SCHAUDER ESTIMATES FOR ELLIPTIC AND PARABOLIC EQUATIONS. Xu-Jia Wang The Australian National University
|
|
- Bertram Hutchinson
- 5 years ago
- Views:
Transcription
1 SCHAUDER ESTIMATES FOR ELLIPTIC AND PARABOLIC EQUATIONS Xu-Jia Wang The Austalian National Univesity Intouction The Schaue estimate fo the Laplace equation was taitionally built upon the Newton potential theoy. Diffeent poofs wee foun late by Campanato [Ca], in which he intouce the Campanato space; Peete [P], who use the convolution of functions; Tuinge [T], who use the mollification of functions; an Simon [Si], who use a blowup agument. Also a petubation agument was foun by Safonov [S1,S2] an Caffaelli [C1, CC] fo fully nonlinea unifomly elliptic equations, which also applies to the Laplace equation. In this note we give an elementay an simple poof fo the Schaue estimates fo elliptic an paabolic equations. Ou poof allows the ight han sie to be Dini continuous an also give a shap estimate fo the moulus of continuity of the secon eivatives. It also yiels the log-lipschitz continuity of the gaient fo equations with boune ight han sie. Moeove, it also applies to nonlinea equations. Consie the Laplace equation 1. The Laplace equation u = f in (), (1.1) whee () is the unit ball in the Eucliean space R n. Suppose f is Dini continuous, namely <, whee = sup x y < f(x) f(y). Then we have the following estimate fo the moulus of continuity of D 2 u. Theoem 1. Let u C 2 be a solution of (1.1). Then x, y /2 (), D 2 u(x) D 2 u(y) C n [ sup u + + ], (1.2) 2 whee = x y, C n > epens only on n. It follows that if f C α ( ), then [ u C 2,α (/2 ) C n sup u + f Cα() ] α(1 α) if α (, 1), (1.3) D 2 u(x) D 2 u(y) C n (sup u + f C,1 log ) if α = 1. (1.4) * Wok suppote by the Austalian Reseach Council. 1
2 Poof. We will use the following elementay estimates fo hamonic functions, D k w() C n,k k sup B w, (1.5) whee C n,k epens only on n an k. Simple poofs of (1.5) can be foun in [E2]. Denote B k = B ρ k() (ρ = 1 2 ). Fo k =, 1,, let u k be the solution of u k = f() in B k, u k = u on B k. Then (u k u) = f() f. By the maximum pinciple, Hence Since u k+1 u k is hamonic, by (1.5) we have u k u L (B k ) Cρ 2k ω(ρ k ). (1.6) u k u k+1 L (B k+1 ) Cρ 2k ω(ρ k ). (1.7) D(u k u k+1 ) L (B k+2 ) Cρ k ω(ρ k ), D 2 (u k u k+1 ) L (B k+2 ) Cω(ρ k ). (1.8) Since u C 2, by (1.6), u k minus the quaatic pat of u is hamonic an is equal to o(ρ 2k ) in B k. Hence by (1.5), Du() = lim k Du k (), Fo any given point z nea the oigin, we have D 2 u() = lim k D 2 u k (). (1.9) D 2 u(z) D 2 u() I 1 + I 2 + I 3 =: (1.1) D 2 u k (z) D 2 u k () + D 2 u k () D 2 u() + D 2 u(z) D 2 u k (z). Let k 1 such that ρ k+4 z ρ k+3. Then by (1.8), we have z I 2 C ω(ρ k ) C. (1.11) j=k Similaly we can estimate I 3, though the solutions of v = f(z) in B j (z) an v = u on B j (z) fo j = k, k + 1,. To estimate I 1, enote h j = u j u j 1. By (1.5) an (1.7) we have D 2 h j (z) D 2 h j () Cρ j ω(ρ j ) z. (1.12) Hence I 1 D 2 u k 1 (z) D 2 u k 1 () + D 2 h k (z) D 2 h k () D 2 u (z) D 2 u () + k j=1 D2 h j (z) D 2 h j () C z ( u L + C ρ j ω(ρ j ) ) C z ( u L + C z ). (1.13) 2 Combining (1.1), (1.11), an (1.13) we obtain (1.2). This completes the poof. 2
3 Similaly we have the estimate at the bounay. Theoem 1. Let u C 2 ( {x n }) be a solution of u = f an u = on {x n = }. Suppose f is Dini continuous. Then x, y /2 {x n }, the estimate (1.2) hols. The poof is the same as that of Theoem 1, povie we eplace B k by B k {x n } an note that if w is a hamonic function in {x n } an w = on T, then w is hamonic in afte o extension in x n. Replacing the secon eivatives in the poof of (1.4) by the fist eivatives, an letting u k be the solution of u k = in B k, u k = u on B k, we also obtain the following log-lipschitz continuity fo Du, which was use in [Y] to establish the global existence of smooth solutions to the 2- Eule equation. Coollay 1. Let u C 1 be a solution of (1.1). Then x, y /2 (), Du(x) Du(y) C n (sup u + f L log ). (1.14) 2. Linea paabolic equations The above poof also applies to equations with vaiable coefficients. Let us consie the linea paabolic equation aij (x, t)u xi x j u t = f(x, t) in Q 1. (2.1) We enote Q = {(x, t) R n R 1 : x <, 2 < t }. Theoem 2. Let u C 2,1 x,t be a solution of (2.1). Suppose f an a ij ae Dini continuous. Then fo any points p 1 = (x 1, t 1 ), p 2 = (x 2, t 2 ) Q 1/2, [ xu(p 2 1 ) xu(p 2 2 ) C n sup u + Q 1 [ + C n sup xu 2 Q 1 ω f () ω a () + + ] ω f () 2 ω a () 2 ], (2.2) whee = p 1 p 2 (paabolic istance), ω f () = sup p1 p 2 < f(p 1 ) f(p 2 ), an ω a () = sup i,j ω aij (). Note that the moulus of continuity of t u follows fom (2.2) an equation (2.1). If a ij an f ae Höle continuous, by the intepolation inequality [L], we obtain the Schaue estimate fo paabolic equations. That is if a ij, f C α (Q 1 ) fo some α (, 1), then u 2+α,1+α/2 C x,t (Q 1/2 ) C[ ] sup u + f C α (Q 1 ). (2.3) Q 1 If α = 1, we have an estimate simila to (1.4). 3
