Hardy spaces for semigroups with Gaussian bounds

Size: px
Start display at page:

Download "Hardy spaces for semigroups with Gaussian bounds"

Transcription

1 Annali di Maemaica : hps://doi.og/1.17/s y Hady spaces fo semigoups wih Gaussian bounds Jacek Dziubański 1 Macin Peisne 1 Received: 3 July 217 / Acceped: 16 Ocobe 217 / Published online: 5 Novembe 217 The Auhos 217. This aicle is an open access publicaion Absac Le T = e L be a semigoup of self-adjoin linea opeaos acing on L 2,μ, whee, d,μis a space of homogeneous ype. We assume ha T has an inegal kenel T x, y which saisfies he uppe and lowe Gaussian bounds: C 1 μbx, exp c 1 dx, y 2 / C 2 T x, y μbx, exp c 2 dx, y 2 /. By definiion, f belongs o H 1 L if f H 1 L = sup > T f x L 1,μ <. We pove ha hee is a funcion ωx, < c ωx C, such ha H 1 L admis an aomic decomposiion wih aoms saisfying: supp a B, a L μb 1, and he weighed cancelaion condiion axωxdμx =. Keywods Hady space Maximal funcion Aomic decomposiion Gaussian bounds Hölde esimaes Mahemaics Subjec Classificaion Pimay 42B3; Seconday 42B25 42B35 35J1 1 Inoducion Le, d be a meic space equipped wih a nonnegaive Boel measue μ. We shall assume ha μ = and <μbx, <, >, whee Bx, = {y dx, y } denoes he closed ball ceneed a x and adius. Suppose, d,μis a space of homoge- The eseach was suppoed by he Polish Naional Science Cene Naodowe Cenum Nauki Gan No. DEC 212/5/B/ST1/672. B Macin Peisne macin.peisne@uw.edu.pl Jacek Dziubański jacek.dziubanski@mah.uni.woc.pl 1 Insyu Maemayczny, Uniwesye Wocławski, pl. Gunwaldzki 2/4, Wocław, Poland

2 966 J. Dziubański, M. Peisne neous ype in he sense of Coifman and Weiss [8], which means ha he doubling condiion holds, namely: Thee is C > such ha μbx, 2 CμBx, fo > andx. I is well known ha he doubling condiion implies ha hee ae q > andc d > such ha μbx, s C d s q μbx, fo x, >, and s Suppose ha L is a nonnegaive densely defined self-adjoin linea opeao on L 2,μ. Le T = e L, >, denoe he semigoup of linea opeaos geneaed by L.Weimpose ha hee exiss T x, y, such ha T f x = T x, y f y dμy. 1.2 Clealy, T x, y = T y, x fo > and a.e. x, y. Moeove, we assume he following lowe and uppe Gaussian bounds, ha is, hee ae consans c 1 c 2 > andc > such ha C 1 μbx, exp c 1dx, y 2 C T x, y μbx, exp c 2dx, y fo > and a.e. x, y. I is well known ha 1.3 implies ha fo evey n N we have n n T x, y C n n μbx, exp c ndx, y2, 1.4 fo > and a.e. x, y wih some C n, c n >. Fo his fac see, e.g., [2, 7.1], [1,27]. The Hady space H 1 L elaed o L is defined by means of he maximal funcion of he semigoup T, namely { } H 1 L := f L 1,μ f H 1 L := sup T f <. > L 1,μ On he ohe hand, we define aomic Hady spaces as follows. Suppose we have a space wih a doubling measue σ and a quasi-meic ρ. We call a funcion a an ρ, σ -aom if hee exiss a ball B = B ρ x, := {x ρx, x } such ha: supp a B, a σb 1,and ax dσx =. B By definiion, a funcion f L 1,σbelongs o Ha 1ρ, σ, ifheeexisρ, σ -aoms a k and complex numbes λ k, such ha f = λ k a k k=1 and λ k <. If such sequences exis, we define he nom f H 1 a ρ,σ o be he infimum of k=1 λ k in he above pesenaions of f. Noice ha in his paagaph we have changed he noaion. This is because in he aicle we will use diffeen meics and measues. Fo x le Φ x :,, be he nondeceasing funcion defined by The fis main esul of his pape is he following. k=1 Φ x = μbx,. 1.5

3 Hady spaces fo semigoups wih Gaussian bounds 967 Theoem 1 Suppose ha, d,μ is a space of homogeneous ype and assume ha fo each x he funcion Φ x is a bijecion on,. Le a nonnegaive self-adjoin linea opeao L on L 2,μ be given such ha he semigoup T = e L saisfies 1.3. Then hee exis a consan C > and a funcion ω on, < C 1 ωx C, such ha he spaces H 1 L and Ha 1 d,ωμcoincide and he coesponding noms ae equivalen, C 1 f H 1 a d,ωμ f H 1 L C f H 1 a d,ωμ. Moeove, ω is L-hamonic, ha is T ω = ω fo >. Le us noice ha he assumpion on Φ x implies ha μ = and μ is nonaomic. This will be used lae on. By definiion, we call a semigoup consevaive if T x, y dμy = fo > andx. Theoem 2 Suppose ha, d,μis a space of homogeneous ype and assume ha fo each x he funcion Φ x is a bijecion on,. Le a nonnegaive self-adjoin linea opeao LonL 2,μbe given such ha he semigoup T = e L saisfies 1.3 and 1.6. Then, he spaces H 1 L and Ha 1 d,μcoincide and he coesponding noms ae equivalen, i.e., hee exiss C > such ha C 1 f H 1 a d,μ f H 1 L C f H 1 a d,μ, I appeas ha Theoem 2 is equivalen o Theoem 1, see Sec. 3. Le us also emphasize ha we do no equie any egulaiy condiions on he kenels T x, y. Howeve,iuns ou ha 1.3 implies Hölde-ype esimaes on T x, y, which ae cucial fo his pape. This will be discussed in Sec. 4 see Theoem 5 and Coollay 14. In fac, Sec. 4 gives a sho, independen, and self-conained poof of Hölde-ype esimaes of he hea kenel ha saisfies 1.3, which can be ineesing in is own igh. Fuhemoe, alhough Theoems 1 and 2 ae saed fo he hea semigoup, we would like o emphasize ha he same heoems can be poved fo he Hady space H 1 L associaed wih he Poisson semigoup e L as well, see Theoem 4 and Remak 21. The heoy of he classical Hady spaces on he Euclidean spaces R n has is oigin in sudying holomophic funcions of one vaiable in he uppe half-plane. The eade is efeed o he oiginal woks of Sein and Weiss [32], Bukholde e al. [6], Feffeman and Sein [15]. Vey impoan conibuion o he heoy is he aomic decomposiion of he elemens of he H p spaces poved by Coifman [7] in he one-dimensional case and hen by Lae [23] fo H p R n. The heoy was hen exended o he space of homogeneous ype see, e.g., [8,24, 33]. Fo moe infomaion concening he classical Hady spaces, hei chaaceizaions and hisoical commens we efe he eade o Sein [31]. A vey geneal appoach o he heoy of Hady spaces associaed wih semigoups of linea opeaos saisfying he Davies Gaffney esimaes was inoduced by Hofmann e al. [2] see also[1,3]. Le us poin ou ha he classical Hady spaces can be hough as hose associaed wih he classical hea semigoup e. Finally we wan o emak ha he pesen pape akes moivaion fom [13,14], whee he auhos sudied H 1 spaces associaed wih Schödinge opeaos + V on R n, n 3, wih Geen bounded poenials V. In wha follows C and c denoe diffeen consans ha may depend on C d, q, C, c 1, c 2. By U V we undesand U CV and U V means C 1 V U CV.

4 968 J. Dziubański, M. Peisne The pape is oganized as follows. In Sec. 2 we pove ha esimae 1.3 implies he exisence of an L-hamonic funcion ω such ha < C 1 ωx C. The equivalence of Theoems 1 and 2 is a consequence of he Doob ansfom, see Sec. 3. Then a poof of Theoem 2 is given in a few seps. Fis, in Sec. 4 we pove Hölde-ype esimaes fo a consevaive semigoup. Then, in Sec. 5 we inoduce a new quasi-meic d and sudy is popeies. In Sec. 6 we apply a heoem of Uchiyama on he space, d,μo complee he poof of Theoem 2. Finally, in Sec. 7 we povide some examples of semigoups ha saisfy assumpions of Theoem 1. 2 Gaussian esimaes and bounded hamonic funcions In his secion we assume ha he semigoup T saisfies 1.3. Clealy, C 1 T x, ydμy C fo all > and a.e. x. Fo a posiive inege n define ω n x = 1 n T s x, ydμy ds. n Then, C 1 ω n x C. Recall ha a meic space wih he doubling condiion is sepaable, hen so is L 1,μ. Using he Banach Alaoglu heoem fo L,μ hee exiss a subsequence n k and ω L,μ, such ha ω nk ω in -weak opology. Obviously, C 1 ωy C. Ou goal is o pove ha T ωx = ωx fo >. To his end, we wie T x, yωy dμy = lim T x, yω nk y dμy k 1 nk = lim T +s x, z dμz ds k n k = lim ω 1 nk + n k x + lim T s x, z dμz ds k k n k n k 1 lim T s x, z dμz ds. k n k Since he las wo limis end o zeo, as k, we obain T x, yωy dμy = lim ω n k x. 2.1 k Fom 2.1 we ge ha lim k ω nk x exiss fo a.e. x and he limi has o be ωx. Moeove, T ωx = ωx. Thus we have poved he following poposiion. Poposiion 3 Assume ha a semigoup T saisfies 1.3. Then hee exiss a funcion ω and C > such ha < C 1 ωx C and T ωx = ωx fo evey >.

