Heat kernel and Harnack inequality on Riemannian manifolds
|
|
- Rudolph Horn
- 5 years ago
- Views:
Transcription
1 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 propery 7 5 Relaive Faber-Krahn inequaliy 9 6 On-diagonal lower esimae 11 7 Harnack inequaliy and Li-Yau esimae 11 8 Esimaes of derivaives of he hea kernel 13 1 Laplace operaor and hea kernel A weighed manifold is a couple, μ where is a Riemannian manifold and μ is a measure on wih smooh posiive densiy wih respec o he Riemannian measure μ 0 ; ha is, dμ = h 2 dμ 0 where h, h > 0. The weighed Laplace operaor Δ on is defined by Δ = 1 h 2 div h 2. Observe ha Δ is a symmeric operaor wih respec o measure μ. Indeed, for all f, g 0, Δf gdμ = div h 2 f gdμ 0 = h 2 f, g dμ 0 1
2 whence Δf gdμ = fδgdμ. Furhermore, he operaor Δ wih he domain 0 is admis he Friedrichs exension o a self-adjoin operaor in L 2, μ, which will also be denoed by Δ. The hea semigroup {exp Δ} 0 is defined by means of specral heory as a family of operaors exp Δ in L 2, μ, and he hea kernel p x, y is a unique smooh posiive funcion of > 0 and x, y such ha e Δ f x = p x, y f y dμ y, for all f L 2, μ. I is known ha p x, y exiss on any weighed manifold and coincides wih he minimal posiive fundamenal soluion of he hea equaion u = Δu on R +. Besides, he hea kernel saisfies he following properies. symmery: p x, y = p y, x. he semigroup ideniy: p +s x, y = p x, y dμ y 1. p x, z p s z, y dμ z. 1 Recall ha in R n wih he Lebesgue measure μ, Δ is he classical Laplace operaor Δ = n k=1, and is hea kernel is given by he Gauss-Weiersrass formula 2 x 2 k p x, y = 1 4π n/2 exp x y 2. 4 Explici formulas for he hea kernel exis also in hyperbolic spaces H n when μ is he Riemannian measure. For example in H 3 p x, y = 1 4π 3/2 r sinh r exp r For arbirary H n he formula looks complicaed, bu i implies he following esimae, for all > 0 and x, y H n : p x, y n r r exp λ r2 n/2 4 λr, 3 where λ = n 12 4 is he boom of he specrum of he Laplace operaor on H n. 2
3 2 Uniform Faber-Krahn inequaliy Le, μ be a weighed manifold. For any relaively compac open se Ω, denoe by λ 1 Ω he smalles eigenvalue of he weak Dirichle problem for Δ in Ω. Le Λ be a funcion on 0, +. We say ha a weighed manifold, μ saisfies he uniform Faber-Krahn inequaliy wih funcion Λ if, for any non-empy relaively compac open se Ω, λ 1 Ω Λ μ Ω. 4 For example, R n saisfies he Faber-Krahn inequaliy wih funcion Λ v = cv 2/n. Also, any aran-hadamard manifold of dimension n saisfies he Faber- Krahn inequaliy wih he same funcion Λ bu possibly wih a differen consan c. If K is a k-dimensional compac manifold hen he Riemannian produc = R m K saisfies he Faber-Krahn inequaliy wih funcion { v Λ v = c 2/n, v 1, v 2/m 5, v 1, where n = dim = k + m. Any n-dimensional manifold wih bounded geomery saisfies he Faber-Krahn inequaliy wih he funcion { v Λ v = c 2/n, v 1, v 2 6, v 1. Theorem 1 Assume ha, μ saisfies he Faber-Krahn inequaliy 4 wih a posiive coninuous decreasing funcion Λ such ha dv <. 7 vλ v 0 Then, for all > 0, sup p x, x 4 x γ/2, 8 where he funcion γ is defined by he ideniy = γ 0 dv vλv. 9 Approach o he proof. Assuming ha 4 holds, one deduces he following Nash ype inequaliy: for any non-zero funcion u D, 2 u 2 dμ 1 ε u 2 L 2Λ u 2 L 1, 10 ε u 2 L 2 for any ε 0, 1. Then one applies Nash s argumen: exending 10 o u = p x, and noicing ha u 2 dμ = uδudμ = 1 d 2 d u 2 L 11 2 and u L 1 1, one obains from 10 and 11 a differenial inequaliy for u 2 L 2 = p 2 x, x, whence he resul follows. 3
