WHITE NOISE APPROACH TO STOCHASTIC INTEGRATION

Size: px
Start display at page:

Download "WHITE NOISE APPROACH TO STOCHASTIC INTEGRATION"

Transcription

1 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON L. ACCARD*-W. AYED**-H. OUERDANE*** Absrac. We exend o whie noise inegrals he scalar ype inegraor ineqaliies inrodced by Accardi, Fagnola and Qaegeber [1] as a generalizaion of he Hdson Parhasarahy basic esimaes on sochasic inegrals. We se hese esimaes as reglariy resls, showing ha some Hida disribions are in fac elemens of he Fock space. We also se hem o prove an analoge reglariy resl for solions of whie noise eqaions wih bonded coefficiens. The whie noise approach o sochasic calcls emerged, beween 1993 and 1995, from he sochasic limi of qanm heory as a new approach [7] o boh classical and qanm sochasic calcls [9], [16]. The main achievemens of he new approach have been: (i) The idenificaion of boh classical and qanm sochasic eqaions wih whie noise Hamilonian eqaions. (ii) The explanaion of he emergence of he niariy condiions of Hdson and Parhsarahy as expression of he symmericiy of he associaed Hamilonian eqaion. (iii) The explici expression of he coefficiens of he sochasic eqaion as (nonlinear) fncions of he coefficiens of he associaed Hamilonian eqaion. (iv) The emergence of a naral nonlinear exension of sochasic calcls. The deep and srprising resls obained in his direcion in he qadraic case sgges ha he compleion of his programme for he higher powers of whie noise is one of he mos challenging and fascinaing problems of conemporary sochasic analysis. None of hese resls cold have been even formlaed in he framework of he sal (classical or qanm) sochasic analysis. However he exciing new developmens emerged from he whie noise approach o sochasic calcls delayed a sysemaic exposiion of is basic analyical ools sch as whie noise inegrals, whie noise eqaions, he heory of disribions on he sandard simplex, he casal normal order,... A large lierare exised in he firs wo of he above menioned direcions, in he framework of Hida s whie noise analysis. However o creae a bridge beween hese resls and hose of classical and qanm sochasic analysis, one needs some reglariy resls, i.e. condiions which assre ha objecs, which a priori are Hida disribions, are in fac vecors in a Hilber space. Sch reglariy condiions will be formlaed here in erms of esimaes on whie noise inegrals. Esimaes of his ype were developed in [3] and hey were srong enogh o prove an exisence heorem for a mlidimensional whie noise inegral eqaion. However, as we shall see in a forhcoming paper [8], hese esimaes were no srong enogh o prove he fndamenal resl of he heory, i.e. he niariy condiion. The main resls of he presen paper are: (i): The exension of he whie noise esimaes of [3] o a larger domain (he maximal algebraic domain inrodced in Secion 1) on he lines of [5]. (ii): The inrodcion of he noion of whie noise adapedness and he proof, nder his assmpion (which reqires a whie noise wih 1 dimensional parameer), of he whie noise analoge of he scalar ype inegraor ineqaliies of Accardi, Fagnola and Qaegeber [1] which, in heir rn, generalize he basic Hdson Parhasarahy esimae on sochasic inegrals (cf. Proposiion 5.6 in [15]). Key words and phrases. Whie noise-maximal algebraic domain, Esimaes on whie noise sochasic inegrals. *:Universià di Roma Tor Vergaa, Cenro Vio Volerra 133 Rome, aly. Mail: accardi volerra.ma.niroma.i. **:Universiy of Tnis El Manar, Deparmen of Mahemaics 16 Tnis, Tnisia. Mail: wided.ayed ipein.rn.n. ***:Universiy of Tnis El Manar, Deparmen of Mahemaics 16 Tnis, Tnisia. Mail: habib.oerdiane fs.rn.n. AMS classificaion: 6H4-6H15. 1

2 L. ACCARD*-W. AYED**-H. OUERDANE*** The presen paper is he firs sep of or plan o complee he programme iniiaed in [3] of giving a sysemaic derivaion of he whie noise niariy condiions. Here we only deal wih he basic esimaes on sochasic inegrals and wih he corresponding exisence heorem for sochasic differenial eqaions. Noaions n his secion, in order o fix or noaions, we review some well known maerial. The erms qanm whie noise and free field are synonyms: he former is more sed in mahemaics, he laer in physics. Since classical whie noise is inclded in qanm whie noise, in he following we will se he erm whie noise o mean he more general (qanm) case. A sandard way o consrc whie noises is hrogh he Fock space. We will consider he scalar Boson Fock space over L (R d ): F(L (R d )) : F : no L sym(r dn ) n F n ; F : C F n : L sym(r dn ), n 1,,... is he Hilber space of sqare inegrable fncions of n-variables in R d, symmeric nder he permaion of heir argmens. f S is a sbspace of L (R d ) we will se he noaion F(S) : n syms no which is clearly a sbspace of F(L (R d )) becase, for each n, n syms F n. The elemens of F n are called n-paricle vecors and he se of n-paricle vecors, for all n N, is also called he se of nmber vecors. For an elemen ψ (n) F n we wrie ψ (n) ψ (n) (s 1,..., s n ), s i R d and, for any permaion π, on {1,..., n} one has: ψ (n) (s 1,..., s n ) ψ (n) (s π(1),..., s π(n) ). So an elemen of he Boson Fock space F is a seqence of fncions ψ {ψ (), ψ (1), ψ (),...} where ψ () C, ψ (n) F n, n 1,,... and ψ ψ (n) L (R dn ) < More explicily ψ n ψ () + n1 R dn ψ (n) (s 1,..., s n ) ds 1...ds n The inner prodc of elemens ψ {ψ (n) } n and φ {φ(n) } n in F is given by (ψ, φ) (ψ (n), φ (n) ) ψ () φ () + ψ (n) (s 1,..., s n )φ (n) (s 1,..., s n )ds 1...ds n R dn n n1 The vecor Φ (1,,,...) is called he vacm vecor. A vecor ψ (ψ (n) ) sch ha here exiss f L (R d ) wih he propery ha, n N, we have (.1) ψ (n) (s 1,, s n ) 1 n! f(s 1 )f(s ) f(s n ) ; a.e for n 1 ψ ( ) 1Φ ψ Φ is called an exponenial vecor wih es fncion f and denoed or ψ(f) (ψ (n) f ).

