Existence for some vectorial elliptic problems with measure data **)
|
|
- Matilda Wiggins
- 8 years ago
- Views:
Transcription
1 Riv. Mat. Univ. Parma 7) 5 006), -46 F RANCESCO L EONETTI and P IER INCENZO P ETRICCA *) Existence for some vectorial elliptic problems with measure data **) - Introduction The study of elliptic boundary value problems with measure data div a x; u x); Du x))) ˆ m in u ˆ 0 received great attention starting from[]. In such a paper the scalar case u R n! R has been considered and the model operator is the p-laplacian a i x; u; j) ˆjjj p j i. Some years later [], the anisotropic p i -laplacian has been dealt with a i x; u; j) ˆjj i j p i j i, that is, each component of the gradient D i u may have a different exponent p i ; this seems useful when dealing with some reinforced materials, []; see also [0], example.7., page 69. Let us point out that both [] and[] deal with the scalar case u! R; as far as the vectorial case u! R N is concerned, some contributions appeared in [7] and[4], where the vectorial p-laplacian is considered. In this paper we deal with the anisotropic *) F. Leonetti Dipartimento di Matematica Pura ed Applicata, UniversitaÁ di L'Aquila, 6700 L'Aquila, Italy; leonetti@univaq.it; P.. Petricca ia Sant'Amasio, 009 Sora, Italy. **) Received November 7 th 005 and in revised formmarch nd 006. AMS classification 5J60, 5D05, 5J55. We acknowledge the support of MIUR, GNAMPA, INdAM and CARISPAQ. [] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA
2 4 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [] vector valued case < Pn D i jd i uj pi D i u) ˆ m u ˆ 0 in where u R n! R N with n, N, is a bounded open set and m ˆ m ;...; m N ) is a finite Radon measure on R n with values into R N. In this paper we prove existence of weak solutions for the Dirichlet problem.) in Section we give the precise result, whose proof appears in Section. We thank the referee for useful remarks and suggestions. - Notations and statements We study existence of weak solutions for the Dirichlet problem < Pn D i jd i uj pi D i u) ˆ m in u ˆ 0 where u R n! R N with n, N, is a bounded open set and m ˆ m ;...; m N ) is a finite Radon measure on R n with values into R N. We need some restrictions on the exponents p i ; we introduce the harmonic mean and we assume that p < n and p ˆ X n n p i! p n ) p )n < p p n ) i < n p i f;...; ng The right hand side of.) can be written as n p ) n p p i ˆ p i p n ) p n ) < thus p i < n p ) p n ) p i so we can take exponents q ;...; q n such that p i < q i < n p ) p n ) p i i f;...; ng;
3 [] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA 5 and we set q ˆ min q i ; q ˆ X n i n! ; q i q ˆ q n In this paper we will prove the following Theorem.. Under the previous assumptions there exists u W ;q 0 ; RN ) \ L q ; R N ) with D i u L q i ; R N ) i f;...; ng such that X n X N jd i uj pi D i u b D i W b dl n ˆ XN W b dm b W Cc ; RN ) bˆ bˆ In this theoremwe may take n ˆ, p ˆ p ˆ and p ; ); this example shows that our theoremcannot be derived from[5], []. The previous theoremimproves on [9] we remove the restriction on the support of the measure m and we allow a wider range for p i. - Proof of the Theorem Let fq k g kn be a decreasing sequence of positive numbers converging to zero. We mollify our measure m and we obtain smooth functions with f k ˆ m r Qk * m sup k f k k L ) jmj Rn ) < k We set p ˆ min i p i and we use direct methods in the calculus of variations in order to find n o u k ˆ u W ;p 0 ; R N ) D i u L p i ; R N ) i f;...; ng ; such that X n X N jd i u k j pi D i u b k D iw b dl n ˆ XN W b f b k dln W bˆ bˆ We bound u k we use a componentwise truncation argument [7], [] and estimates
4 6 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [4] on level sets []; we set 0 0 t L >< t L L < t < L M t) ˆ t L > M t) t < 0 and we use the following test function W in.) we fix a f;...; Ng and we take W ˆ W ;...; W N ) with W b ˆ 0 for b 6ˆ a and W a ˆ M u a k ), where ua k is the a-th component of u k ˆ u k ;...; un k ). We define B L;k ˆ x L u a k x) < L ; and we insert the previous W into.) we get X n Di u k p i Di u a k dx ˆ fk a M ua k ) dx B L;k Since jm t)j, we can use.) so that the right hand side of.) is bounded by jmj R n ). Let us look at the left hand side since p i, we have Di u a p i k Di u k p i thus we get 4 Since we can select X n B L;k Di u a p i k dx c k ; L N q i < n p ) p n ) p i; n p ) u 0; 0; ) p n ) such that q i up i for every i. Now, without loss of generality, we can assume that q i ˆ up i for every i and u is close to n p ) p n )
5 [5] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA 7 Let us remark that < q i < p i for every i f;...; ng and q < p < n. Now we follow [] we set u)q l ˆ u so that l > ; we use Holder inequality Di u a q i k dx ˆ Di u a q i k ju a k j) lq i=p i ju a k j)lq i=p i dx 5 4 Di u a p i k ju a k j) l dx5 6 ˆ X 4 6 X 4 q i =p i Di u a p i k ju a 7 k j) l dx5 Lˆ0 B L;k L) l Di u a p i 7 k dx5 4 ju a k j)lq i= p i q i ) dx5 q i =p i q i =p i Lˆ0 B L;k q i =p i 4 ju a k j)lq i= p i q i ) dx5 4 ju a k dx j)q 5 q i=p i q i =p i We keep in mind.4) and l > we get 6 Di u a q i k dx c 4 ju a k dx j)q 5 q i=p i We use the anisotropic embedding theorem [] and we get u a L k q ) c Y n Di u a =n k L q i ) c Y n 4 4 ju a k j)q dx5 7 ˆ c 4 4 ju a k j)q dx5 [ =q i ) =p i )]=n u)= up) We recall that p < n, so u)= up) < =q thus.7) gives u a k L q ) c 5 k N; a ˆ ;...; N