4 Poof. Denote Q k = Q ρ k() (ρ = 1 2 ). Let u k be the solution of aij ()u xi x j u t = f() in Q k, u k = u on p Q k, whee p enotes the paabolic bounay. Then v = u u k satisfies aij ()v xi x j v t = f f() + (a ij () a ij (x))u xi x j. (2.4) By the maximum pinciple, u k u L (Q k ) Cρ 2k [ω f (ρ k ) + ω a (ρ k )η], whee η = sup xu. 2 Hence u k u k+1 L (Q k+1 ) Cρ 2k [ω f (ρ k ) + ω a (ρ k )η]. (2.5) Theefoe similaly as (1.8), sup Qk+2 { x(u 2 k u k+1 ), t (u k u k+1 ) } C[ω f (ρ k ) + ω a (ρ k )η]. (2.6) The est of the poof is the same as that of Theoem 1 an is omitte hee. 3. Fully nonlinea equations 3.1. Fully nonlinea, unifomly elliptic equations. The agument in 1 also applies to fully nonlinea unifomly elliptic equations. simplicity we consie the equation Fo F (D 2 u) = f(x) in (), (3.1) whee F is C 1,1. The estimates can be extene to opeatos of the fom F (D 2 u, x) by the feezing coefficient metho as in 2. We nee an a pioi estimate as (1.4). Assumption (a). Fo any solution to F (D 2 u + M) = c in B, whee c is a constant an M is a symmetic constant matix such that F (M) = c, we have the estimate whee ᾱ (, 1], C is inepenent of M, c an. u C 2,ᾱ (B /2 ) C 2 ᾱ u L ( ), (3.2) If F is concave o convex, the inteio C 2,ᾱ estimate fo some ᾱ (, 1] was establishe inepenently by Evans [E1] an Kylov [K]. Similaly to Theoem 1 we then have 4
5 Theoem 3. Let u C 2 be a solution of (3.1). Then x, y /2 (), If f C α ( ), we have D 2 u(x) D 2 u(y) C [ 1 ᾱ sup u + + ᾱ u C 2,α (/2 ) C [ ] sup u + f C α ( ) 1+ᾱ ]. (3.3) if < α < ᾱ, (3.4) D 2 u(x) D 2 u(y) Cᾱ[ sup u + f C α log ] if α = ᾱ, (3.5) u C 2,ᾱ (/2 ) C [ ] sup u + f C α ( ) if ᾱ < α 1. (3.6) The constant C epens on n, ᾱ, C in (3.2), an the ellipticity constants (least an lagest eigenvalues of { ij F ()}). Poof. The poof is vey simila to that of Theoem 1. Let u k be the solution of F (D 2 u k ) = f() in B k, u k = u on B k. (3.7) By Assumption (a), u k u k+1 satisfies a lineaize equation of F with coefficients in Cᾱ. Hence by the Schaue estimate fo linea elliptic equations, D 2 (u k u k+1 ) Bk+2 Cρ 2k u k u k+1 L Cω(ρ k ). (3.8) It follows that D 2 u k () is convegent if f is Dini continuous. By Assumption (a) an since u C 2, we have D 2 u k () D 2 u(). The only iffeence in the est pat of the poof is that (1.12) shoul be eplace by whee h k = u k u k+1. D 2 h k (z) D 2 h k () Cρ kᾱ ω(ρ k ) z ᾱ, (3.9) 3.2. The Monge-Ampèe equations. Estimate (1.2) (o (3.3) with ᾱ = 1) hols fo stictly convex solutions to the Monge- Ampèe equation etd 2 u = f(x) in, (3.1) whee C f C fo positive constants C, C, an = sup x y < f(x) f(y) (equivalent to sup x y < f 1/n (x) f 1/n (y) ). The constant C epens on n, C, C, an the moulus of convexity of u. The poof is simila to that of Theoem 1, except that we fist nee to nomalize the solution as follows. By subtacting a linea function, we assume u() = an Du() =. Denote S h = {x, u(x) < h}. Fo a sufficiently small h >, fist make unimoula linea tansfom T such that B R T (S h ) B nr. Then make a ilation x x/r an u u/r 2 such that S 1 B n an is invaiant une the changes. 5 is small. The Monge-Ampèe opeato
6 Now efine u k as in (3.7) (fo the Monge-Ampee equation it is moe convenient to use level sets than balls in (3.7)). We nee to veify Assumption (a) (with ᾱ = 1) fo all k. It suffices to show that the set E k = {x R n u k (x) < inf u k + ρ 2(k+1) } has a goo shape, namely B Rk E k B 2nRk fo concentate balls B Rk an B 2nRk. But this is guaantee at k = an also at k > by inuction, as long as ρ is chosen small an is sufficiently small. We wish to iscuss the egulaity of the Monge-Ampèe equation with moe etails in a sepaate wok Remaks. (i) By Aleksanov s maximum pinciple [GT], we can eplace = osc B f by = n f f() L n (B ) in the above poofs. (ii) By the existence an uniqueness of weak o viscosity solutions to the Diichlet poblem, the above theoems also hol fo weak o viscosity solutions. (iii) The shap estimate (1.2) fo the Laplace equation was establishe in [B] by elicate singula integal estimates. (iv) Theoem 3 with f C α (α < ᾱ) was pove by Safonov [S1, S2] an Caffaelli [C1, CC] by a petubation agument, using appoximation by quaatic polynomials. See also [K] fo the case when f is Dini continuous. Ou poof allow the case α ᾱ in (3.5) an (3.6) above. (v) The C 2,α estimate fo stictly convex solutions to the Monge-Ampèe equation (3.1) was pove in [C2]. When the Höle continuity of f is elaxe to Dini continuity, the continuity of D 2 u was pove