3 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 3 Definiion.1. Le S(R dn ) denoe he Schwarz space, i.e. he se of infiniely differeniable complex valed fncions h on R nd sch ha, for any α, β N nd one has: Define he sbspaces of F: h α,β sp x R nd x α D (β) h(x) < F(S(R d )) : D S : {ψ F : n N, ψ (n) S(R dn )} { } N : ψ D S : ψ (n) for almos all n N (1.1.a) (1.1.b) DS : N D S These are he vecors in F for which all componens, wih he excepion of a mos a finie nmber are eqal o zero. They are called finie paricle vecors. We also define: DS 1 : {ψ D S : n ψ (n) < } (1.1.c) D 1 : {ψ F : n1 n1 n ψ (n) < } (1.1.d) Similarly we define D C, D C, D 1 C by replacing in (1.1.a), (1.1.b), (1.1.c) he Schwarz space S(Rnd ) wih he space C(R nd ) L (R nd ) where C(R nd ) denoes he space of coninos fncions on R nd. Remark.1. Each of he 3 spaces D S, D S, D1 S is dense in F. Definiion.. For any s R d, n N and for any ψ D 1 we fix a represenaive ψ (n) (s 1,,, s n ) in he Lebesge class of ψ (n) and we define: a-: he annihilaion densiy a s as he linear operaor: (.) (.3) (.4) (.5) a s : ψ D 1 (a s ψ) (n) (s 1, s,, s n ) n + 1ψ (n+1) (s, s 1, s,, s n ) F (den1) which associaes o ψ D 1 he F valed linear fncional on he sqare inegrable fncions on R d : f n + 1 dsf(s)ψ (n+1) (s, s 1, s,, s n ) : (A f ψ) (n) (s 1,, s n ) A f is called he annihilaion operaor. follows ha A f ψ a s f(s)ψds. R d b-: he creaion densiy a + s as he linear operaor: a + s : ψ F (a + s ψ) (n) (s 1, s,, s n ) 1 n δ(s s i )ψ (n 1) (s 1,, ŝ i,, s n ) n (den) which associaes o ψ D 1 he F valed linear fncional on he sqare inegrable fncions on R d : f 1 n f(s i )ψ (n 1) (s 1,, ŝ i,, s n ) : (A + n f ψ)(n) (s 1,, s n ) A + f is called he creaion operaor and we ge: (A + f ψ)(n) (s 1,, s n ) 1 n δ(s s i )f(s)ψ (n 1) (s 1,, ŝ i,, s n )ds n R d (a + s ψ) (n) f(s)ds. R d

4 4 L. ACCARD*-W. AYED**-H. OUERDANE*** follows ha (.6) A + f ψ R d a + s f(s)ψds. c-: he nmber densiy is defined on D 1 by: n s a + s a s Using (den1) and (den), for any ψ D 1, one has n (n s ψ) (n) (s 1, s,, s n ) δ(s s i )ψ (n) (s, s 1,, ŝ i,, s n ) which allows o inerpre he nmber densiy in he same way as he creaion densiy. Remark.. Taking f χ [,] in.3 and.6, we obain: (.7) and (.8) A A + o o a s ds a + s ds. (den3) (den4) These noaions are hose for whie noise over R, a, a +, since a Brownian moion ( classical or qanm ) is obained by inegraing a whie noise.also, we ge [4] he commaion relaions: [A, A + s ] min(s, ) ; [A, A s ] [A +, A+ s ] (5.5) A Φ (5.6) Proposiion.1. The operaors inrodced in Definiion (.) are well defined and depend only on he seqence (ψ (n) ) (and no on he represenaives of is elemens). Moreover A f : F n F n 1 ; A f F, n 1,, A + f : F n F n+1, n, 1,, The creaion and he annihilaion operaors are adjoin o each oher on D 1, and we have: (.9) A f Φ Proof. For any measrable fncion ψ (n) he righ hand side of (den1) is well defined and he ideniy ϕ (n 1), (A f ψ) (n 1) f(s n ) ψ (n) (s 1,, s n )ϕ (n 1) (s 1,, s n 1 )ds 1 ds n R dn shows ha he Lebesge class of (A f ψ) (n 1) does no depend on he choice of ψ (n) (s 1,, s n ) b only on is Lebesge class ψ (n). The fac ha ψ (ψ (n) ) D 1 and he Schwarz ineqaliy he seqence ((A f ψ) (n) ) defines a coninos linear fncional on F hence a niqe elemen in F. f ψ D 1 and f L (R d ), A + f ψ is in F becase: A + f ψ (A + f ψ)(n) (s 1,..., s n ) ds 1...ds n n1 R dn ( 1 n n1 n1 R dn n f(s i )ψ (n 1) (s 1,, ŝ i,, s n ) R dn n f(s 1 )ψ (n 1) (s,,, s n ) ds 1...ds n ds 1...ds n

5 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 5 f { n ψ (n 1) L (R (n 1)d ) } < n1 The same argmen sed above shows ha he Lebesge class of (a + f )(n) only depends on he classes of f and ψ (n 1). The remaining saemens are proved in a similar way. Definiion.3. We can exend he definiion of nmber operaor; le T ˆ B(L (R d )) be a pre closed linear operaor wih inegral kernel τ, i.e.for all f L (R d ): T f(x) τ(x, y)f(y)dy The nmber operaor N T is defined by: N T τ(x, y)a + x a y dxdy Noice ha, for all f Dom(T ) L (R d ) and for all exponenial vecors, one has: N T dx dyτ(x, y)f(y)a + x dx(t f)(x)a + x A + T f. We allow τ(x, y) o be a disribion: he choice τ(x, y) V (x)δ(x y) allows o inclde all he mliplicaion operaors. Remark.3. The Boson commaion relaions: [a s1, a + s ] δ(s 1 s ).c are inerpreed weakly on D 1 and easily verified on ha domain. 1. The Maximal Algebraic Domain D 1 is no an invarian domain nder he acion of all creaion, annihilaion, nmber and Weyl operaors. There is a nmber of invarian domains which are sefl in differen siaions [9]. n his secion we inrodce he smalles domain conaining he vacm and invarian nder he acion of all hese operaors. We call i maximal algebraic domain ha is he larges domain obainable from he vacm wih prely algebraic operaions on he basic operaors. Definiion 1.1. The maximal algebraic domain denoed by D MAD is by definiion he linear span of he vecors se { } (1.1) DMAD A + f n A + f 1,, /f, f 1,, f n L (R d ), n 1 where A + f f. for f L (R d ) is he creaor operaor, and is he exponenial vecors wih es fncion Since D MAD conains he exponenial vecors i is dense in F. Lemma 1.1. For every f, f 1,, f n L (R d ) one has Dom(A + f n A + f 1 ); n 1. Proof. We will prove by indcion on n 1, ha for any f, f 1,, f n L (R d ), one has A + f n A + f 1 F, so for n 1, since for all f, g L (R d ), we have (see [3]) : [A f, A + g ] f, g

