BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS
|
|
- Kelley Sanders
- 5 years ago
- Views:
Transcription
1 BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS XUAN THINH DUONG, JI LI, AND ADAM SIKORA Absrac Le M be a manifold wih ends consruced in [2] and be he Laplace-Belrami operaor on M In his noe, we show he weak ype, and L p boundedness of he Hardy-Lilewood maximal funcion and of he maximal funcion associaed wih he hea semigroup M fx = sup exp fx on L p M for < p The significance of hese resuls comes from he fac ha M does no saisfies he doubling condiion Inroducion The heory of Calderón-Zygmund operaors has played a crucial role in harmonic analysis and is wide applicaions in he las half a cenury or so We refer readers o he excellen book [7] and he references herein In he sandard Calderón-Zygmund heory, an essenial feaure is he so-called doubling condiion Le us recall ha a meric space X, d, µ equipped wih a meric d and a measure µ saisfies he doubling condiion if here exiss a consan C such ha for all x X and r > 0 µbx, 2r CµBx, r Many meric spaces in classical analysis saisfy he doubling condiion such as he Euclidean spaces and heir smooh domains wih Lebesgue measure, Lie groups and manifolds of polynomial growh However, here are significan applicaions for which underlying ambien spaces do no saisfy he doubling condiion, for example domains of Euclidean spaces wih rough boundaries, Lie groups and manifolds wih exponenial growh To hese non-doubling spaces, he sandard Calderón-Zygmund heory esablished in he 70 s and 80 s is no applicable Recen works of Nazarov, Treil, Volberg, Tolsa and ohers, see for example [3, 4, 5, 6, 8, 9] show ha a large par of he sandard Calderön-Zygmund heory can be adaped o he case of non-doubling spaces which saisfy a mild growh condiion In [], Duong and A McInosh also obain esimaes for cerain singular inegrals acing on some domains which do no necessarily saisfy he doubling condiion However, he heory of singular inegrals This work was sared during he second named auhor s say a Macquarie Universiy J Li was suppored by a scholarship from Macquarie Universiy during , and is suppored by China Posdocoral Science Foundaion funded projec Gran No and he Fundamenal Research Funds for he Cenral Universiies No lgpy Mahemaics Subjec Classificaion: Primary 42B5; Secondary 35P99 37
2 38 XUAN THINH DUONG, JI LI, AND ADAM SIKORA on non-doubling spaces is far from being complee and here are sill many significan open problems in his opic In his noe, we sudy he boundedness of cerain maximal funcions on non-doubling manifolds wih ends More specifically, we will show he weak ype, of he Hardy-Lilewood maximal funcion and he maximal funcion associaed wih he hea semigroup of he Laplace-Belrami operaor as well as L p boundedness for hese maximal operaors for < p Le us recall ha he maximal funcion associaed wih he hea semigroup is defined by he following formula M fx = sup exp fx for f L p M, p The behaviour of he kernels of he semigroup exp on manifolds wih ends was sudied in [2] For he convenience of reader, we recall he main resul of [2] in he nex secion as i plays a key role in our esimaes of he operaor M 2 Manifolds wih ends Le M be a complee non-compac Riemannian manifold Le K M be a compac se wih non-empy inerior and smooh boundary such ha M\K has k conneced componens E,, E k and each E i is non-compac We say in such a case ha M has k ends wih respec o K and refer o K as he cenral par of M In many cases, each E i is isomeric o he exerior of a compac se in anoher manifold M i In such case, we wrie M = M M 2 M k and refer o M as a conneced sum of he manifolds M i, i =, 2,, k Following [2] we consider he following model case Fix a large ineger N which will be he opological dimension of M and, for any ineger m [2, N], define he manifold R m by R m = R m S N m The manifold R m has opological dimension N bu is dimension a infiniy is m in he sense ha V x, r r m for r, see [2, 3] Thus, for differen values of m, he manifold R m have differen dimension a infiniy bu he same opological dimension N, This enables us o consider finie conneced sums of he R m s Fix N and k inegers N, N 2,, N k [2, N] such ha Nex consider he manifold N = max{n, N 2,, N k } M = R N R N 2 R N k In [2] Grigoryan and Saloff-Cose esablish boh he global upper bound and lower bound for he hea kernel acing on his model class Now we recall he firs par of heir resuls wih he hypohesis ha n := min i k N i > 2 Le K be he cenral par of M and E,, E k be he ends of M so ha E i is isomeric o he complemen of a compac se in R N i Wrie E i = R N i \K