in [W1]. (vi) Simila estimate to (1.14) also hols fo the paabolic equation (2.1) an fully nonlinea equation (3.1), but it is not tue fo the Monge-Ampèe equation (3.1), by an example in [W2]. Refeences [B] C. Buch, The Dini conition an egulaity of weak solutions of elliptic equations, J. Diff. Equa. 3 (1978), [C1] L.A. Caffaelli, Inteio a pioi estimates fo solutions of fully nonlinea equations, Ann. of Math. (2) 13 (1989), [C2] L.A. Caffaelli, Inteio W 2,p estimates fo solutions of Monge-Ampèe equations, Ann. Math., 131(199), [CC] L.A. Caffaelli an X. Cabe, Fully nonlinea elliptic equations, Ame. Math. Soc., [Ca] S. Campanato, Popiet i una famiglia i spazi funzionali, Ann. Scuola Nom. Sup. Pisa (3) 18(1964), [E1] L.C. Evans, Classical solutions of fully nonlinea, convex, secon oe elliptic equations, Comm. Pue Appl. Math., 25(1982), [E2] L.C. Evans, Patial Diffeential equations, Ame. Math. Soc., [GT] D. Gilbag an N.S. Tuinge, Elliptic patial iffeential equations of secon oe, Spinge, [K] J. Kovats, Fully nonlinea elliptic equations an the Dini conition, Comm. PDE 22 (1997), no , [K] N.V. Kylov, Bounely inhomogeneous elliptic an paabolic equations, Iz. Aka. Nauk. SSSR 46(1982), ; English tanslation in Math. USSR (1983). [L] G.M. Liebeman, Secon oe paabolic iffeential equations, Wol Scientific, [P] J. Peete, On convolution opeatos leaving L p,λ spaces invaiant, Ann. Mat. Pua Appl. 72 (1966),
7 [S1] M.V. Safonov, The classical solution of the elliptic Bellman equation, Dokl. Aka. Nauk SSSR 278(1984), ; English tanslation in Soviet Math Doklay 3(1984), [S2] M.V. Safonov, Classical solution of secon-oe nonlinea elliptic equations, Izv. Aka. Nauk SSSR Se. Mat. 52(1988), ; English tanslation in Math. USSR-Izv. 33(1989), [Si] L. Simon, Schaue estimates by scaling, Calc. Va. PDE, 5(1997), [T] N.S. Tuinge, A new appoach to the Schaue estimates fo linea elliptic equations, Poc. Cente Math. Anal., Austal. Nat. Univ., 14(1986), [Y] V. Yuovich, Non-stationay flows of an ieal incompessible flui (in Russian), Z. Vyčisl. Mat. i Mat. Fiz. 3(1963), [W1] X.-J. Wang, Remaks on the Regulaity of Monge-Ampèe equations, Poc. Inte. Conf. Nonlinea PDE, es: G.C. Dong an F.H. Lin, 1992, pp [W2] X.-J. Wang, Some counteexamples to the egulaity of Monge-Ampèe equations. Poc. Ame. Math. Soc. 123 (1995), Cente fo Mathematics an its Applications, Austalian National Univesity, Canbea ACT 2, Austalia aess: wang@maths.anu.eu.au 7
GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS
Annales Academiæ Scientiaum Fennicæ Mathematica Volumen 32, 2007, 595 599 GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS Teo Kilpeläinen, Henik Shahgholian and Xiao Zhong
More informationRegularity for Fully Nonlinear Elliptic Equations with Neumann Boundary Data
Communications in Patial Diffeential Equations, 31: 1227 1252, 2006 Copyight Taylo & Fancis Goup, LLC ISSN 0360-5302 pint/1532-4133 online DOI: 10.1080/03605300600634999 Regulaity fo Fully Nonlinea Elliptic
More informationMath 124B February 02, 2012
Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial
More informationMeasure Estimates of Nodal Sets of Polyharmonic Functions
Chin. Ann. Math. Se. B 39(5), 08, 97 93 DOI: 0.007/s40-08-004-6 Chinese Annals of Mathematics, Seies B c The Editoial Office of CAM and Spinge-Velag Belin Heidelbeg 08 Measue Estimates of Nodal Sets of
More informationSOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS
Fixed Point Theoy, Volume 5, No. 1, 2004, 71-80 http://www.math.ubbcluj.o/ nodeacj/sfptcj.htm SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS G. ISAC 1 AND C. AVRAMESCU 2 1 Depatment of Mathematics Royal
More information556: MATHEMATICAL STATISTICS I
556: MATHEMATICAL STATISTICS I CHAPTER 5: STOCHASTIC CONVERGENCE The following efinitions ae state in tems of scala anom vaiables, but exten natually to vecto anom vaiables efine on the same obability
More informationQuantum Mechanics I - Session 5
Quantum Mechanics I - Session 5 Apil 7, 015 1 Commuting opeatos - an example Remine: You saw in class that Â, ˆB ae commuting opeatos iff they have a complete set of commuting obsevables. In aition you
More information< 1. max x B(0,1) f. ν ds(y) Use Poisson s formula for the ball to prove. (r x ) x y n ds(y) (x B0 (0, r)). 1 nα(n)r n 1
7 On the othe hand, u x solves { u n in U u on U, so which implies that x G(x, y) x n ng(x, y) < n (x B(, )). Theefoe u(x) fo all x B(, ). G ν ds(y) + max g G x ν ds(y) + C( max g + max f ) f(y)g(x, y)
More informationHölder Continuity for Local Minimizers of a Nonconvex Variational Problem
Jounal of Convex Analysis Volume 10 003), No., 389 408 Hölde Continuity fo Local Minimizes of a Nonconvex Vaiational Poblem Giovanni Cupini Dipatimento di Matematica U. Dini, Univesità di Fienze, Viale