6 6 L. ACCARD*-W. AYED**-H. OUERDANE*** i follows: A + f 1 A + f 1, A + f 1, A f1 A + f 1 f 1 +, A + f 1 A f1 f 1 + A f1, A f1 f 1 + f 1, f < Sppose ha for any f, f 1,, f n L (R d ), we have A + f n A + f 1 L (R d ). To prove ha A + f n+1 A + f n A + f 1 F, we will se he fac: F and le f, f 1,, f n+1 n+1 A fn+1 A + f n+1 A + f n A + f 1 f n+1, f A + f n A + f 1 + f n+1, f j A + f n+1 Aˆ fj A + f 1 F hen: A + f n+1 A + f 1 A + f n A + f 1, A fn+1 A + f n+1 A + f 1 n+1 f n+1, f A + f n A + f 1 + A + f n A + f 1, A + f n+1 Aˆ fj A + f 1 f n+1, f j j1 ( ) n+1 max f j A + j,,n+1 f n A + f 1 A + f n A + f 1 + A + f n+1 Aˆ fj A + f 1 < Now, o prove some propery of invariance of D MAD, we will recall he definiion of he Fock-Weyl represenaion of L (R d ) given in [3], in he following: he Weyl operaor W f is an elemen of he niary grop U(F) wih he srong operaors opology. Moreover W f acs on he exponenial vecor ψ g as: j1 j1 we also have he following properies 1-: -: W f (ψ g ) e 1 f f,g ψ(g + f). W g Φ e 1 g ψ g (W g ) A f W g A f + i f, g 1..a or eqivalenly [A f, W g ] i f, g W g 1..b Lemma 1.. For every g, f 1,, f n L (R d ) and T ˆ B(L (R d )), he linear span of he vecors A + f n A + f 1 ψ g is he smalles vecor sbspace of F conaining he vacm vecor and invarian nder he acion of he operaors (1.) A + f, A f, W h, N T where W h, N T are he Weyl and he nmber operaors. Moreover, on he domain D MAD, one has: (A + f ) A f (N T ) N T

7 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 7 Proof. Le g, f 1,, f n L (R d ), sing (1..a), he prove of he fac ha A f A + f n A + f 1 ψ g D MAD follows from A f A + f n A + f 1 ψ g f, g A + f n A + f 1 ψ g + n f, f j A + f n Aˆ fj A + f 1 ψ g D MAD. To prove ha W f A + f n A + f 1 ψ g D MAD, i is sfficien o prove ha W f A + f n A + f 1 W g Φ D MAD. Hence j1 W f A + f n A + f 1 W g Φ W f A + f n A + f 1 Wf W f W g Φ n [W f A + f i Wf ]W f W g Φ n [A + f i + i f, f i ]e im f,g W (f+g) Φ {j 1,,j α} {1,,n} λ α [A + f j1 A + f jα W (f+g) Φ] D MAD where λ α : ( i ) n α {h 1,...,h n α }{j 1,...,j α} c {1,...,n} f, f i Le f, f 1 (L (R d )), hen sing (1.3) [N T, A + f ] A+ (T f), N T A + T f, we obain: N T A + f 1 A + f 1 N T + A + T f1 A + f 1 A + T f + T f1, f D MAD by indcion, sppose ha for f, g, f 1,, f n+1 belongs o L (R d ) one has N T A + f n A + f 1 ψ g D MAD and sing (1.3), we ge: N T A + f n+1 A + f n, A + f 1 ψ g A + f n+1 N T A + f n A + f 1 ψ g + A + (T f n+1 ) A+ f n A + f 1 ψ g D MAD Corollary 1.1. Denoe by P W he *algebra generaed by he operaors (1.) acing on D MAD which called he polynomial-weyl algebra. We have: D MAD P W Φ Proof. is clear ha D MAD P W Φ The converse inclsion, i.e: P W Φ D MAD follows easily from he relaions (1..a), (1..b) and (.9).

8 8 L. ACCARD*-W. AYED**-H. OUERDANE***. Whie noise sochasic inegrals n his secion we will discss whie noise and sochasic inegrals in R d raher han in R becase exacly he same formlae are valid in he 1-and in he d-dimensional case, b, as we shall see in Secion (3), some esimaes are slighly worse in he non adaped case, compared o he will be called whie noise adaped. We define he operaors: A(F ) < F, A > ds F s a s ; A + (F ) < A +, F > R d ds a + s F s R d where F is a complex valed fncion on R d. The generalizaion of hese inegrals o he case when F in an operaor valed fncion are called righ (resp. lef) sochasic inegrals wih respec o a s (resp. a + s ). Similarly one defines he wo-sided sochasic inegral: R d ds a + s F s a s. is clear ha, he exisence of lef and wo sided sochasic inegral, (also of righ ones if he inegrand process F s is nbonded), reqires some compaibiliy condiions on he domains. Definiion.1. Le L : L(D) be he space of maps F : R d L(D, F) s F s where L(D, F) is he space of linear operaors on he Fock space F densely defined on a domain D, sch ha for any ϕ, ψ D, he maps are locally inegrable. s R d < ψ, F s ϕ >; s F s ψ ϕ, ψ D Elemens of L will be called processes or, if confsion may arise, D-processes. Remark.1. f D D MAD, hen he map s a s is in L, while he map s a + s is no in L.1. Righ annihilaor sochasic inegral. Definiion.. The righ annihilaor sochasic inegral of F L is he operaor: ψ ds F s a s ψ R d (.1.a) where he inegral is mean as a Bochner inegral in he Fock space. is defined for each ψ F sch ha a s ψ is in he domain of F s for each s and he vecor valed fncion s R d F s a s ψ is Bochner inegrable [14]. Lemma.1. The sochasic inegral (.1.a) is defined for all processes F L and for all vecors ψ DC 1 sch ha n dsf s ψ (n) (s,.) < (.1.b) R d n n his case he inegral (.1.a) is eqal o where ψ (n+1) (s,.) is he fncion R d F s a s dsψ n n + 1 R d dsf s ψ (n+1) (s,.) (s 1,..., s n ) R dn ψ (n+1) (s, s 1,..., s n ) (.1.d)