3 BOUNDEDNESS OF MAXIMAL FUNCTIONS 39 Thus, x R N i \K means ha he poin x M belongs o he end associaed wih R N i For any x M, define x := sup dx, z, z K where d = dx, y is he geodesic disance in M One can see ha x is separaed from zero on M and x + dx, K For x M, le Bx, r := {y M : dx, y < r} be he geodesic ball wih cener x M and radius r > 0 and le V x, r = µbx, r where µ is a Riemannian measure on M Throughou he paper, we ake he simple case k = 2 for he model of meric spaces wih non-doubling measure, ie, we se M = R n R m wih 2 < n < m Then, from he consrucion of he manifold M, we can see ha a V x, r r m for all x M, when r ; b V x, r r n for Bx, r R n, when r > ; and b V x, r r m for x R n \K, r > 2 x, or x R m, r > I is no difficul o check ha M does no saisfy he doubling condiion Indeed, consider a sequence of balls Bx k, r k R n such ha r k = x k > and r k as k Then V x k, r k r k n However, V x k, 2r k r k m and he doubling condiion fails Le be he Laplace-Belrami operaor on M and e he hea semigroup generaed by We denoe by p x, y he hea kernel associaed o e We recall here he following heorem which is he main resuls obain in [2] Theorem A [2] Le M = R m R n wih 2 < n < m Then he hea kernel p x, y saisfies he following esimaes For and all x, y M, p x, y C V x, exp c 2 For x, y K and all >, p x, y C n/2 exp c 3 For x R m \K, y K and all >, p x, y C n/2 x m 2 + m/2 4 For x R n \K, y K and all >, p x, y C n/2 x n 2 + n/2 5 For x R m \K, y R n \K and all >, p x, y C n/2 x m 2 + m/2 y n 2 dx, y2 dx, y2 exp c exp c exp c dx, y2 dx, y2 dx, y2
4 40 XUAN THINH DUONG, JI LI, AND ADAM SIKORA 6 For x, y R m \K and all >, C n/2 p x, y x m 2 y m 2 exp 7 For x, y R n \K and all >, p x, y C n/2 x n 2 y n 2 exp c x 2 + y 2 c x 2 + y 2 + C m/2 exp c + C n/2 exp c dx, y2 dx, y2 3 The boundedness of Hardy-Lilewood maximal funcion In his secion we consider M = R m R n for m > n > 2 A main difficuly which we encouner in our sudy is ha he doubling condiion fails in his seing However, local doubling sill holds, ie he doubling condiion holds for a ball Bx, r under he addiional assumpion r Le us recall nex he sandard definiion of uncenered Hardy Lilewood Maximal funcion For any p [, ] and any funcion f L p le { } Mfx = fz dz : x By, r V y, r sup y M, r>0 By,r Also we have he cenered Hardy Lilewood Maximal funcion For any p [, ] and any funcion f L p we se M c fx = sup fz dz r>0 V x, r Bx,r I is sraighforward o see ha M c fx Mfx for all x Moreover in he doubling seing 2 Mf CM c f, where C is he same consan as in he doubling condiion However, we poin ou ha esimae 2 does no hold in he seing M = R m R n wih m > n > 2 More specifically, one has he following proposiion Proposiion In he seing M = R m R n wih m > n > 2, he esimae Mf CM c f fails for any consan C Proof Denoe he characerisic funcions of he ses R m \K, R n \K and K by χ, χ 2 and χ 3, respecively Le f = χ 2 Then for any fixed x R m, we firs noe ha χ 2 ydy V B B for any B x Furhermore, we can consruc balls B x such ha he ball B wih cenre z, radius r, lying mosly in R n by choosing z R n, r large enough and dz, x = r ɛ for ɛ sufficienly small This implies ha Mfx = sup χ 2 ydy = B x V B Now consider he cenered Hardy Lilewood Maximal funcion M c f By he definiion for any r > 0, fzdz = C V x, r r m dz Bx,r B Bx,r R n \K
5 BOUNDEDNESS OF MAXIMAL FUNCTIONS 4 This implies ha r > x and he erm C r m Bx,r R n \K dz is comparable r x n o r m I is easy o check ha he maximal value of he above erm is comparable o n x n / m x m, m n m n which shows ha Mf is no poinwise bounded by any muliple of M c f since he maximal value depends on x and ends o zero when x goes o This proves Proposiion Theorem 2 The maximal funcion Mf is of weak ype, and bounded on all L p spaces for < p Proof Here and hroughou he paper, for he sake of simpliciy we use o denoe he measure of he ses in M I is sraighforward ha he maximal funcion Mf is bounded on L We will show ha he weak ype, esimae {x: Mfx > α} C f α holds, hen he L p boundedness of Mf follows from he Marcinkiewicz inerpolaion heorem We consider wo cases: Case : f α < Following he sandard proof of weak ype for Maximal operaor we noe ha for any x {x: Mfx > α} here exis a ball such ha x By, r and 3 fz dz > α V y, r By,r This implies f = M fz dz By,r fz dz > αv y, r Therefore > f α > V y, r, hence r and he ball By, r saisfies doubling condiion so one can use sandard Viali covering argumen o prove weak ype, esimae in his case Case 2 : f α Firs we spli M ino hree componens R m \K, R n \K and K, and denoe heir characerisic funcions by χ, χ 2 and χ 3, respecively Since he maximal funcion Mf is sublinear, i is enough o show ha each of he hree erms Mχ f, Mχ 2 f and Mχ 3 f is of weak ype, We firs consider Mχ f Then {x : Mχ fx > α} {x R m \K : Mχ fx > α} + {x R n \K : Mχ fx > α} + {x K : Mχ fx > α} =: I + I 2 + I 3
