ORTHOGONALITY IN S 1 AND S SPACES AND NORMAL DERIVATIONS

Size: px
Start display at page:

Download "ORTHOGONALITY IN S 1 AND S SPACES AND NORMAL DERIVATIONS"

Transcription

1 J. OPERATOR THEORY 51(2004), c Copyrigh by Thea, 2004 ORTHOGONALITY IN S 1 AND S SPACES AND NORMAL DERIVATIONS DRAGOLJUB J. KEČKIĆ Communicaed by Florian-Horia Vasilescu Absrac. We inroduce ϕ-gaeaux derivaive, and use i o give he necessary and sufficien condiions for he operaor Y o be orhogonal (in he sense of James) o he operaor X, in boh spaces S 1 and S (nuclear and compac operaors on a Hilber space). Furher, we apply hese resuls o prove ha here exiss a normal derivaion A such ha ran A ker A S 1, and a relaed resul concerning S. Keywords: Gaeaux derivaive, orhogonaliy in Banach spaces, Schaen ideals, derivaion, elemenary operaor. MSC (2000): Primary 46G05, 47B10, 47B47; Secondary 47A30, 46B INTRODUCTION Le H denoe a separable Hilber space, and le S p denoe he Schaen ideal of ( + ) 1/p hose compac operaors X acing on H such ha X p = s (X) p < +, where s (X) = λ (X X) 1/2. Also, le S denoe he ideal of all compac operaors equipped wih he usual norm. Le us recall ha hese (Schaen) norms are special cases of so called uniarily invarian norms, associaed wih some wosided ideal of compac operaors. For furher deails he reader is referred o [6]. I is well known ha S 2 has a Hilber space srucure, wih he inner produc X, Y = r (XY ), and ha his is no rue in oher S p. Neverheless, in all Banach spaces we can define he orhogonaliy in he following way (orhogonaliy in he sense of R.C. James). =1

2 90 Dragolub J. Kečkić Definiion 0.1. Le X be a Banach space. We say ha y X is orhogonal o x X if for all complex numbers λ here holds (0.1) x + λy x. Remark 0.2. If X is a Hilber space, hen from (0.1) we can easily derive x, y = 0. Remark 0.3. In Banach spaces, orhogonaliy from he previous definiion is no symmerical, i.e. y orhogonal o x does no imply x orhogonal o y. Remark 0.4. Definiion 0.1 has a naural geomeric inerpreaion. Namely, y x if and only if he complex line {x + λy : λ C} is disoin wih he open ball K(0, x ), i.e. if and only if his complex line is a angen one. Such an orhogonaliy relaion is closely relaed wih Gaeaux derivaive of he norm and he smoohness of he sphere of radius x. Definiion 0.5. The vecor x is a smooh poin of he sphere S(0, x ) if here exiss a unique suppor funcional F x X, such ha F x (x) = x and F x = 1. Proposiion 0.6. If here exiss he Gaeaux derivaive of he norm a he poin x, i.e. if here exiss he i = 0, hen i is equal o R 0 x+y x Re F x (y), where F x is he funcional from he previous definiion. Moreover, in his case y is orhogonal o x if and only if F x (y) = 0. I is also well known ha if Banach space X has a sricly convex dual space hen every nonzero poin is a smooh poin of he corresponding sphere. For deails see [1] and references herein. Orhogonaliy in he sense of James were used in invesigaion of so called elemenary operaors, inroduced by Lumer and Rosenblum ([11]). Definiion 0.7. Le (A 1, A 2,..., A n ) and (B 1, B 2,..., B n ) be he n-uples of bounded Hilber space operaors. The mapping X o B(H) is called he elemenary operaor or elemenary mapping. n =1 A XB from B(H) Remark 0.8. The same name elemenary operaors is used for operaors of he same form, which maps J o J, where J is some wo sided ideal equipped wih a uniarily invarian norm. The firs resul concerning he orhogonaliy in he sense of James and elemenary operaors was given by Anderson ([2]).

3 Orhogonaliy in S 1 and S 91 Proposiion 0.9. If A is a normal operaor on a separable Hilber space H, hen AS = SA implies ha for all bounded X here holds AX XA + S S. In view of Definiion 0.1, i means ha he range of he mappings A : B(H) B(H), A (X) = AX XA is orhogonal o is kernel. This resul has been generalized in wo direcions, by exending he class of elemenary mappings, and by exending his inequaliy o he oher uniarily invarian norms; see for insance [4], [5], [8], [9]. In [2], Anderson also proved ha equaliy ran A ker A = B(H) is rue in very special cases, for example if and only if he specrum of he normal operaor A in Proposiion 0.9 is finie. In [8] here was conecured ha i migh be J = ran A J ker A J if he ideal J is separable. In Secion 3, we shall give he negaive answer o his hypohesis. The Gaeaux derivaive echnique was used in [3], [10] and [12], in order o characerize hose operaors o which he range of a derivaion is orhogonal. In hese papers, he aenion was direced o S p ideals for some p > 1, and o smooh poins in S 1 and S, like in he following proposiion, aken from [10]. Proposiion Le A be a bounded Hilber space operaor. The range of a derivaion A is orhogonal o an operaor S in S p if and only if A S = SA, where S = U S p 1, and S = U S. Smooh poins in S 1 and S, were characerized by Holub ([7]). Proposiion The operaor X is a smooh poin of he corresponding sphere in S 1 if and only if eiher X is inecive or X is inecive. The operaor X is a smooh poin of he corresponding sphere in S if and only if i aains is norm a he unique vecor (up o a complex scalar). The main purpose of his noe is o characerize he orhogonaliy in he sense of James in S 1 and S a he poins which are no smooh, and o apply hese characerizaions o elemenary operaors. Namely, among oher hings, we prove ha for a normal derivaion A : S p S p here holds ran A ker A = S p for 1 < p < +, and ha such compleeness resul fails for p = 1. In he case p = + he siuaion is more complicaed. Some resuls concerning more general elemenary operaors are also given.