5 Hady spaces fo semigoups wih Gaussian bounds Doob ansfom In his secion we wok in a slighly moe geneal scheme. Le,μbe a σ -finie measue space and L be a self-adjoin opeao on L 2,μ. We assume ha he songly coninuous semigoup T = exp L admis a nonnegaive inegal kenel T x, y, soha T f x = T x, y f y dμy. Moeove, assume ha hee exiss ω saisfying < C 1 ωx C, haisl-hamonic. Namely, fo evey > one has T x, yωy dμy = ωx fo a.e. x. Obviously, his implies ha sup x,> T x, y dμy C. Define a new measue dνx = ω 2 x dμx and a new kenel K x, y = T x, y ωxωy. 3.1 The semigoup K given by K f x = K x, y f y dνy is a songly coninuous semigoup of self-adjoin inegal opeaos on L 2,ν. The mapping L 2,μ f ω 1 f L 2,ν is an isomeic isomophism wih he invese L 2,ν g ωg L 2,μ. Clealy, K gx = ωx 1 T ωgx. Moeove, he posiive inegal kenel K x, y is consevaive, ha is, K x, y dνy = ωx 1 T ωx = 1. Thus he above change of measue and opeaos, which is called Doob s ansfom see, e.g., [16], conjugaes he semigoup T wih he consevaive semigoup K. I is clea ha he opeaos K ae conacions on L 1,ν. Consequenly, K is a songly coninuous semigoup of linea opeaos on L 1,ν. To see his, i suffices o show ha lim K χ A χ A L 1,ν = fo any measuable se A of finie measue. We have ha lim K χ A χ A dν lim K χ A χ A L 2 A,ννA 1/2 =. On he ohe hand K χ A x dνx = νa = χ A L 1,ν. Hence, K χ A x dνx = K χ A xdνx = K χ A xdνx K χ A x dνx A c A c A = χ A xdνx K χ A x dνx as, A A which complees he poof of he song coninuiy of K on L 1,ν.

6 97 J. Dziubański, M. Peisne Fuhe, we easily see ha he semigoup T is songly coninuous on L 1,μ. Indeed, if f L 1,μhen g = ω 1 f L 1,νand T f f L 1,μ = K gx gx ωx 1 dνx K gx gx dνx as. Now we discuss he equivalence of Theoems 1 and 2. LeT and K be he semigoups elaed by 3.1 wih geneaos L and R, especively. I easily follows fom he Doob ansfom ha f H 1 L if and only if ω 1 f H 1 R and f H 1 L ω 1 f H 1 R.In ohe wods H 1 L f ω 1 f H 1 R is an isomophism of he spaces. Assume ha he space H 1 R admis an aomic decomposiion wih aoms ha saisfy he cancelaion condiion wih espec o he measue ν,haiseveyg H 1 R can be wien as g = λ j a j wih j λ j g H 1 R and a j ae aoms wih he popey a j dν =. Then evey f H 1 L admis aomic decomposiion f = λ j b j wih aoms b j ha saisfy cancelaion condiion b j ω dμ =. 4 Hölde-ype esimaes on he semigoups In his secion we conside a consevaive semigoup T having an inegal kenel T x, y ha saisfies uppe and lowe Gaussian bounds 1.3. Le P x, y = π 1/2 e u T 2 /4ux, y du 4.1 u be he kenels of he subodinae semigoup P = e L. Theoem 4 Le L be a nonnegaive self-adjoin linea opeao on L 2,μsuch ha he semigoup T = e L saisfies 1.3 and 1.6. Then hee is a consan α>such ha dy, z α P x, y P x, z P x, y 4.2 wheneve dy, z. Theoem 5 Unde he assumpions of Theoem 4 hee ae consans α, c > such ha T x, y T x, z μbx, dy, z α 1 cdx, y2 exp 4.3 wheneve dy, z. Hölde egulaiy of semigoups saisfying Gaussian bounds was consideed in vaious seings by many auhos. We efe he eade o Gigo yan [16], Hebisch and Saloff-Cose [19], Saloff-Cose [28], Gyya and Saloff-Cose [17], Benico, Coulhon, and Fey [2], and efeences heein. Hee we pesen a sho alenaive poof of 4.3. To his end we shall fis pove some auxiliay poposiions and hen Theoem 4. Finally, a he end of his secion, we shall make use of funcional calculi deducing Theoem 5 fom Theoem 4.

7 Hady spaces fo semigoups wih Gaussian bounds 971 Poposiion 6 Fo x, y and > we have P x, y 1 μ B x, + dx, y + dx, y. 4.4 Poof Conside fis he case dx, y. Thendx, y +. The uppe bound follows by 1.3and1.1. Indeed, P x, y 1/4 1 du μ B x, 2 + μbx, 1 u u 1/4 1/4 μbx, 1 du + μbx, 1 u μbx, 1. Also, 1.3 implies lowe bounds, since P x, y 1 1/4 1/4 e u μbx, du μ B x, u e u 2 u q du u e u exp 4c 1 u du μbx, 1. μ B x, u 2 u 2 u Le us now un o he case dx, y.thendx, y + dx, y.using1.3, we have P x, y Moeove, by 1.1, e u exp 4c 2 udx, y 2 /2 du = μ B x, u 2 u 2 /dx,y 2 + = J 1 + J 2. 2 /dx,y J 1 2 /dx,y 2 2 /dx,y 2 μ B μ B 1 x, 1 du 2 u u x, dx,y 2 du u 1 μ Bx, dx, y dx, y 4.6 and J 2 1 exp 4c 2 udx, y 2 / 2 2dx, y μ Bx, dx, y 2 /dx,y 2 1 μ Bx, dx, y u q du u dx, y. 4.7 Esimaes give uppe esimae. Fo he lowe esimae, ecall ha dx, y and obseve ha

8 972 J. Dziubański, M. Peisne P x, y 2 2 /dx,y 2 2 /dx,y 2 e u exp 4c1 udx, y 2 / 2 μ B x, 2 u /dx,y 2 du μbx, dx, y/2 2 /dx,y 2 u 1 μbx, dx, y dx, y. du u Coollay 7 Thee is a consan C > such ha if dy, z, hen C 1 P x, y C. 4.8 P x, z Poof The coollay is a simple consequence of 4.4. Fo he poof one may conside wo cases: dx, y 2 hen dx, z 3anddx, y >2 hen dx, y dx, z. Poposiion 8 Thee exiss a consan γ, 1 such ha he following saemen holds: If hee ae y, z,, a 1, b 1 > given such ha dy, z < and fo all x we have a 1 P x, y P x, z b 1, 4.9 hen hee is a subineval [a 2, b 2 ] [a 1, b 1 ] such ha b 2 a 2 = γb 1 a 1 and fo all 2 and all x one has a 2 P x, y P x, z b 2. Poof The poof, which akes some ideas fom [21], is an adaped vesion of he poof of [13, Pop. 3.1]. Fo he eade convenience we pesen he deails. Le m = a 1 + b 1 /2and θ = b 1 a 1 /a 1 + b 1, 1, sohaa 1 = 1 θm and b 1 = 1 + θm. Define { Ω + = x m P } x, y P x, z b 1, Ω = \Ω +. Obviously, eihe μω Bz, μbz, /2oμΩ + Bz, μbz, /2. Hee we shall assume ha he lae holds. The poof in he opposie case is simila. Denoe B = Bz,, s =.Fox,wehave P x, y m1 θ P s x,wp w, z dμw + m P s x,wp w, z dμw Ω Ω + = m1 θp x, z + mθ P s x,wp w, z dμw Ω + m1 θp x, z + mθ P s x,wp w, z dμw Ω + B m1 θp x, z + mθ μb 2 Noice ha dw, z s and, by Coollay 7, inf P sx,w inf P w, z = J. w B w B inf w B P sx,w P s x, z.

9 Hady spaces fo semigoups wih Gaussian bounds 973 Since s, Poposiion 6 implies and Theefoe P s x, z P x, z inf w B P w, z μb 1. J m 1 θ+ κθ P x, z = m 1 θ1 κ P x, z, 4.1 whee κ, 2. Moeove, fom 4.9 and he semigoup popey we easily ge P x, y b 1 P s x,wp w, z dμw b 1 P x, z Defining γ = 1 κ/2, 1, b 2 = b 1 and a 2 = m 1 θ+ κθ, wehave b 2 a 2 = 2mθ 1 κ/2 = b 1 a 1 1 κ/2 = γb 1 a 1. Now 4.1 ogehe wih 4.11gives a 2 P x, y P x, z b 2 fo x. Poof of Thoem 4 Having Coollay 7 and Poposiion 8 poved, we follow agumens of [13] o obain he heoem. By Coollay 7 hee ae b 1 > a 1 > such ha fo y, z and > saisfying dy, z < we have a 1 P x, y P x, z b 1 fo all x. Fom Poposiion 8 we deduce ha hee exiss ωy, z such ha P x, y lim = ωy, z unifomly in x P x, z I follows fom 4.1 ha P x, y dμy = 1. Recall ha P x, y = P y, x. Using 4.12, P y, x 1 = P y, x dμx = P z, x P z, x dμx ωy, z. Thus ωy, z = 1. Assume ha dy, z <. Len N be such ha dy, z 2 n < 2dy, z. Se = 2 n. Clealy, dy, z and a 1 P x, y P x, z b 1. Obseve ha n log/dy, z. Applying Poposiion 8 n-imes we aive a P x, y P x, z 1 dy, z α γ n γ c log/dy,z, wih α>and he poof of Theoem 4 is finished.