4 3 Gaussian upper bounds Fix some value D 0, + ] and consider he following weighed inegral of he hea kernel: d E, x := p 2 2 x, z x, z exp dμz. 12 D A priori, he value of E, x may be +. For example, in R n E, x = if D 2. Lemma 2 For all x, y, > 0, he following inequaliy holds p x, y E/2, xe/2, y exp d2 x, y. 13 Proof. For any poins x, y, z, le us denoe α = dy, z, β = dx, z and γ = dx, y. By he riangle inequaliy, α 2 + β γ2. y γ α x β z Figure 1: We have hen p x, y = p /2 x, zp /2 y, zdμz p /2 x, ze β2 D p/2 y, ze α2 D e γ2 dμz which was o be proved. p 2 /2x, ze 2β2 D dμz 1 2 = E/2, xe/2, y exp d2 x, y 1 p 2 /2y, ze 2α2 2 D dμy e γ2 Lemma 3 If D 2 hen for any x, he funcion E, x is decreasing in. In paricular, if E, x < for some = 0 hen E, x < for all > 0. Approach o he proof. The proof of he monooniciy of E, x amouns o verifying ha is ime derivaive is non-posiive. I is essenial for he proof ha d x, 1, which implies ha he funcion ξ, x = d2 x,y saisfies D, ξ + D 4 ξ
5 Theorem 4 Assume ha, for some x and for all > 0, p x, x γ, 15 where γ is an increasing posiive funcion on R + saisfying he doubling condiion: γ 2 Aγ for all > 0 16 for some consan A > 1. Then, for any D > 2 and all > 0, for some ε = ε D > 0 and = A,, D. E, x γε, 17 By puing ogeher Theorem 4 and Lemma 2, we obain he following resul. orollary 5 Assume ha, for some poins x, y and for all > 0, p x, x γ 1 and p y, y γ 2, 18 where γ 1 and γ 2 are increasing posiive funcion on R + boh saisfying 16. Then, for any D > 2 and all > 0, p x, y γ1 εγ 2 ε exp d2 x, y. 19 orollary 6 On any weighed manifold, μ and for any D > 2, E, x is finie for all > 0, x. oreover, he funcion E, x is coninuous and monoone decreasing. Skech of proof. By Theorem 4 and Lemma 3, i suffices o prove ha for any x here exis posiive consans and T such ha p x, x n/2, for all 0 < < T, 20 where n = dim. Fix a small relaively compac open se Ω conaining he poin x. By compacness argumen, he weighed manifold Ω, μ saisfies he following Faber-Krahn inequaliy: for all open ses U Ω, such ha μ U 1 2 μ Ω, λ 1 U cμ U 2/n, where c > 0 depends on Ω. Hence, by a sligh modificaion of Theorem 1, we obain ha he hea kernel p Ω of Ω, μ saisfies he esimae p Ω x, x n/2, for all 0, T, 5
6 where and T depend on Ω. onsider he funcion u, y = p x, y p Ω x, y and exend i o 0 by seing u, y 0. This funcion saisfies in R Ω he equaion u = Δu and hence i is -smooh in R Ω. In paricular, he funcion u, x is bounded on [0, T ], say u, x. Then we obain, for all 0 < < T, whence 20 follows. p x, x = p Ω x, x + u, x n/2 +, Theorem 7 On any weighed manifold, μ and for any D > 2, here exiss a posiive coninuous funcion Φ, x on R +, which is decreasing in and such ha he following inequaliy holds p x, y Φ, xφ, y exp λ min d2 x, y, 21 for all x, y and > 0, where λ min is he boom of he specrum of Δ on. Proof. Le us firs se Φ, x = E 1, x By orollary 6, his funcion is finie. By Lemma 3, he funcion Φ, x is decreasing in. By Lemma 2, we obain p x, y Φ, xφ, y exp d2 x, y. 23 This esimaes sill does no mach 21 because of he lack of he erm λ min. To handle i, le us find a posiive smooh funcion h saisfying on he equaion Δh + λh = 0 where λ = λ min. onsider he measure μ defined by d μ = h 2 dμ and he hea kernel p on he weighed manifold, μ. Applying 23 on, μ, we obain ha here exiss a funcion Φ, x decreasing in such ha p x, y Φ, x Φ, y exp Using he relaion beween he hea kernels d2 x, y p x, y = p x, yhxhye λ, and 24, we obain 21 wih Φ, x = Φ, xh x.. 24 Remark. As i follows from he consrucion of he funcion Φ, x and from he proof of orollary 6, for any compac se K here exis posiive consans and T such ha Φ, x n/4 for all x K and 0 < < T. 25 6