6 42 XUAN THINH DUONG, JI LI, AND ADAM SIKORA The esimae for I follows from he classical weak ype, esimae since χ f is a funcion on R m \K and he measure on R m \K saisfies he doubling condiion To esimae I 2, we noe ha for all x R n \K, { sup By, r : r > dx, y and By, r Rm \K The above inequaliy implies ha 4 Mχ fx C χ f x n Hence x R n \K I 2 {x R n \K : C χ f x n > α} C χ f α } C f α C x n To esimae I 3, we noe ha he measure of K is finie Therefore I 3 K C f α To prove he weak, esimae of Mχ 2 f we noe ha {x : Mχ 2 fx > α} {x R m \K : Mχ 2 fx > α} + {x R n \K : Mχ 2 fx > α} + {x K : Mχ 2 fx > α} =: II + II 2 + II 3 II 2 and II 3 can be verified following he same seps as for I and I 3, respecively To esimaes II we observe ha 5 Mχ 2 fx C χ 2f x m Hence II 2 C f α Similarly, o deal wih Mχ 3 f we noe ha x R m \K {x : Mχ 3 fx > α} {x R m \K : Mχ 3 fx > α} + {x R n \K : Mχ 3 fx > α} + {x K : Mχ 3 fx > α} =: III + III 2 + III 3 The esimae of III follows immediaely since he measure on R m \K K saisfies he doubling condiion The esimae of III 3 is he same as ha of I 3 or II 3 Nex o esimaes III 2 we furher decompose {x R n \K} ino wo pars {x R n \K : x 2} and {x R n \K : x > 2} For he firs par we direcly have {x R n \K : x 2, Mχ 3 fx > α} C C f α For he second par, similar o he esimae of I 2, we noe ha for all x R n \K and x > 2, Hence, { sup : r > dx, y and By, r K By, r Mχ 3 fx C χ 3f x n x R n \K and x > 2, } C x n
7 which implies ha BOUNDEDNESS OF MAXIMAL FUNCTIONS 43 {x R n \K : x > 2, Mχ 3 fx > α} C f α Combining he esimaes of Mχ f, Mχ 2 f and Mχ 3 f we verify 3 The proof of Theorem 2 is now complee 4 The boundedness of he maximal funcion M In his secion we prove ha he hea maximal operaor saisfies weak ype, and is bounded on L p for < p We noe ha when he hea semigroup has a Gaussian upper bound, hen he maximal funcion corresponding o hea semigroup is poinwise dominaed by he Hardy-Lilewood maximal operaor In his case, he weak ype, esimae of M follows from he weak ype, esimae of he Hardy-Lilewood maximal funcion However, in considered seing his is no longer he case and he operaor M can no be conrolled by he Hardy-Lilewood maximal funcion We can see his via he esimaes of he hea semigroup in he proof of Theorem 3 below where we give a direc proof of he weak ype esimaes of he hea maximal operaor The following heorem is he main resul of his secion Theorem 3 Le M be he operaor defined by Then M is weak ype, and for any funcion f L p, < p, he following esimaes hold M f L p M C f L p M Proof We firs show ha M is weak ype,, ie, we need o prove ha here exiss a posiive consan C such ha for any f L M and for any λ > 0, 6 { x M : sup exp fx > λ } C λ f L M Fix f L M Similarly as in Secion 3 we se f x = fxχ R m \Kx, f 2 x = fxχ R n \Kx and f 3 x = fxχ K x, where K is he cener of M To prove 6, i suffices o verify ha he following hree esimaes hold: 7 { x R m \K : sup exp fx > λ } C λ f L M; 8 9 { x R n \K : sup exp fx > λ } C λ f L M; { x K : sup exp fx > λ } C λ f L M
8 44 XUAN THINH DUONG, JI LI, AND ADAM SIKORA We firs consider 7 Since M is a sublinear operaor, we have { x R m \K : sup exp fx > λ } { x R m \K : sup exp f x > λ } + { x R m \K : sup exp f 2 x > λ } + { x R m \K : sup exp f 3 x > λ } =: I + I 2 + I 3 To esimae I we consider wo cases Case : > By Theorem A Poin 6 + y 2 exp f x C R m \K n 2 x m 2 y m 2 exp c x 2 + cdx, y2 exp fy dy m 2 =: I + I 2 To esimae I we noe ha n/2 n/2 + y 2 x m 2 y m 2 exp c x 2 C x m 2 y m 2 + x 2 + y 2 n 2 x m 2+n x m since y and n > 2 Hence, I C R m \K x m 2+n fydy C f L M x m To esimae I 2 we noe ha if x R m \K hen cdx, y2 exp fy dy CM R m \Kfx R m \K m 2 where M R m \Kfx is he Hardy-Lilewood maximal funcion acing on R m \K Case 2: By Theorem A Poin exp f x exp R m \K m 2 n 2 cdx, y2 fy dy Again he righ-hand side of above esimae is bounded by M R m \Kfx These esimaes prove weak ype, for I since R m \K saisfies doubling condiion Nex we show weak ype esimaes for I 2 We also consider wo cases