6 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [6] We insert this bound into.6) and we get 9 Di u a k L q i ) c 6 k N; i ˆ ;...n; a ˆ ;...; N Because of weak compactness, there exists u W ;q 0 ; RN ) \ L q ; R N ), with D i u L q i ; R N ) i f;...; ng, s i L q i p i ; R N ) and h i L q i ; R) for every i f;...; ng such that, up to a subsequence, 0 u k * u in W ;q 0 ; RN ); u k! u ae in ; D i u k * D i u in L q i ; R N ) i f;...; ng; jd i u k j p i D i u k * s i in L q i p i ; R N ) i f;...; ng; 4 We claimthat jd i u k D i uj * h i 0 in L q i ; R) i f;...; ng 5 h i ˆ 0 in i f;...; ng thus 6 D i u k! D i u in L ; R N ) i f;...; ng We prove claim.5) following [4]. We fix a smooth v R n! R N ; later, v will be chosen as a linear Taylor polynomial of u. We take cut off functions f R n! R and h R N! R such that f C c ; R); h C c RN ; R); with 0 f and 0 h. We take c R N! R N as follows c z) ˆ g jzj) z jzj where g C 0; ); R) with g and g 0 non-negative and bounded; moreover, we require that c j supp h) ˆ Id. Note s z) ˆ g0 jzj) zs z a jzj g jzj) d sa zs z a jzj jzj thus 7 X N aˆ j a XN s z)js 0 z; j R N
7 [7] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA 9 For every j f;...; ng it results that 0 jd j u k D j ujh u k v)fdx jd j u k D j vjh u k v)fdx jd j v D j ujh u k v)fdx jd j u k D j vj p j h u k v)fdxa jd j v D j ujh u k v)fdx =p j h u k v)fdxa =p j Let ~p ˆ max i p i. Then, using the monotonicity of z!jzj p z and the equality c ˆId on supp h), we get 0 T j k ˆ jd j u k D j vj p j h u k v)fdx 9 Xn Xn ~p jd i u k D i vj p i h u k v)fdx Xn ~p ˆ Xn ~p < ˆ ~p X n hjd i u k j pi D i u k jd i vj pi D i v; D i u k D i vih u k v)fdx hjd i u k j pi D i u k ; D i c u k v))ih u k v)fdx hjd i vj pi D i v; D i u k D i vih u k v)fdx hjd i u k j pi D i u k ; D i c u k v))ifdx hjd i vj pi D i v; D i u k D i vih u k v)fdx 9 = hjd i u k j pi D i u k ; D i c u k v))i[ h u k v)]fdx ;
8 40 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [] We recall.) and we get 0 X n ˆ Xn hjd i u k j pi D i u k ; D i c u k v))ifdx hjd i u k j pi D i u k ; D i c u k v)f)idx hjd i u k j pi D i u k ; c u k v)d i fidx ˆ hm r Qk ; c u k v)fidx Moreover,.7) implies Xn hjd i u k j pi D i u k ; c u k v)d i fidx hjd i u k j pi D i u k ; D i c u k v))i[ h u k v)]fdx X N aˆ jd i u k j p i D i u a k X N sˆ We insert.0) and.) into.9) we get 0 T j k ˆ jd j u k D j vj p j h u k v)fdx < ~p hm r Qk ; c u k v)fidx Xn X N aˆ jd i u k j p i D i u a k X N s u k v)d i v s [ h u k v)]fdx hjd i u k j pi D i u k ; c u k v)d i s u k v)d i v s [ h u k v)]fdx 9 = hjd i vj pi D i v; D i u k D i vih u k v)fdx ; We now use.),.),.),.4) and we keep in mind that h; c; Dc are
9 [9] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA 4 continuous and bounded for every j ˆ ;...; n we get T j ˆ limsup T j k k! < ~p sup jc z)j fdjmj zr N Xn X N X N s a i aˆ sˆ 0 lim lim hs i ; c u v)d i s u v)d iv s [ h u v)]fdx 9 = hjd i vj pi D i v; D i u D i vih u v)fdx ; ; k! k! jd j u k D j ujh u k v)fdx ˆ h j h u v)fdx; jd j v D j ujh u k v)fdx ˆ jd j v D j ujh u v)fdx; lim k! h u k v)fdx ˆ h u v)fdx Take the limsup in.). We get, for every j ˆ ;...; n, 0 h j h u v)fdx 7 T j 0 h u v)fdx A =p j jd j v D j ujh u v)fdx where T j has been estimated in.). For a. e. a and every j ˆ ;...; n, we have see [6] and []) ju x) [u a) Du a) x a)]j lim dx ˆ 0; R!0 R 9 0 lim R!0 lim R!0 jdu x) Du a)jdx ˆ 0; js j x) s j a)jdx ˆ 0;
10 4 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [0] lim R!0 jh j x) h j a)jdx ˆ 0; jmj B a; R)) limsup R!0 L n B a; R)) < where L n is the Lebesgue measure in R n and f x)dx ˆ L n f x)dx A) A We choose v to be the linear Taylor polynomial of u in a v x) ˆ u a) Du a) x a) Since we are still free to select f, h and c, let f R x) ˆ ~ x a f R n ; f ~ C R c B 0; ); R); 0 f ~ ; f x)dx ~ ˆ R n h R y) ˆ ~h y ; ~h Cc R B 0; ); R); 0 ~h ; ~h jb 0; ) ˆ ; c R y) ˆ R~c y ; R with ~c as in the above discussion. Then.7) can be written as follows 0 h j h R u v)f R dx A where 4 0 T j =pj B 0 T j ;R ˆ limsup k! ~p sup jc R z)j zr N Xn X N X N s a i aˆ sˆ C h R u v)f R dxa =p j jd j u k D j vj p j h R u v)f R dx f R djmj jd j v D j ujh R u v)f R dx hs i ; c R u v)d i f R a s u v)d iv s [ h R u v)]f R dx ) hjd i vj pi D i v; D i u D i vih R u v)f R dx
11 [] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA 4 Recalling.),...,.) and the definitions of h R, f R, we get 5 h j h R u v)f R dx ˆ h j a); lim R! lim R!0 Tj ;R ˆ 0; h R u v)f R dx ; lim R!0 jd j v D j ujh R u v)f R dx ˆ 0 As far as.6) is concerned, we give some details in the Appendix. Let us take R! 0 in.) we get, for every j ˆ ;...; n, 9 h j a) ˆ 0 for a.e a thus our claim.5) is proved. Now we have.6), thus, up to a subsequence, 40 Du k! Du ae in The previous pointwise convergence and the estimate jdi u k j pi D i u k q i ˆ Di u k p i p L i L q i ) c 7; k N; i f;...; ng ) allow us to get 4 jd i u k j p i D i u k * jd i uj p i D i u in L q i p i ; R N ) i f;...; ng Thus we can pass to the limit, as k!, in.) and it turns out that u solves.). This ends the proof. p 4 - Appendix For the convenience of the reader, we give some details about the proof of.6). We look at inequality.4) it suffices to prove that all the four integrals go to zero when R! 0. We keep in mind that 4 4 jc R z)j c R 0 f R x) R n
