardi Dipartimento di Matematica "Tullio Levi-Civita" Università di Padova Workshop "Optimal Control and MFGs" Pavia, September 19 21, 2018 Martino
More informationDynamical systems with Gaussian and Levy noise: analytical and stochastic approaches
Dynamical systems with Gaussian and Levy noise: analytical and stochastic approaches Noise is often considered as some disturbing component of the system. In particular physical situations, noise becomes
More informationBSDEs and PDEs with discontinuous coecients Applications to homogenization K. Bahlali, A. Elouain, E. Pardoux. Jena, March 2009
BSDEs and PDEs with discontinuous coecients Applications to homogenization K. Bahlali, A. Elouain, E. Pardoux. Jena, 16-20 March 2009 1 1) L p viscosity solution to 2nd order semilinear parabolic PDEs
More informationHJB equations. Seminar in Stochastic Modelling in Economics and Finance January 10, 2011
Department of Probability and Mathematical Statistics Faculty of Mathematics and Physics, Charles University in Prague petrasek@karlin.mff.cuni.cz Seminar in Stochastic Modelling in Economics and Finance
More informationExam February h
Master 2 Mathématiques et Applications PUF Ho Chi Minh Ville 2009/10 Viscosity solutions, HJ Equations and Control O.Ley (INSA de Rennes) Exam February 2010 3h Written-by-hands documents are allowed. Printed
More informationOn the infinity Laplace operator
On the infinity Laplace operator Petri Juutinen Köln, July 2008 The infinity Laplace equation Gunnar Aronsson (1960 s): variational problems of the form S(u, Ω) = ess sup H (x, u(x), Du(x)). (1) x Ω The
More informationErgodic Theorems. Samy Tindel. Purdue University. Probability Theory 2 - MA 539. Taken from Probability: Theory and examples by R.
Ergodic Theorems Samy Tindel Purdue University Probability Theory 2 - MA 539 Taken from Probability: Theory and examples by R. Durrett Samy T. Ergodic theorems Probability Theory 1 / 92 Outline 1 Definitions
More informationHomogenization and Multiscale Modeling
Ralph E. Showalter http://www.math.oregonstate.edu/people/view/show Department of Mathematics Oregon State University Multiscale Summer School, August, 2008 DOE 98089 Modeling, Analysis, and Simulation
More informationHomogenization of stochastic Hamilton-Jacobi equations: brief review of methods and applications
Homogenization of stochastic Hamilton-Jacobi equations: brief review of methods and applications Elena Kosygina Department of Mathematics Baruch College One Bernard Baruch Way, Box B6-23 New York, NY 11
More informationUNIVERSITÀ DI TORINO QUADERNI. del. Dipartimento di Matematica. Guy Barles & Francesca Da Lio
UNIVERSITÀ DI TORINO QUADERNI del Dipartimento di Matematica Guy Barles & Francesca Da Lio ON THE BOUNDARY ERGODIC PROBLEM FOR FULLY NONLINEAR EQUATIONS IN BOUNDED DOMAINS WITH GENERAL NONLINEAR NEUMANN
More informationHomogenization and error estimates of free boundary velocities in periodic media
Homogenization and error estimates of free boundary velocities in periodic media Inwon C. Kim October 7, 2011 Abstract In this note I describe a recent result ([14]-[15]) on homogenization and error estimates
More informationNonlinear Elliptic Systems and Mean-Field Games
Nonlinear Elliptic Systems and Mean-Field Games Martino Bardi and Ermal Feleqi Dipartimento di Matematica Università di Padova via Trieste, 63 I-35121 Padova, Italy e-mail: bardi@math.unipd.it and feleqi@math.unipd.it