9 BOUNDEDNESS OF MAXIMAL FUNCTIONS 45 Case : > By Theorem A Poin 5 exp f 2 x C n 2 x + m 2 m 2 y n 2 R n \K =: I 2 + I 22 exp cdx, y2 fy dy Similarly as in he esimae for I we ge n 2 I 2 C fy dy R n \K n 2 x m 2 + dx, y 2 n 2 C x m 2+n fy dy C f x m, R n \K since n > 2, x and in his case, dx, y x To esimae I 22 we noe ha m I 22 C R n \K m 2 y n 2 + dx, y 2 m fy dy m 2 C R n \K + dx, y 2 m fy dy m C R n \K fy dy + dx, y 2m m since y By decomposing he Poisson kernel ino + dx, y 2m annuli, i is easy o see ha he las erm of he above inequaliy is bounded by CM R n \Kfx Case 2: Again by Theorem A Poin cdx, y2 exp f 2 x C exp fy dy R n \K m 2 Hence i is bounded by CMfx Similar o I, we have I 2 C f λ Now we consider I 3 Case : > By Theorem A Poin 3 exp f 3 x C K n 2 x + cdx, y2 exp fy dy m 2 m 2 =: I 3 + I 32 To esimae I 3 we noe ha n 2 I 3 C n 2 x m 2 + dx, y 2 n 2 K C f x m, fy dy C f x m+n 2
10 46 XUAN THINH DUONG, JI LI, AND ADAM SIKORA where we use he facs ha n > 2, x > and ha in his case, dx, y x Similarly, m 2 I 32 C fy dy C f m 2 + dx, y 2 m 2 x m Case 2: By Theorem A Poin exp f 3 x exp K K m 2 cdx, y2 fy dy Hence i is bounded by CMfx Combining he esimaes of he wo cases, we obain I 3 C f L M λ The esimaes of I, I 2 and I 3 ogeher imply 7 We now urn o he esimae of 8 Similarly o he proof of 7, we have { x R n \K : sup exp fx > λ } { x R n \K : sup exp f x > λ } + { x R n \K : sup exp f 2 x > λ } + { x R n \K : sup exp f 3 x > λ } =: II + II 2 + II 3 We noe ha he esimae of II is similar o ha of I 2, while he esimae of II 2 is similar o ha of I Moreover, he esimae of II 3 is similar o ha of I 3 Therefore we can verify ha 8 holds Finally, we urn o he esimae of 9 We have { x K : sup exp fx > λ } { x K : sup exp f x > λ } + { x K : sup exp f 2 x > λ } + { x K : sup exp f 3 x > λ } =: III + III 2 + III 3 Also, we poin ou ha he esimae of III is similar o ha of I 3 and ha he esimae of III 2 is similar o ha of II 3 Concerning he erm III 3, we firs noe ha in his case x K We have exp f 3 x C K m 2 exp cdx, y2 fy dy I is easy o see ha he righ-hand side of he above inequaliy is bounded by CMfx Thus, we have III 3 C f λ
11 BOUNDEDNESS OF MAXIMAL FUNCTIONS 47 Hence, we can see ha 9 holds Now 7, 8 and 9 ogeher imply ha 6 holds, ie, M is of weak ype, Nex, noe ha he semigroup exp is submarkovian so M is bounded on L M This ogeher wih 6, implies ha M is bounded on L p M for all < p < The proof of Theorem 3 is complee References X T Duong and A McInosh, Singular inegral operaors wih non-smooh kernels on irregular domains, Rev Ma Iberoamericana 5 999, A Grigor yan and L Saloff-Cose, Hea kernel on manifolds wih ends, Ann Ins Fourier Grenoble, no5, , F Nazarov, S Treil and A Volberg, Cauchy inegral and Calderón-Zygmund operaors on nonhomogeneous spaces, Inerna Mah Res Noices, Vol 5, 997, p F Nazarov, S Treil and A Volberg, Weak ype esimaes and Colar inequaliies for Calderón-Zygmund operaors on nonhomogeneous spaces, Inerna Mah Res Noices, Vol 9, 998, p F Nazarov, S Treil and A Volberg, The T b- heorem on non-homogeneous spaces, Aca Mah, Vol 90, 2003, No 2, p J Maeu, P Maila, A Nicolau, J Orobig, BMO for non doubling measures, Duke Mah J, , EM Sein, Harmonic analysis: Real variable mehods, orhogonaliy and oscillaory inegrals, Princeon Univ Press, Princeon, NJ, X Tolsa, BMO, H, and Calderón-Zygmund operaors for non doubling measures, Mah Ann , X Tolsa, A proof of he weak, inequaliy for singular inegrals wih non doubling measures based on a Calderón-Zygmund decomposiion, Publ Ma , Xuan Thinh Duong, Deparmen of Mahemaics, Macquarie Universiy, NSW 209 Ausralia address: xuanduong@mqeduau Ji Li, Deparmen of Mahemaics, Sun Ya-sen Universiy, Guangzhou, 50275, China address: liji6@mailsysueducn Adam Sikora, Deparmen of Mahemaics, Macquarie Universiy, NSW 209 Ausralia address: adamsikora@mqeduau
Convergence of the Neumann series in higher norms
Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann
More informationCHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR
Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 31, 2006, 39 46 CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR Joaquim Marín and Javier
More informationTriebel Lizorkin space estimates for multilinear operators of sublinear operators
Proc. Indian Acad. Sci. Mah. Sci. Vol. 3, No. 4, November 2003, pp. 379 393. Prined in India Triebel Lizorkin space esimaes for mulilinear operaors of sublinear operaors LIU LANZHE Deparmen of Applied
More informationLecture 10: The Poincaré Inequality in Euclidean space
Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?