12 44 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [] then 0 sup zr N jc R z)j jmj B a; R)) f R djmj c R R n and the right hand side goes to zero because of.). Now we deal with the second integral in the right hand side of.4) hs i x); c R u x) v x))d i f R x)idx hs i a); c R u x) v x))d i f R x)idx hs i x) s i a); c R u x) v x))d i f R x)idx ˆ I R II R Note that then We recall that D i f R x) ˆ R n h D ~ i f x a i R R ~c z) ˆ z for z B 0; supp ~h) c R u v) ˆ u v on ju vj R thus it is convenient to let A R ˆ x B a; R) ju x) v x)j R > We define v n to be the n dimensional Lebesgue measure of the unit ball in R n ; then L n B a; R)) ˆ v n R n and 0 Ln A R ) R n v n ju x) v x)j dx R
13 [] EXISTENCE FOR SOME ECTORIAL ELLIPTIC PROBLEMS WITH MEASURE DATA 45 We use.) and we get 4 L n A R ) lim R!0 R n ˆ 0 Now we are able to deal with I R as follows 0 I R ˆ h R n hs i a); c R u x) v x)) D i f ~ x a i R R idx A R 44 h R n hs i a); c R u x) v x)) D i f ~ x a i R R idx na R Ln A R ) R n js i a)jc Di f ~ L R n ) v njs i a)j Di f ~ L R n ) Using 4.) and.) we get ju x) v x)j dx R 45 lim R!0 I R ˆ 0 As far as II R is concerned, we argue as follows 0 II R c v Di n f ~ L R n ) js i x) s i a)jdx thus we can use.0) and we get 46 lim II R ˆ 0 R!0 Limits 4.5) and 4.6) guarantee that the second integral in.4) goes to zero when R! 0. In a similar manner we can show that the third integral goes to zero. The fourth integral is easier to be dealt with. Thus we have established.6). References [] L. AMBROSIO, N. FUSCO and D. PALLARA, Functions of bounded variation and free discontinuity problems, Mathematical Monographs, Oxford University Press, New York 000. [] L. BOCCARDO and T. GALLOUET, Non-linear elliptic and parabolic equations involving measure data, J. Funct. Anal. 7 99),
14 46 FRANCESCO LEONETTI and PIER INCENZO PETRICCA [4] [] L. BOCCARDO, T.GALLOUET and P. MARCELLINI, Anisotropic equations in L, Differential Integral Equations 9 996), 09-. [4] G. DOLZMANN, N. HUNGERBUHLER and S. MULLER, The p-harmonic system with measure-valued right hand side, Ann. Inst. H. Poincare Anal. Non LineÂaire 4 997), [5] G. DOLZMANN, N. HUNGERBUHLER and S. MULLER, Non-linear elliptic systems with measure-valued right hand side, Math. Z., 6 997), [6] L. C. EANS and R.F. GARIEPY, Measure theory and fine properties of functions, CRC Press, Boca Raton, FL 99. [7] M. FUCHS and J. REULING, Non-linear elliptic systems involving measure data, Rend. Mat. Appl. 7) 5 995), -9. [] F. LEONETTI, Maximum principle for vector-valued minimizers of some integral functionals, Boll. Un. Mat. Ital. 5-A 99), [9] F. LEONETTI and P.. PETRICCA, Anisotropic elliptic systems with measure data, Preprint 6, Dip. Mat. Pura Appl. Univ. L'Aquila 004). [0] J. L. LIONS, Quelques methodes de resolution des problemes aux limites non lineaires, Dunod, Gauthier - illars, Paris 969. [] Q. TANG, Regularity of minimizers of non-isotropic integrals of the calculus of variations, Ann. Mat. Pura Appl. 4) 64 99), [] M. TROISI, Teoremi di inclusione per spazi di Sobolev non isotropi, Ricerche Mat. 969), -4. [] S. ZHOU, A note on nonlinear elliptic systems involving measures, Electron. J. Differential Equations, ), -6. Abstract We study the Dirichlet problem < Pn D i jd i uj pi D i u) ˆ m u ˆ 0 in where u R n! R N with n, N, is a bounded open set and m ˆ m ;...; m N ) is a finite Radon measure on R n with values into R N. Under some restrictions on the exponents p i, we prove existence of a weak solution u. ***
CONSTANT-SIGN SOLUTIONS FOR A NONLINEAR NEUMANN PROBLEM INVOLVING THE DISCRETE p-laplacian. Pasquale Candito and Giuseppina D Aguí
Opuscula Math. 34 no. 4 2014 683 690 http://dx.doi.org/10.7494/opmath.2014.34.4.683 Opuscula Mathematica CONSTANT-SIGN SOLUTIONS FOR A NONLINEAR NEUMANN PROBLEM INVOLVING THE DISCRETE p-laplacian Pasquale
More informationExistence de solutions à support compact pour un problème elliptique quasilinéaire
Existence de solutions à support compact pour un problème elliptique quasilinéaire Jacques Giacomoni, Habib Mâagli, Paul Sauvy Université de Pau et des Pays de l Adour, L.M.A.P. Faculté de sciences de
More informationA PRIORI ESTIMATES FOR SEMISTABLE SOLUTIONS OF SEMILINEAR ELLIPTIC EQUATIONS. In memory of Rou-Huai Wang
A PRIORI ESTIMATES FOR SEMISTABLE SOLUTIONS OF SEMILINEAR ELLIPTIC EQUATIONS XAVIER CABRÉ, MANEL SANCHÓN, AND JOEL SPRUCK In memory of Rou-Huai Wang 1. Introduction In this note we consider semistable
More information1. INTRODUCTION. u yy. u yx
Rend. Mat. Acc. Lincei s. 9, v. 16:159-169 005) Analisi funzionale. Ð On weak Hessian determinants. Nota di LUIGI D'ONOFRIO, FLAIA GIANNETTI eluigi GRECO, presentata *) dal Socio C. Sbordone. ABSTRACT.