7 4 ean-value propery Here we presen an alernaive mehod of obaining Gaussian upper bounds, which avoids using E, x and, insead, is based on a cerain inegral esimae of he hea kernel and he mean-value propery. The following heorem shows ha he Gaussian exponenial erm appears naurally in he hea kernel upper esimaes on arbirary manifolds. Theorem 8 Le, μ be a weighed manifold and le A and B be wo μ-measurable ses on. Then p x, ydμxdμy μaμb exp d2 A, B, 26 4 A B where da, B is he geodesic disance beween ses A and B. To obain poinwise bounds from 26 one needs o combine i wih a mean-value propery. Definiion. We say ha he manifold admis he mean-value propery V if, for all > τ > 0, x and for any posiive soluion us, η of he hea equaion in he cylinder τ, ] Bx, τ, we have u, x τv x, τ τ Bx, τ us, zdμzds. 27 s,x u= u - -,x x _ Bx, Figure 2: Theorem 9 Assume ha he mean-value propery V holds on he manifold. Then, for all x and > 0, p x, x 7 V x,. 28
8 oreover, for all x, y, > 0, D > 2, p x, y V x, /2V y, /2 exp d2 x, y. 29 Theorem 9 admis a localized version. We say ha he manifold admis a resriced mean-value propery V xyτ 0, for some x, y and τ 0 R +, if he inequaliy 27 holds for all τ 0, τ 0 ] in each of he balls B x, τ and B y, τ. If admis V xyτ 0 hen similarly o he above heorem we obain p x, y V x, τv y, τ exp d2 x, y where τ = min/2, τ 0. Observe ha he propery V xyτ 0 holds on any manifold: for any given x, y, here exiss τ 0 such ha V xyτ 0 is rue. However, he consan in he mean-value inequaliy 27 depends on he cerain geomeric properies of he balls Bx, τ 0 and By, τ 0. Definiion. We say ha a weighed manifold, μ saisfies he volume doubling propery if, for all x and r > 0, V x, 2r V x, r. 30 I is known ha he volume doubling condiion implies he volume comparison condiion: for all 0 < r < R and x, V x, R V x, r N R, 31 r wih some N > 0. Assuming 31, one can improve he esimae 29 as follows. Theorem 10 Assume ha, μ saisfies he mean-value propery V and he volume comparison 31. Then, for all x, y and > 0, p x, y where d = dx, y. V x, V y, 1 + d N 1 exp d2 4 Noe for comparison ha on S n he hea kernel a he poles x, y admis he esimae p x, y c 1 + d n 1 exp d2, 0, n/2 4 which shows he sharpness of
9 5 Relaive Faber-Krahn inequaliy Le, μ be a geodesically complee weighed manifold. Definiion. We say ha, μ saisfies he relaive Faber-Krahn inequaliy if here exis posiive consans δ, c such ha, for any geodesic ball B x, r on and for any non-empy relaively compac open se Ω B x, r, λ 1 Ω c r 2 V x, r μ Ω δ. 33 For example, he relaive Faber-Krahn inequaliy holds in R n wih δ = 2/n since V x, r = cr n and hence 33 amouns o he uniform Faber-Krahn inequaliy 4 wih Λ v = cv 2/n. Theorem 11 If has non-negaive Ricci curvaure and μ is he Riemannian volume hen, μ saisfies he relaive Faber-Krahn inequaliy. Approach o he proof. The following key propery of manifolds of nonnegaive Ricci curvaure is used in he proof of his heorem. For any x, y le γ x,y : [0, L] be a shores geodesic beween x and y, where L = d x, y, γ x,y 0 = x and γ x,y L = y. For any x and 0 < s < 1, define a homohey Γ x s : by Γ x s y = γ x,y sl. Γ x s A A x y Γ x s y Figure 3: Homohey Γ x s Then here exiss c > 0 such ha for any 1 2 s 1 and any Borel se A, μ Γ x s A cμ A. 34 Furhermore, if a homohey wih he propery 34 can be defined on some manifold, μ hen his manifold saisfies he relaive Faber-Krahn inequaliy. The class of weighed manifolds wih he relaive Faber-Krahn inequaliy is much wider han hose wih non-negaive Ricci curvaure. In paricular, his class is sable under quasi-isomery. Anoher example of sabiliy: a conneced sum of k copies of he same manifold saisfying he relaive Faber-Krahn inequaliy also saisfies he relaive Faber-Krahn inequaliy. 9