More informationA STABILITY RESULT FOR p-harmonic SYSTEMS WITH DISCONTINUOUS COEFFICIENTS. Bianca Stroffolini. 0. Introduction
Electonic Jounal of Diffeential Equations, Vol. 2001(2001), No. 02, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.swt.edu o http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) A STABILITY RESULT
More information15 Solving the Laplace equation by Fourier method
5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the
More informationL p Theory for the Multidimensional Aggregation Equation
L p Theoy fo the Multiimensional Aggegation Equation Anea L. Betozzi, Thomas Lauent* & Jesus Rosao Novembe 19, 29 Abstact We consie well-poseness of the aggegation equation tu + iv(uv) =, v = K u with
More informationOn absence of solutions of a semi-linear elliptic equation with biharmonic operator in the exterior of a ball
Tansactions of NAS of Azebaijan, Issue Mathematics, 36, 63-69 016. Seies of Physical-Technical and Mathematical Sciences. On absence of solutions of a semi-linea elliptic euation with bihamonic opeato
More informationESSENTIAL NORM OF AN INTEGRAL-TYPE OPERATOR ON THE UNIT BALL. Juntao Du and Xiangling Zhu
Opuscula Math. 38, no. 6 (8), 89 839 https://doi.og/.7494/opmath.8.38.6.89 Opuscula Mathematica ESSENTIAL NORM OF AN INTEGRAL-TYPE OPERATOR FROM ω-bloch SPACES TO µ-zygmund SPACES ON THE UNIT BALL Juntao
More informationA NOTE ON VERY WEAK SOLUTIONS FOR A CLASS OF NONLINEAR ELLIPTIC EQUATIONS
SARAJEVO JOURNAL OF MATHEMATICS Vol3 15 2007, 41 45 A NOTE ON VERY WEAK SOLUTIONS FOR A CLASS OF NONLINEAR ELLIPTIC EQUATIONS LI JULING AND GAO HONGYA Abstact We pove a new a pioi estimate fo vey weak
More informationExceptional regular singular points of second-order ODEs. 1. Solving second-order ODEs
(May 14, 2011 Exceptional egula singula points of second-ode ODEs Paul Gaett gaett@math.umn.edu http://www.math.umn.edu/ gaett/ 1. Solving second-ode ODEs 2. Examples 3. Convegence Fobenius method fo solving
More informationDoubling property for the Laplacian and its applications (Course Chengdu 2007)
Doubling popety fo the Laplacian and its applications Couse Chengdu 007) K.-D. PHUNG The oiginal appoach of N. Gaofalo and F.H. Lin Fo simplicity, we epoduce the poof of N. Gaofalo and F.H. Lin in the
More informationOn the integration of the equations of hydrodynamics
Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious
More informationGreen s Identities and Green s Functions
LECTURE 7 Geen s Identities and Geen s Functions Let us ecall The ivegence Theoem in n-dimensions Theoem 7 Let F : R n R n be a vecto field ove R n that is of class C on some closed, connected, simply
More informationPerron s method for nonlocal fully nonlinear equations
Peon s method fo nonlocal fully nonlinea equations Chenchen Mou Depatment of Mathematics, UCLA Los Angeles, CA 90095, U.S.A. E-mail: muchenchen@math.ucla.edu Abstact This pape is concened with existence
More informationSOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES
italian jounal of pue and applied mathematics n. 35 015 (433 44) 433 SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF OPERATOR MATRICES Watheq Bani-Domi Depatment of Mathematics
More information2017Ψ9 ADVANCES IN MATHEMATICS (CHINA) Sep., 2017
Λ46 Λ5Ω ff fl Π Vol. 46, No. 5 2017Ψ9 ADVANCES IN MATHEMATICS CHINA) Sep., 2017 doi: 10.11845/sxjz.2015219b Boundedness of Commutatos Geneated by Factional Integal Opeatos With Vaiable Kenel and Local
More informationJournal of Inequalities in Pure and Applied Mathematics
Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics
More informationGLOBAL SMOOTH AXISYMMETRIC SOLUTIONS OF 3-D INHOMOGENENOUS INCOMPRESSIBLE NAVIER-STOKES SYSTEM
GLOBAL SMOOTH AXISYMMETRIC SOLUTIONS OF 3-D INHOMOGENENOUS INCOMPRESSIBLE NAVIER-STOKES SYSTEM HAMMADI ABIDI AND PING ZHANG Abstact In this pape, we investigate the global egulaity to 3-D inhomogeneous
More informationThis aticle was oiginally published in a jounal published by Elsevie, the attached copy is povided by Elsevie fo the autho s benefit fo the benefit of the autho s institution, fo non-commecial eseach educational
More informationGeneral Relativity Homework 5
Geneal Relativity Homewok 5. In the pesence of a cosmological constant, Einstein s Equation is (a) Calculate the gavitational potential point souce with = M 3 (). R µ Rg µ + g µ =GT µ. in the Newtonian
More informationDouble sequences of interval numbers defined by Orlicz functions
ACTA ET COENTATIONES UNIVERSITATIS TARTUENSIS DE ATHEATICA Volume 7, Numbe, June 203 Available online at www.math.ut.ee/acta/ Double sequences of inteval numbes efine by Olicz functions Ayhan Esi Abstact.