More informationMaster Thesis. Nguyen Tien Thinh. Homogenization and Viscosity solution
Master Thesis Nguyen Tien Thinh Homogenization and Viscosity solution Advisor: Guy Barles Defense: Friday June 21 th, 2013 ii Preface Firstly, I am grateful to Prof. Guy Barles for helping me studying
More informationOn the long time behavior of the master equation in Mean Field Games
On the long time behavior of the master equation in Mean Field Games P. Cardaliaguet (Paris-Dauphine) Joint work with A. Porretta (Roma Tor Vergata) Mean Field Games and Related Topics - 4 Rome - June
More informationStochastic Volatility and Correction to the Heat Equation
Stochastic Volatility and Correction to the Heat Equation Jean-Pierre Fouque, George Papanicolaou and Ronnie Sircar Abstract. From a probabilist s point of view the Twentieth Century has been a century
More informationLaplace s Equation. Chapter Mean Value Formulas
Chapter 1 Laplace s Equation Let be an open set in R n. A function u C 2 () is called harmonic in if it satisfies Laplace s equation n (1.1) u := D ii u = 0 in. i=1 A function u C 2 () is called subharmonic
More informationTRANSPORT IN POROUS MEDIA
1 TRANSPORT IN POROUS MEDIA G. ALLAIRE CMAP, Ecole Polytechnique 1. Introduction 2. Main result in an unbounded domain 3. Asymptotic expansions with drift 4. Two-scale convergence with drift 5. The case
More informationStochastic Homogenization for Reaction-Diffusion Equations
Stochastic Homogenization for Reaction-Diffusion Equations Jessica Lin McGill University Joint Work with Andrej Zlatoš June 18, 2018 Motivation: Forest Fires ç ç ç ç ç ç ç ç ç ç Motivation: Forest Fires
More informationMathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio ( )
Mathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio (2014-2015) Etienne Tanré - Olivier Faugeras INRIA - Team Tosca November 26th, 2014 E. Tanré (INRIA - Team Tosca) Mathematical
More informationMATHER THEORY, WEAK KAM, AND VISCOSITY SOLUTIONS OF HAMILTON-JACOBI PDE S
MATHER THEORY, WEAK KAM, AND VISCOSITY SOLUTIONS OF HAMILTON-JACOBI PDE S VADIM YU. KALOSHIN 1. Motivation Consider a C 2 smooth Hamiltonian H : T n R n R, where T n is the standard n-dimensional torus
More informationHomogenization of a Hele-Shaw-type problem in periodic time-dependent med
Homogenization of a Hele-Shaw-type problem in periodic time-dependent media University of Tokyo npozar@ms.u-tokyo.ac.jp KIAS, Seoul, November 30, 2012 Hele-Shaw problem Model of the pressure-driven }{{}
More informationRandom and Deterministic perturbations of dynamical systems. Leonid Koralov
Random and Deterministic perturbations of dynamical systems Leonid Koralov - M. Freidlin, L. Koralov Metastability for Nonlinear Random Perturbations of Dynamical Systems, Stochastic Processes and Applications
More informationElliptic Operators with Unbounded Coefficients
Elliptic Operators with Unbounded Coefficients Federica Gregorio Universitá degli Studi di Salerno 8th June 2018 joint work with S.E. Boutiah, A. Rhandi, C. Tacelli Motivation Consider the Stochastic Differential
More informationDifferential Games II. Marc Quincampoix Université de Bretagne Occidentale ( Brest-France) SADCO, London, September 2011
Differential Games II Marc Quincampoix Université de Bretagne Occidentale ( Brest-France) SADCO, London, September 2011 Contents 1. I Introduction: A Pursuit Game and Isaacs Theory 2. II Strategies 3.