More informationWissenschaftliche Artikel (erschienen bzw. angenommen)
Schriftenverzeichnis I. Monographie [1] Convex variational problems. Linear, nearly linear and anisotropic growth conditions. Lecture Notes in Mathematics 1818, Springer, Berlin-Heidelberg- New York, 2003.
More informationEXISTENCE AND NON-EXISTENCE RESULTS FOR A NONLINEAR HEAT EQUATION
Sixth Mississippi State Conference on Differential Equations and Computational Simulations, Electronic Journal of Differential Equations, Conference 5 (7), pp. 5 65. ISSN: 7-669. UL: http://ejde.math.txstate.edu
More informationHOMEWORK 5 SOLUTIONS. n!f n (1) lim. ln x n! + xn x. 1 = G n 1 (x). (2) k + 1 n. (n 1)!
Math 7 Fall 205 HOMEWORK 5 SOLUTIONS Problem. 2008 B2 Let F 0 x = ln x. For n 0 and x > 0, let F n+ x = 0 F ntdt. Evaluate n!f n lim n ln n. By directly computing F n x for small n s, we obtain the following
More informationMathematics for Econometrics, Fourth Edition
Mathematics for Econometrics, Fourth Edition Phoebus J. Dhrymes 1 July 2012 1 c Phoebus J. Dhrymes, 2012. Preliminary material; not to be cited or disseminated without the author s permission. 2 Contents
More informationAn optimal transportation problem with import/export taxes on the boundary
An optimal transportation problem with import/export taxes on the boundary Julián Toledo Workshop International sur les Mathématiques et l Environnement Essaouira, November 2012..................... Joint
More informationA new continuous dependence result for impulsive retarded functional differential equations
CADERNOS DE MATEMÁTICA 11, 37 47 May (2010) ARTIGO NÚMERO SMA#324 A new continuous dependence result for impulsive retarded functional differential equations M. Federson * Instituto de Ciências Matemáticas
More informationInner Product Spaces
Math 571 Inner Product Spaces 1. Preliminaries An inner product space is a vector space V along with a function, called an inner product which associates each pair of vectors u, v with a scalar u, v, and
More informationON COMPLETELY CONTINUOUS INTEGRATION OPERATORS OF A VECTOR MEASURE. 1. Introduction
ON COMPLETELY CONTINUOUS INTEGRATION OPERATORS OF A VECTOR MEASURE J.M. CALABUIG, J. RODRÍGUEZ, AND E.A. SÁNCHEZ-PÉREZ Abstract. Let m be a vector measure taking values in a Banach space X. We prove that
More informationFinite speed of propagation in porous media. by mass transportation methods
Finite speed of propagation in porous media by mass transportation methods José Antonio Carrillo a, Maria Pia Gualdani b, Giuseppe Toscani c a Departament de Matemàtiques - ICREA, Universitat Autònoma
More informationExtremal equilibria for reaction diffusion equations in bounded domains and applications.
Extremal equilibria for reaction diffusion equations in bounded domains and applications. Aníbal Rodríguez-Bernal Alejandro Vidal-López Departamento de Matemática Aplicada Universidad Complutense de Madrid,
More information1 Norms and Vector Spaces
008.10.07.01 1 Norms and Vector Spaces Suppose we have a complex vector space V. A norm is a function f : V R which satisfies (i) f(x) 0 for all x V (ii) f(x + y) f(x) + f(y) for all x,y V (iii) f(λx)
More informationMultigrid preconditioning for nonlinear (degenerate) parabolic equations with application to monument degradation
Multigrid preconditioning for nonlinear (degenerate) parabolic equations with application to monument degradation M. Donatelli 1 M. Semplice S. Serra-Capizzano 1 1 Department of Science and High Technology
More informationNo: 10 04. Bilkent University. Monotonic Extension. Farhad Husseinov. Discussion Papers. Department of Economics
No: 10 04 Bilkent University Monotonic Extension Farhad Husseinov Discussion Papers Department of Economics The Discussion Papers of the Department of Economics are intended to make the initial results
More informationSome remarks on Phragmén-Lindelöf theorems for weak solutions of the stationary Schrödinger operator
Wan Boundary Value Problems (2015) 2015:239 DOI 10.1186/s13661-015-0508-0 R E S E A R C H Open Access Some remarks on Phragmén-Lindelöf theorems for weak solutions of the stationary Schrödinger operator
More information1. Introduction. PROPER HOLOMORPHIC MAPPINGS BETWEEN RIGID POLYNOMIAL DOMAINS IN C n+1
Publ. Mat. 45 (2001), 69 77 PROPER HOLOMORPHIC MAPPINGS BETWEEN RIGID POLYNOMIAL DOMAINS IN C n+1 Bernard Coupet and Nabil Ourimi Abstract We describe the branch locus of proper holomorphic mappings between
More informationOn the largest prime factor of x 2 1
On the largest prime factor of x 2 1 Florian Luca and Filip Najman Abstract In this paper, we find all integers x such that x 2 1 has only prime factors smaller than 100. This gives some interesting numerical
More informationMATH 425, PRACTICE FINAL EXAM SOLUTIONS.