More informationA PROOF OF THE INF-SUP CONDITION FOR THE STOKES EQUATIONS ON LIPSCHITZ DOMAINS
A PROOF OF THE INF-SUP CONDITION FOR THE STOKES EQUATIONS ON LIPSCHITZ DOMAINS JAMES H. BRAMBLE Abstact. The pupose of this pape is to pesent a athe simple poof of an inequality of Nečas [9] which is equivalent
More informationExistence and Uniqueness of Positive Radial Solutions for a Class of Quasilinear Elliptic Systems
JOURAL OF PARTIAL DIFFERETIAL EQUATIOS J Pat Diff Eq, Vol 8, o 4, pp 37-38 doi: 48/jpdev8n46 Decembe 5 Existence and Uniqueness of Positive Radial Solutions fo a Class of Quasilinea Elliptic Systems LI
More informationEquilibria of a cylindrical plasma
// Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the
More informationPH126 Exam I Solutions
PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium
More informationYUXIANG LI DEPARTMENT OF MATHEMATICAL SCIENCES, TSINGHUA UNIVERSITY, BEIJING , P.R.CHINA.
SOME REMARKS ON WILLMORE SURFACES EMBEDDED IN R 3 YUXIANG LI DEPARTMENT OF MATHEMATICAL SCIENCES, TSINGHUA UNIVERSITY, BEIJING 100084, P.R.CHINA. EMAIL: YXLI@MATH.TSINGHUA.EDU.CN. Abstact. Let f : C R
More informationThe first nontrivial curve in the fučĺk spectrum of the dirichlet laplacian on the ball consists of nonradial eigenvalues
enedikt et al. ounday Value Poblems 2011, 2011:27 RESEARCH Open Access The fist nontivial cuve in the fučĺk spectum of the diichlet laplacian on the ball consists of nonadial eigenvalues Jiřĺ enedikt 1*,
More informationElectric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions
Poblem 1: Electic Potential an Gauss s Law, Configuation Enegy Challenge Poblem Solutions Consie a vey long o, aius an chage to a unifom linea chage ensity λ a) Calculate the electic fiel eveywhee outsie
More informationRADIAL POSITIVE SOLUTIONS FOR A NONPOSITONE PROBLEM IN AN ANNULUS
Electonic Jounal of Diffeential Equations, Vol. 04 (04), o. 9, pp. 0. ISS: 07-669. UL: http://ejde.math.txstate.edu o http://ejde.math.unt.edu ftp ejde.math.txstate.edu ADIAL POSITIVE SOLUTIOS FO A OPOSITOE
More informationHIGHER REGULARITY OF THE FREE BOUNDARY IN THE OBSTACLE PROBLEM FOR THE FRACTIONAL LAPLACIAN
HIGHER REGULARITY OF THE FREE BOUNDARY IN THE OBSTACLE PROBLEM FOR THE FRACTIONAL LAPLACIAN YASH JHAVERI AND ROBIN NEUMAYER Abstact. We pove a highe egulaity esult fo the fee bounday in the obstacle poblem
More informationOn the regularity of the axisymmetric solutions of the Navier-Stokes equations
Math. Z. 9, 645 67 () Digital Object Identifie (DOI).7/s97 On the egulaity of the axisymmetic solutions of the Navie-Stokes equations Dongho Chae, Jihoon Lee Depatment of Mathematics, Seoul National Univesity,
More informationA THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM
A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM DIEGO AVERNA AND GABRIELE BONANNO Abstact. The aim of this pape is twofold. On one hand we establish a thee citical
More informationKOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS
Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,
More informationBrief summary of functional analysis APPM 5440 Fall 2014 Applied Analysis
Bief summay of functional analysis APPM 5440 Fall 014 Applied Analysis Stephen Becke, stephen.becke@coloado.edu Standad theoems. When necessay, I used Royden s and Keyzsig s books as a efeence. Vesion
More informationf h = u, h g = v, we have u + v = f g. So, we wish
Answes to Homewok 4, Math 4111 (1) Pove that the following examples fom class ae indeed metic spaces. You only need to veify the tiangle inequality. (a) Let C be the set of continuous functions fom [0,
More informationarxiv: v1 [math.na] 8 Feb 2013
A mixed method fo Diichlet poblems with adial basis functions axiv:1302.2079v1 [math.na] 8 Feb 2013 Nobet Heue Thanh Tan Abstact We pesent a simple discetization by adial basis functions fo the Poisson
More informationNumerical approximation to ζ(2n+1)
Illinois Wesleyan Univesity Fom the SelectedWoks of Tian-Xiao He 6 Numeical appoximation to ζ(n+1) Tian-Xiao He, Illinois Wesleyan Univesity Michael J. Dancs Available at: https://woks.bepess.com/tian_xiao_he/6/
More informationA Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationDISCONTINUOUS SOLUTIONS OF LINEAR, DEGENERATE ELLIPTIC EQUATIONS
DISCONTINUOUS SOLUTIONS OF LINEAR, DEGENERATE ELLIPTIC EQUATIONS XIAO ZHONG Abstact. We give examples of discontinuous solutions of linea, degeneate elliptic equations with divegence stuctue. These solve
More informationON LACUNARY INVARIANT SEQUENCE SPACES DEFINED BY A SEQUENCE OF MODULUS FUNCTIONS
STUDIA UNIV BABEŞ BOLYAI, MATHEMATICA, Volume XLVIII, Numbe 4, Decembe 2003 ON LACUNARY INVARIANT SEQUENCE SPACES DEFINED BY A SEQUENCE OF MODULUS FUNCTIONS VATAN KARAKAYA AND NECIP SIMSEK Abstact The
More informationConjugate Gradient (CG) Method
Optimization II Conugate Gaient CG Metho Anothe metho oes not equie explicit secon eivatives, an oes not even stoe appoximation to Hessian matix CG geneates sequence of conugate seach iections, implicitly
More informationLocalization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix
Jounal of Sciences, Islamic Republic of Ian (): - () Univesity of Tehan, ISSN - http://sciencesutaci Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matix H Ahsani
More informationarxiv: v2 [math.ap] 4 Jan 2018
Existence of C α solutions to intego-pdes axiv:1801.0108v [math.ap] 4 Jan 018 Chenchen Mou Depatment of Mathematics, UCLA Los Angeles, CA 90095, U.S.A. E-mail: muchenchen@math.ucla.edu Abstact This pape
More informationDo not turn over until you are told to do so by the Invigilator.