9 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 9 Proof. We sar from he explici form of he righ annihilaor on a vecor ψ D 1 C (.1) (a s ψ) (n) n + 1ψ (n+1) (s,.) Therefore, in he noaion (.1) F s a s ψds ds n + 1Fs ψ (n+1) (s,.) R d R d n (.1.c) Now by assmpion, for each n, he fncion s R d F s ψ (n+1) (s,.) is Bochner inegrable. Moreover, becase of (.1.b), he series on he righ hand side of (.1.c) is absolely convergen. Therefore, one can exchange he series and he inegral. This gives (.1.d). f ψ ; an he exponenial vecors, he explici form of he sochasic inegral (.1.a) is (.) ds F s a s R d ds f(s)f s R d where he righ hand side of (.) is defined on he se of he exponenial vecors wih es fncion in L (R d ) sch ha he vecor valed fncion s f(s)f s is Bochner inegrable... The lef creaor sochasic inegral. Definiion.3. The lef creaor sochasic inegrals of a measrable elemen F L; F : s F s is he operaor: ψ ds a + s F s ψ R d and i is given by he formla for he scalar case: ( ) (n)(s1 (.3) ds a + s F s ψ,..., s n ) 1 n (F si ψ) (n 1) (s 1,..., ŝ i,..., s n ), n 1 R d n where ψ is in he domain of he operaor F s for all s R +. Remark.. This definiion has a meaning for any measrable fncion s F s, he naral domain of he lef creaor sochasic inegral is {ψ : ( ds a + s F s ψ) (n) n1 R d L (R nd ) < } or more explicily, a vecor ψ in D( ds a + s F s ) if and only if ψ D(F s ), s R d R d n (F s1 ψ) (n 1) (s,..., s n ) ds 1...ds n < n1 R dn We wan now o obain esimaes on he norm of ds a + s F s ψ which garanees ha he sochasic R inegral exis. An example of sch esimaes is given by d he following lemma: Lemma.. Le ψ belong o D(F s ) for all s R d. Then one has, for each n N ( ) (n) (.4) ds a + s F s ψ n ds (F s ψ) (n 1) R d R d

10 1 L. ACCARD*-W. AYED**-H. OUERDANE*** Proof We have ( ) (n) dsa + s F s ψ 1... ds 1...ds n (F si ψ) (n 1) (s 1,..., ŝ i,..., s n ), (F sj ψ) (n 1) (s 1,..., ŝ j,..., s n ) n i,j 1 (Fsi i,j... ds 1...ds n ψ) (n 1) (s 1,..., ŝ i,..., s n ) (F sj ψ) (n 1) (s 1,..., ŝ j,..., s n ) n n ds ds...ds n (F s ψ) (n 1) (s,..., s n ) n ds (F s ψ) (n 1) n R n R d(n 1) R d.3. The normally ordered wo-sided inegral. Definiion.4. n he above noaions, he wo-sided normally ordered inegral of F L: ds a + s F s a s R d is defined,weakly on he maximal algebraic domain: ξ, η D MAD, ξ, ds a + s F s a s η ds a s ξ, F s a s η R d R d n pariclar, on exponenial vecors one has ( ), ds a + s F s a s ψ g ds f(s)g(s), F s ψ g R d R d Lemma.3. For any n N and for any exponenial vecor one has he esimae ( ) (n) (.5) ds a + s F s a s n ds f(s) (F s ) (n 1) R d R d 3. Mlidimensional esimaes on D MAD (C) n his secion, we prove some esimaes on he maximal algebraic domain in he mlidimensional case. Since D MAD is linearly spanned by he vecors of he form A + f n A + f 1, hen i is sefl o have esimaes on he norm of hese vecors. Recall ha F Γ(L (R d )) he symmeric Fock space over L (R d ) and D MAD (C) is he maximal algebraic domain i.e. he linear span of he vecors in he se { } D C A + f n A + f 1,, /f, f 1,, f n C L (R d ) C(R d ), n 1 (4.1.1) Lemma 3.1. We have: a) (3.1) [a s, A + f ] f(s) where f is a es fncion in L (R d ). b) ] (3.) [a s, A + A + fn f1 where f 1,, f n are es fncions in L (R d ). Proof. a) For all ψ D MAD We have: (A + f (ψ))(n) (s 1,, s n ) 1 n n f i (s)a + f n A n f(s i )ψ (n 1) (s 1,, ŝ i,, s n )

11 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 11 Using ha: we obain: (a s ψ) (n) (s 1,, s n ) n + 1ψ (n+1) (s, s 1,, s n ) where s n+1 s. Moreover: hen: (a s A + f (ψ))(n) (s 1,, s n ) n + 1(A + f (ψ))(n+1) (s, s 1,, s n ) n+1 n + 1 f(s i )ψ (n) (s 1,, ŝ i,, s n+1 ) n + 1 (A + f a sψ) (n) (s 1,, s n ) 1 n 1 n n+1 f(s i )ψ (n) (s 1,, ŝ i,, s n+1 ) n f(s i )(a s ψ) (n 1) (s 1,, ŝ i,, s n ) n f(s i ) n(ψ) (n) (s, s 1,, ŝ i,, s n 1 ) ( (a s A + f ψ)(n) (A + f a sψ) (n)) (s 1,, s n ) n+1 f(s i )ψ (n) (s 1,, ŝ i,, s n+1 ) f(s n+1 )ψ (n) (s 1,, s n ) f(s)ψ (n) (s 1,, s n ) ((a s A + f ψ)(n) (A + f a sψ) (n) ) (s 1,, s n ) n f(s i)(ψ) (n) (s, s 1,, ŝ i,, s n 1 ) b) This resl will be proved by indcion on n: le P n be he following propery: ] [a s, A + A + fn f1 n f i (s)a + f n A. Using a) he case n 1 was verified, so we sppose ha P n was verified, hen we will prove P n+1 so: ] [a s, A + A + a fn+1 f1 s A + f n+1 A + f 1 A + f n+1 A + f 1 a s ] [a s, A + A + fn+1 f n A + f 1 + A + f n+1 a s A + f n A + f 1 A + f n+1 A + f 1 a s ] [a s, A ]A + + A + + A [a + fn+1 fn f1 fn+1 s, A + A + fn f1 n f n+1 (s)a + f n A + f 1 + A + f n+1 f i (s)a + f n A n+1 f i (s)a + f n+1 A Proposiion 3.1. (Righ annihilaor esimaes) For each F L and for each bonded sbse R d, i follows :