MATH 45, PRACTICE FINAL EXAM SOLUTIONS. Exercise. a Is the operator L defined on smooth functions of x, y by L u := u xx + cosu linear? b Does the answer change if we replace the operator L by the operator
More informationFACTORING POLYNOMIALS IN THE RING OF FORMAL POWER SERIES OVER Z
FACTORING POLYNOMIALS IN THE RING OF FORMAL POWER SERIES OVER Z DANIEL BIRMAJER, JUAN B GIL, AND MICHAEL WEINER Abstract We consider polynomials with integer coefficients and discuss their factorization
More informationShape Optimization Problems over Classes of Convex Domains
Shape Optimization Problems over Classes of Convex Domains Giuseppe BUTTAZZO Dipartimento di Matematica Via Buonarroti, 2 56127 PISA ITALY e-mail: buttazzo@sab.sns.it Paolo GUASONI Scuola Normale Superiore
More informationDifferentiating under an integral sign
CALIFORNIA INSTITUTE OF TECHNOLOGY Ma 2b KC Border Introduction to Probability and Statistics February 213 Differentiating under an integral sign In the derivation of Maximum Likelihood Estimators, or
More informationProperties of BMO functions whose reciprocals are also BMO
Properties of BMO functions whose reciprocals are also BMO R. L. Johnson and C. J. Neugebauer The main result says that a non-negative BMO-function w, whose reciprocal is also in BMO, belongs to p> A p,and
More informationPacific Journal of Mathematics
Pacific Journal of Mathematics GLOBAL EXISTENCE AND DECREASING PROPERTY OF BOUNDARY VALUES OF SOLUTIONS TO PARABOLIC EQUATIONS WITH NONLOCAL BOUNDARY CONDITIONS Sangwon Seo Volume 193 No. 1 March 2000
More informationA SURGERY RESULT FOR THE SPECTRUM OF THE DIRICHLET LAPLACIAN. Keywords: shape optimization, eigenvalues, Dirichlet Laplacian
A SURGERY RESULT FOR THE SPECTRUM OF THE DIRICHLET LAPLACIA DORI BUCUR AD DARIO MAZZOLEI Abstract. In this paper we give a method to geometrically modify an open set such that the first k eigenvalues of
More informationUNIVERSITETET I OSLO
NIVERSITETET I OSLO Det matematisk-naturvitenskapelige fakultet Examination in: Trial exam Partial differential equations and Sobolev spaces I. Day of examination: November 18. 2009. Examination hours:
More informationMetric Spaces. Chapter 1
Chapter 1 Metric Spaces Many of the arguments you have seen in several variable calculus are almost identical to the corresponding arguments in one variable calculus, especially arguments concerning convergence
More informationAn example of a computable
An example of a computable absolutely normal number Verónica Becher Santiago Figueira Abstract The first example of an absolutely normal number was given by Sierpinski in 96, twenty years before the concept
More informationIntroduction to the Finite Element Method
Introduction to the Finite Element Method 09.06.2009 Outline Motivation Partial Differential Equations (PDEs) Finite Difference Method (FDM) Finite Element Method (FEM) References Motivation Figure: cross
More informationContinued Fractions and the Euclidean Algorithm
Continued Fractions and the Euclidean Algorithm Lecture notes prepared for MATH 326, Spring 997 Department of Mathematics and Statistics University at Albany William F Hammond Table of Contents Introduction
More informationKATO S INEQUALITY UP TO THE BOUNDARY. Contents 1. Introduction 1 2. Properties of functions in X 4 3. Proof of Theorem 1.1 6 4.
KATO S INEQUALITY UP TO THE BOUNDARY HAÏM BREZIS(1),(2) AND AUGUSTO C. PONCE (3) Abstract. We show that if u is a finite measure in then, under suitable assumptions on u near, u + is also a finite measure
More informationAn ultimate Sobolev dimension-free imbedding
An ultimate Sobolev dimension-free imbedding Alberto FIORENZA Universitá di Napoli "Federico II" Memorial seminar dedicated to Prof. RNDr. Miroslav Krbec, DrSc. Praha, November 8, 212 () 1 / 25 PRAHA 1995
More informationRESONANCES AND BALLS IN OBSTACLE SCATTERING WITH NEUMANN BOUNDARY CONDITIONS
RESONANCES AND BALLS IN OBSTACLE SCATTERING WITH NEUMANN BOUNDARY CONDITIONS T. J. CHRISTIANSEN Abstract. We consider scattering by an obstacle in R d, d 3 odd. We show that for the Neumann Laplacian if
More informationRev. Mat. Iberoam, 17 (1), 49{419 Dynamical instability of symmetric vortices Lus Almeida and Yan Guo Abstract. Using the Maxwell-Higgs model, we prove that linearly unstable symmetric vortices in the
More informationA class of infinite dimensional stochastic processes
A class of infinite dimensional stochastic processes John Karlsson Linköping University CRM Barcelona, July 7, 214 Joint work with Jörg-Uwe Löbus John Karlsson (Linköping University) Infinite dimensional
More informationExistence and multiplicity of solutions for a Neumann-type p(x)-laplacian equation with nonsmooth potential. 1 Introduction
Electronic Journal of Qualitative Theory of Differential Equations 20, No. 7, -0; http://www.math.u-szeged.hu/ejqtde/ Existence and multiplicity of solutions for a Neumann-type p(x)-laplacian equation
More informationOPTIMAL CONTROL OF A COMMERCIAL LOAN REPAYMENT PLAN. E.V. Grigorieva. E.N. Khailov
DISCRETE AND CONTINUOUS Website: http://aimsciences.org DYNAMICAL SYSTEMS Supplement Volume 2005 pp. 345 354 OPTIMAL CONTROL OF A COMMERCIAL LOAN REPAYMENT PLAN E.V. Grigorieva Department of Mathematics
More information9 Multiplication of Vectors: The Scalar or Dot Product
Arkansas Tech University MATH 934: Calculus III Dr. Marcel B Finan 9 Multiplication of Vectors: The Scalar or Dot Product Up to this point we have defined what vectors are and discussed basic notation
More informationReference: Introduction to Partial Differential Equations by G. Folland, 1995, Chap. 3.