4 92 Dragolub J. Kečkić 1. ϕ-gateaux DERIVATIVES In his secion we inroduce ϕ-gaeaux derivaive and, in Theorem 1.4, we give he necessary and sufficien condiion for a vecor y from an arbirary Banach space o be orhogonal (in he sense of James) o a vecor x, in erms of inroduced ϕ-gaeaux derivaive. Definiion 1.1. Le (X, ) be an arbirary Banach space. ϕ-gaeaux derivaive of he norm a he poin x, and in y-direcion is x + e iϕ y x D ϕ,x (y) =. 0 + Proposiion 1.2. (i) The funcion α x,y () = x + e iϕ y is convex. (ii) D ϕ,x (y) is he righ derivaive of he funcion α x,y a he poin 0, and aking ino accoun (i) D ϕ,x (y) always exiss. Proof. Obvious. Proposiion 1.3. (i) D ϕ,x is subaddiive, posiively homogeneous funcional on X; (ii) D ϕ,x (e iθ y) = D ϕ+θ,x (y); (iii) D ϕ,x (y) y. Proof. (i) We have x + e iϕ (y 1 + y 2 ) x 2 + eiϕ y 1 + x, 2 + eiϕ y 2 and, by aking a i we obain D ϕ,x (y 1 + y 2 ) = 0 + x + e iϕ (y 1 + y 2 ) x 0 + x + 2e iϕ y 1 + x + 2e iϕ y 2 2 x 2 = D ϕ,x (y 1 ) + D ϕ,x (y 2 ), which proves he subaddiiviy. Posiive homogeneiy is obvious. (ii) Obvious. (iii) I is enough o see ha x + e iϕ y x x + e iϕ y x = y. The previous simple consrucion allows us o characerize he orhogonaliy in he sense of James, in all Banach spaces (wihou care of smoohness) via ϕ- Gaeaux derivaive. Theorem 1.4. The vecor y is orhogonal o x in he sense of James if and only if inf ϕ D ϕ,x(y) 0. Proof. Le us firs prove he only if par of he saemen. Indeed, le y be orhogonal o x in he sense of James, i.e. le for all λ C here holds x + λy x. 0 for all > 0, and passing o he i we ge D ϕ,x (y) 0 for an arbirary ϕ. Then x+eiϕ y x

5 Orhogonaliy in S 1 and S 93 Le us, now, prove he oher, if, par of he saemen. We have D ϕ,x (e i(π ϕ) x + e iϕ e i(π ϕ) x x 1 1 x) = = x = x From his, and from subaddiiviy we ge x = D ϕ,x (e i(π ϕ) x) D ϕ,x (µy) D ϕ,x (e i(π ϕ) x) D ϕ,x (µy e i(π ϕ) x) µy e i(π ϕ) x = x + µ( e i(ϕ π) )y = x + λy, if we ake µ = e i(π ϕ) λ. Remark 1.5. We can see ha he previous heorem is reasonable if we look a i from an oher aspec. Namely, y is orhogonal o x if and only if he convex funcion α x,y () aains is minimum a he origin. We conclude his secion wih wo examples concerning wo classical Banach spaces. Example 1.6. In he space L 1 (X, µ) he funcion g is orhogonal o f, in he sense of James if and only if e iθ() g() dµ() g() dµ(), {f 0} {f=0} where f() = f() e iθ(). Indeed, in he L 1 space here holds { } D ϕ,f (g) = Re e iϕ e iθ() g() dµ() + g() dµ(), since {f 0} f() + ρe iϕ g() f() = ρ 0 + ρ (here g() = g() e iψ() ), and also f()+ρeiϕ g() f() ρ g f if and only if inf ϕ Re { {f 0} } e iϕ e iθ() g() dµ() + {f=0} { cos(ϕ θ() + ψ()) g(), f() 0, g(), f() = 0. g(). Thus, we ge {f=0} g() dµ() 0. However, he infimum will be aained for ha ϕ, for which e iϕ e iθ() g() dµ() = e iθ() g() dµ(), {f 0} and he resul follows. {f 0} Example 1.7. In he c 0 space, y is orhogonal o x if and only if here does no exis he open angle D = {z : α < arg z < β}, wih β α < π, such ha ξ ν η ν D for all hose ν for which ξ ν = x holds.

6 94 Dragolub J. Kečkić Le k 1, k 2,..., k n be all of indices, for which ξ k = x holds, and le δ > 0 be a real number such ha sup ξ ν = x δ, and le ξ ν = ξ ν e iθν. Now, for ν k < δ 2 y we have: { ξν + e iϕ η ν x δ 2 for ν = k ξ ν + e iϕ η ν x δ 2 for ν k. Thus x + e iϕ y = max 1 n ξ k + e iϕ η k, implying x + e iϕ y x D ϕ,x (y) = = x = max 1 n Re {eiϕ e iθ k ηk }, max 1 n 1 + eiϕ η k ξ k 1 aking ino accoun ha for all n-uples of complex numbers here holds max{ 1 + z 1, 1 + z 2,..., 1 + z n } 1 = max{re z 1, Re z 2,..., Re z n }. 0 + So, we have: y is orhogonal o x if and only if inf ϕ max ν=k Re e iϕ e iθ ν η ν ORTHOGONALITY IN S 1 AND S Theorem 2.1. Le X, Y S 1. Then, here holds 0 + X + Y S1 X S1 = Re {r (U Y )} + QY P S1, where X = U X is he polar decomposiion of he operaor X, P = P ker X, Q = P ker X. For he proof of his heorem we need hree echnical lemmas. Lemma 2.2. Le X = U X and X + Y = V X + Y be he polar decomposiions of he operaors X and X + Y, le Q(P ) be he proecor o he kernel of X (X), and le {χ } be some complee orhonormal sysem in ker X. Then: (i) V n x Ux, srongly, for all x ran X, and for some sequence n 0 +. Also, V n x U x, srongly, for all x ran X, and for some (or same) sequence n 0 +. (ii) n + V n (I Q)Y χ, χ = 0, provided ha Y is nuclear. Proof. (i) Le e be some complee orhonormal sysem in H. For each, he family {V e : > 0} is a bounded family, and hence here exiss a sequence n 0, such ha V n e converges weakly. Moreover, using Canor s diagonal process, we conclude ha here exiss a sequence n 0 such ha V n e converges weakly for all, and herefore V n converges weakly. Le V 0 denoe he weak i of he sequence V n. Now, for all y, z H we have V n X + n Y z, y =