12 1 L. ACCARD*-W. AYED**-H. OUERDANE*** (3.3) i): for each nmber vecor: ψ A + f n A + f 1 Φ where f 1,, f n are es fncions in L (R d ), we have: ds F s a s ψ c ψ, ϕ J(ψ) ( ) 1 ds F s ϕ where { } J(ψ) : A + f n A Φ, /1 i n D MAD c ψ, : max 1in ( f i, ) (3.1.a) ( f i, : ) 1 f i (s) ds (3.1.b) ii): For each vecor ψ A + f n A + f 1 and for f, f 1,, f n, R d (as in (i) above), (3.3) hold wih J(ψ) {A + f n... Â+ f i, A + f n, 1 i n} (3.1.c) c ψ, max 1in ( f i,, f, ) (3.1.d) so Proof i) Using lemma (3.1) and he fac ha a s Φ, we have for f 1,, f n L (R d ): [ ds F s a s A + f n A + f 1 Φ ds F s a s, A + f n A + f 1 ]Φ ds F s a s A + f n A + f 1 Φ ds F s ds F s n f i (s)a + f n A Φ n f i (s)a + f n A Φ n ds f i (s) F s A + f n A Φ n ( ) 1 ( ) 1 ds f i (s) ds F s A + f n A Φ n ( ) 1 c ψ, ds F s A + f n A Φ and his proves (3.3) where c ψ, is given by (3.1.b). ii) For ψ A + f n A + f 1, where f, f 1,, f n are es fncions and is an exponenial vecor, we have: [ ds F s a s A + f n A + f 1 ds F s a s, A + f n A + f 1 ] + ds F s f(s)a + f n A + f 1 [ n ] ds F s f i (s)a + f n A + f(s)a + f n A + f 1

13 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 13 so: [ ds F s a s A + f n A ˆ + f i A + n ] f 1 ds F s f i (s)a + f n A + f(s)a + f n A + f 1 where c ψ, is as in (3.1.d) [ n ] ds F s f i (s)a + f n A + F s f(s)a + f n A + f 1 [ ds n ] F s f i (s)a + f n A + F s f(s)a + f n A + f1 [ n ] ds f i (s) F s A + f n A + f(s) F s A + f n A + f 1 n ( f i (s) ds ) 1 ( ) 1 ds F s A + f n A ( ) 1 ( ) 1 + f(s) ds ds F s A + f n A + f 1 n ( ) 1 c ψ, ds F s A + f n A ( ) 1 + ds F s A + f n A + f Mlidimensional lef creaor esimae. Lemma 3.. Consider he sochasic inegral A + (F )ψ : ds a + s F s ψ, R d where F L and s, ψ Dom(F s ) sch ha n (F s1 ψ) (n 1) (s,..., s n ) ds 1...ds n <, hen n1 R dn A + (F )ψ where. is he norm defined by: (3.4) ψ : n d F ψ + dsd (F s ψ)(,.) n ψ (n) Proof A + (F )ψ, A+ (F )ψ ds d a + s F s ψ, a + F ψ ds d F s ψ, [a s, a + ]F ψ + d F ψ, F ψ + dsd a F s ψ, a s F ψ. ds d F s ψ, a + a sf ψ

14 14 L. ACCARD*-W. AYED**-H. OUERDANE*** Now consider he inegral: J : ds d a F s ψ, a s F ψ dsd (n + 1) (F s ψ) (n+1) (, σ)(f ψ) (n+1) (s, σ)dσ R nd n Using Cachy Schwars ineqaliy and Lebesge heorem, we ge: J (n + 1) dsd (F s ψ) (n+1) (,.) L (R nd ) n (n + 1) + dsd (F ψ) (n+1) (s,.) L (R nd ) n (n + 1) dsd (F s ψ) (n+1) (,.) L (R nd ) n dsd (F s ψ)(,.) where. is he norm (3.4). Remark 3.1. This esimae in he mlidimensional case is no sefl o prove he convergence of ieraed series, b as i follows, we can find a good esimae in he whie noise adaped and onedimensional case. 4. Whie noise adaped sochasic inegral eqaion n his secion, we will show ha he whie noise adapness condiion gives he opporniy o have more precise resls wih more reglariy. We will generalize some resls proved by Hdson and Parhasarahy in wo direcions: (i) he adapness condiion will be replaced by whie noise adapness [15] (ii) he esimae will be valid no only on he exponenial domain, b on he whole maximal algebraic domain. A firs, we recall ha a sochasic process in F, indexed by R +, is a family (F ) of elemens of L(D, F) saisfying ha for each ψ D, he map F ψ is Borel measrable. Alernaively, a sochasic process indexed by R + can be looked as a map R + F L(D, F) wih he above menioned measrabiliy propery. We remark ha elemens of L can be regarded as sochasic processes. n he nex, we shall only deal wih processes indexed by R +. Definiion 4.1. A process (F ) is said o be whie noise adaped if for any m {a, a +, a a + }, we have: (4.1) ψ D MAD, F s m ψ m F s ψ, s <. Lemma 4.1. f a process (F ) is adaped in he sense of Hdson and Parhasarahy, i is whie noise adaped. Proof. Le (F ) an adaped process in he sense of Hdson and Parhasarahy [15], which means ha for any exponenial vecor ] [, for R + one has: F (F ] ) [