10 974 J. Dziubański, M. Peisne Finally, we devoe he emaining pa of his secion fo deducing Theoem 5 fom Theoem 4. This is done by using a funcional calculi. Fis, we need some pepaaoy facs. Recall ha q is a fixed consan saisfying 1.1. By W 2,σ R we denoe he Sobolev space wih he nom f W 2,σ R = 1 + ξ 2 σ f ξ 1/2 2 dξ. R Le ξde L ξ be he specal esoluion fo L. Fo a bounded funcion m on [, he fomula m L = mξ de L ξ defines a bounded linea opeao on L 2,μ. Fuhe we shall use he following lemma, whose poof based on finie speed popagaion ofhewaveequaionsee[9] can be found in [11]. Lemma 9 [11, Lemma 4.8] Le κ>1/2, β>. Then hee exiss a consan C > such ha fo evey even funcion m W 2,β/2+κ R and evey g L 2,μ, supp g By,, we have dx,y >2 fo j Z. m2 j Lgx 2 dx, y β dμx C2 j β m 2 W 2,β/2+κ R g 2 L 2,μ Poposiion 1 Le β>qand κ>1/2. Thee is a consan C > such ha fo evey F W 2,β/2+κ R wih supp F 1/2, 2 he inegal kenels F2 j Lx, y of he opeaos F2 j L saisfy F2 j Lx, y dμx C F W 2,β/2+κ R fo j Z. Poof Fo y and j Z se U = By, 2 j, U k = By, 2 k j \ By, 2 k j 1, k = 1, 2,...Defineg j,k,y x = T 2 2 j x, yχ Uk x, k =, 1, 2,... Then, using 1.1and 1.3, we have g j,y,k L 2,μ a k μu 1/2, 4.13 whee a k = C C q 2 kq exp c 2 2 2k 2 is a apidly deceasing sequence. Le mξ be he even exension of e ξ 2 Fξ. Obviously, m W 2,β/2+κ R F W 2,β/2+κ R. Then, F2 j L = m2 j LT 2 2 j, and, consequenly, F2 j Lx, y = m2 j Lg j,y,k x k= By he Cauchy Schwaz inequaliy, 1.1, and 4.13 wege m2 j Lg j,y,k L 1 By,2 k j+1,μ μby, 2k j+1 1/2 m2 j Lg j,y,k L 2,μ μby, 2 k j+1 1/2 μby, 2 j μby, 2 j 1/2 m L R g j,y,k L 2,μ 2 kq a k m W 2,β/2+κ R. 4.15

11 Hady spaces fo semigoups wih Gaussian bounds 975 We un o esimae m2 j Lg j,y,k L 1 By,2 k j+1 c,μ. Uilizing he Cauchy Schwaz inequaliy and Lemma 9, we obain, dx,y>2k j+1 [ [ m2 j Lg j,y,k x dμx dx,y>2k j+1 dx,y>2k j+1 m2 j Lg j,y,k x 2 dx, y β 1/2 dμx] dx, y β 1/2 dμx] 2 k j 2 k j dx, y ] β 1/2 dμx 2 k j. [ 2 kβ/2 m W 2,β/2+κ R g j,y,k L 2,μ dx,y>2k j Recall ha β>qand hence is no difficul o check ha 1.1 leads o dx, y β dμx 2 kq μu dx,y>2k j+1 2 k j Thus, by 4.13, 4.16, and 4.17, we ge m2 j Lg j,y,k x dμx 2 kβ/2 2 kq/2 m W 2,β/2+κ Ra k, dx,y>2k j+1 which, combined wih 4.15and4.14, complees he poof of he poposiion. Fo > se ψ ξ = exp ξ ξ 2. Lemma 11 The opeaos ψ L have inegal kenels Ψ x, y ha saisfy Ψ x, y dμy C. sup x, > Poof Denoing θ ξ = exp ξ 2 exp ξ 1, whee,ξ >, we have ψ L = T + θ L. Clealy, by 1.3, sup,x> T x, y dμy C. Thus we concenae ou aenion on θ L. Le η Cc 1/2, 2 be a paiion of uniy such ha θ ξ = θ ξη2 j ξ = θ, j ξ. j Z j Z Denoe θ, j ξ = θ, j 2 j ξ = ηξθ 1 2 j ξ. One can easily veify ha fo n N {} hee ae consans C n, c n > such ha dn dξ θ { L 2 j n, j C fo j log 2 n R exp c n 2 2 j. fo j log 2

12 976 J. Dziubański, M. Peisne In ohe wods, fo abiay N, θ, j W 2,N R CN. j Z Using Poposiion 1 wih a fixed N > q/2+1 we ge ha he inegal kenels Θ, j x, y of he opeaos θ, j L = θ, j 2 j L saisfy Θ, j x, y dμy θ, j W 2,N R. Theefoe, Θ x, y = j Z Θ, j x, y is he inegal kenel of θ L and i saisfies Θ x, y dμy C. sup,x> Poof of Theoem 5 By he specal heoem T = ψ LP and T x, y = Ψ x,wp w, y dμw. Using Theoem 4 ogehe wih Lemma 11 and Poposiion 6, fo dy, z, wehave T x, y T x, z = Ψ x,wp w, y P w, z dμw dy, z α Ψ x,w P w, y dμw 4.18 μby, dy, z α 1. We claim ha fo dy, z one has T x, y T x, z μby, 1 dy, z α/2 exp cdx, y To pove he claim we conside wo cases. Case 1: 2dy, z dx, y. Recall ha dy, z; hus, dx, y 2 and 4.19 follows diecly fom Case 2: 2dy, z dx, y. In his case dx, y dx, z, soby1.3 we obain exp c 2dx,y 2 exp c 2dx,z 2 T x, y T x, z μby, + μbz, μby, cdx, y2 exp, whee in he las inequaliy we have uilized ha μbz, μby,, since dy, z <. By aking he geomeic mean of 4.18 and4.2 we obain To finish he poof obseve ha 4.19 implies 4.3. Indeed, μbx, = μby, μbx, μby, μby, μby, + dx, y μby,

13 Hady spaces fo semigoups wih Gaussian bounds 977 μby, 1 + dx, y q and using he exponen faco we can eplace μby, by μbx,. Remak 12 Le us emak ha Lemma 11, which is cucial in ou poof of Theoem 5, can be poved by applying funcional calculus of Hebisch [18]. Thus, Theoem 5 can be also obained wihou using he finie popagaion speed of he soluion of he wave equaion 2 + Lu, x =, u, x = u x, u, x =. As a consequence of 1.4andTheoem5 we ge wha follows. Coollay 13 The funcion T x, y is coninuous on,. As a diec consequence of Theoem 5 and Doob ansfom see 3.1 we ge he following coollay. Noice ha in Coollay 14 we do no assume ha T x, y is consevaive. Coollay 14 Assume ha he semigoup T saisfies 1.3. Then hee ae consans α, c > such ha T x, y ωxωy T x, z μbx, dy, z 1 ωxωz wheneve dy, z. α exp cdx, y2 5 Measues and disances To pove Theoem 2 we inoduce a new quasi-meic d on, which is elaed o d and μ. To his end, se dx, y = inf μb, whee he infimum is aken ove all closed balls B conaining x and y see, e.g., [8,25]. Denoe Bx, = { y dx, y }. In he lemma below we sae some popeies of d, which ae known among specialiss, and which we shall need lae on. Since hei poofs ae vey sho and i is difficul fo us o indicae one efeence which conains all of hem, we povide he deails fo he convenience of he eade. Lemma 15 The funcion d has he following popeies: a hee exiss C b > such ha fo x, y we have Cb 1 μbx, dx, y dx, y μbx, dx, y. 5.1 b d is a quasi-meic, namely hee exiss A 1 such ha dx, y A 1 dx, z + dz, y. Moeove, if he measue μ has no aoms and μ =, hen: c he measue μ is egula wih espec o d, namely fo x and >, μ Bx, ;