10 Theorem 12 The relaive Faber-Krahn inequaliy implies he volume doubling and he mean value propery. ombining wih Theorem 9 or 10, we obain hea kernel bounds under he relaive Faber-Krahn inequaliy. Theorem 13 The following condiions are equivalen: a, μ saisfies he relaive Faber-Krahn inequaliy. b, μ saisfies he volume doubling propery and he hea kernel on, μ admis he esimae p x, x V x,, 35 for all x and > 0. c, μ saisfies he volume doubling propery and he hea kernel on, μ admis he esimae p x, y V x, exp c d2 x, y, 36 for all x, y and > 0. The consan c in he exponenial in 36 can be made arbirarily close o 1. In 4 fac, i can be aken exacly 1 a he expense of addiional facors as in he following 4 saemen. Theorem 14 Le, μ saisfy he relaive Faber-Krahn inequaliy. addiion ha for some N > 0 and for all 0 < r < R and x, Assume in Then, for all x, y and > 0, p x, y V x, V y, V x, R V x, r 1 + N R. 37 r N 1 d x, y exp d x, y Noe ha he volume comparison 37 follows from he relaive Faber-Krahn inequaliy 33 wih N = 2 δ. However, N in 37 does no have o be 2 δ. 10
11 6 On-diagonal lower esimae The following resul allows o obain an on-diagonal lower bound from an upper bound. Theorem 15 Assume ha for some poin x, V x, 2r V x, r for all r > 0 and Then, for all > 0, p x, x V x,, for all > 0. c p x, x V x,. 39 orollary 16 The following condiions are equivalen: a, μ saisfies he relaive Faber-Krahn inequaliy. b The hea kernel on, μ saisfies he esimaes p x, y V x, exp c d2 x, y. 40 for all x, y and > 0, and p x, x c V x,, 41 /2 for all x and > 0. orollary 17 If has non-negaive Ricci curvaure and μ is he Riemannian volume hen he hea kernel on, μ saisfies he upper bounds 36, 38 and he lower bound Harnack inequaliy and Li-Yau esimae In his secion we assume ha, μ is a geodesically complee weighed manifold. We say ha he hea kernel on, μ saisfies he Li-Yau esimae if, for all x, y and > 0, p x, y V x, exp c d2 x, y. 42 P. Li and S.-T. Yau proved his esimae on geodesically complee Riemannian manifolds wih non-negaive Ricci curvaure using he gradien esimaes see Theorem 22 below. 11
12 We say ha, μ saisfies he uniform parabolic Harnack inequaliy if, for any ball B z, r on and for any posiive soluion u, x of he hea equaion in he cylinder = 0, r 2 B z, r, he following holds: sup u, x inf u, x + where = 1 4 r2, 1 2 r2 B z, 1 2 r and + = 3 4 r2, r 2 B z, 1 2 r. r 2 3 /4r /2r 2 1 /4r 2-0 Bz, 1 /2r Bz,r Figure 4: ylinders + and I is well known ha he Harnack inequaliy holds for uniformly parabolic equaions in R n. The relaion o hea kernels is given by he following saemen. Theorem 18 A manifold, μ saisfies he Li-Yau esimae if and only if i saisfies he uniform Harnack inequaliy. To characerize manifolds wih he Harnack inequaliy, we need one more noion. We say ha a weighed manifold saisfies he weak Poincaré inequaliy if here exiss ε 0, 1 such ha for any ball B z, r and for any funcion u 1 B z, r, u s 2 dμ r 2 u 2 dμ. 43 inf s R Bz,εr The erm weak refers here o he facor ε < 1. Bz,r Theorem 19 A manifold, μ saisfies he Harnack inequaliy if and only if i saisfies he doubling volume propery and he Poincaré inequaliy. Hence, he Li-Yau esimae holds if and only if he doubling volume propery and he Poincaré inequaliy hold. Theorem 19 admis a localized version: Harnack inequaliy holds in all balls of radii R if and only if he doubling volume propery and Poincaré inequaliy hold in all balls of radii R. The proof of Theorem 19 uses he following resul, which is of is own ineres. 12