15 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 15 so a s F a s (F ] ) [, s > a s F (F ] ) a s [, s > F a s, s > Then, we conclde ha (F ) is whie noise adaped The Hdson-Parhasarahy esimae. n he following secion we will prove ha he whie noise approach allows o obain a sronger resl. n fac he nex esimae was proved by Hdson and Parhasarahy [15], in he adaped case and here we given a differen proof of he same resl b for general kind of processes, and his sing he whie noise approach. Proposiion 4.1. For all srongly coninos processes (F s ) s on D MAD (C), we have: (4.) ds F s a s e ds F s f(s) so Proof. Le be an exponenial vecor wih es fncion f, hen, we denoe by: () () dsf s a s ds F s a s For fixed, d > and arbirary fncion F (), we se he noaion df () F ( + d) F () (finie difference). n his noaion one has he algebraic ideniy: d (), () d(), () + d(), d() + d(), d() Denoe Re Re +d +d ds F s f(s), () + ds f(s) F s, () + +d +d h( 1, ) : f( 1 )f( ) F 1, F d 1 F 1 f( 1 ), +d d F f( ) +d d 1 d f( 1 )f( ) F 1, F. Since he map s F s is coninos, we dedce ha he map ( 1, ) h( 1, ) is niformly bonded on [, + d] for each R +, in fac: sing his and he ideniy 1 d Re we ge, for d herefore +d h( 1, ) f sp s [,+d] 1 d d (), () F s f(s)ds, () + 1 d F s +d d d (), () Re F f(), () +d d 1 d h( 1, ) d d (), () F f() + ()

16 16 L. ACCARD*-W. AYED**-H. OUERDANE*** Ths, by Gronwall lemma: which is (4.). () e d f() F dimensional, whie noise adaped lef creaor esimae. We need he following preliminary resl, which is re in arbirary dimensions. Lemma 4.. For all ψ in D MAD (C) saisfying (4.3) ψ : n n ψ (n) <. Then for each s 1 R d, he following series: (n + 1) ds ds n+1 ψ (n+1) (s 1, s,, s n+1 ) R dn is finie a.e. n Proof Using he Dini heorem and (4.3), we ge ψ ds 1 (n + 1) ds ds n+1 ψ (n+1) (s 1, s,, s n+1 ) <. R d R dn n Then, we dedce ha for each s 1 in R d we have (n + 1) ds ds n+1 ψ (n+1) (s 1, s,, s n+1 ) < a.e. R dn n. Proposiion 4.. (1-dimensional lef creaor esimaes) For all whie noise adaped processes (F s ) s and all ψ D MAD (C) sch ha he map ( 1, ) F 1 ψ(,.) is coninos for 1, in every inerval of R + for he norm (3.4), we have, for any T < + (4.4) dsa + s F s ψ e (C T,ψ J(ψ) ) F s ψ i ds where J(ψ) is he sbse of F defined by. denoes he cardinaliy, ψ i J(ψ) J(ψ) {ψ i A + f n... Â+ f i, A + f n 1 i n} D MAD, C T,ψ where f,t sp [,T ] f(). Proof. Le ψ A + f n A + f 1, and max c T,ψ i, c T,ψi max ( f j,t, f,t ). ψ i J(ψ) 1jn A (F )ψ ds a + s F s ψ so o esimae A (F )ψ i is sfficien o esimae d A (F )ψ, A (F )ψ for his we obain d A (F )ψ, A (F )ψ da (F )ψ, A (F )ψ + A (F )ψ, da (F )ψ + da (F )ψ, da (F )ψ (4.1.a)

17 For he erm da (F )ψ, da (F )ψ, we obain Denoe by: A : WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 17 Re da (F )ψ, A (F )ψ + da (F )ψ, da (F )ψ da (F )ψ, da (F )ψ +d A +d +d +d +d +d + +d +d + d 1 a + 1 F 1 ψ, +d d a + F ψ +d d 1 d a + 1 F 1 ψ, a + F ψ +d d 1 d F 1 ψ, a 1 a + F ψ +d d 1 d F 1 ψ, δ( 1 )F ψ +d d 1 d F 1 ψ, a + a 1 F ψ d 1 F 1 ψ, F 1 ψ +d d 1 d a F 1 ψ, a 1 F ψ hen, we ge: +d +d d 1 d n +d d 1 d a F 1 ψ, a 1 F ψ R nd (a F 1 ψ) (n) (s 1, s,, s n ) (a 1 F ψ) (n) (s 1, s,, s n )ds 1... ds n +d +d d 1 d (n + 1) (F 1 ψ) (n+1) (, s 1, s,, s n ) R nd n where: (F ψ) (n+1) ( 1, s 1, s,, s n )ds 1... ds n +d +d d 1 d g( 1, ) g( 1, ) : (n + 1) (F 1 ψ) (n+1) (, σ)(f ψ) (n+1) ( 1, σ)dσ a.e. R dn n : NF 1 ψ(,.), F ψ( 1,.) The coniniy of he map: ( 1, ) g( 1, )a.e. on [, + d], is a conseqence of he following ineqaliies: ɛ > g( 1 + ɛ, + ɛ) g( 1, ) NF 1 +ɛψ( + ɛ,.), F +ɛψ( 1 + ɛ,.) NF 1 ψ(,.), F ψ( 1,.) N(F 1 +ɛψ( + ɛ,.) F 1 ψ(,.)), F +ɛψ( 1 + ɛ,.) + NF 1 ψ(,.), F +ɛψ( 1 + ɛ,.) F ψ( 1,.) N(F 1 +ɛψ( + ɛ,.) F 1 ψ(,.). F +ɛψ( 1 + ɛ,.) + NF 1 ψ(,.). (F +ɛψ( 1 + ɛ,.) F ψ( 1,.) and of he coniniy of ( 1, ) F 1 ψ(,.) in he norm (3.4). Since g is bonded in [, + d] i follows ha: A β(d), where β >, i.e. A O(d ). n conclsion: 1 d d A (F )ψ, A (F )ψ 1 d Re +d dsa + s F s ψ, A (F )ψ + 1 d +d d 1 F 1 ψ, F 1 ψ + 1 d A