UNIVERSITY OF EAST ANGLIA School of Mathematics Main Seies UG Examination 2015 16 FLUID DYNAMICS WITH ADVANCED TOPICS MTH-MD59 Time allowed: 3 Hous Attempt QUESTIONS 1 and 2, and THREE othe questions.
More informationarxiv: v1 [math.ap] 18 Jan 2019
manuscripta mathematica manuscript No. (will be inserted by the editor) Yongpan Huang Dongsheng Li Kai Zhang Pointwise Boundary Differentiability of Solutions of Elliptic Equations Received: date / Revised
More informationSupplementary Information for On characterizing protein spatial clusters with correlation approaches
Supplementay Infomation fo On chaacteizing potein spatial clustes with coelation appoaches A. Shivananan, J. Unnikishnan, A. Raenovic Supplementay Notes Contents Deivation of expessions fo p = a t................................
More informationTHE HERMITE POLYNOMIAL & QUANTIZATION OF THE HARMONIC OSCILLATOR
THE HERMITE POLYNOMIAL & QUANTIZATION OF THE HARMONIC OSCILLATOR TIMOTHY JONES Abstact. The hamonic oscillato possesses a singula place in quantum mechanics. It is use in a wie vaiety of moels. Hee we
More informationAsymptotically Lacunary Statistical Equivalent Sequence Spaces Defined by Ideal Convergence and an Orlicz Function
"Science Stays Tue Hee" Jounal of Mathematics and Statistical Science, 335-35 Science Signpost Publishing Asymptotically Lacunay Statistical Equivalent Sequence Spaces Defined by Ideal Convegence and an
More informationCOLLAPSING WALLS THEOREM
COLLAPSING WALLS THEOREM IGOR PAK AND ROM PINCHASI Abstact. Let P R 3 be a pyamid with the base a convex polygon Q. We show that when othe faces ae collapsed (otated aound the edges onto the plane spanned
More informationJENSEN S INEQUALITY FOR DISTRIBUTIONS POSSESSING HIGHER MOMENTS, WITH APPLICATION TO SHARP BOUNDS FOR LAPLACE-STIELTJES TRANSFORMS
J. Austal. Math. Soc. Se. B 40(1998), 80 85 JENSEN S INEQUALITY FO DISTIBUTIONS POSSESSING HIGHE MOMENTS, WITH APPLICATION TO SHAP BOUNDS FO LAPLACE-STIELTJES TANSFOMS B. GULJAŠ 1,C.E.M.PEACE 2 and J.
More informationOn the Boundary Regularity for the 6D Stationary Navier-Stokes Equations
On the Bounday Regulaity fo the D Stationay Navie-Stokes Equations Jitao LIU, Wendong WANG, and Zhouping XIN The Institute of Mathematical Sciences, The Chinese Univesity of Hong Kong, Shatin, N.T., Hong
More informationBoundedness for Marcinkiewicz integrals associated with Schrödinger operators
Poc. Indian Acad. Sci. (Math. Sci. Vol. 24, No. 2, May 24, pp. 93 23. c Indian Academy of Sciences oundedness fo Macinkiewicz integals associated with Schödinge opeatos WENHUA GAO and LIN TANG 2 School
More informationResults on the Commutative Neutrix Convolution Product Involving the Logarithmic Integral li(
Intenational Jounal of Scientific and Innovative Mathematical Reseach (IJSIMR) Volume 2, Issue 8, August 2014, PP 736-741 ISSN 2347-307X (Pint) & ISSN 2347-3142 (Online) www.acjounals.og Results on the
More informationBOUNDARY REGULARITY FOR THE POISSON EQUATION IN REIFENBERG-FLAT DOMAINS. Antoine Lemenant. Yannick Sire
BOUNDARY REGULARITY FOR THE POISSON EQUATION IN REIFENBERG-FLAT DOMAINS Antoine Lemenant LJLL, Univesité Pais-Dideot, CNRS Pais, Fance Yannick Sie LATP, Univesité Aix-Maseille, CNRS Maseille, Fance Abstact
More informationJANOWSKI STARLIKE LOG-HARMONIC UNIVALENT FUNCTIONS
Hacettepe Jounal of Mathematics and Statistics Volume 38 009, 45 49 JANOWSKI STARLIKE LOG-HARMONIC UNIVALENT FUNCTIONS Yaşa Polatoğlu and Ehan Deniz Received :0 :008 : Accepted 0 : :008 Abstact Let and
More informationA CHARACTERIZATION ON BREAKDOWN OF SMOOTH SPHERICALLY SYMMETRIC SOLUTIONS OF THE ISENTROPIC SYSTEM OF COMPRESSIBLE NAVIER STOKES EQUATIONS
Huang, X. and Matsumua, A. Osaka J. Math. 52 (215), 271 283 A CHARACTRIZATION ON BRAKDOWN OF SMOOTH SPHRICALLY SYMMTRIC SOLUTIONS OF TH ISNTROPIC SYSTM OF COMPRSSIBL NAVIR STOKS QUATIONS XIANGDI HUANG
More informationN igerian Journal of M athematics and Applications V olume 24, (2015),
N igeian Jounal of M athematics an Applications V olume 24, 205), 228 236 c N ig. J. M ath. Appl. http : //www.kwsman.com Flow of an Incompessible MHD Thi Gae Flui Though a Cylinical Pipe with Isothemal
More informationMATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE. We consider second order constant coefficient scalar linear PDEs on R n. These have the form
MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE ANDRAS VASY We conside second ode constant coefficient scala linea PDEs on R n. These have the fom Lu = f L = a ij xi xj + b i xi + c i whee a ij b i and
More informationarxiv: v1 [math.ca] 31 Aug 2009