More informationDynamical properties of Hamilton Jacobi equations via the nonlinear adjoint method: Large time behavior and Discounted approximation
Dynamical properties of Hamilton Jacobi equations via the nonlinear adjoint method: Large time behavior and Discounted approximation Hiroyoshi Mitake 1 Institute of Engineering, Division of Electrical,
More informationasymptotic behaviour of singularly perturbed control systems in the non-periodic setting
UNIVERSITÀ DI ROMA LA SAPIENZA Doctoral Thesis asymptotic behaviour of singularly perturbed control systems in the non-periodic setting Author Nguyen Ngoc Quoc Thuong Supervisor Prof. Antonio Siconolfi
More informationAsymptotic behavior of infinity harmonic functions near an isolated singularity
Asymptotic behavior of infinity harmonic functions near an isolated singularity Ovidiu Savin, Changyou Wang, Yifeng Yu Abstract In this paper, we prove if n 2 x 0 is an isolated singularity of a nonegative
More informationOn continuous time contract theory
Ecole Polytechnique, France Journée de rentrée du CMAP, 3 octobre, 218 Outline 1 2 Semimartingale measures on the canonical space Random horizon 2nd order backward SDEs (Static) Principal-Agent Problem
More informationSobolev Spaces. Chapter 10
Chapter 1 Sobolev Spaces We now define spaces H 1,p (R n ), known as Sobolev spaces. For u to belong to H 1,p (R n ), we require that u L p (R n ) and that u have weak derivatives of first order in L p
More informationHomogenization for chaotic dynamical systems
Homogenization for chaotic dynamical systems David Kelly Ian Melbourne Department of Mathematics / Renci UNC Chapel Hill Mathematics Institute University of Warwick November 3, 2013 Duke/UNC Probability
More informationOn differential games with long-time-average cost
On differential games with long-time-average cost Martino Bardi Dipartimento di Matematica Pura ed Applicata Università di Padova via Belzoni 7, 35131 Padova, Italy bardi@math.unipd.it Abstract The paper
More informationLong time behaviour of periodic solutions of uniformly elliptic integro-differential equations
1/ 15 Long time behaviour of periodic solutions of uniformly elliptic integro-differential equations joint with Barles, Chasseigne (Tours) and Ciomaga (Chicago) C. Imbert CNRS, Université Paris-Est Créteil
More informationOn Ergodic Impulse Control with Constraint
On Ergodic Impulse Control with Constraint Maurice Robin Based on joint papers with J.L. Menaldi University Paris-Sanclay 9119 Saint-Aubin, France (e-mail: maurice.robin@polytechnique.edu) IMA, Minneapolis,
More informationMulti-dimensional Stochastic Singular Control Via Dynkin Game and Dirichlet Form
Multi-dimensional Stochastic Singular Control Via Dynkin Game and Dirichlet Form Yipeng Yang * Under the supervision of Dr. Michael Taksar Department of Mathematics University of Missouri-Columbia Oct
More information13 The martingale problem
19-3-2012 Notations Ω complete metric space of all continuous functions from [0, + ) to R d endowed with the distance d(ω 1, ω 2 ) = k=1 ω 1 ω 2 C([0,k];H) 2 k (1 + ω 1 ω 2 C([0,k];H) ), ω 1, ω 2 Ω. F
More informationUniformly Uniformly-ergodic Markov chains and BSDEs
Uniformly Uniformly-ergodic Markov chains and BSDEs Samuel N. Cohen Mathematical Institute, University of Oxford (Based on joint work with Ying Hu, Robert Elliott, Lukas Szpruch) Centre Henri Lebesgue,
More informationMATH 819 FALL We considered solutions of this equation on the domain Ū, where
MATH 89 FALL. The D linear wave equation weak solutions We have considered the initial value problem for the wave equation in one space dimension: (a) (b) (c) u tt u xx = f(x, t) u(x, ) = g(x), u t (x,
More informationVISCOSITY SOLUTIONS OF HAMILTON-JACOBI EQUATIONS, AND ASYMPTOTICS FOR HAMILTONIAN SYSTEMS
VISCOSITY SOLUTIONS OF HAMILTON-JACOBI EQUATIONS, AND ASYMPTOTICS FOR HAMILTONIAN SYSTEMS DIOGO AGUIAR GOMES U.C. Berkeley - CA, US and I.S.T. - Lisbon, Portugal email:dgomes@math.ist.utl.pt Abstract.
More informationHJ equations. Reachability analysis. Optimal control problems
HJ equations. Reachability analysis. Optimal control problems Hasnaa Zidani 1 1 ENSTA Paris-Tech & INRIA-Saclay Graz, 8-11 September 2014 H. Zidani (ENSTA & Inria) HJ equations. Reachability analysis -
More informationOn nonlocal Hamilton-Jacobi equations related to jump processes, some recent results
On nonlocal Hamilton-Jacobi equations related to jump processes, some recent results Daria Ghilli Institute of mathematics and scientic computing, Graz, Austria 25/11/2016 Workshop "Numerical methods for
More informationc 2004 Society for Industrial and Applied Mathematics
SIAM J. COTROL OPTIM. Vol. 43, o. 4, pp. 1222 1233 c 2004 Society for Industrial and Applied Mathematics OZERO-SUM STOCHASTIC DIFFERETIAL GAMES WITH DISCOTIUOUS FEEDBACK PAOLA MAUCCI Abstract. The existence
More informationLandesman-Lazer type results for second order Hamilton-Jacobi-Bellman equations
Author manuscript, published in "Journal of Functional Analysis 258, 12 (2010) 4154-4182" Landesman-Lazer type results for second order Hamilton-Jacobi-Bellman equations Patricio FELMER, Alexander QUAAS,
More informationThe tree-valued Fleming-Viot process with mutation and selection
The tree-valued Fleming-Viot process with mutation and selection Peter Pfaffelhuber University of Freiburg Joint work with Andrej Depperschmidt and Andreas Greven Population genetic models Populations
More informationHomogenization of micro-resonances and localization of waves.