18 18 L. ACCARD*-W. AYED**-H. OUERDANE*** and, if d, we ge d d A (F )ψ, A (F )ψ Re a + F ψ, dsa + s F s ψ + F ψ, F ψ. Le ψ A + f m in D MAD (C) where f, f 1... f m are es fncions in C, and F is a whie noise adaped process, for each, so we obain: since: so: where hen a + F ψ, ds a + s F s a A + f n We denoe by where ds a + s F s ψ ds F ψ, a a + s F s ψ ds F ψ, a + s F s a ψ ds F ψ, a + s F s a ψ ds a + s F s [a, A + f n ] ds + ds a + s F s [ n ds a + s F s dsf()a + f n ] f i ()A + f n... Â+ f i + f()a + f n ds a + s F s a s A + f n... Â+ f i... A + f i [ n ] ds a + s F s f i ()A + f n... Â+ f i + f()a + f n n [ ] ds a + s F s f i ()A + f n... Â+ f i... A + f i + ds a + s F s f()a + f n n ds f i ()a + s F s A + f n... Â+ f i... A + f 1 + ds a + s F s f()a + f n [ n c T,ψ We noe ha ψ i F ψ : ds a + s F s A + f n... Â+ f i + c T,ψ max 1in ( f i,t, f,t ) ds a + s F s A + f n ], d d A (F )ψ, A (F )ψ n F ψ + c T,ψ [ A (F )ψ ] + ds a + s F s A + f n... Â+ f i A (F )ψ F ψ ψ i F ψ A (F )ψ i F ψ {ψ i A + f n... Â+ f i, A + f n, 1 i n} A (F )ψ i A (F )ψ F ψ

19 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 19 and A (F )ψ i ds F s ψ i + c T,ψi j ds A s (F )ψ ij A (F )ψ F ψ where C T,ψ max ψi F c T,ψi. A (F )ψ F ψ ψ i F ψ F s ψ i ds + C T,ψ F ψ ψ i F ψ F s ψ i ds + C T,ψ F ψ by Gronwall lemma, we obain A (F )ψ A (F )ψ F ψ e (C T,ψ F ψ ) ψ i F ψ A s (F )ψ F ψ ds A s (F )ψ F ψ ds F s ψ i ds. So we ge he resl where J(ψ) F ψ. Corollary 4.1. For ψ, we have, sing he fac ha F is whie noise adaped and Gromwall lemma: ds a + s F s e f,t ds [ f + 1] F s. The above esimae is similar o hose proved by Hdson and Parhasaray on he exponenial vecors. Corollary 4.. Le (F ) be a whie noise adaped process sch ha, for each n N and es fncions f, f 1 f n in C, he map ( 1, ) F 1 ψ(,.); ψ A + f n A + f 1 D MAD (C) is coninos nder he norm (3.4). Then he following ineqaliy holds for any T < : (4.5) ds a + s F s a s ψ c T,ψ ds F s ψ i ψ i J(ψ) where J(ψ) D, c T,ψ are defined by { } J(ψ) A + f n A + f 1, A + f n A, : 1 i n c T,ψ n max 1in ( f i,t, f,t )c T,ψ max 1in (e(c T,ψ F )T, e (c T,ψ i F i )T ) where f i,t sp s [,T ] f(s) and c T,ψ, c T,ψi are defined as in (4.1.a)

20 L. ACCARD*-W. AYED**-H. OUERDANE*** Proof. Using lemma (4.1), we ge: ds a + s F s a s ψ [ n ] ds a + s F s F s f i (s)a + f n A + f(s)a + f n A + f 1 + ds a + s F s n F s f i (s)a + f n A ˆ + f i A + f 1 ds a + s F s f(s)a + f n A + f1 [ n n. max ( f i,t ) 1in + f,t ds a + s F s A + f n A + f1 ds a + s F s A + f n A ψ ] max (n f i,t f,t ) max 1in 1in (e(c T,ψ F )T, e (c T,ψ i F i )T ) n [ ds F s A + f n A ] + ds F s A + f n A + f1. where (c T,ψ F ), (c T,ψi F i ) are defined as in (4.1.a). Corollary 4.3. Le (F ) be a whie noise adaped process sch ha, for each n N and es fncions f, f 1 f n in C, he map ( 1, ) F 1 ψ(,.); ψ A + f n A + f 1 D MAD (C) is coninos nder he norm (3.4). Then he following ineqaliies hold for any T < : (4.6) (4.7) a-: b-: where and ds F s a s ψ c ψ, ϕ J(ψ) ( ) 1 ds F s ϕ J(ψ) {A + f n... Â+ f i, A + f n, 1 i n} dsa + s F s ψ c ψ, max 1in ( f i,, f, ) e (C T,ψ J(ψ) ) where J(ψ) is he sbse of F defined by ψ i J(ψ) F s ψ i ds J(ψ) {ψ i A + f n... Â+ f i, A + f n 1 i n} D MAD,. denoes he cardinaliy, C T,ψ where f,t sp [,T ] f(). c-: (4.8) ds a + s F s a s ψ c T,ψ max c T,ψ i, c T,ψi max ( f j,t, f,t ). ψ i J(ψ) 1jn ds ψ i J(ψ) F s ψ i (4.1.a)

21 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 1 where J(ψ) D, c T,ψ are defined by { } J(ψ) A + f n A + f 1, A + f n A, : 1 i n c T,ψ n max 1in ( f i,t, f,t )c T,ψ max 1in (e(c T,ψ F )T, e (c T,ψ i F i )T ) where f i,t sp s [,T ] f(s) and c T,ψ, c T,ψi are defined as in (4.1.a). Proof. a- is obained by aking [, ] in proposiion 3.1. Also he proof of b- and c- are obained by replacing o by in hose of proposiion 4. and corollary 4.1. Corollary 4.4. Le H S a Hilber space called iniial space. The ineqaliies (3.3), (4.4), (4.5) are verified if we ake ψ ψ H S F where is in he iniial space H S and ψ is an elemen of he maximal algebraic domain. Proof. Using he fac ha: F ψ F ψ and he ineqaliies (3.3), (4.4) and (4.5), one has: ( ) 1 F s a s ds ψ c ψ, ds F s ϕ ϕ J(ψ) dsa + s F s ψ e (c T,ψ J(ψ) ) a + s F s a s ds ψ c T,ψ ψ i J(ψ) ds ψ i J(ψ) F s ψ i ds F s ψ i where c ψ,, c T,ψ and c T,ψ are defined in proposiions (3.1), (4.) and Corollary (4.1). 5. Normally ordered whie noise sochasic differenial eqaion 5.1. nrodcion and definiions. The normally ordered whie noise sochasic differenial eqaion: (5.1) U a + E U + F U a + a + G U a + H U U() U where (E ), (F ), (G ) and (H ) be measrable and locally bonded operaors acing on he iniial space H S. The meaning of eqaion (5.1) can be specified in wo differen ways: (i): as an inegral eqaion, i.e. (5.) U U + ds a + s E s U s + ds F s U s a s + ds a + s G s U s a s + ds H s U s where he inegrals on he righ hand side are defined in secion (3.1). (ii): as a weak eqaion in some domain D 1 ( or choice of his domain will be specified laer): (5.3) φ, U ψ a φ, E U ψ + φ, F U a ψ + a φ, E U a ψ + φ, E U ψ where φ and ψ are in D 1. Since also he noion of sochasic inegral reqires he specificaion of some domain, he wo mehods may lead o ineqivalen noions of solion. However he main goal of he heory is o prodce solions which are niary (in pariclar bonded). Wihin his class i can be proved ha, for a large family of coefficien processes (inclding he consan bonded ones, which are he mos sed in applicaions) he wo eqaions lead o he same solion.