7 Orhogonaliy in S 1 and S 95 (X + n Y )z, y. However, X + n Y converges srongly (even uniformly) o X, as well as X + n Y converges srongly o X, and passing o he i we ge V 0 X z, y = Xz, y = U X z, y for all z, y H. Thus V 0 x = Ux for all x ran X. Since ran X is dense in ran X, we obain ha V n converges weakly o Ux for all x ran X. However, his convergence is moreover srong. Indeed, le x be an arbirary vecor from ran X. Then here exiss z H such ha x = X z. We have ha V n X + n Y z ends weakly o Ux. Bu, V n X + n Y z = (X + n Y )z which ends srongly o Xz = Ux. Thus V n X + n Y z ends srongly o Ux. Now we have V n x Ux V n ( X z X + n Y z) + V n X + n Y z Xz, which ends o zero as n ends o infiniy. In a similar way, we can obain ha V n x ends o U x for all x ran X and for some (same) sequence n. (ii) By par (i) we have ha P V n (I Q)Y P converges srongly o P U (I Q)Y P, and by Theorem III.6.3. from [6] P V n (I Q)Y P ends o P U (I Q)Y P in nuclear norm, since Y is nuclear operaor. However, V n (I Q)Y χ, χ is precisely he race of he nuclear operaor P V n (I Q)Y P and herefore i ends o he race of he operaor P U (I Q)Y P. Bu P U = 0 and he proof is complee. Lemma 2.3. Le A be a bounded operaor, whose (usual) norm is a mos one, and le {ϕ } be an arbirary orhonormal sysem. Then, we have X 1 AXϕ, ϕ. Proof. Indeed AXϕ, ϕ r (AX) A X 1 X 1. Lemma 2.4. Le ϕ be some orhonormal sysem (no necessarily complee) in H. (i) for any vecor f H, and for all ε > 0, here exiss a vecor f, such ha f f < ε and f, ϕ < +. { (ii) he se F = A S 1 : } Aϕ < + is dense in S 1. Proof. (i) Le f = f 1 + f 2, f 1 L{ϕ }, f 2 L{ϕ }. Since here holds f 1 2 = f 1, ϕ 2, here exiss n 0, such ha f 1, ϕ 2 < ε 2. We define >n 0 f as f = f 1, ϕ ϕ + f 2. We have f, ϕ = f 1, ϕ < +, and n 0 n 0 also f f 2 = f 1, ϕ ϕ 2 = f 1, ϕ 2 < ε 2. >n 0 >n 0 k=1 k=1 (ii) Le Y S 1, and le Z = N σ k, f k g k (0 < σ k+1 σ k, f k, g k orhonormal sysems) be a finie rank operaor such ha Y Z 1 < ε 2. By he previous par of he saemen, here exis vecors f k, such ha f k, ϕ < +, and f k f k < ε 2 k σ k. Le A = N σ k, f k g k. We have A Z 1 = N σ k, f k k=1

8 96 Dragolub J. Kečkić f k g k 1 N k=1 k=1 σ k f k f k ε 2, and hence A Y 1 < ε. On he oher hand Aϕ N σ k ϕ, f k g k = N σ k ϕ, f k < +. k=1 Now, we are in a posiion o prove Theorem 2.1. Proof of Theorem 2.1. Le X = s, ϕ ψ be he Schmid expansion of he operaor X, and le χ be a complee orhonormal sysem in ker X. Then, aking ino accoun Lemma 2.3, we have: 1 { X + Y 1 X 1 } = 1 { X + Y 1 } s 1 ( U (X + Y )ϕ, ϕ + V (X + Y )χ, χ s ), where V : ker X ker X is given by QY P = V QY P. Furher 1 { X + Y 1 X 1 } 1 { X ϕ, ϕ + U Y ϕ, ϕ + V (X + Y )χ, χ = 1 { ( s + U Y ϕ, ϕ + ) V Y χ, χ s }. Bu, since V Q = V and P χ = χ he las expression is equal o 1 { X + Y 1 X 1 } = 1 { ( s + U Y ϕ, ϕ + ) V } QY P χ, χ s s + (r (U Y ) + QY P 1 ) s = Re (r (U Y ) + QY P 1 ), X+Y and hus 1 X Re (r (U Y )) + QY P 1. { We shall derive he opposie inequaliy for hose Y which belong o F = A S 1 : } Aϕ < +. I will be enough, since we will ge wo sublinear X+Y bounded funcionals Y 1 X and Y Re r (U Y ) + QY P 1, ha coincide on he se F which is dense by Lemma 2.4. Also, in he following, wherever V as 0 +, is wrien, i means V n as n +, where n is a sequence s }

9 Orhogonaliy in S 1 and S 97 from Lemma 2.2. (We do no need o care abou i, since by Proposiion 1.2 (ii) always exiss he i ha we consider.) A he firs we have 1 } { X + Y 1 X 1 (2.1) = 1 { X + Y ϕ, ϕ + X + Y χ, χ s }. However, 1 X + Y χ, χ = 1 V (X + QY )χ, χ + V (I Q)Y χ, χ, and also, QY P 1 V QY P χ, χ = V QY χ, χ = 1 V (X + QY )χ, χ, so ha a real number 1 X + Y χ, χ is equal o a sum of a complex number whose modulus is less or equal o QY P 1, and an oher complex number, whose modulus is, for small enough, less or equal o ε (Lemma 2.2). Thus, for small enough, we ge 1 X + Y χ, χ QY P 1 + ε. On he oher hand, by Jensen s inequaliy applied o he inegraion wih respec o he specral measure we have: X + Y ϕ, ϕ X + Y 2 ϕ, ϕ = = s 2 + 2Re Y ϕ, s ψ + 2 Y ϕ 2 and, applying (2.1) 1 { X + Y 1 X 1 } = s 2 + 2Re Y ϕ, s ψ + 2 Y ϕ 2 + QY P 1 + ε s 2 + 2Re Y ϕ, s ψ + 2 Y ϕ 2 s + QY P 1 + ε s = 2Re Y ϕ, s ψ + 2 Y ϕ 2 ) + QY P 1 + ε ( s 2 + 2Re Y ϕ, s ψ + 2 Y ϕ 2 + s Re Y ϕ, ψ + QY P 1 + ε = Re Y ϕ, Uϕ + QY P 1 + ε = Re (r U Y ) + QY P 1 + ε.