14 978 J. Dziubański, M. Peisne d fo x and > hee exiss R > such ha Bx, Bx, R and μbx, R μ Bx, ; e fo x and R > hee exiss > such ha Bx, R Bx, and μ Bx, μbx, R. Poof a Se R = dx, y. Clealy, dx, y μbx, R, asx and y belong o Bx, R. On he ohe hand, if x and y belong o a ball B = Bz,, henr 2; hence, Bx, R Bz, 3 and μbx, R μbz, 3 μbz,. By aking he infimum ove all balls B conaining boh x and y, we conclude ha μbx, R C dx, y. b Fo evey x, y, z,wehavedx, y dx, z+dz, y. Assume ha = dx, z dz, y. Thenx, y Bz,. By using a, we deduce ha dx, y μbz, dz, x dx, z + dz, y. c Given x, by ou addiional assumpions, he funcion, μbx, is inceasing and { μbx, as, μbx, + as +. Le x and >. Fo evey y Bx,, wehaveμbx, dx, y dx, y. Hence R = sup {dx, y y Bx, } < +. Le y Bx, such ha dx, y R 2.Then Bx, Bx, R Bx, 2dx, y. 5.2 Hence μ Bx, μbx, R μbx, 2dx, y μbx, dx, y dx, y. 5.3 On he ohe hand, T = inf{ > μbx, } >. As μbx, T/2 <, wehave dx, y <, foeveyy Bx, T/2; hence, Bx, T/2 Bx,. Consequenly, μbx, 2T μbx, T/2 μ Bx,, which ogehe wih 5.3 complees he poof of c. d is a simple consequence of 5.2, 5.3, and c. e Se = μbx, R. Ify Bx, R, hen dx, y and, consequenly, Bx, R Bx,. Clealy, by c, μ Bx, = μbx, R. Le us ecall ha in Theoems 1 and 2 we assume ha Φ x is a bijecion on,. This obviously implies ha μ = and ha μ is nonaomic. As a consequence of d and e of Lemma 15 we obain he following coollay. Coollay 16 Suppose haμ hasno aoms andμ =. Then, he aomic Hady spaces H 1 a d,μand H 1 a d,μcoincide and he coesponding aomic noms ae equivalen. We finish his secion by Lemma 17, which is used lae on. Define A 2 := C b C d 2 q 3, whee C d, q, andc b ae as in 1.1and5.1.

15 Hady spaces fo semigoups wih Gaussian bounds 979 Lemma 17 Suppose ha we have a space of homogeneous ype, d, μ such ha he funcion Φ x defined in 1.5 is a bijecion on,. Assume ha x,, > ae elaed by = μbx, and saisfy: dy, z, A 2 dy, z <. Then dx, y 2dx, z. Poof Suppose, owad a conadicion, ha dx, y <.Fom5.1wege = μbx, μby, 2 C d 2 q μby, C d 2 q μby, dy, z C d 2 q C b dy, z <, so he fis inequaliy is poved. Similaly, assume dx, z <dx, y/2. Then dx, y/2 dy, z 2dx, y. Thus, using 5.1, dy, z Cb 1 μby, dy, z C 1 b C d2 q 1 μby, dx, y Cb 1 C d2 q 2 μbx, dx, y Cb 1 C d2 q 3 μbx, = A 1 2 and we come o a conadicion. 6 Poof of Theoem 2 In ode o pove Theoem 2 we shall use a esul of Uchiyama [33], which we sae below in Theoem 18. Denoe by, d,μ he space equipped wih a quasi-meic d and a nonnegaive measue μ, wheeμ =. Assume moeove ha μ Bx,, 6.1 whee x, > and Bx, is a ball in he quasi-meic d.lea 1 be a consan in he quasi-iangle inequaliy, i.e., dx, y A 1 dx, z + dz, y, x, y, z. 6.2 Addiionally, we impose ha hee exis consans γ 1,γ 2,γ 3 >, A A 1 and a coninuous funcion T, x, y of vaiables x, y and > such ha T, x, x 1, U 1 T, x, y dx, 1 γ1 y, U 2 if dy, z < + dx, y/4a, hen U 3 T, x, y T, x, z γ2 1 dy, z 1 + dx, 1 γ3 y, fo all x, y, z and >. As in [33], we conside he maximal funcion f + x = sup T, x, y f y dμy > { and he Hady space H 1, T = f L 1,μ f H 1, T := f + L }. 1,μ < Recall ha he aomic space Ha 1 d,μis defined in Sec. 1.

16 98 J. Dziubański, M. Peisne Theoem 18 [33], Coollay 1 Suppose ha, d,μ, T saisfy 6.1, 6.2, U1, U2, and U3. Then he spaces H 1, T and H 1 a d,μcoincide and f H 1, T f H 1 a d,μ. Assume ha he kenel T x, y saisfies 1.3 and he semigoup T is consevaive. Recall ha in Sec. 4 we poved Hölde-ype esimae 4.3 fo T x, y. Define T, x, y by T, x, y := T x, y, whee = x, is such ha μbx, =. 6.3 In wha follows, > and x ae always elaed by 6.3. Le us noice ha fom Coollay 13 and by he assumpion ha Φ x is a coninuous bijecion on, we have ha T is a coninuous funcion on,. Theoem 19 Suppose ha T x, y saisfies uppe and lowe Gaussian bounds 1.3 and he semigoup T is consevaive. Then he kenel T, x, y saisfies U1, U2, and U3. Poof On-diagonal lowe esimae U1 is an immediae consequence of lowe Gaussian bound 1.3. Fo evey fixed δ>, he uppe esimae T, x, y dx, 1 δ y 6.4 follows fom he uppe esimaes fo T x, y, moe pecisely by combining wih T, x, y 1 exp 1 + dx, 1+δ y cdx, y2 μbx, dx, y 1+δ μbx, dx, y q1+δ cdx, y 2 exp The lae esimae holds fo any δ>. Thus U2 is poved wih any γ 1 >. To finish he poof we need Hölde-ype esimae U3. This is poved in Poposiion 2 below. Poposiion 2 Le α be a consan as in Theoem 5. Thee exiss A A 1 such ha fo δ>we have T, x, y T, x, z dx, 1 δ y dy, z α q 6.7 if dy, z + dx, y/4a. Poof Se A = maxa 1, A 2,see6.2 and Lemma 17. Assuming ha dy, z + dx, y/4a le us begin wih some obsevaions. Fisly, we claim ha i suffices o pove 6.7fo dy, z </2A. Indeed, if dy, z > /2A, hen dy, z dx, y/2a and, consequenly, dx, y A 1 dx, z + A 1 dz, y A 1 dx, z + dx, y/2.

17 Hady spaces fo semigoups wih Gaussian bounds 981 So, dx, y dx, z and 6.7 follows fom 6.4 by using he iangle inequaliy. Fom now on we assume ha dy, z </2A. Secondly, if dy, z, hen using 1.1and5.1, dy, z μby, dy, z 1/q μby, μby, dy, z 1/q μby, + dx, y 1/q 6.8 μbx, dy, z 1/q dx, y 1 +. Thidly, if dy, z, hen using 1.1and5.1, 1 μby, dy, z μby, = dy, z μbx, μby, dy, z μby, + dx, y μby, dy, z dx, y q Le us un o he poof of 6.7. Case 1: dy, z dx, y/2. Then dx, y dx, z. Thus, accoding o 1.3and4.3 combined wih 6.8and6.9 we obain T, x, y T, x, z 1 exp 1 exp dx, y cdx, y2 dy, z α min, 1 dy, z cdx, y2 1 δ dy, z α/q 1 + α/q, dx, y α whee in he las inequaliy we have used 6.6. Case 2: dy, z >dx, y/2and > dy, z.then dx, y μbx, =.Using 4.3and6.8, T, x, y T, x, z 1 dy, z α α/q dy, 1 z. Case 3: dy, z >dx, y/2 and < dy, z. Then, dy, z /2A /2A 2 and by Lemma 17 we have 2dx, z >dx, y. Hence, using 6.5and6.9, T, x, y T, x, z 1 cdx, y2 exp 1 cdx, y2 dy, z α/q dx, y α exp dy, z α/q 1 + dx, y 1 δ, whee in he las inequaliy we have used 6.6. This finishes he poof of Poposiion 2.

18 982 J. Dziubański, M. Peisne Poof of Theoem 2 Assuming 1.3 and1.6 we obain Hölde-ype esimae 4.3. Recall once moe ha he assumpion on Φ x implies μ = and μ is nonaomic. Then we define a new quasi-meic d. By Coollay 16 we ge ha H 1 a d,μ = H 1 a d,μ.weapply Theoem 18 o he space, d,μ. The assumpions of Theoem 18 ae veified in Theoem 19 and Poposiion 2. In his way we ge f H 1, T f H 1 a d,μ. Using once again he assumpion on Φ x and he definiion of T we easily obseve ha f H 1, T = f H 1 L, which finishes he poof of Theoem 2. Le us ecall ha Theoem 1 follows fom Theoem 2. This is elaboaed a he end of Sec. 3. Remak 21 Unde he assumpions of Theoem 1 one can pove, by he same mehods, ha he Hady space H 1 { L = f L 1,μ } f H 1 L := sup P f x < > L 1,μ coincides wih Ha 1 d,ωμ and he coesponding noms ae equivalen. To his end, one uses: Poposiion 6, Doob s ansfom, Theoem 4, andtheoem18 applied o he kenel P, x, y = P x, y, whee = x, is defined by he elaion μbx, =. 7 Examples In his secion we give examples of self-adjoin semigoups wih he wo-sided Gaussian bounds. 7.1 Laplace Belami opeaos Le, g be a complee Riemannian manifold wih he Riemannian disance dx, y and he Riemannian measue μ saisfying he doubling popey and he Poincaé inequaliy f f B 2 dμ C 2 f 2 dμ fo all >, Bx, Bx,2 whee denoes he gadien on. I is well known ha he kenel of he hea semigoup geneaed by he Laplace Belami opeao saisfies wo-sided Gaussian bounds 1.3 and Hölde esimaes 4.3. Fo deails and moe infomaion concening he hea equaion on Riemannian manifolds we efe he eade o [28] and efeences heein. 7.2 Schödinge opeaos On = R d wih he Euclidean meic and he Lebesgue measue we conside he Schödinge opeao L = + V, whee is he sandad Laplacian and V is a locally inegable funcion.