Homogenization of micro-resonances and localization of waves. Valery Smyshlyaev University College London, UK July 13, 2012 (joint work with Ilia Kamotski UCL, and Shane Cooper Bath/ Cardiff) Valery Smyshlyaev
More informationNew Identities for Weak KAM Theory
New Identities for Weak KAM Theory Lawrence C. Evans Department of Mathematics University of California, Berkeley Abstract This paper records for the Hamiltonian H = p + W (x) some old and new identities
More informationPROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS
PROBABILITY: LIMIT THEOREMS II, SPRING 218. HOMEWORK PROBLEMS PROF. YURI BAKHTIN Instructions. You are allowed to work on solutions in groups, but you are required to write up solutions on your own. Please
More informationMean field games and related models
Mean field games and related models Fabio Camilli SBAI-Dipartimento di Scienze di Base e Applicate per l Ingegneria Facoltà di Ingegneria Civile ed Industriale Email: Camilli@dmmm.uniroma1.it Web page:
More informationBrownian Motion. 1 Definition Brownian Motion Wiener measure... 3
Brownian Motion Contents 1 Definition 2 1.1 Brownian Motion................................. 2 1.2 Wiener measure.................................. 3 2 Construction 4 2.1 Gaussian process.................................
More informationSome notes on viscosity solutions
Some notes on viscosity solutions Jeff Calder October 11, 2018 1 2 Contents 1 Introduction 5 1.1 An example............................ 6 1.2 Motivation via dynamic programming............. 8 1.3 Motivation
More informationi=1 α i. Given an m-times continuously
1 Fundamentals 1.1 Classification and characteristics Let Ω R d, d N, d 2, be an open set and α = (α 1,, α d ) T N d 0, N 0 := N {0}, a multiindex with α := d i=1 α i. Given an m-times continuously differentiable
More informationLIFE SPAN OF BLOW-UP SOLUTIONS FOR HIGHER-ORDER SEMILINEAR PARABOLIC EQUATIONS
Electronic Journal of Differential Equations, Vol. 21(21), No. 17, pp. 1 9. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu LIFE SPAN OF BLOW-UP
More informationControlled Diffusions and Hamilton-Jacobi Bellman Equations
Controlled Diffusions and Hamilton-Jacobi Bellman Equations Emo Todorov Applied Mathematics and Computer Science & Engineering University of Washington Winter 2014 Emo Todorov (UW) AMATH/CSE 579, Winter
More information(MITAKE Hiroyoshi) Joint work with Q. Liu (U. Pittsburgh) Oct/5/2012
(MITAKE Hiroyoshi) ( ) Joint work with ( ), Q. Liu (U. Pittsburgh) Oct/5/2012 in, IV 1 0 Introduction (Physical Background) Morphological stability ( ) in crystal growth: Burton, Cabrera, Frank 51 (Micro
More informationReview For the Final: Problem 1 Find the general solutions of the following DEs. a) x 2 y xy y 2 = 0 solution: = 0 : homogeneous equation.