10 98 Dragolub J. Kečkić The inequaliy 2Re Y ϕ, s ψ + 2 Y ϕ 2 ) ( s 2 + 2Re Y ϕ 2Re Y ϕ, ψ + Y ϕ, s ψ + 2 Y ϕ 2 + s allows us o ake a i as 0 + under he sum. The resul now follows, since ε can be arbirarily small. The following corollary characerizes orhogonaliy in he sense of James in he space S 1. Corollary 2.5. The operaor Y is orhogonal o he operaor X in he space S 1 if and only if r (U Y ) QY P S1, where X = U X, P = P kerx, and Q = P kerx. Proof. By Theorem 1.4, Y is orhogonal o X if and only if inf D ϕ,x(y ) ϕ 0. However, by Theorem 2.1, here holds inf D ϕ,x(y ) = inf Re ϕ ϕ (eiϕ r (U Y )) + QY P 1, and we ge he resul, by choosing he mos suiable ϕ. Theorem 2.6. Le X, Y be in S. Then we have X + Y X 0 + = max Re U Y f, f, f Φ where X = U X, and Φ is he characerisic subspace of he operaor X wih respec o is eigenvalue s 1. For he proof of his heorem we need a echnical lemma, as well. Lemma 2.7. Le A be a posiive compac operaor, le Φ be he subspace where A aains is norm, le Φ γ be he se of hose vecors from he Hilber space H which forms wih Φ an angle less or equal o γ. Le, furher, B be a selfadoin compac operaor, such ha B δ, where δ is a real number such ha 2δ s 1(A) s 2(A) 2δ an γ. Then we have A + B = max (A + B)f, f. f Φ γ, Proof. If he uni vecor x is represened as x = f + g, where f Φ, g Φ, g hen x Φ γ if and only if f an γ. Also, s 2(A) = max Af, f. Since f Φ he operaor A + B is compac and selfadoin, here exiss a uni vecor x such ha (A + B)x, x = A + B. If we represen his vecor as x = f + g, hen i will be (A + B)x, x = (A + B)f, f + 2Re Bf, g + (A + B)g, g. Bu, since (A+B)f, f A+B f 2, Bf, g δ f g, (A+B)g, g (s 2 +δ) g 2, we have A + B A + B f 2 + 2δ f g + (s 2 + δ) g 2, i.e. (s 1 δ) g A + B g 2δ f + (s 2 + δ) g, aking ino accoun A + B s 1 δ, respecively (s 1 s 2 2δ) g 2δ f, from which we conclude x Φ γ.

11 Orhogonaliy in S 1 and S 99 Proof of Theorem 2.6. A firs, we have X + Y X (X + Y )(X + Y ) 1/2 X = X X + (X Y + Y X) + 2 Y Y X 2 = 0 + ( X X + (X Y + Y X) + 2 Y Y 1/2 + X ). I is obvious ha he denominaor X X + (X Y + Y X) + 2 Y Y 1/2 + X ends o 2 X. Le us consider he i of he numeraor. The operaors X X and (X Y +Y X)+ 2 Y Y saisfy he assumpions of Lemma 2.7, for an arbirary γ > 0 and for he corresponding small enough, and we ge X X + (X Y + Y X) + 2 Y Y s = 0 + max f Φ γ (X X + (X Y + Y X) + 2 Y Y )f, f s 2 1 max [ (X Y + Y X)f, f + Y Y f, f ] = max 2Re Y f, Xf. 0 + f Φ γ f Φ γ On he oher hand X X + (X Y + Y X) + 2 Y Y s = 0 + max (X X + (X Y + Y X) + 2 Y Y )f, f s 2 1 f Φ max f Φ so ha for all γ > 0 we have [ (X Y + Y X)f, f + Y Y f, f ] = max 2Re Y f, Xf, f Φ 1 X max X + Y X Re Y f, Xf 1 f Φ γ 0 + X max f Φ γ Noe ha inf max γ>0 f Φ γ Re Y f, Xf = max Re Y f, Xf, f Φ Re Y f, Xf. since Y and X are coninuous in he sphere meric. So, we can ge he resul, by aking an infimum over all γ, since for f Φ here holds Xf = X Uf. Corollary 2.8. In he space S he following hree condiions are muually equivalen: (i) Y is orhogonal o X in he sense of James. (ii) inf 0 ϕ<2π max f Φ Re e iϕ U Y f, f 0, where X = U X and Φ is he subspace where he operaor X aains is norm.

12 100 Dragolub J. Kečkić (iii) There exiss he vecor f Φ such ha Y f Xf. Proof. The equivalence beween (i) and (ii) follows from Theorems 1.4 and 2.6. However, he condiion (ii) ells us ha he numerical range of he operaor U Y (on he subspace Φ) has in he complex plane, such a posiion ha i conains a leas one value wih posiive real par, under all roaions around he zero, i.e. ha is no conained in an open half-plane, whose boundary conains he origin. Bu by Toepliz-Haussdorf Theorem he numerical range is a closed convex se, so he las condiion is equivalen o he condiion ha he numerical range of he operaor U Y conains he origin. Since he vecors Uf and Xf always have he same direcion, we conclude ha (iii) is equivalen o (ii). 3. THE SUM OF THE RANGE AND THE KERNEL OF THE ELEMENTARY OPERATORS Le us, firs, recall some facs concerning ideals of compac operaors. Proposiion 3.1. If J is a separable ideal of compac operaors, associaed wih some uniarily invarian norm, hen is dual is isomerically isomorphic wih anoher ideal of compac operaors (no necessarily separable) and i admis he represenaion: ϕ Y (X) = r (XY ). Proof. This is, in fac, Theorem III from [6]. Proposiion 3.2. Le J be some separable ideal of compac operaors, and le E : J J be some elemenary operaor given by E(X) = n A XB. Then is conugae operaor E : J J has he form E (Y ) = n B Y A. Proof. We have ( n ) ϕ Y (E(X)) = r (E(X)Y ) = r A XB Y = r ( X =1 =1 =1 n ) B Y A = r (XE (Y )) = ϕ E (Y )(X). =1 Consider an arbirary separable ideal of compac operaors J, such ha J is sricly convex. According o Proposiion 0.9, for all X J here exiss a unique operaor X J such ha X(X) = X and X = 1. If, moreover, J is reflexive hen he mapping X X, X = ω(x) is a biecion (and also involuion) of he uni spheres of he spaces J and J. Moreover, Y is orhogonal o X in he space J if and only if X(Y ) = 0.