19 Hady spaces fo semigoups wih Gaussian bounds 983 I is well known see, e.g., [29] ha fo V, d 3, he semigoup T = e L admis kenels T x, y wih he uppe and lowe Gaussian bounds 1.3 if and only if V is a Geen bounded poenial, ha is, sup x y 2 d V y dy <. 7.1 x R d R d Hady spaces associaed wih Schödinge opeaos on R d saisfying 7.1 wee sudied in [13]. Acually, as we have aleady menioned, his wok moivaed us o sudy he poblem of H 1 spaces wih he Gaussian bounds in he genealiy as in Theoems 1 and 2. Ou second example concens Schödinge opeaos L = + V wih nonposiive poenials. Fo d 3fixp 1, p 2 > 1 saisfying p 1 < d/2 < p 2. Then hee is a consan cp 1, p 2, d > such ha if V and V L p 1 R d + V L p 2 R d cp 1, p 2, d, hen he inegal kenel T x, y of he semigoup T = e L exiss and saisfies wo-sided Gaussian bounds T x, y d/2 x y 2 exp The esul can be found in Zhang [35]. A slighly diffeen poof of 7.2, based on bidges of he Gauss Weiesass semigoup, can be obained by using Lemma 1.2 ogehe wih Poposiion 2.2 of [4]. 7.3 Bessel Schödinge opeao Le α> 1 and conside =, and dμx = x α dx. Noice ha he space,μ wih he Euclidean meic d e x, y = x y is a space of homogeneous ype. We conside he classical Bessel opeao B f x = f x α x f x, which is self-adjoin posiive on L 2,μ, and he associaed semigoup of linea opeaos S = e B. I is well known ha S is consevaive and has he inegal kenel S x, y = 2 1 exp x2 + y 2 xy I α 1/2 xy α 1/2, see, e.g., [5, Chape 6]. Hee I α 1/2 denoes he modified Bessel funcion of he fis kind, see, e.g., [34]. The kenel S x, y saisfies wo-sided Gaussian esimaes C 1 μ Bx, exp c 1 x y 2 C S x, y μ Bx, exp c 2 x y Fo a sho poof of 7.4 see[12, poof of Lemma 4.2]. Theefoe, using Theoem 2 we obain aomic chaaceizaion of H 1 B ha was peviously poved in [3]. In his subsecion we conside peubaions of B of he fom L = B + V,

20 984 J. Dziubański, M. Peisne whee a poenial V is nonnegaive and locally inegable. Moe pecisely, on L 2,μwe define he quadaic fom Q f, g = f xg x dμx + V x f xgx dμx, wih he domain Dom Q = cl { f Cc 1 [, f + = } { f L 2,μ } Vf L 2,μ, whee cla sands fo he closue of he se A in he nom f L 2,μ + f L 2,μ.The fom Q is posiive and closed. Thus, i coesponds o he unique self-adjoin opeao L on L 2,μwih he domain Dom L = { f DomQ h L 2,μ g DomQ Q f, g = } h g dμ. By definiion, Lf = h when f, h ae elaed as above. Le T = exp L be he semigoup geneaed by L. The Feynman Kac fomula saes ha T f x = E exp x V b s ds f b, 7.5 whee b s is he Bessel pocess on, associaed wih S.Using7.5 one ges ha he semigoup T has fom 1.2, whee T x, y S x, y. 7.6 Theefoe he uppe Gaussian esimaes fo T x, y follows simply fom 7.4 fo any locally inegable V. On he ohe hand, he elaion beween S x, y and T x, y is given by he peubaion fomula S x, y = T x, y + S s x, zv zt s z, y dμz ds 7.7 Fom now on we conside only α>1. We ae ineesed in poving he lowe Gaussian esimaes, bu his can be done only fo some poenials V. Fo ohe poenials Hady spaces may have a local chaace, see, e.g., [22]. Le Ɣx, y = S x, y d be he fomal kenel of B 1. In addiion o V Lloc 1 and V, we shall need one moe assumpion, a vesion of he global Kao condiion, cf. 7.1, V Kao := sup Ɣx, yv y dμy <. 7.8 x Fomally, we can ephase his as B 1 V L,μ. Le us poin ou ha Ɣx, y x + y α+1. This can be easily obained fom 7.3 and well-known asympoics fo he Bessel funcion I α 1/2, see also [26, Sec.2]. In Lemmas 22 and 23 we pove ha unde assumpion 7.8 lowe Gaussian esimaes 1.3 hold fo T x, y. The esimaes ae poved in a simila way as in he case of he Schödinge opeao on he Euclidean space. Fo he convenience of he eade we povide he deails.

21 Hady spaces fo semigoups wih Gaussian bounds 985 Lemma 22 Suppose ha V Kao <. If x y, hen T x, y C 1 l μbx, 1. Poof Fis we shall pove Lemma 22 wih an addiional assumpion ha V Kao ε fo a fixed small ε>. By 7.7and7.6, S x, y T x, y = S s x, zv zt s z, ydμz ds = μbx, /2 1 V zt s z, y dμz ds + μby, 1 /2 μbx, 1 V Kao. /2 S s x, zv z dμz ds... ds +... ds /2 By choosing pope ε>wededuce he hesis fom lowe esimae 7.4foS x, y. Now assume ha he nom V Kao < is abiay. Fix q > 1, such ha V Kao = qε. Se V q x = V x/q, Vq Kao = ε, andlet q be he semigoup elaed o L q = B + V q. Using 7.5 and Hölde s inequaliy, T χby, μby, x = E x exp [E x exp [ = T q χby, μby, V b s q χ By, b ds q μby, V b s χby, b ds q μby, q x] [ S χby, μby, ] q [ E x χby, b μby, x ] q/q ] q q 7.9 Le us noice ha T x, y = lim μ By, 1 T x, z dμz By, fo a.e. x, y. By leing in7.9, using 7.4 and he fis pa of he poof, fo a.e. x, y we obain ha T x, y T q x, y q S x, y q/q μbx, 1. Lemma 23 Suppose ha V Kao <. Then T x, y μbx, 1 c x y 2 exp. Poof Assume ha x y 2 / 1andsem = 4 x y 2 / 4. Fo i =,...,m, le x i = x + iy x/m, sohax = x, x m = y, and x i+1 x i = x y /m. Denoe B i = Bx i, /4 m and obseve ha y i+1 y i y i x i + x i x i+1 + x i+1 y i+1 4 m + 2 m + 4 m = m

22 986 J. Dziubański, M. Peisne fo y i B i and y i+1 B i+1. Now we use he semigoup popey, Lemma 22, andhe doubling popey of μ o obain T x, y =... T /m x, y 1 T /m y 1, y 2...T /m y m 1, y dμy 1... dμy m 1 c1 m 1... μbx, /m 1...μBy m 1, /m 1 dμy 1... dμy m 1 B 1 B m 1 c2 m 1 μbx, /m 1 μb 1...μB m 1 μbx 1, /m...μbx m 1, /m c3 m μbx, 1 = μbx, 1 m ln c 1 e 3 μbx, 1 e c x y 2. Noice ha c 1, c 2, c 3,andc in his esimae depend only on he consan C l fom Lemma 22 and he doubling consan of μ. Obviously, he space, d e,μsaisfies he assumpions of Theoem 1. Since we have he wo-sided Gaussian esimaes fo T see Lemma 22,7.6, and 7.4 we obain he following coollay. Coollay 24 Suppose ha α>1and V saisfies 7.8. Thenheeexissω such ha < C 1 ωx C, T ω = ω fo > and H 1 L = Ha 1d e,ωμ. Moeove, f H 1 L f H 1 a d e,ω μ. Acknowledgemens We wan o hank Pascal Auche, Fédéic Benico, Li Chen, and Gzegoz Plebanek fo hei emaks. We ae gealy indeb o Jacek Zienkiewicz fo convesaions concening Schödinge opeaos. The auhos ae gaeful o he efeee fo he/his helpful commens which impoved he pesenaion he pape. Open Access This aicle is disibued unde he ems of he Ceaive Commons Aibuion 4. Inenaional License hp://ceaivecommons.og/licenses/by/4./, which pemis unesiced use, disibuion, and epoducion in any medium, povided you give appopiae cedi o he oiginal auhos and he souce, povide a link o he Ceaive Commons license, and indicae if changes wee made. Refeences 1. Ausche, P., Duong,.T., McInosh, A.: Boundedness of banach space valued singula inegal opeaos and hady spaces. Unpublished pepin Benico, F., Coulhon, T., Fey, D.: Gaussian hea kenel bounds hough ellipic Mose ieaion. J. Mah. Pues Appl , Beanco, J.J., Dziubański, J., Toea, J.L.: On Hady spaces associaed wih Bessel opeaos. J. Anal. Mah. 17, Bogdan, K., Dziubański, J., Szczypkowski, K.: Shap Gaussian esimaes fo Schödinge hea kenels: L p inegabiliy condiions. Aiv e-pins Boodin, A.N., Salminen, P.: Handbook of Bownian Moion Facs and Fomulae. Pobabiliy and is Applicaions, 2nd edn. Bikhäuse, Basel Bukholde, D.L., Gundy, R.F., Silvesein, M.L.: A maximal funcion chaaceizaion of he class H p. Tans. Am. Mah. Soc. 157, Coifman, R.R.: A eal vaiable chaaceizaion of H p. Sud. Mah. 51, Coifman, R.R., Weiss, G.: Exensions of Hady spaces and hei use in analysis. Bull. Am. Mah. Soc. 834, Coulhon, T., Sikoa, A.: Gaussian hea kenel uppe bounds via he Phagmén-Lindelöf heoem. Poc. Lond. Mah. Soc , Davies, E.B.: Hea Kenels and Specal Theoy, Cambidge Tacs in Mahemaics, vol. 92. Cambidge Univesiy Pess, Cambidge Dziubański, J., Peisne, M.: Remaks on specal muliplie heoems on Hady spaces associaed wih semigoups of opeaos. Rev. Un. Ma. Agenina 52,