More informationThe Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions
More informationHeat kernel and Harnack inequality on Riemannian manifolds
Hea kernel and Harnack inequaliy on Riemannian manifolds Alexander Grigor yan UHK 11/02/2014 onens 1 Laplace operaor and hea kernel 1 2 Uniform Faber-Krahn inequaliy 3 3 Gaussian upper bounds 4 4 ean-value
More informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More informationOscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson
PROCEEDINGS OF THE FOURTH INTERNATIONAL CONFERENCE ON DYNAMICAL SYSTEMS AND DIFFERENTIAL EQUATIONS May 4 7, 00, Wilmingon, NC, USA pp 0 Oscillaion of an Euler Cauchy Dynamic Equaion S Huff, G Olumolode,
More informationGRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256
Tile Auhor(s) GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION Zhao, Liang Ciaion Osaka Journal of Mahemaics. 51(1) P.45-P.56 Issue Dae 014-01 Tex Version publisher URL hps://doi.org/10.18910/9195
More informationAverage Number of Lattice Points in a Disk
Average Number of Laice Poins in a Disk Sujay Jayakar Rober S. Sricharz Absrac The difference beween he number of laice poins in a disk of radius /π and he area of he disk /4π is equal o he error in he
More informationDifferential Harnack Estimates for Parabolic Equations
Differenial Harnack Esimaes for Parabolic Equaions Xiaodong Cao and Zhou Zhang Absrac Le M,g be a soluion o he Ricci flow on a closed Riemannian manifold In his paper, we prove differenial Harnack inequaliies
More informationExistence of positive solution for a third-order three-point BVP with sign-changing Green s function
Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion
More informationREMARK ON THE PAPER ON PRODUCTS OF FOURIER COEFFICIENTS OF CUSP FORMS 1. INTRODUCTION
REMARK ON THE PAPER ON PRODUCTS OF FOURIER COEFFICIENTS OF CUSP FORMS YUK-KAM LAU, YINGNAN WANG, DEYU ZHANG ABSTRACT. Le a(n) be he Fourier coefficien of a holomorphic cusp form on some discree subgroup
More informationarxiv: v1 [math.pr] 19 Feb 2011
A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of
More informationAnn. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:
Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS
More informationarxiv:math/ v1 [math.nt] 3 Nov 2005
arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming
More informationMonotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type
In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria
More informationPOSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION
Novi Sad J. Mah. Vol. 32, No. 2, 2002, 95-108 95 POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION Hajnalka Péics 1, János Karsai 2 Absrac. We consider he scalar nonauonomous neural delay differenial
More informationL p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity
ANNALES POLONICI MATHEMATICI LIV.2 99) L p -L q -Time decay esimae for soluion of he Cauchy problem for hyperbolic parial differenial equaions of linear hermoelasiciy by Jerzy Gawinecki Warszawa) Absrac.
More informationA remark on the H -calculus
A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has
More informationMapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)
Applied Mahemaics E-Noes, 15(215), 14-21 c ISSN 167-251 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Mapping Properies Of The General Inegral Operaor On The Classes R k (ρ, b) And V k
More informationarxiv: v1 [math.ca] 15 Nov 2016
arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy
More informationMatrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality
Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]
More informationSection 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients
Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous
More informationA NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION
Bull. London Mah. Soc. 39 2007 482 486 C 2007 London Mahemaical Sociey doi:10.1112/blms/bdm032 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON and S. M. GONEK Absrac Le πs denoe he
More informationGeneralized Chebyshev polynomials
Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT
More informationarxiv: v1 [math.fa] 9 Dec 2018
AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse
More informationExample on p. 157
Example 2.5.3. Le where BV [, 1] = Example 2.5.3. on p. 157 { g : [, 1] C g() =, g() = g( + ) [, 1), var (g) = sup g( j+1 ) g( j ) he supremum is aken over all he pariions of [, 1] (1) : = < 1 < < n =
More informationarxiv: v1 [math.pr] 4 Aug 2016
Hea kernel esimaes on conneced sums of parabolic manifolds arxiv:68.596v [mah.pr] 4 Aug 26 Alexander Grigor yan Deparmen of Mahemaics Universiy of Bielefeld 335 Bielefeld, Germany grigor@mah.uni-bielefeld.de
More information4 Sequences of measurable functions
4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences
More informationRiesz transform characterization of Hardy spaces associated with Schrödinger operators with compactly supported potentials
Ark. Ma., 48 (21), 31 31 DOI: 1.17/s11512-1-121-5 c 21 by Insiu Miag-Leffler. All righs reserved Riesz ransform characerizaion of Hardy spaces associaed wih Schrödinger operaors wih compacly suppored poenials
More informationSobolev-type Inequality for Spaces L p(x) (R N )
In. J. Conemp. Mah. Sciences, Vol. 2, 27, no. 9, 423-429 Sobolev-ype Inequaliy for Spaces L p(x ( R. Mashiyev and B. Çekiç Universiy of Dicle, Faculy of Sciences and Ars Deparmen of Mahemaics, 228-Diyarbakir,
More informationWe just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n
Lecure 3 - Kövari-Sós-Turán Theorem Jacques Versraëe jacques@ucsd.edu We jus finished he Erdős-Sone Theorem, and ex(n, F ) ( /(χ(f ) )) ( n 2). So we have asympoics when χ(f ) 3 bu no when χ(f ) = 2 i.e.
More informationHamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:
M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno
More informationEndpoint Strichartz estimates
Endpoin Sricharz esimaes Markus Keel and Terence Tao (Amer. J. Mah. 10 (1998) 955 980) Presener : Nobu Kishimoo (Kyoo Universiy) 013 Paricipaing School in Analysis of PDE 013/8/6 30, Jeju 1 Absrac of he
More informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationEssential Maps and Coincidence Principles for General Classes of Maps
Filoma 31:11 (2017), 3553 3558 hps://doi.org/10.2298/fil1711553o Published by Faculy of Sciences Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Essenial Maps Coincidence
More informationLIPSCHITZ ESTIMATES FOR MULTILINEAR COMMUTATOR OF LITLLEWOOD-PALEY OPERATOR. Zhang Mingjun and Liu Lanzhe
3 Kragujevac J. Mah. 27 (2005) 3 46. LIPSCHITZ ESTIMATES FOR MULTILINEAR COMMUTATOR OF LITLLEWOOD-PALEY OPERATOR Zhang Mingjun and Liu Lanzhe Deparen of Maheaics Hunan Universiy Changsha, 40082, P.R.of
More informationCONTRIBUTION TO IMPULSIVE EQUATIONS
European Scienific Journal Sepember 214 /SPECIAL/ ediion Vol.3 ISSN: 1857 7881 (Prin) e - ISSN 1857-7431 CONTRIBUTION TO IMPULSIVE EQUATIONS Berrabah Faima Zohra, MA Universiy of sidi bel abbes/ Algeria
More information23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes
Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals
More information2. Nonlinear Conservation Law Equations
. Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear
More informationSTABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES
Novi Sad J. Mah. Vol. 46, No. 1, 2016, 15-25 STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES N. Eghbali 1 Absrac. We deermine some sabiliy resuls concerning
More informationLINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS
LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS MICHAEL DORFF AND J. SZYNAL Absrac. Differen mehods have been used in sudying he univalence of he inegral ) α ) f) ) J α, f)z) = f ) d, α,
More informationA Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero
JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar
More informationProperties Of Solutions To A Generalized Liénard Equation With Forcing Term
Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick
More informationOn a Fractional Stochastic Landau-Ginzburg Equation
Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn
More informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationMODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE
Topics MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES 2-6 3. FUNCTION OF A RANDOM VARIABLE 3.2 PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE 3.3 EXPECTATION AND MOMENTS
More informationHarnack inequalities and Gaussian estimates for a class of hypoelliptic operators
Harnack inequaliies and Gaussian esimaes for a class of hypoellipic operaors Sergio Polidoro Diparimeno di Maemaica, Universià di Bologna Absrac We announce some resuls obained in a recen sudy [14], concerning
More informationTO our knowledge, most exciting results on the existence
IAENG Inernaional Journal of Applied Mahemaics, 42:, IJAM_42 2 Exisence and Uniqueness of a Periodic Soluion for hird-order Delay Differenial Equaion wih wo Deviaing Argumens A. M. A. Abou-El-Ela, A. I.
More informationdi Bernardo, M. (1995). A purely adaptive controller to synchronize and control chaotic systems.
di ernardo, M. (995). A purely adapive conroller o synchronize and conrol chaoic sysems. hps://doi.org/.6/375-96(96)8-x Early version, also known as pre-prin Link o published version (if available):.6/375-96(96)8-x
More informationMath 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:
Mah 4 Eam Review Problems Problem. Calculae he 3rd Taylor polynomial for arcsin a =. Soluion. Le f() = arcsin. For his problem, we use he formula f() + f () + f ()! + f () 3! for he 3rd Taylor polynomial
More informationOperators related to the Jacobi setting, for all admissible parameter values
Operaors relaed o he Jacobi seing, for all admissible parameer values Peer Sjögren Universiy of Gohenburg Join work wih A. Nowak and T. Szarek Alba, June 2013 () 1 / 18 Le Pn α,β be he classical Jacobi
More informationOn the probabilistic stability of the monomial functional equation
Available online a www.jnsa.com J. Nonlinear Sci. Appl. 6 (013), 51 59 Research Aricle On he probabilisic sabiliy of he monomial funcional equaion Claudia Zaharia Wes Universiy of Timişoara, Deparmen of
More informationA Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball
A Noe on Superlinear Ambrosei-Prodi Type Problem in a Ball by P. N. Srikanh 1, Sanjiban Sanra 2 Absrac Using a careful analysis of he Morse Indices of he soluions obained by using he Mounain Pass Theorem
More informationOn Oscillation of a Generalized Logistic Equation with Several Delays
Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid
More informationMEASURE DENSITY AND EXTENSION OF BESOV AND TRIEBEL LIZORKIN FUNCTIONS