13 Orhogonaliy in S 1 and S 101 Theorem 3.3. Le J be a reflexive ideal in B(H) such ha J is sricly convex, and le E : J J be an elemenary operaor given by E(X) = n A XB. Then ran E is orhogonal (in he sense of James) o he operaor S if and only if ω(s) = S ker E. Proof. Taking ino accoun Proposiions 0.6 and 3.2, we have ha ran E S implies ha for all X J, S(E(X)) = 0 or (E ( S))(X) = 0, for all X, and consequenly E ( S) = 0. Remark 3.4. Theorem 3.3 is he general resul and i holds on an arbirary Banach space. Lema 3.5. Le X be a reflexive Banach space and le V be a closed subspace of X. If V = {x X : v V v + x x } = {0} hen V = X. Proof. This is Lemma 3.6. from [14]. Theorem 3.6. Le J saisfy he assumpions of he previous heorem, and le E : J J be an elemenary operaor given by E(X) = AXB + CXD, where A, B, C and D are normal operaor such ha AC = CA, BD = DB and A A + C C > 0, B B + D D > 0. Then J = ran E ker E. Proof. In [8], i is proved ha for such elemenary operaors is range is orhogonal o is kernel, and by his and by previous Theorem we have he following implicaions: E(S) = 0 X J, E(X) + S S E ( S) = 0 =1 X J, E (X) + S S E ( S) = 0 E(S) = 0. Thus we have E(S) = 0 if and only if E(X) S for all X J. From he orhogonaliy of he range and he kernel i follows ha he sum ran E + ker E is closed. Indeed, if x n + y n for x n ran E, y n ker E ends o z, hen, by inequaliy y n y m x n + y n x m y m we conclude ha y n is a Cauchy sequence, and herefore y n y ker E. Furher x n z y ran E, and hus z ran E + ker E. Suppose ha E(X) + Y + Z J Z J, for all X, and for all Y ker E. By choosing Y = 0 we see ha Z ker E. Now, we can pu Y = Z and X = 0, implying Z = 0. Hence (ran E + ker E) = {0}. This, by Lemma 3.5, finishes he proof. Corollary 3.7. Le p > 1, and le E : S p S p, E(X) = AXB + CXD, where A, B, C and D are as in he previous heorem. Then S p = ran E ker E. Moreover, for any elemenary operaor on S p i is valid ha ran E is orhogonal o S if and only if E ( S p 1 U ) = 0. Proof. I is well known ha S p = S q, q > 1, and ha S q is sricly convex (Clarckson-McCarhy inequaliies; see [13]). Furher, we can easily check ha in he case of S p, S = 1 S p 1 U, which concludes he proof. S p/q p

14 102 Dragolub J. Kečkić Remark 3.8. The special case of his heorem is Proposiion 3 from [10]. Theorem 3.9. There exiss a normal derivaion A : S 1 S 1, A (X) = AX XA, wih AA = A A such ha S 1 ran A ker A. Proof. Le H = l 2 (Z), and le A be he bilaeral shif operaor, i.e. for all n Z le Ae n = e n 1. Le us, firs, perceive ha he kernel of he derivaion A is rivial. Indeed, le X ker A. Then AX = XA, implies Xe i, e = Xe i, A e 1 = AXe i, e 1 = XAe i, e 1 = Xe i 1, e 1. However, aking ino accoun he compacness of he operaor X we ge 0 = Xe i+n, e +n = Xe i, e, for n + all i, Z, and herefore X = 0. Thus ran A ker A = ran A. Le us now consruc he operaor S S 1 in he following way: { Se = 0 for 0, Se = 1 2 e 1 for > 0. If S = U S hen clearly U e = 0 for < 0, and U e = e +1 for 0. We shall prove ha ran A is orhogonal o S. Indeed, his orhogonaliy is, by Corollary 2.5, equivalen o r (U (AX XA)) Q(AX XA)P 1, where P = P ker S and Q = P ker S. However r (U (AX XA)) = r ((AU U A)X), whereas AU U A =, e 0 e 0, and, in fac r (U (AX XA)) = Xe 0, e 0. On he oher hand i is easy o check ha P = P, Q = P L(...,e 2,e 1,e 0) L(...,e, 2,e 1) and we ge (aking in Lemma 2.3 he bounded operaor A ) Q(AX XB)P S1 + Q(AX XA)P e +1, e = = = 1 = = Xe 0, e 0, finishing he proof. + = ( AXe +1, e XAe +1, e ) = (AX XA)P e +1, Qe 1 = ( Xe +1, e +1 Xe, e ) Remark The rivial kernel of he derivaion from he previous heorem is a compleely unessenial deail. Indeed, considering Hilber space H H and he operaor A I on i, we can consruc a normal derivaion which has he same properies as ha in Theorem 3.9, and whose kernel is nonrivial. Theorem There exiss a normal derivaion B : S S, B (X) = BX XB, wih BB = B B, and an operaor S S such ha ran B is orhogonal o S, and S / ker B. Proof. Le A be he operaor from he proof of Theorem 3.9, and le B = A I acing on H = l 2 (Z) C. Furher, le S = S 1 2I, where S 1 : l 2 (Z) l 2 (Z) is any operaor of norm a mos one. The operaor S aains is norm a he unique (up o a scalar) vecor ϕ = 0 1 l 2 (Z) C. I is obvious ha Sϕ = 2ϕ, Bϕ = B ϕ = ϕ, and herefore (BX XB)ϕ, Sϕ = 2 Xϕ, B ϕ 2 XBϕ, ϕ = 2 Xϕ, ϕ 2 Xϕ, ϕ = 0.

15 Orhogonaliy in S 1 and S 103 Thus ran B S. On he oher hand BS = SB implies AS 1 = S 1 A, and S 1 = 0. So if we ake S 1 0 we are done. Remark I is no possible o prove S ran B ker B. On he conrary, he sum ran B ker B is always equal o S. Namely, le f Y S be a funcional of he form f Y (X) = r (XY ) for some Y S 1 = S which annihilaes ran B. I immediaely follows BY Y B = 0, i.e. Y ker B. Since f Y (Y ) 0, f Y can no annihilae ker B. Thus ran B + ker B is always dense in S. Remark One can find ha Remark 3.12 is in a confusion wih Theorem However, his is a consequence of he fac ha boh V = {X S : U V, X + U U } and V = {X S : U V, X + U X }, in general, does no make a subspace, bu a cone! Acknowledgemens. The auhor is deeply graeful o Professor V.S. Shulman for suggesions in formulaing Theorem 3.11, and o Professor D.R. Jocić for suggesions in proving Theorem 2.1. REFERENCES 1. T.J. Abazoglu, Norm derivaives on spaces of operaors, Mah. Ann. 239(1979), J. Anderson, On normal derivaions, Proc. Amer. Mah. Soc. 38(1973), S. Bouali, S. Cherki, Approximaion by generalized commuaors, Aca Sci. Mah. (Szeged) 63(1997), B.P. Duggal, A remark on normal derivaions, Proc. Amer. Mah. Soc. 126(1998), B.P. Duggal, Range-kernel orhogonaliy of he elemenary operaors X np A ixb i X, Linear Algebra Appl. 337(2001), i=1 6. I.C. Gohberg, M.G. Kreĭn, Inroducion o he Theory of Linear Nonselfadoin Operaors, Transl. Mah. Monogr., vol. 18, Amer. Mah. Soc., Providence, RI, J.R. Holub, On he meric geomery of ideals of operaors on Hilber space, Mah. Ann. 201(1973), D. Kečkić, Orhogonaliy of he range and he kernel of some elemenary operaors, Proc. Amer. Mah. Soc. 128(2000), F. Kianeh, Normal derivaions in norm ideals, Proc. Amer. Mah. Soc. 123(1995), F. Kianeh, Operaors ha are orhogonal o he range of a derivaion, J. Mah. Anal. Appl. 203(1996), G. Lumer, M. Rosenblum, Linear operaor equaions, Proc. Amer. Mah. Soc. 10(1959), P.J. Maher, Commuaor approximans, Proc. Amer. Mah. Soc. 115(1992), B. Simon, Trace Ideals and heir Applicaions, London Mah. Soc. Lecure Noe Ser., vol. 35, Cambridge Univ. Press, Cambridge 1979.