13 Theorem 20 If, μ saisfies he Poincaré inequaliy and he volume doubling propery hen i saisfies he relaive Faber-Krahn inequaliy. Noe ha he converse o Theorem 20 is no rue: i is possible o show ha a conneced sum of wo copies of R n, n 3, saisfies he relaive Faber-Krahn inequaliy bu no he Poincaré inequaliy. Using orollary 16, we obain ha he Poincaré inequaliy and he doubling volume propery imply he upper bound and he on-diagonal lower bound in 42. The off-diagonal lower bound requires addiional ools, which we do no ouch here and which are similar o oser s original proof of he Harnack inequaliy in R n. onnecion o he Ricci curvaure comes from he following saemen. Theorem 21 If has non-negaive Ricci curvaure and μ is he Riemannian volume hen, μ saisfies he Poincaré inequaliy and he volume doubling propery. In fac, boh Poincaré inequaliy and volume doubling propery come from he propery 34 of he homohey on such manifolds. learly, Theorems 21 and 20 imply Theorem 11. Successive applicaion of Theorems 21, 19, and 18 yields he following resul. Theorem 22 If has non-negaive Ricci curvaure and μ is he Riemannian volume hen he hea kernel on, μ saisfies he Li-Yau esimae 42. The above resuls are schemaically presened on he diagram: Homohey propery = Ricci 0 = Gradien esimaes Vol doubling & Poincaré Harnack inequaliy p x, y exp Relaive Faber-Krahn inequaliy Vol doubling & V inequaliy p x, y exp c p x, x V x, Vol doubling c d2 x,y V x, c d2 x,y V x, 8 Esimaes of derivaives of he hea kernel Fix some D 2, + ] and consider again he quaniy d E, x = p 2 2 x, y x, y exp dμy, D as well as E 1, x = d p 2 2 x, y x, y exp dμy D 13
14 and E 2, x = d Δp 2 2 x, y x, y exp dμy D where boh operaors and Δ ac on he variable y. ore generally, se d E n, x = n p 2 2 x, y x, y exp dμy D where { Δ n n/2, n even, = Δ n 1 2, n odd. The quaniy E n can be used o obain poinwise esimaes for he ime derivaive of he hea kernel. The following inequaliy is similar o Lemma 2. Lemma 23 For all x, y and > 0, we have n p x, y n E 2n /2, xe/2, y exp Approach o proof. Using he semigroup ideniy p x, y = p s x, zp s y, zdμz, we obain n n p x, y = = d2 x, y. n n p sx, zp s y, zdμz Δ n z p s x, zp s y, zdμz. Taking s = /2 and using auchy-schwarz inequaliy as in Lemma 2, we finish he proof. This mehod does no work for esimaing x p x, y as we would need z under he inegral. However, if one knows a priori ha x p x, z z p x, z hen one can obain in he same way a poinwise esimae for x p x, y. Our nex purpose is o obain he esimaes for E n, x. Theorem 24 For any x, he funcion E n x, is a finie, coninuous, and decreasing as long as D > 2. Theorem 25 Assume ha, for some x and all 0, T E x, 1 f 14
15 where f is some posiive L 1 loc funcion on 0, T. Define a funcion f n on 0, T by inducion as follows: f 0 = f, f n+1 = 0 f n τ dτ. Then, for all 0, T, where c = D 2 D/2+8. E n x, c n f n In fac, f n can be defined explicily by f n = For example, if f = α hen f n = n α+n. 0 τ n 1 f τ dτ. n 1! orollary 26 If, μ saisfies he relaive Faber-Krahn inequaliy 33 hen for all x, y and > 0 N+n+1 n p 1 + dx,y d x, y2 n x, y V n x, V y, exp, 4 where N is he exponen of he volume comparison condiion
arxiv: 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 informationConvergence 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 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 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 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 informationOFF-DIAGONAL UPPER ESTIMATES FOR THE HEAT KERNEL OF THE DIRICHLET FORMS ON METRIC SPACES
OFF-DIAGONAL UPPER ESTIMATES FOR THE HEAT KERNEL OF THE DIRIHLET FORMS ON METRI SPAES ALEXANDER GRIGOR YAN AND JIAXIN HU Absrac We give equivalen characerizaions for off-diagonal upper bounds of he hea
More informationBOUNDEDNESS 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 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 informationCourse Notes for EE227C (Spring 2018): Convex Optimization and Approximation
Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3
More informationEXERCISES FOR SECTION 1.5
1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler
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 informationOptimality Conditions for Unconstrained Problems
62 CHAPTER 6 Opimaliy Condiions for Unconsrained Problems 1 Unconsrained Opimizaion 11 Exisence Consider he problem of minimizing he funcion f : R n R where f is coninuous on all of R n : P min f(x) x
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 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 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 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 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 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 information15. Vector Valued Functions
1. Vecor Valued Funcions Up o his poin, we have presened vecors wih consan componens, for example, 1, and,,4. However, we can allow he componens of a vecor o be funcions of a common variable. For example,
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 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 informationA sphere theorem on locally conformally flat even-dimensional manifolds
A sphere heorem on locally conformally fla even-dimensional manifol Giovanni CATINO a, Zindine DJADLI b and Cheikh Birahim NDIAYE c a Universià di Pisa - Diparimeno di aemaica Largo Bruno Ponecorvo, 5
More informationt 2 B F x,t n dsdt t u x,t dxdt
Evoluion Equaions For 0, fixed, le U U0, where U denoes a bounded open se in R n.suppose ha U is filled wih a maerial in which a conaminan is being ranspored by various means including diffusion and convecion.
More informationFinish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!
MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his
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 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 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 informationNEW APPROACH TO DIFFERENTIAL EQUATIONS WITH COUNTABLE IMPULSES
1 9 NEW APPROACH TO DIFFERENTIAL EQUATIONS WITH COUNTABLE IMPULSES Hong-Kun ZHANG Jin-Guo LIAN Jiong SUN Received: 1 January 2007 c 2006 Springer Science + Business Media, Inc. Absrac This paper provides
More informationLecture 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 informationCHAPTER 2 Signals And Spectra
CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par
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 information6. Stochastic calculus with jump processes
A) Trading sraegies (1/3) Marke wih d asses S = (S 1,, S d ) A rading sraegy can be modelled wih a vecor φ describing he quaniies invesed in each asse a each insan : φ = (φ 1,, φ d ) The value a of a porfolio
More informationClass Meeting # 10: Introduction to the Wave Equation
MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion
More informationGuest Lectures for Dr. MacFarlane s EE3350 Part Deux
Gues Lecures for Dr. MacFarlane s EE3350 Par Deux Michael Plane Mon., 08-30-2010 Wrie name in corner. Poin ou his is a review, so I will go faser. Remind hem o go lisen o online lecure abou geing an A
More informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
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 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 information( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is
UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires
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 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 informationThe Poisson Equation and Hermitian-Einstein Metrics on Holomorphic Vector Bundles over Complete Noncompact Kähler Manifolds