23 Hady spaces fo semigoups wih Gaussian bounds Dziubański, J., Peisne, M., Wóbel, B.: Mulivaiae Hömande-ype muliplie heoem fo he Hankel ansfom. J. Fouie Anal. Appl. 192, Dziubański, J., Zienkiewicz, J.: On isomophisms of Hady spaces associaed wih Schödinge opeaos. J. Fouie Anal. Appl. 193, Dziubański, J., Zienkiewicz, J.: A chaaceizaion of Hady spaces associaed wih ceain Schödinge opeaos. Poenial Anal. 413, Feffeman, C., Sein, E.M.: H p spaces of seveal vaiables. Aca Mah , Gigo yan, A.: Hea Kenel and Analysis on Manifolds, AMS/IP Sudies in Advanced Mahemaics, vol. 47. Ameican Mahemaical Sociey, Inenaional Pess, Povidence, Boson Gyya, P., Saloff-Cose, L.: Neumann and Diichle hea kenels in inne unifom domains. Aséisque 336, viii Hebisch, W.: Funcional calculus fo slowly decaying kenels. Unpublished. hp:// pl/~hebisch/ 19. Hebisch, W., Saloff-Cose, L.: On he elaion beween ellipic and paabolic Hanack inequaliies. Ann. Ins. Fouie Genoble 515, Hofmann, S., Lu, G., Miea, D., Miea, M., Yan, L.: Hady spaces associaed o non-negaive self-adjoin opeaos saisfying Davies-Gaffney esimaes. Mem. Am. Mah. Soc , vi Jeison, D.S., Kenig, C.E.: Bounday value poblems on Lipschiz domains, Sudies in paial diffeenial equaions, MAA Sud. Mah., vol. 23. Mahemaical Associaion of Ameica, Washingon pp Kania, E., Peisne, M.: Hady spaces fo Bessel-Schödinge opeaos. aiv e-pins Lae, R.H.: A chaaceizaion of H p R n in ems of aoms. Sud. Mah. 621, Macías, R.A., Segovia, C.: A decomposiion ino aoms of disibuions on spaces of homogeneous ype. Adv. Mah. 333, Macías, R.A., Segovia, C.: Lipschiz funcions on spaces of homogeneous ype. Adv. Mah. 333, Nowak, A., Sempak, K.: Poenial opeaos associaed wih Hankel and Hankel-Dunkl ansfoms. J. Anal. Mah. 131, Ouhabaz, E.M.: Analysis of Hea Equaions on Domains, London Mahemaical Sociey Monogaphs Seies, vol. 31. Pinceon Univesiy Pess, Pinceon Saloff-Cose, L.: Aspecs of Sobolev-Type Inequaliies, London Mahemaical Sociey Lecue Noe Seies, vol Cambidge Univesiy Pess, Cambidge Semenov, YuA: Sabiliy of L p -specum of genealized Schödinge opeaos and equivalence of Geen s funcions. In. Mah. Res. No. 12, Song, L., Yan, L.: A maximal funcion chaaceizaion fo Hady spaces associaed o nonnegaive selfadjoin opeaos saisfying Gaussian esimaes. Adv. Mah. 287, hps://doi.og/1. 116/j.aim Sein, E.M.: Hamonic Analysis: Real-Vaiable Mehods, Ohogonaliy, and Oscillaoy Inegals. Pinceon Mahemaical Seies, vol. 43. Pinceon Univesiy Pess, Pinceon Wih he assisance of Timohy S. Muphy, Monogaphs in Hamonic Analysis, III 32. Sein, E.M., Weiss, G.: On he heoy of hamonic funcions of seveal vaiables. I. The heoy of H p - spaces. Aca Mah. 13, Uchiyama, A.: A maximal funcion chaaceizaion of H p on he space of homogeneous ype. Tans. Am. Mah. Soc. 2622, Wason, G.N.: A Teaise on he Theoy of Bessel Funcions, Cambidge Mahemaical Libay. Cambidge Univesiy Pess, Cambidge Repin of he second 1944 ediion 35. Zhang, Q.S.: A shap compaison esul concening Schödinge hea kenels. Bull. Lond. Mah. Soc. 354,

336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f

336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f TAMKANG JOURNAL OF MATHEMATIS Volume 33, Numbe 4, Wine 2002 ON THE OUNDEDNESS OF A GENERALIED FRATIONAL INTEGRAL ON GENERALIED MORREY SPAES ERIDANI Absac. In his pape we exend Nakai's esul on he boundedness

More information

On Control Problem Described by Infinite System of First-Order Differential Equations

On Control Problem Described by Infinite System of First-Order Differential Equations Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical

More information

7 Wave Equation in Higher Dimensions

7 Wave Equation in Higher Dimensions 7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,

More information

Variance and Covariance Processes

Variance and Covariance Processes Vaiance and Covaiance Pocesses Pakash Balachandan Depamen of Mahemaics Duke Univesiy May 26, 2008 These noes ae based on Due s Sochasic Calculus, Revuz and Yo s Coninuous Maingales and Bownian Moion, Kaazas

More information

GRADIENT ESTIMATES, POINCARÉ INEQUALITIES, DE GIORGI PROPERTY AND THEIR CONSEQUENCES

GRADIENT ESTIMATES, POINCARÉ INEQUALITIES, DE GIORGI PROPERTY AND THEIR CONSEQUENCES GRADIENT ESTIMATES, POINCARÉ INEQUALITIES, DE GIORGI PROPERTY AND THEIR CONSEQUENCES FRÉDÉRIC ERNICOT, THIERRY COULHON, DOROTHEE FREY Absac. On a doubling meic measue space endowed wih a caé du champ,

More information

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,

More information

Deviation probability bounds for fractional martingales and related remarks

Deviation probability bounds for fractional martingales and related remarks Deviaion pobabiliy bounds fo facional maingales and elaed emaks Buno Sausseeau Laboaoie de Mahémaiques de Besançon CNRS, UMR 6623 16 Roue de Gay 253 Besançon cedex, Fance Absac In his pape we pove exponenial

More information

POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli

POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli Opuscula Mah. 35, no. (205), 5 9 hp://dx.doi.og/0.7494/opmah.205.35..5 Opuscula Mahemaica POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n Abdelwaheb Dhifli Communicaed

More information

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal

More information

Research Article A Note on Multiplication and Composition Operators in Lorentz Spaces

Research Article A Note on Multiplication and Composition Operators in Lorentz Spaces Hindawi Publishing Copoaion Jounal of Funcion Spaces and Applicaions Volume 22, Aicle ID 29363, pages doi:.55/22/29363 Reseach Aicle A Noe on Muliplicaion and Composiion Opeaos in Loenz Spaces Eddy Kwessi,

More information

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security 1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,

More information

THE MODULAR INEQUALITIES FOR A CLASS OF CONVOLUTION OPERATORS ON MONOTONE FUNCTIONS

THE MODULAR INEQUALITIES FOR A CLASS OF CONVOLUTION OPERATORS ON MONOTONE FUNCTIONS PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 5, Numbe 8, Augus 997, Pages 93 35 S -9939(973867-7 THE MODULAR INEQUALITIES FOR A CLASS OF CONVOLUTION OPERATORS ON MONOTONE FUNCTIONS JIM QILE

More information

K. G. Malyutin, T. I. Malyutina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE

K. G. Malyutin, T. I. Malyutina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE Математичнi Студiї. Т.4, 2 Maemaychni Sudii. V.4, No.2 УДК 57.5 K. G. Malyuin, T. I. Malyuina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE

More information

functions on localized Morrey-Campanato spaces over doubling metric measure spaces

functions on localized Morrey-Campanato spaces over doubling metric measure spaces JOURNAL OF FUNCTION SPACES AND APPLICATIONS Volume 9, Numbe 3 2), 245 282 c 2, Scienific Hoizon hp://www.jfsa.ne oundedness of Lusin-aea and gλ funcions on localized Moey-Campanao spaces ove doubling meic

More information

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as

More information

@FMI c Kyung Moon Sa Co.