5 Potential Theory Reference: Introduction to Partial Differential Equations by G. Folland, 995, Chap. 3. 5. Problems of Interest. In what follows, we consider Ω an open, bounded subset of R n with C 2
More informationA survey on multivalued integration 1
Atti Sem. Mat. Fis. Univ. Modena Vol. L (2002) 53-63 A survey on multivalued integration 1 Anna Rita SAMBUCINI Dipartimento di Matematica e Informatica 1, Via Vanvitelli - 06123 Perugia (ITALY) Abstract
More informationAn Introduction to the Navier-Stokes Initial-Boundary Value Problem
An Introduction to the Navier-Stokes Initial-Boundary Value Problem Giovanni P. Galdi Department of Mechanical Engineering University of Pittsburgh, USA Rechts auf zwei hohen Felsen befinden sich Schlösser,
More informationThe Heat Equation. Lectures INF2320 p. 1/88
The Heat Equation Lectures INF232 p. 1/88 Lectures INF232 p. 2/88 The Heat Equation We study the heat equation: u t = u xx for x (,1), t >, (1) u(,t) = u(1,t) = for t >, (2) u(x,) = f(x) for x (,1), (3)
More informationSequences and Series
Sequences and Series Consider the following sum: 2 + 4 + 8 + 6 + + 2 i + The dots at the end indicate that the sum goes on forever. Does this make sense? Can we assign a numerical value to an infinite
More informationVariational approach to restore point-like and curve-like singularities in imaging
Variational approach to restore point-like and curve-like singularities in imaging Daniele Graziani joint work with Gilles Aubert and Laure Blanc-Féraud Roma 12/06/2012 Daniele Graziani (Roma) 12/06/2012
More informationSHARP BOUNDS FOR THE SUM OF THE SQUARES OF THE DEGREES OF A GRAPH
31 Kragujevac J. Math. 25 (2003) 31 49. SHARP BOUNDS FOR THE SUM OF THE SQUARES OF THE DEGREES OF A GRAPH Kinkar Ch. Das Department of Mathematics, Indian Institute of Technology, Kharagpur 721302, W.B.,
More information9 More on differentiation
Tel Aviv University, 2013 Measure and category 75 9 More on differentiation 9a Finite Taylor expansion............... 75 9b Continuous and nowhere differentiable..... 78 9c Differentiable and nowhere monotone......
More informationBANACH AND HILBERT SPACE REVIEW
BANACH AND HILBET SPACE EVIEW CHISTOPHE HEIL These notes will briefly review some basic concepts related to the theory of Banach and Hilbert spaces. We are not trying to give a complete development, but
More informationCURVES WHOSE SECANT DEGREE IS ONE IN POSITIVE CHARACTERISTIC. 1. Introduction
Acta Math. Univ. Comenianae Vol. LXXXI, 1 (2012), pp. 71 77 71 CURVES WHOSE SECANT DEGREE IS ONE IN POSITIVE CHARACTERISTIC E. BALLICO Abstract. Here we study (in positive characteristic) integral curves
More informationThe Henstock-Kurzweil-Stieltjes type integral for real functions on a fractal subset of the real line
The Henstock-Kurzweil-Stieltjes type integral for real functions on a fractal subset of the real line D. Bongiorno, G. Corrao Dipartimento di Ingegneria lettrica, lettronica e delle Telecomunicazioni,
More informationMATH 4330/5330, Fourier Analysis Section 11, The Discrete Fourier Transform
MATH 433/533, Fourier Analysis Section 11, The Discrete Fourier Transform Now, instead of considering functions defined on a continuous domain, like the interval [, 1) or the whole real line R, we wish
More information1 if 1 x 0 1 if 0 x 1
Chapter 3 Continuity In this chapter we begin by defining the fundamental notion of continuity for real valued functions of a single real variable. When trying to decide whether a given function is or
More informationWeek 1: Introduction to Online Learning
Week 1: Introduction to Online Learning 1 Introduction This is written based on Prediction, Learning, and Games (ISBN: 2184189 / -21-8418-9 Cesa-Bianchi, Nicolo; Lugosi, Gabor 1.1 A Gentle Start Consider
More informationON THE EXISTENCE AND LIMIT BEHAVIOR OF THE OPTIMAL BANDWIDTH FOR KERNEL DENSITY ESTIMATION
Statistica Sinica 17(27), 289-3 ON THE EXISTENCE AND LIMIT BEHAVIOR OF THE OPTIMAL BANDWIDTH FOR KERNEL DENSITY ESTIMATION J. E. Chacón, J. Montanero, A. G. Nogales and P. Pérez Universidad de Extremadura
More information1. Introduction. O. MALI, A. MUZALEVSKIY, and D. PAULY
Russ. J. Numer. Anal. Math. Modelling, Vol. 28, No. 6, pp. 577 596 (2013) DOI 10.1515/ rnam-2013-0032 c de Gruyter 2013 Conforming and non-conforming functional a posteriori error estimates for elliptic
More informationModern Optimization Methods for Big Data Problems MATH11146 The University of Edinburgh
Modern Optimization Methods for Big Data Problems MATH11146 The University of Edinburgh Peter Richtárik Week 3 Randomized Coordinate Descent With Arbitrary Sampling January 27, 2016 1 / 30 The Problem
More informationRepresentation of functions as power series
Representation of functions as power series Dr. Philippe B. Laval Kennesaw State University November 9, 008 Abstract This document is a summary of the theory and techniques used to represent functions
More informationIRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL. 1. Introduction
IRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL R. DRNOVŠEK, T. KOŠIR Dedicated to Prof. Heydar Radjavi on the occasion of his seventieth birthday. Abstract. Let S be an irreducible
More informationAN INTRODUCTION TO NUMERICAL METHODS AND ANALYSIS
AN INTRODUCTION TO NUMERICAL METHODS AND ANALYSIS Revised Edition James Epperson Mathematical Reviews BICENTENNIAL 0, 1 8 0 7 z ewiley wu 2007 r71 BICENTENNIAL WILEY-INTERSCIENCE A John Wiley & Sons, Inc.,
More informationNotes V General Equilibrium: Positive Theory. 1 Walrasian Equilibrium and Excess Demand
Notes V General Equilibrium: Positive Theory In this lecture we go on considering a general equilibrium model of a private ownership economy. In contrast to the Notes IV, we focus on positive issues such
More informationError Bound for Classes of Polynomial Systems and its Applications: A Variational Analysis Approach
Outline Error Bound for Classes of Polynomial Systems and its Applications: A Variational Analysis Approach The University of New South Wales SPOM 2013 Joint work with V. Jeyakumar, B.S. Mordukhovich and
More informationTHE FUNDAMENTAL THEOREM OF ALGEBRA VIA PROPER MAPS
THE FUNDAMENTAL THEOREM OF ALGEBRA VIA PROPER MAPS KEITH CONRAD 1. Introduction The Fundamental Theorem of Algebra says every nonconstant polynomial with complex coefficients can be factored into linear
More informationn k=1 k=0 1/k! = e. Example 6.4. The series 1/k 2 converges in R. Indeed, if s n = n then k=1 1/k, then s 2n s n = 1 n + 1 +...