16 104 Dragolub J. Kečkić 14. A. Turnšek, Orhogonaliy in C p classes, Monash. Mah. 132(2001), DRAGOLJUB J. KEČKIĆ Faculy of Mahemaics Universiy of Belgrade Sudenski rg Beograd YUGOSLAVIA keckic@poincare.maf.bg.ac.yu Received November 13, 2001; revised Sepember 15, 2002 and February 22, 2003.

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

Optimality Conditions for Unconstrained Problems

Optimality 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 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

On Carlsson type orthogonality and characterization of inner product spaces

On 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 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

A remark on the H -calculus

A remark on the H -calculus A remark on he H -calculus Nigel J. Kalon Absrac If A, B are secorial operaors on a Hilber space wih he same domain range, if Ax Bx A 1 x B 1 x, hen i is a resul of Auscher, McInosh Nahmod ha if A has

More information

A problem related to Bárány Grünbaum conjecture

A problem related to Bárány Grünbaum conjecture Filoma 27:1 (2013), 109 113 DOI 10.2298/FIL1301109B Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma A problem relaed o Bárány Grünbaum

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

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

Fréchet derivatives and Gâteaux derivatives

Fréchet derivatives and Gâteaux derivatives Fréche derivaives and Gâeaux derivaives Jordan Bell jordan.bell@gmail.com Deparmen of Mahemaics, Universiy of Torono April 3, 2014 1 Inroducion In his noe all vecor spaces are real. If X and Y are normed

More information

arxiv: v1 [math.pr] 19 Feb 2011

arxiv: 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 information

SOME MORE APPLICATIONS OF THE HAHN-BANACH THEOREM

SOME 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 information

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION

POSITIVE 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 information

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

Matrix 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 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

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

Basic Entropies for Positive-Definite Matrices

Basic Entropies for Positive-Definite Matrices Journal of Mahemaics and Sysem Science 5 (05 3-3 doi: 0.65/59-59/05.04.00 D DAVID PUBLISHING Basic nropies for Posiive-Definie Marices Jun Ichi Fuii Deparmen of Ars and Sciences (Informaion Science, Osaa

More information

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien

More information

Essential Maps and Coincidence Principles for General Classes of Maps

Essential 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 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

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 Notes 2. The Hilbert Space Approach to Time Series

Lecture Notes 2. The Hilbert Space Approach to Time Series Time Series Seven N. Durlauf Universiy of Wisconsin. Basic ideas Lecure Noes. The Hilber Space Approach o Time Series The Hilber space framework provides a very powerful language for discussing he relaionship

More information

arxiv: v1 [math.fa] 9 Dec 2018

arxiv: 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 information

LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS

LINEAR 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 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

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

t 2 B F x,t n dsdt t u x,t dxdt

t 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 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

Nonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique

Nonlinear Fuzzy Stability of a Functional Equation Related to a Characterization of Inner Product Spaces via Fixed Point Technique Filoma 29:5 (2015), 1067 1080 DOI 10.2298/FI1505067W Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Nonlinear Fuzzy Sabiliy of a Funcional

More 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

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Finish 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 information

Undetermined coefficients for local fractional differential equations

Undetermined 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 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

The motions of the celt on a horizontal plane with viscous friction

The motions of the celt on a horizontal plane with viscous friction The h Join Inernaional Conference on Mulibody Sysem Dynamics June 8, 18, Lisboa, Porugal The moions of he cel on a horizonal plane wih viscous fricion Maria A. Munisyna 1 1 Moscow Insiue of Physics and

More information

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:

Hamilton- 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 information

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu

11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning

More information

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b) Applied Mahemaics E-Noes, 15(215), 14-21 c ISSN 167-251 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Mapping Properies Of The General Inegral Operaor On The Classes R k (ρ, b) And V k

More information

Positive continuous solution of a quadratic integral equation of fractional orders

Positive continuous solution of a quadratic integral equation of fractional orders Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.

More 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

arxiv: v1 [math.fa] 12 Jul 2012

arxiv: v1 [math.fa] 12 Jul 2012 AN EXTENSION OF THE LÖWNER HEINZ INEQUALITY MOHAMMAD SAL MOSLEHIAN AND HAMED NAJAFI arxiv:27.2864v [ah.fa] 2 Jul 22 Absrac. We exend he celebraed Löwner Heinz inequaliy by showing ha if A, B are Hilber

More information

Representation of Stochastic Process by Means of Stochastic Integrals

Representation 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 information

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind

Orthogonal Rational Functions, Associated Rational Functions And Functions Of The Second Kind Proceedings of he World Congress on Engineering 2008 Vol II Orhogonal Raional Funcions, Associaed Raional Funcions And Funcions Of The Second Kind Karl Deckers and Adhemar Bulheel Absrac Consider he sequence

More information

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX

THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he

More information

10. State Space Methods

10. 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 information

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

Ordinary Differential Equations

Ordinary Differential Equations Ordinary Differenial Equaions 5. Examples of linear differenial equaions and heir applicaions We consider some examples of sysems of linear differenial equaions wih consan coefficiens y = a y +... + a

More information

Existence of positive solutions for second order m-point boundary value problems

Existence of positive solutions for second order m-point boundary value problems ANNALES POLONICI MATHEMATICI LXXIX.3 (22 Exisence of posiive soluions for second order m-poin boundary value problems by Ruyun Ma (Lanzhou Absrac. Le α, β, γ, δ and ϱ := γβ + αγ + αδ >. Le ψ( = β + α,