Review For the Final: Problem 1 Find the general solutions of the following DEs. a) x 2 y xy y 2 = 0 solution: y y x y2 = 0 : homogeneous equation. x2 v = y dy, y = vx, and x v + x dv dx = v + v2. dx =
More informationBridging the Gap between Center and Tail for Multiscale Processes
Bridging the Gap between Center and Tail for Multiscale Processes Matthew R. Morse Department of Mathematics and Statistics Boston University BU-Keio 2016, August 16 Matthew R. Morse (BU) Moderate Deviations
More informationThe Hopf - Lax solution for state dependent Hamilton - Jacobi equations
The Hopf - Lax solution for state dependent Hamilton - Jacobi equations Italo Capuzzo Dolcetta Dipartimento di Matematica, Università di Roma - La Sapienza 1 Introduction Consider the Hamilton - Jacobi
More informationPartial Differential Equations
Part II Partial Differential Equations Year 2015 2014 2013 2012 2011 2010 2009 2008 2007 2006 2005 2015 Paper 4, Section II 29E Partial Differential Equations 72 (a) Show that the Cauchy problem for u(x,
More information(d). Why does this imply that there is no bounded extension operator E : W 1,1 (U) W 1,1 (R n )? Proof. 2 k 1. a k 1 a k
Exercise For k 0,,... let k be the rectangle in the plane (2 k, 0 + ((0, (0, and for k, 2,... let [3, 2 k ] (0, ε k. Thus is a passage connecting the room k to the room k. Let ( k0 k (. We assume ε k
More informationHomogenization with stochastic differential equations
Homogenization with stochastic differential equations Scott Hottovy shottovy@math.arizona.edu University of Arizona Program in Applied Mathematics October 12, 2011 Modeling with SDE Use SDE to model system
More informationAppearance of Anomalous Singularities in. a Semilinear Parabolic Equation. (Tokyo Institute of Technology) with Shota Sato (Tohoku University)
Appearance of Anomalous Singularities in a Semilinear Parabolic Equation Eiji Yanagida (Tokyo Institute of Technology) with Shota Sato (Tohoku University) 4th Euro-Japanese Workshop on Blow-up, September
More informationADJOINT METHODS FOR OBSTACLE PROBLEMS AND WEAKLY COUPLED SYSTEMS OF PDE. 1. Introduction
ADJOINT METHODS FOR OBSTACLE PROBLEMS AND WEAKLY COPLED SYSTEMS OF PDE F. CAGNETTI, D. GOMES, AND H.V. TRAN Abstract. The adjoint method, recently introduced by Evans, is used to study obstacle problems,
More informationAnnealed Brownian motion in a heavy tailed Poissonian potential
Annealed Brownian motion in a heavy tailed Poissonian potential Ryoki Fukushima Research Institute of Mathematical Sciences Stochastic Analysis and Applications, Okayama University, September 26, 2012
More informationAsymptotic Behavior of Infinity Harmonic Functions Near an Isolated Singularity
Savin, O., and C. Wang. (2008) Asymptotic Behavior of Infinity Harmonic Functions, International Mathematics Research Notices, Vol. 2008, Article ID rnm163, 23 pages. doi:10.1093/imrn/rnm163 Asymptotic
More informationCalculating the domain of attraction: Zubov s method and extensions
Calculating the domain of attraction: Zubov s method and extensions Fabio Camilli 1 Lars Grüne 2 Fabian Wirth 3 1 University of L Aquila, Italy 2 University of Bayreuth, Germany 3 Hamilton Institute, NUI
More informationConstrained Optimal Stopping Problems
University of Bath SAMBa EPSRC CDT Thesis Formulation Report For the Degree of MRes in Statistical Applied Mathematics Author: Benjamin A. Robinson Supervisor: Alexander M. G. Cox September 9, 016 Abstract
More informationMarkov Chain BSDEs and risk averse networks
Markov Chain BSDEs and risk averse networks Samuel N. Cohen Mathematical Institute, University of Oxford (Based on joint work with Ying Hu, Robert Elliott, Lukas Szpruch) 2nd Young Researchers in BSDEs
More informationp 1 ( Y p dp) 1/p ( X p dp) 1 1 p
Doob s inequality Let X(t) be a right continuous submartingale with respect to F(t), t 1 P(sup s t X(s) λ) 1 λ {sup s t X(s) λ} X + (t)dp 2 For 1 < p
More informationStability of Stochastic Differential Equations
Lyapunov stability theory for ODEs s Stability of Stochastic Differential Equations Part 1: Introduction Department of Mathematics and Statistics University of Strathclyde Glasgow, G1 1XH December 2010