MEASURE DENSITY AND EXTENSION OF BESOV AND TRIEBEL LIZORKIN FUNCTIONS TONI HEIKKINEN, LIZAVETA IHNATSYEVA, AND HELI TUOMINEN* Absrac. We show ha a domain is an exension domain for a Haj lasz Besov or for
More informationarxiv: v1 [math.fa] 27 Aug 2013
HARDY SPACES AND HEAT KERNEL REGULARITY arxiv:38.587v [mah.fa] 27 Aug 23 APTISTE DEVYVER Absrac. In his paper, we show he equivalence beween he boundedness of he Riesz ransform d /2 on L p, p 2,p ), andhe
More informationCash Flow Valuation Mode Lin Discrete Time
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics
More informationProduct of Fuzzy Metric Spaces and Fixed Point Theorems
In. J. Conemp. Mah. Sciences, Vol. 3, 2008, no. 15, 703-712 Produc of Fuzzy Meric Spaces and Fixed Poin Theorems Mohd. Rafi Segi Rahma School of Applied Mahemaics The Universiy of Noingham Malaysia Campus
More informationOPTIMAL FUNCTION SPACES FOR THE LAPLACE TRANSFORM. f(s)e ts ds,
OPTIMAL FUNCTION SPACES FOR THE LAPLACE TRANSFORM EVA BURIÁNKOVÁ, DAVID E. EDMUNDS AND LUBOŠ PICK Absrac. We sudy he acion of he Laplace ransform L on rearrangemen-invarian funcion spaces. We focus on
More informationOn Ternary Quadratic Forms
On Ternary Quadraic Forms W. Duke Deparmen of Mahemaics, Universiy of California, Los Angeles, CA 98888. Inroducion. Dedicaed o he memory of Arnold E. Ross Le q(x) = q(x, x, x ) be a posiive definie ernary
More informationSupplement for Stochastic Convex Optimization: Faster Local Growth Implies Faster Global Convergence
Supplemen for Sochasic Convex Opimizaion: Faser Local Growh Implies Faser Global Convergence Yi Xu Qihang Lin ianbao Yang Proof of heorem heorem Suppose Assumpion holds and F (w) obeys he LGC (6) Given
More informationSome Ramsey results for the n-cube
Some Ramsey resuls for he n-cube Ron Graham Universiy of California, San Diego Jozsef Solymosi Universiy of Briish Columbia, Vancouver, Canada Absrac In his noe we esablish a Ramsey-ype resul for cerain
More informationOn Two Integrability Methods of Improper Integrals
Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169
More informationThe L p -Version of the Generalized Bohl Perron Principle for Vector Equations with Infinite Delay
Advances in Dynamical Sysems and Applicaions ISSN 973-5321, Volume 6, Number 2, pp. 177 184 (211) hp://campus.ms.edu/adsa The L p -Version of he Generalized Bohl Perron Principle for Vecor Equaions wih
More informationAn Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.
1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard
More information11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu
ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning
More informationOn some Properties of Conjugate Fourier-Stieltjes Series
Bullein of TICMI ol. 8, No., 24, 22 29 On some Properies of Conjugae Fourier-Sieljes Series Shalva Zviadadze I. Javakhishvili Tbilisi Sae Universiy, 3 Universiy S., 86, Tbilisi, Georgia (Received January
More informationt j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i)
A NOTE ON WRONSKIANS AND THE ABC THEOREM IN FUNCTION FIELDS OF RIME CHARACTERISTIC Julie Tzu-Yueh Wang Insiue of Mahemaics Academia Sinica Nankang, Taipei 11529 Taiwan, R.O.C. May 14, 1998 Absrac. We provide
More informationBoundedness and Exponential Asymptotic Stability in Dynamical Systems with Applications to Nonlinear Differential Equations with Unbounded Terms
Advances in Dynamical Sysems and Applicaions. ISSN 0973-531 Volume Number 1 007, pp. 107 11 Research India Publicaions hp://www.ripublicaion.com/adsa.hm Boundedness and Exponenial Asympoic Sabiliy in Dynamical
More informationMulti-component Levi Hierarchy and Its Multi-component Integrable Coupling System
Commun. Theor. Phys. (Beijing, China) 44 (2005) pp. 990 996 c Inernaional Academic Publishers Vol. 44, No. 6, December 5, 2005 uli-componen Levi Hierarchy and Is uli-componen Inegrable Coupling Sysem XIA
More informationEXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 206 (206, No. 39, pp.. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO
More informationExistence Theory of Second Order Random Differential Equations
Global Journal of Mahemaical Sciences: Theory and Pracical. ISSN 974-32 Volume 4, Number 3 (22), pp. 33-3 Inernaional Research Publicaion House hp://www.irphouse.com Exisence Theory of Second Order Random
More informationSOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM
SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM FRANCISCO JAVIER GARCÍA-PACHECO, DANIELE PUGLISI, AND GUSTI VAN ZYL Absrac We give a new proof of he fac ha equivalen norms on subspaces can be exended
More informationNEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS
QUANTUM PROBABILITY BANACH CENTER PUBLICATIONS, VOLUME 43 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 998 NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS MAREK
More informationQUANTITATIVE DECAY FOR NONLINEAR WAVE EQUATIONS
QUANTITATIVE DECAY FOR NONLINEAR WAVE EQUATIONS SPUR FINAL PAPER, SUMMER 08 CALVIN HSU MENTOR: RUOXUAN YANG PROJECT SUGGESTED BY: ANDREW LAWRIE Augus, 08 Absrac. In his paper, we discuss he decay rae for