More information

Course Notes for EE227C (Spring 2018): Convex Optimization and Approximation

Course 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 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

Lie Derivatives operator vector field flow push back Lie derivative of

Lie Derivatives operator vector field flow push back Lie derivative of Lie Derivaives The Lie derivaive is a mehod of compuing he direcional derivaive of a vecor field wih respec o anoher vecor field We already know how o make sense of a direcional derivaive of real valued

More information

On Gronwall s Type Integral Inequalities with Singular Kernels

On 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

Cash Flow Valuation Mode Lin Discrete Time

Cash Flow Valuation Mode Lin Discrete Time IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728,p-ISSN: 2319-765X, 6, Issue 6 (May. - Jun. 2013), PP 35-41 Cash Flow Valuaion Mode Lin Discree Time Olayiwola. M. A. and Oni, N. O. Deparmen of Mahemaics

More information

On fuzzy normed algebras

On fuzzy normed algebras Available online a www.jnsa.com J. Nonlinear Sci. Appl. 9 (2016), 5488 5496 Research Aricle On fuzzy normed algebras Tudor Bînzar a,, Flavius Paer a, Sorin Nădăban b a Deparmen of Mahemaics, Poliehnica

More information

Some Ramsey results for the n-cube

Some 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

arxiv: v1 [math.ca] 15 Nov 2016

arxiv: v1 [math.ca] 15 Nov 2016 arxiv:6.599v [mah.ca] 5 Nov 26 Counerexamples on Jumarie s hree basic fracional calculus formulae for non-differeniable coninuous funcions Cheng-shi Liu Deparmen of Mahemaics Norheas Peroleum Universiy

More information

An introduction to evolution PDEs November 16, 2018 CHAPTER 5 - MARKOV SEMIGROUP

An introduction to evolution PDEs November 16, 2018 CHAPTER 5 - MARKOV SEMIGROUP An inroucion o evoluion PDEs November 6, 8 CHAPTER 5 - MARKOV SEMIGROUP Conens. Markov semigroup. Asympoic of Markov semigroups 3.. Srong posiiviy coniion an Doeblin Theorem 3.. Geomeric sabiliy uner Harris

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

Notes for Lecture 17-18

Notes 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 information

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick

More 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

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

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

Clarke s Generalized Gradient and Edalat s L-derivative

Clarke s Generalized Gradient and Edalat s L-derivative 1 21 ISSN 1759-9008 1 Clarke s Generalized Gradien and Edala s L-derivaive PETER HERTLING Absrac: Clarke [2, 3, 4] inroduced a generalized gradien for real-valued Lipschiz coninuous funcions on Banach

More information

arxiv: v1 [math.fa] 19 May 2017

arxiv: v1 [math.fa] 19 May 2017 RELATIVE ENTROPY AND TSALLIS ENTROPY OF TWO ACCRETIVE OPERATORS M. RAÏSSOULI1,2, M. S. MOSLEHIAN 3, AND S. FURUICHI 4 arxiv:175.742v1 [mah.fa] 19 May 217 Absrac. Le A and B be wo accreive operaors. We

More information

MATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018

MATH 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 information

Homework sheet Exercises done during the lecture of March 12, 2014

Homework sheet Exercises done during the lecture of March 12, 2014 EXERCISE SESSION 2A FOR THE COURSE GÉOMÉTRIE EUCLIDIENNE, NON EUCLIDIENNE ET PROJECTIVE MATTEO TOMMASINI Homework shee 3-4 - Exercises done during he lecure of March 2, 204 Exercise 2 Is i rue ha he parameerized

More information

Model Reduction for Dynamical Systems Lecture 6

Model Reduction for Dynamical Systems Lecture 6 Oo-von-Guericke Universiä Magdeburg Faculy of Mahemaics Summer erm 07 Model Reducion for Dynamical Sysems ecure 6 v eer enner and ihong Feng Max lanck Insiue for Dynamics of Complex echnical Sysems Compuaional

More information

We just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n

We just finished the Erdős-Stone Theorem, and ex(n, F ) (1 1/(χ(F ) 1)) ( n Lecure 3 - Kövari-Sós-Turán Theorem Jacques Versraëe jacques@ucsd.edu We jus finished he Erdős-Sone Theorem, and ex(n, F ) ( /(χ(f ) )) ( n 2). So we have asympoics when χ(f ) 3 bu no when χ(f ) = 2 i.e.

More information

Roughness in ordered Semigroups. Muhammad Shabir and Shumaila Irshad

Roughness in ordered Semigroups. Muhammad Shabir and Shumaila Irshad World Applied Sciences Journal 22 (Special Issue of Applied Mah): 84-105, 2013 ISSN 1818-4952 IDOSI Publicaions, 2013 DOI: 105829/idosiwasj22am102013 Roughness in ordered Semigroups Muhammad Shabir and

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. 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 information

arxiv: v1 [math.gm] 4 Nov 2018

arxiv: v1 [math.gm] 4 Nov 2018 Unpredicable Soluions of Linear Differenial Equaions Mara Akhme 1,, Mehme Onur Fen 2, Madina Tleubergenova 3,4, Akylbek Zhamanshin 3,4 1 Deparmen of Mahemaics, Middle Eas Technical Universiy, 06800, Ankara,

More information

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations

Some 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 information

EXISTENCE AND ITERATION OF MONOTONE POSITIVE POLUTIONS FOR MULTI-POINT BVPS OF DIFFERENTIAL EQUATIONS

EXISTENCE AND ITERATION OF MONOTONE POSITIVE POLUTIONS FOR MULTI-POINT BVPS OF DIFFERENTIAL EQUATIONS U.P.B. Sci. Bull., Series A, Vol. 72, Iss. 3, 2 ISSN 223-727 EXISTENCE AND ITERATION OF MONOTONE POSITIVE POLUTIONS FOR MULTI-POINT BVPS OF DIFFERENTIAL EQUATIONS Yuji Liu By applying monoone ieraive meho,

More information

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems. Mah 2250-004 Week 4 April 6-20 secions 7.-7.3 firs order sysems of linear differenial equaions; 7.4 mass-spring sysems. Mon Apr 6 7.-7.2 Sysems of differenial equaions (7.), and he vecor Calculus we need