6 Series We call a normed space (X, ) a Banach space provided that every Cauchy sequence (x n ) in X converges. For example, R with the norm = is an example of Banach space. Now let (x n ) be a sequence
More informationFurther Study on Strong Lagrangian Duality Property for Invex Programs via Penalty Functions 1
Further Study on Strong Lagrangian Duality Property for Invex Programs via Penalty Functions 1 J. Zhang Institute of Applied Mathematics, Chongqing University of Posts and Telecommunications, Chongqing
More informationSome stability results of parameter identification in a jump diffusion model
Some stability results of parameter identification in a jump diffusion model D. Düvelmeyer Technische Universität Chemnitz, Fakultät für Mathematik, 09107 Chemnitz, Germany Abstract In this paper we discuss
More informationON NONNEGATIVE SOLUTIONS OF NONLINEAR TWO-POINT BOUNDARY VALUE PROBLEMS FOR TWO-DIMENSIONAL DIFFERENTIAL SYSTEMS WITH ADVANCED ARGUMENTS
ON NONNEGATIVE SOLUTIONS OF NONLINEAR TWO-POINT BOUNDARY VALUE PROBLEMS FOR TWO-DIMENSIONAL DIFFERENTIAL SYSTEMS WITH ADVANCED ARGUMENTS I. KIGURADZE AND N. PARTSVANIA A. Razmadze Mathematical Institute
More informationDIRICHLET S PROBLEM WITH ENTIRE DATA POSED ON AN ELLIPSOIDAL CYLINDER. 1. Introduction
DIRICHLET S PROBLEM WITH ENTIRE DATA POSED ON AN ELLIPSOIDAL CYLINDER DMITRY KHAVINSON, ERIK LUNDBERG, HERMANN RENDER. Introduction A function u is said to be harmonic if u := n j= 2 u = 0. Given a domain
More informationCONTRIBUTIONS TO ZERO SUM PROBLEMS
CONTRIBUTIONS TO ZERO SUM PROBLEMS S. D. ADHIKARI, Y. G. CHEN, J. B. FRIEDLANDER, S. V. KONYAGIN AND F. PAPPALARDI Abstract. A prototype of zero sum theorems, the well known theorem of Erdős, Ginzburg
More information3. INNER PRODUCT SPACES
. INNER PRODUCT SPACES.. Definition So far we have studied abstract vector spaces. These are a generalisation of the geometric spaces R and R. But these have more structure than just that of a vector space.
More informationFuzzy Differential Systems and the New Concept of Stability
Nonlinear Dynamics and Systems Theory, 1(2) (2001) 111 119 Fuzzy Differential Systems and the New Concept of Stability V. Lakshmikantham 1 and S. Leela 2 1 Department of Mathematical Sciences, Florida
More informationFIRST YEAR CALCULUS. Chapter 7 CONTINUITY. It is a parabola, and we can draw this parabola without lifting our pencil from the paper.
FIRST YEAR CALCULUS WWLCHENW L c WWWL W L Chen, 1982, 2008. 2006. This chapter originates from material used by the author at Imperial College, University of London, between 1981 and 1990. It It is is
More informationON LIMIT LAWS FOR CENTRAL ORDER STATISTICS UNDER POWER NORMALIZATION. E. I. Pancheva, A. Gacovska-Barandovska
Pliska Stud. Math. Bulgar. 22 (2015), STUDIA MATHEMATICA BULGARICA ON LIMIT LAWS FOR CENTRAL ORDER STATISTICS UNDER POWER NORMALIZATION E. I. Pancheva, A. Gacovska-Barandovska Smirnov (1949) derived four
More informationLectures 5-6: Taylor Series
Math 1d Instructor: Padraic Bartlett Lectures 5-: Taylor Series Weeks 5- Caltech 213 1 Taylor Polynomials and Series As we saw in week 4, power series are remarkably nice objects to work with. In particular,
More informationTaylor and Maclaurin Series
Taylor and Maclaurin Series In the preceding section we were able to find power series representations for a certain restricted class of functions. Here we investigate more general problems: Which functions
More informationMetric Spaces. Chapter 7. 7.1. Metrics
Chapter 7 Metric Spaces A metric space is a set X that has a notion of the distance d(x, y) between every pair of points x, y X. The purpose of this chapter is to introduce metric spaces and give some
More informationNumerical methods for American options
Lecture 9 Numerical methods for American options Lecture Notes by Andrzej Palczewski Computational Finance p. 1 American options The holder of an American option has the right to exercise it at any moment
More informationDuality of linear conic problems
Duality of linear conic problems Alexander Shapiro and Arkadi Nemirovski Abstract It is well known that the optimal values of a linear programming problem and its dual are equal to each other if at least
More informationChapter 2: Binomial Methods and the Black-Scholes Formula
Chapter 2: Binomial Methods and the Black-Scholes Formula 2.1 Binomial Trees We consider a financial market consisting of a bond B t = B(t), a stock S t = S(t), and a call-option C t = C(t), where the
More informationEXISTENCE OF SOLUTIONS TO NONLINEAR, SUBCRITICAL HIGHER-ORDER ELLIPTIC DIRICHLET PROBLEMS WOLFGANG REICHEL AND TOBIAS WETH
EXISTENCE OF SOLUTIONS TO NONLINEAR, SUBCRITICAL HIGHER-ORDER ELLIPTIC DIRICHLET PROBLEMS WOLFGANG REICHEL AND TOBIAS WETH Abstract. We consider the -th order elliptic boundary value problem Lu = f(x,
More informationConvex Programming Tools for Disjunctive Programs
Convex Programming Tools for Disjunctive Programs João Soares, Departamento de Matemática, Universidade de Coimbra, Portugal Abstract A Disjunctive Program (DP) is a mathematical program whose feasible
More informationMultiple positive solutions of a nonlinear fourth order periodic boundary value problem
ANNALES POLONICI MATHEMATICI LXIX.3(1998) Multiple positive solutions of a nonlinear fourth order periodic boundary value problem by Lingbin Kong (Anda) and Daqing Jiang (Changchun) Abstract.Thefourthorderperiodicboundaryvalueproblemu
More informationAdaptive Online Gradient Descent
Adaptive Online Gradient Descent Peter L Bartlett Division of Computer Science Department of Statistics UC Berkeley Berkeley, CA 94709 bartlett@csberkeleyedu Elad Hazan IBM Almaden Research Center 650
More informationTHE CENTRAL LIMIT THEOREM TORONTO
THE CENTRAL LIMIT THEOREM DANIEL RÜDT UNIVERSITY OF TORONTO MARCH, 2010 Contents 1 Introduction 1 2 Mathematical Background 3 3 The Central Limit Theorem 4 4 Examples 4 4.1 Roulette......................................