More informationASYMPTOTIC FORMS OF WEAKLY INCREASING POSITIVE SOLUTIONS FOR QUASILINEAR ORDINARY DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 2007(2007), No. 126, pp. 1 12. ISSN: 1072-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu (login: fp) ASYMPTOTIC FORMS OF
More informationOrthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind
Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence
More informationExistence of positive solutions for second order m-point boundary value problems
ANNALES POLONICI MATHEMATICI LXXIX.3 (22 Exisence of posiive soluions for second order m-poin boundary value problems by Ruyun Ma (Lanzhou Absrac. Le α, β, γ, δ and ϱ := γβ + αγ + αδ >. Le ψ( = β + α,
More informationMATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence
MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,
More informationMOLECULAR CHARACTERIZATIONS AND DUALITIES OF VARIABLE EXPONENT HARDY SPACES ASSOCIATED WITH OPERATORS
Annales Academiæ Scieniarum Fennicæ Mahemaica Volumen 41, 2016, 357 398 MOLECULAR CHARACTERIZATIONS AND DUALITIES OF VARIABLE EXPONENT HARDY SPACES ASSOCIATED WITH OPERATORS Dachun Yang and Ciqiang Zhuo
More informationMEASURE DENSITY AND EXTENSION OF BESOV AND TRIEBEL LIZORKIN FUNCTIONS
MEASURE DENSITY AND EXTENSION OF BESOV AND TRIEBEL LIZORKIN FUNCTIONS TONI HEIKKINEN, LIZAVETA IHNATSYEVA, AND HELI TUOMINEN* Absrac. We show ha a domain is an exension domain for a Haj lasz Besov or for
More information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationConvergence of Laplacian Eigenmaps
Convergence of Laplacian Eigenmaps ikhail Belkin Deparmen of Compuer Science Ohio Sae Universiy Columbus, OH 4320 mbelkin@cse.ohio-sae.edu Parha Niyogi Deparmen of Compuer Science The Universiy of Chicago
More informationEXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN DIFFERENCE-DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 29(29), No. 49, pp. 2. ISSN: 72-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN
More informationMonochromatic Infinite Sumsets
Monochromaic Infinie Sumses Imre Leader Paul A. Russell July 25, 2017 Absrac WeshowhahereisaraionalvecorspaceV suchha,whenever V is finiely coloured, here is an infinie se X whose sumse X+X is monochromaic.
More informationA Primal-Dual Type Algorithm with the O(1/t) Convergence Rate for Large Scale Constrained Convex Programs
PROC. IEEE CONFERENCE ON DECISION AND CONTROL, 06 A Primal-Dual Type Algorihm wih he O(/) Convergence Rae for Large Scale Consrained Convex Programs Hao Yu and Michael J. Neely Absrac This paper considers
More informationPositive continuous solution of a quadratic integral equation of fractional orders
Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.
More informationWeighted norm inequalities, off-diagonal estimates and elliptic operators. Part III: Harmonic analysis of elliptic operators
Weighed norm inequaliies, off-diagonal esimaes and ellipic operaors. Par III: Harmonic analysis of ellipic operaors Pascal Auscher, José Maria Marell To cie his version: Pascal Auscher, José Maria Marell.
More informationarxiv: v1 [math.pr] 23 Jan 2019
Consrucion of Liouville Brownian moion via Dirichle form heory Jiyong Shin arxiv:90.07753v [mah.pr] 23 Jan 209 Absrac. The Liouville Brownian moion which was inroduced in [3] is a naural diffusion process
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationOn the cohomology groups of certain quotients of products of upper half planes and upper half spaces
On he cohomolog groups of cerain quoiens of producs of upper half planes and upper half spaces Amod Agashe and Ldia Eldredge Absrac A heorem of Masushima-Shimura shows ha he he space of harmonic differenial
More informationBOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS
Elecronic Journal of Differenial Equaions, Vol. 18 (18, No. 8, pp. 1 13. ISSN: 17-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS JACEK
More informationCERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS
SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien
More informationNonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique
Filoma 29:5 (2015), 1067 1080 DOI 10.2298/FI1505067W Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Nonlinear Fuzzy Sabiliy of a Funcional
More informationVariational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial
More informationInternational Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN
Inernaional Journal of Scienific & Engineering Research, Volume 4, Issue 10, Ocober-2013 900 FUZZY MEAN RESIDUAL LIFE ORDERING OF FUZZY RANDOM VARIABLES J. EARNEST LAZARUS PIRIYAKUMAR 1, A. YAMUNA 2 1.
More informationOn Gronwall s Type Integral Inequalities with Singular Kernels
Filoma 31:4 (217), 141 149 DOI 1.2298/FIL17441A Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Gronwall s Type Inegral Inequaliies
More informationHamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t
M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n
More information