More information

On Oscillation of a Generalized Logistic Equation with Several Delays

On 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 information

Logarithmic limit sets of real semi-algebraic sets

Logarithmic limit sets of real semi-algebraic sets Ahead of Prin DOI 10.1515 / advgeom-2012-0020 Advances in Geomery c de Gruyer 20xx Logarihmic limi ses of real semi-algebraic ses Daniele Alessandrini (Communicaed by C. Scheiderer) Absrac. This paper

More information

Differential Harnack Estimates for Parabolic Equations

Differential 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 information

FURTHER EXTENSION OF AN ORDER PRESERVING OPERATOR INEQUALITY. (communicated by M. Fujii)

FURTHER EXTENSION OF AN ORDER PRESERVING OPERATOR INEQUALITY. (communicated by M. Fujii) Journal of Mahemaical Inequaliies Volume, Number 4 (008), 465 47 FURTHER EXTENSION OF AN ORDER PRESERVING OPERATOR INEQUALITY TAKAYUKI FURUTA To he memory of Professor Masahiro Nakamura in deep sorrow

More information

Generalized Snell envelope and BSDE With Two general Reflecting Barriers

Generalized Snell envelope and BSDE With Two general Reflecting Barriers 1/22 Generalized Snell envelope and BSDE Wih Two general Reflecing Barriers EL HASSAN ESSAKY Cadi ayyad Universiy Poly-disciplinary Faculy Safi Work in progress wih : M. Hassani and Y. Ouknine Iasi, July

More information

On the probabilistic stability of the monomial functional equation

On the probabilistic stability of the monomial functional equation Available online a www.jnsa.com J. Nonlinear Sci. Appl. 6 (013), 51 59 Research Aricle On he probabilisic sabiliy of he monomial funcional equaion Claudia Zaharia Wes Universiy of Timişoara, Deparmen of

More information

Attractors for a deconvolution model of turbulence

Attractors for a deconvolution model of turbulence Aracors for a deconvoluion model of urbulence Roger Lewandowski and Yves Preaux April 0, 2008 Absrac We consider a deconvoluion model for 3D periodic flows. We show he exisence of a global aracor for he

More information

Some operator monotone functions related to Petz-Hasegawa s functions

Some operator monotone functions related to Petz-Hasegawa s functions Some operaor monoone funcions relaed o Pez-Hasegawa s funcions Masao Kawasaki and Masaru Nagisa Absrac Le f be an operaor monoone funcion on [, ) wih f() and f(). If f() is neiher he consan funcion nor

More information

2. Nonlinear Conservation Law Equations

2. 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 information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. 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 information

Two Coupled Oscillators / Normal Modes

Two Coupled Oscillators / Normal Modes Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own

More information

On Two Integrability Methods of Improper Integrals

On Two Integrability Methods of Improper Integrals Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169

More 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

A NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University

A NOTE ON THE STRUCTURE OF BILATTICES. A. Avron. School of Mathematical Sciences. Sackler Faculty of Exact Sciences. Tel Aviv University A NOTE ON THE STRUCTURE OF BILATTICES A. Avron School of Mahemaical Sciences Sacler Faculy of Exac Sciences Tel Aviv Universiy Tel Aviv 69978, Israel The noion of a bilaice was rs inroduced by Ginsburg

More information

On Growth Rates of Subadditive Functions for Semiflows

On Growth Rates of Subadditive Functions for Semiflows journal of differenial equaions 48, 334350 (998) aricle no. DE98347 On Growh Raes of Subaddiive Funcions for Semiflows Sebasian J. Schreiber Deparmen of Mahemaics, Wesern Washingon Universiy, Bellingham,

More information

556: MATHEMATICAL STATISTICS I

556: MATHEMATICAL STATISTICS I 556: MATHEMATICAL STATISTICS I INEQUALITIES 5.1 Concenraion and Tail Probabiliy Inequaliies Lemma (CHEBYCHEV S LEMMA) c > 0, If X is a random variable, hen for non-negaive funcion h, and P X [h(x) c] E

More information

Math 315: Linear Algebra Solutions to Assignment 6

Math 315: Linear Algebra Solutions to Assignment 6 Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen

More information

On some Properties of Conjugate Fourier-Stieltjes Series

On some Properties of Conjugate Fourier-Stieltjes Series Bullein of TICMI ol. 8, No., 24, 22 29 On some Properies of Conjugae Fourier-Sieljes Series Shalva Zviadadze I. Javakhishvili Tbilisi Sae Universiy, 3 Universiy S., 86, Tbilisi, Georgia (Received January

More information

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i)

t j i, and then can be naturally extended to K(cf. [S-V]). The Hasse derivatives satisfy the following: is defined on k(t) by D (i) A NOTE ON WRONSKIANS AND THE ABC THEOREM IN FUNCTION FIELDS OF RIME CHARACTERISTIC Julie Tzu-Yueh Wang Insiue of Mahemaics Academia Sinica Nankang, Taipei 11529 Taiwan, R.O.C. May 14, 1998 Absrac. We provide

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

Hamilton Jacobi equations

Hamilton 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 information

LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS. 1. Introduction

LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS. 1. Introduction ARCHIVUM MATHEMATICUM (BRNO) Tomus 43 (2007), 75 86 LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS Mariella Cecchi, Zuzana Došlá and Mauro Marini Absrac. Some

More information

Technical Report Doc ID: TR March-2013 (Last revision: 23-February-2016) On formulating quadratic functions in optimization models.

Technical Report Doc ID: TR March-2013 (Last revision: 23-February-2016) On formulating quadratic functions in optimization models. Technical Repor Doc ID: TR--203 06-March-203 (Las revision: 23-Februar-206) On formulaing quadraic funcions in opimizaion models. Auhor: Erling D. Andersen Convex quadraic consrains quie frequenl appear

More information

CHAPTER 2 Signals And Spectra

CHAPTER 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 information

ON THE DEGREES OF RATIONAL KNOTS

ON THE DEGREES OF RATIONAL KNOTS ON THE DEGREES OF RATIONAL KNOTS DONOVAN MCFERON, ALEXANDRA ZUSER Absrac. In his paper, we explore he issue of minimizing he degrees on raional knos. We se a bound on hese degrees using Bézou s heorem,

More information

Existence of multiple positive periodic solutions for functional differential equations

Existence of multiple positive periodic solutions for functional differential equations J. Mah. Anal. Appl. 325 (27) 1378 1389 www.elsevier.com/locae/jmaa Exisence of muliple posiive periodic soluions for funcional differenial equaions Zhijun Zeng a,b,,libi a, Meng Fan a a School of Mahemaics

More information