More informationZdzislaw Brzeźniak. Department of Mathematics University of York. joint works with Mauro Mariani (Roma 1) and Gaurav Dhariwal (York)
Navier-Stokes equations with constrained L 2 energy of the solution Zdzislaw Brzeźniak Department of Mathematics University of York joint works with Mauro Mariani (Roma 1) and Gaurav Dhariwal (York) Stochastic
More informationMath 4263 Homework Set 1
Homework Set 1 1. Solve the following PDE/BVP 2. Solve the following PDE/BVP 2u t + 3u x = 0 u (x, 0) = sin (x) u x + e x u y = 0 u (0, y) = y 2 3. (a) Find the curves γ : t (x (t), y (t)) such that that
More informationAn inverse source problem in optical molecular imaging
An inverse source problem in optical molecular imaging Plamen Stefanov 1 Gunther Uhlmann 2 1 2 University of Washington Formulation Direct Problem Singular Operators Inverse Problem Proof Conclusion Figure:
More informationReflected Brownian Motion
Chapter 6 Reflected Brownian Motion Often we encounter Diffusions in regions with boundary. If the process can reach the boundary from the interior in finite time with positive probability we need to decide
More informationOn the Bellman equation for control problems with exit times and unbounded cost functionals 1
On the Bellman equation for control problems with exit times and unbounded cost functionals 1 Michael Malisoff Department of Mathematics, Hill Center-Busch Campus Rutgers University, 11 Frelinghuysen Road
More informationStochastic homogenization 1
Stochastic homogenization 1 Tuomo Kuusi University of Oulu August 13-17, 2018 Jyväskylä Summer School 1 Course material: S. Armstrong & T. Kuusi & J.-C. Mourrat : Quantitative stochastic homogenization
More informationHomogenization of Neuman boundary data with fully nonlinear operator
Homogenization of Neuman boundary data with fully nonlinear operator Sunhi Choi, Inwon C. Kim, and Ki-Ahm Lee Abstract We study periodic homogenization problems for second-order nonlinear pde with oscillatory
More informationLAN property for sde s with additive fractional noise and continuous time observation
LAN property for sde s with additive fractional noise and continuous time observation Eulalia Nualart (Universitat Pompeu Fabra, Barcelona) joint work with Samy Tindel (Purdue University) Vlad s 6th birthday,
More informationSébastien Chaumont a a Institut Élie Cartan, Université Henri Poincaré Nancy I, B. P. 239, Vandoeuvre-lès-Nancy Cedex, France. 1.
A strong comparison result for viscosity solutions to Hamilton-Jacobi-Bellman equations with Dirichlet condition on a non-smooth boundary and application to parabolic problems Sébastien Chaumont a a Institut
More informationLarge deviations and averaging for systems of slow fast stochastic reaction diffusion equations.
Large deviations and averaging for systems of slow fast stochastic reaction diffusion equations. Wenqing Hu. 1 (Joint work with Michael Salins 2, Konstantinos Spiliopoulos 3.) 1. Department of Mathematics
More informationWeak Convergence of Numerical Methods for Dynamical Systems and Optimal Control, and a relation with Large Deviations for Stochastic Equations
Weak Convergence of Numerical Methods for Dynamical Systems and, and a relation with Large Deviations for Stochastic Equations Mattias Sandberg KTH CSC 2010-10-21 Outline The error representation for weak
More informationOn some weighted fractional porous media equations
On some weighted fractional porous media equations Gabriele Grillo Politecnico di Milano September 16 th, 2015 Anacapri Joint works with M. Muratori and F. Punzo Gabriele Grillo Weighted Fractional PME
More informationNavier-Stokes equations in thin domains with Navier friction boundary conditions
Navier-Stokes equations in thin domains with Navier friction boundary conditions Luan Thach Hoang Department of Mathematics and Statistics, Texas Tech University www.math.umn.edu/ lhoang/ luan.hoang@ttu.edu
More informationOn a weighted total variation minimization problem
On a weighted total variation minimization problem Guillaume Carlier CEREMADE Université Paris Dauphine carlier@ceremade.dauphine.fr Myriam Comte Laboratoire Jacques-Louis Lions, Université Pierre et Marie