The Poisson Equaion and Hermiian-Einsein Merics on Holomorphic Vecor Bundles over Complee Noncompac Kähler Manifolds LEI NI ABSTRACT. Auhor: Please supply an absrac. 1. INTRODUCTION The exisence of Hermiian-Einsein
More informationPOSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE
Urainian Mahemaical Journal, Vol. 55, No. 2, 2003 POSITIVE AND MONOTONE SYSTEMS IN A PARTIALLY ORDERED SPACE A. G. Mazo UDC 517.983.27 We invesigae properies of posiive and monoone differenial sysems wih
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 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 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 informationSolutions to Assignment 1
MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we
More informationLIPSCHITZ RETRACTIONS IN HADAMARD SPACES VIA GRADIENT FLOW SEMIGROUPS
LIPSCHITZ RETRACTIONS IN HADAMARD SPACES VIA GRADIENT FLOW SEMIGROUPS MIROSLAV BAČÁK AND LEONID V KOVALEV arxiv:160301836v1 [mahfa] 7 Mar 016 Absrac Le Xn for n N be he se of all subses of a meric space
More informationOmega-limit sets and bounded solutions
arxiv:3.369v [mah.gm] 3 May 6 Omega-limi ses and bounded soluions Dang Vu Giang Hanoi Insiue of Mahemaics Vienam Academy of Science and Technology 8 Hoang Quoc Vie, 37 Hanoi, Vienam e-mail: dangvugiang@yahoo.com
More informationEngineering Letter, 16:4, EL_16_4_03
3 Exisence In his secion we reduce he problem (5)-(8) o an equivalen problem of solving a linear inegral equaion of Volerra ype for C(s). For his purpose we firs consider following free boundary problem:
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 information5.1 - Logarithms and Their Properties
Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We
More information1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.
. Use Simpson s rule wih n 4 o esimae an () +. Soluion: Since we are using 4 seps, 4 Thus we have [ ( ) f() + 4f + f() + 4f 3 [ + 4 4 6 5 + + 4 4 3 + ] 5 [ + 6 6 5 + + 6 3 + ]. 5. Our funcion is f() +.
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 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 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 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 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 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 informationCHERNOFF DISTANCE AND AFFINITY FOR TRUNCATED DISTRIBUTIONS *
haper 5 HERNOFF DISTANE AND AFFINITY FOR TRUNATED DISTRIBUTIONS * 5. Inroducion In he case of disribuions ha saisfy he regulariy condiions, he ramer- Rao inequaliy holds and he maximum likelihood esimaor
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 informationarxiv: v1 [math.dg] 7 Nov 2018
A STOCHASTIC APPROACH TO COUNTING PROBLEMS. ADRIEN BOULANGER arxiv:8.02899v [mah.dg] 7 Nov 208 Absrac. We sudy orbial funcions associaed o finiely generaed Kleinian groups acing on he hyperbolic space
More informationMATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018
MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren
More information23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes
Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion
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 informationMA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions
MA 14 Calculus IV (Spring 016) Secion Homework Assignmen 1 Soluions 1 Boyce and DiPrima, p 40, Problem 10 (c) Soluion: In sandard form he given firs-order linear ODE is: An inegraing facor is given by
More information6.2 Transforms of Derivatives and Integrals.
SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.