axiv:98.4578v [math.ca] 3 Aug 9 On L-convegence of tigonometic seies Bogdan Szal Univesity of Zielona Góa, Faculty of Mathematics, Compute Science and Econometics, 65-56 Zielona Góa, ul. Szafana 4a, Poland
More informationA Multivariate Normal Law for Turing s Formulae
A Multivaiate Nomal Law fo Tuing s Fomulae Zhiyi Zhang Depatment of Mathematics and Statistics Univesity of Noth Caolina at Chalotte Chalotte, NC 28223 Abstact This pape establishes a sufficient condition
More informationCLASSIFICATION OF BLOW-UP LIMITS FOR THE SINH-GORDON EQUATION
CLASSIFICATION OF BLOW-UP LIMITS FOR THE SINH-GORDON EQUATION ALEKS JEVNIKAR, JUNCHENG WEI, WEN YANG Abstact. The aim of this pape is to use a selection pocess an a caeful stuy of the inteaction of bubbling
More informationMuch that has already been said about changes of variable relates to transformations between different coordinate systems.
MULTIPLE INTEGRLS I P Calculus Cooinate Sstems Much that has alea been sai about changes of vaiable elates to tansfomations between iffeent cooinate sstems. The main cooinate sstems use in the solution
More informationOn the Poisson Approximation to the Negative Hypergeometric Distribution
BULLETIN of the Malaysian Mathematical Sciences Society http://mathusmmy/bulletin Bull Malays Math Sci Soc (2) 34(2) (2011), 331 336 On the Poisson Appoximation to the Negative Hypegeometic Distibution
More informationIntegral Control via Bias Estimation
1 Integal Contol via Bias stimation Consie the sstem ẋ = A + B +, R n, R p, R m = C +, R q whee is an nknown constant vecto. It is possible to view as a step istbance: (t) = 0 1(t). (If in fact (t) vaies
More informationAnalytical solutions to the Navier Stokes equations
JOURAL OF MATHEMATICAL PHYSICS 49, 113102 2008 Analytical solutions to the avie Stokes equations Yuen Manwai a Depatment of Applied Mathematics, The Hong Kong Polytechnic Univesity, Hung Hom, Kowloon,
More information3.1 Random variables
3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated
More informationHomework Set 3 Physics 319 Classical Mechanics
Homewok Set 3 Phsics 319 lassical Mechanics Poblem 5.13 a) To fin the equilibium position (whee thee is no foce) set the eivative of the potential to zeo U 1 R U0 R U 0 at R R b) If R is much smalle than
More informationLiouville theorems for a singular parabolic differential inequality with a gradient term
Fang and Xu Jounal of Inequalities and Applications 214, 214:62 http://www.jounalofinequalitiesandapplications.com/content/214/1/62 R E S E A R C H Open Access Liouville theoems fo a singula paabolic diffeential
More informationRegularity estimates for fully non linear elliptic equations which are asymptotically convex
Regularity estimates for fully non linear elliptic equations which are asymptotically convex Luis Silvestre and Eduardo V. Teixeira Abstract In this paper we deliver improved C 1,α regularity estimates
More informationDo Managers Do Good With Other People s Money? Online Appendix
Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth
More informationThe inviscid limit of incompressible fluid flow in an annulus
The inviscid limit of incompessible fluid flow in an annulus Saa Fietze, Robet Geity, and Tiago Picon ugust 8, 2006 bstact Incompessible, ciculaly symmetic fluid flow in a two-dimensional annulus = {x
More informationAn Exact Solution of Navier Stokes Equation
An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in
More informationFOURIER-BESSEL SERIES AND BOUNDARY VALUE PROBLEMS IN CYLINDRICAL COORDINATES
FOURIER-BESSE SERIES AND BOUNDARY VAUE PROBEMS IN CYINDRICA COORDINATES The paametic Bessel s equation appeas in connection with the aplace opeato in pola coodinates. The method of sepaation of vaiables
More informationFall 2014 Randomized Algorithms Oct 8, Lecture 3
Fall 204 Randomized Algoithms Oct 8, 204 Lectue 3 Pof. Fiedich Eisenband Scibes: Floian Tamè In this lectue we will be concened with linea pogamming, in paticula Clakson s Las Vegas algoithm []. The main
More informationarxiv: v1 [math.ap] 11 Nov 2016
axiv:6.358v [math.ap] Nov 6 Remaks on the Hady type inequalities with emainde tems in the famewok of equalities Abstact. Shuji Machihaa, Tohu Ozawa, and Hidemitsu Wadade Dedicated to Pofesso Nakao Hayashi
More informationCompactly Supported Radial Basis Functions
Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically
More informationRATE OF CONVERGENCE OF FINITE-DIFFERENCE APPROXIMATIONS FOR DEGENERATE LINEAR PARABOLIC EQUATIONS WITH C 1 AND C 2 COEFFICIENTS
Electonic Jounal of Diffeential Equations, Vol. 2005(2005), No. 102, pp. 1 25. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu o http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) RATE