More informationSUPPLEMENT TO CONTROLLED EQUILIBRIUM SELECTION IN STOCHASTICALLY PERTURBED DYNAMICS
SUPPLEMENT TO CONTROLLED EQUILIBRIUM SELECTION IN STOCHASTICALLY PERTURBED DYNAMICS By Ari Arapostathis, Anup Biswas, and Vivek S. Borkar The University of Texas at Austin, Indian Institute of Science
More informationWalsh Diffusions. Andrey Sarantsev. March 27, University of California, Santa Barbara. Andrey Sarantsev University of Washington, Seattle 1 / 1
Walsh Diffusions Andrey Sarantsev University of California, Santa Barbara March 27, 2017 Andrey Sarantsev University of Washington, Seattle 1 / 1 Walsh Brownian Motion on R d Spinning measure µ: probability
More informationLarge Deviations Principles for McKean-Vlasov SDEs, Skeletons, Supports and the law of iterated logarithm
Large Deviations Principles for McKean-Vlasov SDEs, Skeletons, Supports and the law of iterated logarithm Gonçalo dos Reis University of Edinburgh (UK) & CMA/FCT/UNL (PT) jointly with: W. Salkeld, U. of
More informationON THE POLICY IMPROVEMENT ALGORITHM IN CONTINUOUS TIME
ON THE POLICY IMPROVEMENT ALGORITHM IN CONTINUOUS TIME SAUL D. JACKA AND ALEKSANDAR MIJATOVIĆ Abstract. We develop a general approach to the Policy Improvement Algorithm (PIA) for stochastic control problems
More informationThe Kuratowski Ryll-Nardzewski Theorem and semismooth Newton methods for Hamilton Jacobi Bellman equations
The Kuratowski Ryll-Nardzewski Theorem and semismooth Newton methods for Hamilton Jacobi Bellman equations Iain Smears INRIA Paris Linz, November 2016 joint work with Endre Süli, University of Oxford Overview
More informationLQG Mean-Field Games with ergodic cost in R d
LQG Mean-Field Games with ergodic cost in R d Fabio S. Priuli University of Roma Tor Vergata joint work with: M. Bardi (Univ. Padova) Padova, September 4th, 2013 Main problems Problems we are interested
More informationFrom a Mesoscopic to a Macroscopic Description of Fluid-Particle Interaction
From a Mesoscopic to a Macroscopic Description of Fluid-Particle Interaction Carnegie Mellon University Center for Nonlinear Analysis Working Group, October 2016 Outline 1 Physical Framework 2 3 Free Energy
More informationInput to state Stability
Input to state Stability Mini course, Universität Stuttgart, November 2004 Lars Grüne, Mathematisches Institut, Universität Bayreuth Part IV: Applications ISS Consider with solutions ϕ(t, x, w) ẋ(t) =
More informationWiener Measure and Brownian Motion
Chapter 16 Wiener Measure and Brownian Motion Diffusion of particles is a product of their apparently random motion. The density u(t, x) of diffusing particles satisfies the diffusion equation (16.1) u
More informationON NEUMANN PROBLEMS FOR NONLOCAL HAMILTON-JACOBI EQUATIONS WITH DOMINATING GRADIENT TERMS
ON NEUMANN PROBLEMS FOR NONLOCAL HAMILTON-JACOBI EQUATIONS WITH DOMINATING GRADIENT TERMS DARIA GHILLI Abstract. We are concerned with the well-posedness of Neumann boundary value problems for nonlocal
More informationu( x) = g( y) ds y ( 1 ) U solves u = 0 in U; u = 0 on U. ( 3)
M ath 5 2 7 Fall 2 0 0 9 L ecture 4 ( S ep. 6, 2 0 0 9 ) Properties and Estimates of Laplace s and Poisson s Equations In our last lecture we derived the formulas for the solutions of Poisson s equation
More informationCalculus of Variations. Final Examination
Université Paris-Saclay M AMS and Optimization January 18th, 018 Calculus of Variations Final Examination Duration : 3h ; all kind of paper documents (notes, books...) are authorized. The total score of
More informationIntroduction to asymptotic techniques for stochastic systems with multiple time-scales
Introduction to asymptotic techniques for stochastic systems with multiple time-scales Eric Vanden-Eijnden Courant Institute Motivating examples Consider the ODE {Ẋ = Y 3 + sin(πt) + cos( 2πt) X() = x
More informationTheory of PDE Homework 2
Theory of PDE Homework 2 Adrienne Sands April 18, 2017 In the following exercises we assume the coefficients of the various PDE are smooth and satisfy the uniform ellipticity condition. R n is always an
More information