More informationarxiv: v1 [math.dg] 21 Dec 2007
A priori L -esimaes for degenerae complex Monge-Ampère equaions ariv:07123743v1 [mahdg] 21 Dec 2007 P Eyssidieux, V Guedj and A Zeriahi February 2, 2008 Absrac : We sudy families of complex Monge-Ampère
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 information(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)
Phase Plane Analysis of Linear Sysems Adaped from Applied Nonlinear Conrol by Sloine and Li The general form of a linear second-order sysem is a c b d From and b bc d a Differeniaion of and hen subsiuion
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 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 informationSome New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations
Annals of Pure and Applied Mahemaics Vol. 6, No. 2, 28, 345-352 ISSN: 2279-87X (P), 2279-888(online) Published on 22 February 28 www.researchmahsci.org DOI: hp://dx.doi.org/.22457/apam.v6n2a Annals of
More informationChapter 8 The Complete Response of RL and RC Circuits
Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior
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 informationUndetermined coefficients for local fractional differential equations
Available online a www.isr-publicaions.com/jmcs J. Mah. Compuer Sci. 16 (2016), 140 146 Research Aricle Undeermined coefficiens for local fracional differenial equaions Roshdi Khalil a,, Mohammed Al Horani
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 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 information4.1 - Logarithms and Their Properties
Chaper 4 Logarihmic Funcions 4.1 - Logarihms and Their Properies Wha is a Logarihm? We define he common logarihm funcion, simply he log funcion, wrien log 10 x log x, as follows: If x is a posiive number,
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 informationDIFFERENTIAL GEOMETRY HW 5
DIFFERENTIAL GEOMETRY HW 5 CLAY SHONKWILER 3. Le M be a complee Riemannian manifold wih non-posiive secional curvaure. Prove ha d exp p v w w, for all p M, all v T p M and all w T v T p M. Proof. Le γ
More informationMath Final Exam Solutions
Mah 246 - Final Exam Soluions Friday, July h, 204 () Find explici soluions and give he inerval of definiion o he following iniial value problems (a) ( + 2 )y + 2y = e, y(0) = 0 Soluion: In normal form,
More informationLECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS
LECTURE : GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS We will work wih a coninuous ime reversible Markov chain X on a finie conneced sae space, wih generaor Lf(x = y q x,yf(y. (Recall ha q
More informationCOUPLING IN THE HEISENBERG GROUP AND ITS APPLICATIONS TO GRADIENT ESTIMATES
COUPLING IN THE HEISENBERG GROUP AND ITS APPLICATIONS TO GRADIENT ESTIMATES SAYAN BANERJEE, MARIA GORDINA, AND PHANUEL MARIANO Absrac. We consruc a non-markovian coupling for hypoellipic diffusions which
More informationA combinatorial trace formula
A combinaorial race formula F. R. K. Chung Universiy of Pennsylvania Philadelphia, Pennsylvania 1914 S.-T. Yau Harvard Universiy Cambridge, Massachuses 2138 Absrac We consider he race formula in connecion
More informationHamilton Jacobi equations
Hamilon Jacobi equaions Inoducion o PDE The rigorous suff from Evans, mosly. We discuss firs u + H( u = 0, (1 where H(p is convex, and superlinear a infiniy, H(p lim p p = + This by comes by inegraion
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 informationDifferential Equations
Mah 21 (Fall 29) Differenial Equaions Soluion #3 1. Find he paricular soluion of he following differenial equaion by variaion of parameer (a) y + y = csc (b) 2 y + y y = ln, > Soluion: (a) The corresponding
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 informationNotes for Lecture 17-18
U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up
More informationFirst-Order Recurrence Relations on Isolated Time Scales
Firs-Order Recurrence Relaions on Isolaed Time Scales Evan Merrell Truman Sae Universiy d2476@ruman.edu Rachel Ruger Linfield College rruger@linfield.edu Jannae Severs Creighon Universiy jsevers@creighon.edu.
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 informationOn Carlsson type orthogonality and characterization of inner product spaces
Filoma 26:4 (212), 859 87 DOI 1.2298/FIL124859K Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Carlsson ype orhogonaliy and characerizaion
More informationRepresentation of Stochastic Process by Means of Stochastic Integrals
Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of
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 informationDini derivative and a characterization for Lipschitz and convex functions on Riemannian manifolds
Nonlinear Analysis 68 (2008) 1517 1528 www.elsevier.com/locae/na Dini derivaive and a characerizaion for Lipschiz and convex funcions on Riemannian manifolds O.P. Ferreira Universidade Federal de Goiás,
More informationSTABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS
Elecronic Journal of Differenial Equaions, Vol. 217 217, No. 118, pp. 1 14. ISSN: 172-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS
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 informationPoincare Inequality for Weighted First Order Sobolev Spaces on Loop Spaces
Journal of Funcional Analysis 185, 527563 (2001) doi:10.1006jfan.2001.3775, available online a hp:www.idealibrary.com on Poincare Inequaliy for Weighed Firs Order Sobolev Spaces on Loop Spaces Fuzhou Gong
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 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 information