@FMI c Kyung Moon Sa Co. Annals of Fuzzy Mahemaics Infomaics Volume, No. 2, (Apil 20), pp. 9-3 ISSN 2093 930 hp://www.afmi.o.k @FMI c Kyung Moon Sa Co. hp://www.kyungmoon.com On lacunay saisical convegence in inuiionisic fuzzy

More information

BMOA estimates and radial growth of B φ functions

BMOA estimates and radial growth of B φ functions c Jounal of echnical Univesiy a Plovdiv Fundamenal Sciences and Applicaions, Vol., 995 Seies A-Pue and Applied Mahemaics Bulgaia, ISSN 3-827 axiv:87.53v [mah.cv] 3 Jul 28 BMOA esimaes and adial gowh of

More information

arxiv: v1 [math.co] 4 Apr 2019

arxiv: v1 [math.co] 4 Apr 2019 Dieced dominaion in oiened hypegaphs axiv:1904.02351v1 [mah.co] 4 Ap 2019 Yai Cao Dep. of Mahemaics Univesiy of Haifa-Oanim Tivon 36006, Isael yacao@kvgeva.og.il This pape is dedicaed o Luz Volkmann on

More information

Extremal problems for t-partite and t-colorable hypergraphs

Extremal problems for t-partite and t-colorable hypergraphs Exemal poblems fo -paie and -coloable hypegaphs Dhuv Mubayi John Talbo June, 007 Absac Fix ineges and an -unifom hypegaph F. We pove ha he maximum numbe of edges in a -paie -unifom hypegaph on n veices

More information

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE

More information

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS Mem. Fac. Inegaed As and Sci., Hioshima Univ., Se. IV, Vol. 8 9-33, Dec. 00 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS YOSHIO AGAOKA *, BYUNG HAK KIM ** AND JIN HYUK CHOI ** *Depamen of Mahemaics, Faculy

More information

Heat kernel and Harnack inequality on Riemannian manifolds

Heat 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 information

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion

More information

arxiv: v1 [math.ca] 25 Sep 2013

arxiv: v1 [math.ca] 25 Sep 2013 OUNDEDNESS OF INTRINSIC LITTLEWOOD-PALEY FUNCTIONS ON MUSIELAK-ORLICZ MORREY AND CAMPANATO SPACES axiv:39.652v [mah.ca] 25 Sep 23 YIYU LIANG, EIICHI NAKAI 2, DACHUN YANG AND JUNQIANG ZHANG Absac. Le ϕ

More information

Research Article Weighted Hardy Operators in Complementary Morrey Spaces

Research Article Weighted Hardy Operators in Complementary Morrey Spaces Hindawi Publishing Copoaion Jounal of Funcion Spaces and Applicaions Volume 212, Aicle ID 283285, 19 pages doi:1.1155/212/283285 Reseach Aicle Weighed Hady Opeaos in Complemenay Moey Spaces Dag Lukkassen,

More information

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens

More information

Risk tolerance and optimal portfolio choice

Risk tolerance and optimal portfolio choice Risk oleance and opimal pofolio choice Maek Musiela BNP Paibas London Copoae and Invesmen Join wok wih T. Zaiphopoulou (UT usin) Invesmens and fowad uiliies Pepin 6 Backwad and fowad dynamic uiliies and

More information

A Characterization of Hardy Spaces Associated with Certain Schrödinger Operators

A Characterization of Hardy Spaces Associated with Certain Schrödinger Operators Potential Anal 214) 41:917 93 DOI 1.17/s11118-14-94-2 A Chaacteization of Hady Spaces Associated with Cetain Schödinge Opeatos Jacek Dziubański Jacek Zienkiewicz Received: 6 June 213 / Accepted: 4 Mach

More information

arxiv: v1 [math.ca] 15 Jan 2019

arxiv: v1 [math.ca] 15 Jan 2019 DORRONSORO S THEOREM IN HEISENBERG GROUPS KATRIN FÄSSLER AND TUOMAS ORPONEN axiv:9.4767v [mah.ca] 5 Jan 29 ABSTRACT. A heoem of Doonsoo fom he 98s quanifies he fac ha eal-valued Sobolev funcions on Euclidean

More information

arxiv: v2 [math.pr] 19 Feb 2016

arxiv: v2 [math.pr] 19 Feb 2016 Global Diichle Hea Kenel Esimaes fo Symmeic Lévy Pocesses in Half-space Zhen-Qing Chen and Panki Kim axiv:54.4673v2 [mah.pr] 9 Feb 26 Mach 5, 28 Absac In his pape, we deive explici shap wo-sided esimaes

More information

Degree of Approximation of a Class of Function by (C, 1) (E, q) Means of Fourier Series

Degree of Approximation of a Class of Function by (C, 1) (E, q) Means of Fourier Series IAENG Inenaional Jounal of Applied Mahemaic, 4:, IJAM_4 7 Degee of Appoximaion of a Cla of Funcion by C, E, q Mean of Fouie Seie Hae Kihna Nigam and Kuum Shama Abac In hi pape, fo he fi ime, we inoduce

More information

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u Genealized Mehods of Momens he genealized mehod momens (GMM) appoach of Hansen (98) can be hough of a geneal pocedue fo esing economics and financial models. he GMM is especially appopiae fo models ha

More information

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay) Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens

More information

A note on characterization related to distributional properties of random translation, contraction and dilation of generalized order statistics

A note on characterization related to distributional properties of random translation, contraction and dilation of generalized order statistics PobSa Foum, Volume 6, July 213, Pages 35 41 ISSN 974-3235 PobSa Foum is an e-jounal. Fo eails please visi www.pobsa.og.in A noe on chaaceizaion elae o isibuional popeies of anom anslaion, conacion an ilaion

More information

Convergence of the Neumann series in higher norms

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 information

An Introduction to Malliavin calculus and its applications

An 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 information

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Oscillation 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 information

Riesz transform characterization of Hardy spaces associated with Schrödinger operators with compactly supported potentials

Riesz 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 information

A 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 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 information

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

The 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 information

Monochromatic Wave over One and Two Bars

Monochromatic Wave over One and Two Bars Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,

More information

GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256

GRADIENT 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 information

Quantum Algorithms for Matrix Products over Semirings

Quantum Algorithms for Matrix Products over Semirings CHICAGO JOURNAL OF THEORETICAL COMPUTER SCIENCE 2017, Aicle 1, pages 1 25 hp://cjcscsuchicagoedu/ Quanum Algoihms fo Maix Poducs ove Semiings Fançois Le Gall Haumichi Nishimua Received July 24, 2015; Revised

More information

Order statistics and concentration of l r norms for log-concave vectors

Order statistics and concentration of l r norms for log-concave vectors Jounal of Funcional Analysis 61 011 681 696 www.elsevie.com/locae/jfa Ode saisics and concenaion of l noms fo log-concave vecos Rafał Laała a,b, a Insiue of Mahemaics, Univesiy of Wasaw, Banacha, 0-097

More information

4 Sequences of measurable functions

4 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 information

Dual Hierarchies of a Multi-Component Camassa Holm System

Dual Hierarchies of a Multi-Component Camassa Holm System Commun. heo. Phys. 64 05 37 378 Vol. 64, No. 4, Ocobe, 05 Dual Hieachies of a Muli-Componen Camassa Holm Sysem LI Hong-Min, LI Yu-Qi, and CHEN Yong Shanghai Key Laboaoy of uswohy Compuing, Eas China Nomal

More information

On the local convexity of the implied volatility curve in uncorrelated stochastic volatility models

On the local convexity of the implied volatility curve in uncorrelated stochastic volatility models On he local conexiy of he implied olailiy cue in uncoelaed sochasic olailiy models Elisa Alòs Dp. d Economia i Empesa and Bacelona Gaduae School of Economics Uniesia Pompeu Faba c/ramon Tias Fagas, 5-7

More information

Reichenbach and f-generated implications in fuzzy database relations

Reichenbach and f-generated implications in fuzzy database relations INTERNATIONAL JOURNAL O CIRCUITS SYSTEMS AND SIGNAL PROCESSING Volume 08 Reichenbach and f-geneaed implicaions in fuzzy daabase elaions Nedžad Dukić Dženan Gušić and Nemana Kajmoić Absac Applying a definiion

More information

Boundedness for Marcinkiewicz integrals associated with Schrödinger operators

Boundedness 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 information

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS 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

More information

On the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources

On the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources Jounal of Applied Mahemaics and Physics 25 3 478-487 Published Online May 25 in SciRes. hp://www.scip.og/jounal/jamp hp://dx.doi.og/.4236/jamp.25.356 On he Semi-Discee Davey-Sewason Sysem wih Self-Consisen

More information

A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS

A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS Assoc. Pof. Romeo Negea Ph. D Poliehnica Univesiy of Timisoaa Depamen of Mahemaics Timisoaa, Romania Assoc. Pof. Cipian Peda Ph. D Wes Univesiy

More information

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS

KOEBE 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 information

SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES

SOME 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 information

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero

A 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 information

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type

Monotonic 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 information

Computer Propagation Analysis Tools

Computer Propagation Analysis Tools Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion

More information

GLOBAL REGULARITY IN ORLICZ-MORREY SPACES OF SOLUTIONS TO NONDIVERGENCE ELLIPTIC EQUATIONS WITH VMO COEFFICIENTS

GLOBAL REGULARITY IN ORLICZ-MORREY SPACES OF SOLUTIONS TO NONDIVERGENCE ELLIPTIC EQUATIONS WITH VMO COEFFICIENTS Eleconic Jounal of Diffeenial Equaions, Vol. 208 (208, No. 0, pp. 24. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu o hp://ejde.mah.un.edu GLOBAL REGULARITY IN ORLICZ-MORREY SPACES OF SOLUTIONS TO NONDIVERGENCE

More information

Research Article Weak Type Inequalities for Some Integral Operators on Generalized Nonhomogeneous Morrey Spaces

Research Article Weak Type Inequalities for Some Integral Operators on Generalized Nonhomogeneous Morrey Spaces Hindawi Publishing Copoaion Jounal of Funcion Spaces and Applicaions Volume 23, Aicle ID 8974, 2 pages hp://dx.doi.og/.55/23/8974 Reseach Aicle Weak Type Inequaliies fo Some Inegal Opeaos on Genealized

More information

Sobolev-type Inequality for Spaces L p(x) (R N )

Sobolev-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 information

On a Fractional Stochastic Landau-Ginzburg Equation

On 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 information

Existence of positive solution for a third-order three-point BVP with sign-changing Green s function

Existence 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 information

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

Ann. 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 information

SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS

SOME 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 information

GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS

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 information

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy

More information

Orthotropic Materials

Orthotropic Materials Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε

More information

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2  P 1 =  #P L L, Lecue 36 Pipe Flow and Low-eynolds numbe hydodynamics 36.1 eading fo Lecues 34-35: PKT Chape 12. Will y fo Monday?: new daa shee and daf fomula shee fo final exam. Ou saing poin fo hydodynamics ae wo equaions:

More information

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t Lecue 6: Fiis Tansmission Equaion and Rada Range Equaion (Fiis equaion. Maximum ange of a wieless link. Rada coss secion. Rada equaion. Maximum ange of a ada. 1. Fiis ansmission equaion Fiis ansmission

More information

CS 188: Artificial Intelligence Fall Probabilistic Models

CS 188: Artificial Intelligence Fall Probabilistic Models CS 188: Aificial Inelligence Fall 2007 Lecue 15: Bayes Nes 10/18/2007 Dan Klein UC Bekeley Pobabilisic Models A pobabilisic model is a join disibuion ove a se of vaiables Given a join disibuion, we can

More information

Existence Theory of Second Order Random Differential Equations

Existence 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 information

Asymptotic instability of nonlinear differential equations

Asymptotic instability of nonlinear differential equations Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy

More information

KINEMATICS OF RIGID BODIES

KINEMATICS OF RIGID BODIES KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal 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 information

A characterization of reciprocal processes via an integration by parts formula on the path space

A characterization of reciprocal processes via an integration by parts formula on the path space A chaaceizaion of ecipocal pocesses via an inegaion by pas fomula on he pah space Sylvie Rœlly Cene de Mahémaiques Appliquées UMR CNRS 764 École Polyechnique 928 Palaiseau Cédex, Fance e-mail : oelly@cmapx.polyechnique.f

More information

The sudden release of a large amount of energy E into a background fluid of density

The sudden release of a large amount of energy E into a background fluid of density 10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy

More information

EVENT HORIZONS IN COSMOLOGY

EVENT HORIZONS IN COSMOLOGY Mahemaics Today Vol7(Dec-)54-6 ISSN 976-38 EVENT HORIZONS IN COSMOLOGY K Punachanda Rao Depamen of Mahemaics Chiala Engineeing College Chiala 53 57 Andha Padesh, INDIA E-mail: dkpaocecc@yahoocoin ABSTRACT

More information

LOGARITHMIC ORDER AND TYPE OF INDETERMINATE MOMENT PROBLEMS

LOGARITHMIC ORDER AND TYPE OF INDETERMINATE MOMENT PROBLEMS LOGARITHMIC ORDER AND TYPE OF INDETERMINATE MOMENT PROBLEMS CHRISTIAN BERG AND HENRIK L. PEDERSEN WITH AN APPENDIX BY WALTER HAYMAN We invesigae a efined gowh scale, logaihmic gowh, fo indeeminae momen

More information

BEST CONSTANTS FOR UNCENTERED MAXIMAL FUNCTIONS. Loukas Grafakos and Stephen Montgomery-Smith University of Missouri, Columbia

BEST CONSTANTS FOR UNCENTERED MAXIMAL FUNCTIONS. Loukas Grafakos and Stephen Montgomery-Smith University of Missouri, Columbia BEST CONSTANTS FOR UNCENTERED MAXIMAL FUNCTIONS Loukas Gafakos and Stehen Montgomey-Smith Univesity of Missoui, Columbia Abstact. We ecisely evaluate the oeato nom of the uncenteed Hady-Littlewood maximal

More information

arxiv: v1 [math.fa] 20 Dec 2018

arxiv: v1 [math.fa] 20 Dec 2018 Diffeeniabiliy of he Evoluion Map and Mackey Coninuiy Maximilian Hanusch axiv:1812.08777v1 mah.fa] 20 Dec 2018 Insiu fü Mahemaik Univesiä Padebon Wabuge Saße 100 33098 Padebon Gemany Decembe 20, 2018 Absac

More information

On The Estimation of Two Missing Values in Randomized Complete Block Designs

On The Estimation of Two Missing Values in Randomized Complete Block Designs Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.

More information

Reinforcement learning

Reinforcement learning Lecue 3 Reinfocemen leaning Milos Hauskech milos@cs.pi.edu 539 Senno Squae Reinfocemen leaning We wan o lean he conol policy: : X A We see examples of x (bu oupus a ae no given) Insead of a we ge a feedback

More information

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba THE INTEACTION OF ADIATION AND MATTE: SEMICLASSICAL THEOY PAGE 26 III. EVIEW OF BASIC QUANTUM MECHANICS : TWO -LEVEL QUANTUM SYSTEMS : The lieaue of quanum opics and lase specoscop abounds wih discussions

More information

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity

L 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 information

Example on p. 157

Example 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 information

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

MODULE 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 information

Lecture 28: Convergence of Random Variables and Related Theorems

Lecture 28: Convergence of Random Variables and Related Theorems EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An

More information

Brief summary of functional analysis APPM 5440 Fall 2014 Applied Analysis

Brief 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 information

RADIAL POSITIVE SOLUTIONS FOR A NONPOSITONE PROBLEM IN AN ANNULUS

RADIAL 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 information

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

Hamilton- 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

Properties of the interface of the symbiotic branching model

Properties of the interface of the symbiotic branching model Popeies of he ineface of he symbioic banching model Jochen Blah 1 and Macel Ogiese 1 (Vesion of 4 Mach 1) Absac The symbioic banching model descibes he evoluion of wo ineacing populaions and if saed wih

More information

PHYS PRACTICE EXAM 2

PHYS PRACTICE EXAM 2 PHYS 1800 PRACTICE EXAM Pa I Muliple Choice Quesions [ ps each] Diecions: Cicle he one alenaive ha bes complees he saemen o answes he quesion. Unless ohewise saed, assume ideal condiions (no ai esisance,

More information

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2 156 Thee ae 9 books sacked on a shelf. The hickness of each book is eihe 1 inch o 2 F inches. The heigh of he sack of 9 books is 14 inches. Which sysem of equaions can be used o deemine x, he numbe of

More information

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can. 1 Cicula Moion Radians One evoluion is equivalen o 360 0 which is also equivalen o 2π adians. Theefoe we can say ha 360 = 2π adians, 180 = π adians, 90 = π 2 adians. Hence 1 adian = 360 2π Convesions Rule

More information

Statistical inference versus mean field limit for Hawkes processes

Statistical inference versus mean field limit for Hawkes processes Eleconic Jounal of Saisics Vol. 1 216 1223 1295 ISS: 1935-7524 DOI: 1.1214/16-EJS1142 Saisical infeence vesus mean field limi fo Hawkes pocesses Sylvain Delae Laboaoie de Pobabiliés e Modèles Aléaoies,

More information

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

CHARACTERIZATION 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 information

Lecture 20: Riccati Equations and Least Squares Feedback Control

Lecture 20: Riccati Equations and Least Squares Feedback Control 34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he

More information

A HARDY TYPE GENERAL INEQUALITY IN L p( ) (0, 1) WITH DECREASING EXPONENT

A HARDY TYPE GENERAL INEQUALITY IN L p( ) (0, 1) WITH DECREASING EXPONENT Transacions of NAS of Azerbaijan, 23, vol. XXXIII, No, pp. 45-5. 45 Farman I. MAMEDOV, Firana M. MAMEDOVA A HARDY TYPE GENERAL INEQUALITY IN L p ), ) WITH DECREASING EXPONENT Absrac We derive a Hardy ype

More information

1 Solutions to selected problems

1 Solutions to selected problems 1 Soluions o seleced problems 1. Le A B R n. Show ha in A in B bu in general bd A bd B. Soluion. Le x in A. Then here is ɛ > 0 such ha B ɛ (x) A B. This shows x in B. If A = [0, 1] and B = [0, 2], hen

More information

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias

More information