More informationMean Value Coordinates
Mean Value Coordinates Michael S. Floater Abstract: We derive a generalization of barycentric coordinates which allows a vertex in a planar triangulation to be expressed as a convex combination of its
More informationTheory of Sobolev Multipliers
Vladimir G. Maz'ya Tatyana O. Shaposhnikova Theory of Sobolev Multipliers With Applications to Differential and Integral Operators ^ Springer Introduction Part I Description and Properties of Multipliers
More informationQUANTIZED INTEREST RATE AT THE MONEY FOR AMERICAN OPTIONS
QUANTIZED INTEREST RATE AT THE MONEY FOR AMERICAN OPTIONS L. M. Dieng ( Department of Physics, CUNY/BCC, New York, New York) Abstract: In this work, we expand the idea of Samuelson[3] and Shepp[,5,6] for
More informationOptimal boundary control of quasilinear elliptic partial differential equations: theory and numerical analysis
Optimal boundary control of quasilinear elliptic partial differential equations: theory and numerical analysis vorgelegt von Dipl.-Math. Vili Dhamo von der Fakultät II - Mathematik und Naturwissenschaften
More informationA STABILITY RESULT ON MUCKENHOUPT S WEIGHTS
Publicacions Matemàtiques, Vol 42 (998), 53 63. A STABILITY RESULT ON MUCKENHOUPT S WEIGHTS Juha Kinnunen Abstract We prove that Muckenhoupt s A -weights satisfy a reverse Hölder inequality with an explicit
More informationUniversal Algorithm for Trading in Stock Market Based on the Method of Calibration
Universal Algorithm for Trading in Stock Market Based on the Method of Calibration Vladimir V yugin Institute for Information Transmission Problems, Russian Academy of Sciences, Bol shoi Karetnyi per.
More informationINTEGRAL OPERATORS ON THE PRODUCT OF C(K) SPACES
INTEGRAL OPERATORS ON THE PRODUCT OF C(K) SPACES FERNANDO BOMBAL AND IGNACIO VILLANUEVA Abstract. We study and characterize the integral multilinear operators on a product of C(K) spaces in terms of the
More information1 Completeness of a Set of Eigenfunctions. Lecturer: Naoki Saito Scribe: Alexander Sheynis/Allen Xue. May 3, 2007. 1.1 The Neumann Boundary Condition
MAT 280: Laplacian Eigenfunctions: Theory, Applications, and Computations Lecture 11: Laplacian Eigenvalue Problems for General Domains III. Completeness of a Set of Eigenfunctions and the Justification
More informationNon-Arbitrage and the Fundamental Theorem of Asset Pricing: Summary of Main Results
Proceedings of Symposia in Applied Mathematics Volume 00, 1997 Non-Arbitrage and the Fundamental Theorem of Asset Pricing: Summary of Main Results Freddy Delbaen and Walter Schachermayer Abstract. The
More informationCHAPTER II THE LIMIT OF A SEQUENCE OF NUMBERS DEFINITION OF THE NUMBER e.
CHAPTER II THE LIMIT OF A SEQUENCE OF NUMBERS DEFINITION OF THE NUMBER e. This chapter contains the beginnings of the most important, and probably the most subtle, notion in mathematical analysis, i.e.,
More informationQuasi-static evolution and congested transport
Quasi-static evolution and congested transport Inwon Kim Joint with Damon Alexander, Katy Craig and Yao Yao UCLA, UW Madison Hard congestion in crowd motion The following crowd motion model is proposed
More informationNonparametric adaptive age replacement with a one-cycle criterion
Nonparametric adaptive age replacement with a one-cycle criterion P. Coolen-Schrijner, F.P.A. Coolen Department of Mathematical Sciences University of Durham, Durham, DH1 3LE, UK e-mail: Pauline.Schrijner@durham.ac.uk
More informationGeometrical Characterization of RN-operators between Locally Convex Vector Spaces
Geometrical Characterization of RN-operators between Locally Convex Vector Spaces OLEG REINOV St. Petersburg State University Dept. of Mathematics and Mechanics Universitetskii pr. 28, 198504 St, Petersburg
More informationI. Pointwise convergence
MATH 40 - NOTES Sequences of functions Pointwise and Uniform Convergence Fall 2005 Previously, we have studied sequences of real numbers. Now we discuss the topic of sequences of real valued functions.
More informationThe sum of digits of polynomial values in arithmetic progressions
The sum of digits of polynomial values in arithmetic progressions Thomas Stoll Institut de Mathématiques de Luminy, Université de la Méditerranée, 13288 Marseille Cedex 9, France E-mail: stoll@iml.univ-mrs.fr
More informationEnergy decay rates for solutions of Maxwell s system with a memory boundary condition
Collect. Math. vv, n (yyyy, 6 c 7 Universitat de Barcelona Energy decay rates for solutions of Maxwell s system with a memory boundary condition Serge Nicaise Université de Valenciennes et du Hainaut Cambrésis
More information