More informationA NOTE ON ROTATIONS AND INTERVAL EXCHANGE TRANSFORMATIONS ON 3-INTERVALS KARMA DAJANI
A NOTE ON ROTATIONS AND INTERVAL EXCHANGE TRANSFORMATIONS ON 3-INTERVALS KARMA DAJANI Abstact. Wepove the conjectue that an inteval exchange tansfomation on 3-intevals with coesponding pemutation (1; 2;
More informationOn the global uniform asymptotic stability of time-varying dynamical systems
Stud. Univ. Babeş-Bolyai Math. 59014), No. 1, 57 67 On the global unifom asymptotic stability of time-vaying dynamical systems Zaineb HajSalem, Mohamed Ali Hammami and Mohamed Mabouk Abstact. The objective
More informationUnobserved Correlation in Ascending Auctions: Example And Extensions
Unobseved Coelation in Ascending Auctions: Example And Extensions Daniel Quint Univesity of Wisconsin Novembe 2009 Intoduction In pivate-value ascending auctions, the winning bidde s willingness to pay
More informationSome Lower and Upper Bounds on the Third ABC Co-index
Intenational JMath Combin Vol4(07), 84-90 Some Lowe an Uppe Bouns on the Thi BC Co-inex Deepak S Revanka, Piyanka S Hane, Satish P Hane 3 an Vijay Teli 3 Depatment of Mathematics, KLE, D M S S C E T, Belagavi
More information15. SIMPLE MHD EQUILIBRIA
15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium
More informationChromatic number and spectral radius
Linea Algeba and its Applications 426 2007) 810 814 www.elsevie.com/locate/laa Chomatic numbe and spectal adius Vladimi Nikifoov Depatment of Mathematical Sciences, Univesity of Memphis, Memphis, TN 38152,
More informationRADIALLY SYMMETRIC SOLUTIONS TO THE GRAPHIC WILLMORE SURFACE EQUATION
RADIALLY SYMMETRIC SOLUTIONS TO THE GRAPHIC WILLMORE SURFACE EQUATION JINGYI CHEN AND YUXIANG LI Abstact. We show that a smooth adially symmetic solution u to the gaphic Willmoe suface equation is eithe
More informationNew Singular Standing Wave Solutions Of The Nonlinear Schrodinger Equation
New Singula Standing Wave Solutions Of The Nonlinea Schodinge Equation W. C. Toy Abstact We pove existence, and asymptotic behavio as, of a family of singula solutions of 1) y + y +y y p 1 y = 0, 0 <
More informationRegularity Criteria for the Magneto-micropolar Fluid Equations in Terms of Direction of the Velocity
Applied Mathematical Sciences, Vol. 8, 01, no. 71, 51-59 HIKARI td, www.m-hikai.com http://dx.doi.og/10.1988/ams.01.05 Regulaity Citeia fo the Magneto-micopola Fluid Equations in Tems of Diection of the
More informationMoment-free numerical approximation of highly oscillatory integrals with stationary points
Moment-fee numeical appoximation of highly oscillatoy integals with stationay points Sheehan Olve Abstact We pesent a method fo the numeical quadatue of highly oscillatoy integals with stationay points.
More informationON EXISTENCE, UNIQUENESS AND L r -EXPONENTIAL STABILITY FOR STATIONARY SOLUTIONS TO THE MHD EQUATIONS IN THREE-DIMENSIONAL DOMAINS
ANZIAM J. 46004, 95 09 ON EXISTENCE, UNIQUENESS AND L -EXPONENTIAL STABILITY FOR STATIONARY SOLUTIONS TO THE MHD EQUATIONS IN THREE-DIMENSIONAL DOMAINS CHUNSHAN ZHAO and KAITAI LI Received 4 August, 000;
More informationOn the radial derivative of the delta distribution
On the adial deivative of the delta distibution Fed Backx, Fank Sommen & Jasson Vindas Depatment of Mathematical Analysis, Faculty of Engineeing and Achitectue, Ghent Univesity Depatment of Mathematics,
More informationMathematische Annalen
Math. Ann. 212 354:451 463 DOI 1.17/s28-11-74-6 Mathematische Annalen Estimate an monotonicity of the fist eigenvalue une the Ricci flow Xiaoong Cao Songbo Hou Jun Ling Receive: 9 Septembe 29 / Revise:
More informationAbsorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere
Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in
More informationAn analytical proof of Hardy-like inequalities related to the Dirac operator
An analytical poof of Hady-like inequalities elated to the Diac opeato Jean Dolbeault a,1 Maia J. Esteban a,1 Michael Loss b,2 Luis Vega c,1 a CEREMADE, Univesité Pais-Dauphine, 75775 Pais Cedex 16, Fance
More informationarxiv:gr-qc/ v2 14 Aug 2006
Semilinea wave equations on the Schwazschil manifol I: Local Decay Estimates. P. Blue Mathematics ept., Rutges Univesity Piscataway, NJ 8854, USA A. Soffe Mathematics ept., Institute fo Avance Stuies Pinceton,
More informationInfinitely many solutions and Morse index for non-autonomous elliptic problems
Infinitely many solutions and Mose index fo non-autonomous elliptic poblems Philip Koman Depatment of Mathematical Sciences Univesity of Cincinnati Cincinnati Ohio 45221-0025 Abstact Ou fist esult is a
More information