22 L. ACCARD*-W. AYED**-H. OUERDANE*** 5.. Whie noise adaped normally ordered whie noise eqaion in R d. Using he above resls, we will prove he exisence and he niqeness of solion of a class of whi noise adaped normally ordered whie noise eqaion by: Definiion 5.1. A whie noise adaped normally ordered whie noise eqaion wih coefficiens is a normally ordered whie noise eqaion as defined above: ] (5.4) U [F 1 U a + a + F U + a + F 3 U a + F 4 U d where (F 1 ), (F ), (F 3 ) and (F 4 ) are, whie noise adaped processes in B(H S ) coninos for he norm operaor opology on B(H S ) Exisence and niqeness of he solion of a WN socahsic eqaion. Theorem 5.1. Consider he normally ordered whie noise eqaion: (5.5) U U + ds F 1 s U s a s + ds a + s F s U s + ds a + s F 3 s U s a s + ds F 4 s U s where (F 1 s ) s, (F s ) s, (F 3 s ) s and (F 4 s ) s are locally bonded coninos processes for he norm operaor opology on B(H S ) sch ha he maps: ( 1, ) F 1 ψ(,.), ( 1, ) F 3 1 ψ(,.) (6.6) are coninos for he norm (3.4) for each ψ D MAD (C) and 1, R +. Under he above condiions, eqaion (5.5) has a niqe whie noise adaped locally bonded coninos solion for all U whie noise adaped srongly coninos process on D MAD (C). Proof. i) Exisence. Define by indcion U U, and U n+1 F 1 s U n s a s ds + For simpliciy, we se he noaion: a + s F s U n s ds + U n+1 F i su n s dm i s a + s F 3 s U n s a s ds + F 4 s U n s ds The seqence (U n ) n N is well defined. n fac U is a srongly coninos process on D MAD (C). Sppose ha k n, U k is a whie noise adaped process on D MAD (C), srongly coninos and sch ha he map : ( 1, ) U k 1 ψ(,.) (1.1) is coninos for he norm (3.4). Using he scalar ype inegraor ineqaliies (3.3), (4.4) and (4.5), we have for any T, and each i {1,, 3, 4}: F 1 s U n s a s dsξ J 1 (ξ) (c T,1,η ) a + s F s U n s ds c T,,η a + s F 3 s U n s a s ds c T,3,η F 4 s U n s ds c T,4,η η J (ξ) η J 1 (ξ) η J 3 (ξ) η J 4 (ξ) ds F 1 s U n s η ds F s U n s η ds F 3 s U n s η ds F 4 s U n s η

23 WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 3 where c T,i,η, J i (ξ), i 1,, 3, 4 are defined as in (3.3), (4.4)and (4.5). Then U n ()ξ dm i 1 F i ( 1 )U n 1 (5.6) 1 ξ (5.7) c T,ξ K T ξ 1 J(ξ) d 1 U n 1 1 ξ 1 where: c T,ξ 4 max c T,i,η ; J(ξ) J i (ξ), K T sp F s. i {1,,3,4},η J(ξ) i s [,T ] Le s now prove ha U n+1 saisfy (1.1). n fac ɛ, ɛ > : U n+1 1 +ɛ ψ( + ɛ,.) U n+1 1 ψ(,.) U n+1 1 +ɛ ψ( + ɛ,.) U n+1 1 ψ( + ɛ,.) sing he ineqaliy 5.6, we ge: {c 1,ψ ψ i 1 +ɛ 1 ds F i su n s ψ i ( + ɛ,.) } 1 + {c 1 1,ψ + U n+1 1 ψ( + ɛ,.) U n+1 1 ψ(,.) + 1 +ɛ ψ j 1 dsf i su n s dm i sψ( + ɛ,.) 1 sing or hypohesis, we have he coniniy of he map 1 s F i su n s ψ i ( + ɛ,.) dsf i su n s dm i sψ( + ɛ,.) ψ(,.) U n+1 1 +ɛ ψ( + ɛ,.) U n+1 1 ψ(,.) ds F i su n s [ψ j ( + ɛ,.) ψ(,.) } 1 so i will be niform bonded on he compac [, + ɛ], hen, we obain ha: 1 +ɛ {c 1,ψ ds U s n ψ i ( + ɛ,.) } 1 < Kɛ, K > 1 ψ i Moreover nder he assmpion, he erms 1 ds U s n [ψ j ( + ɛ,.) ψ(,.) } 1 {c 1 1,ψ ψ j vanish when ɛ,so we ge he resl. Becase of he above hypohesis of he indcion, for all Ms i {a s, a + s, a s a + s } and i {1,, 3, 4}, FsU i s n is a coninos process inegrable wih respec o Ms, i hen we have ha U n+1 is a coninos process on D MAD (C) wih he same propery as U n. follows by indcion ha U n is srongly coninos on D MAD (C) for all n N. We will prove now he basic esimae: (5.8) U n ξ max η J(ξ) η. U. J(ξ) n KT n c n T,ξ (µ ξ(, )) n 1 n! For all n N and all T, where: c T,ξ 4 max c T,i,η, J(ξ) J i (ξ), K T sp F s. i {1,,3,4},η J(ξ) i s [,T ] Using he scalar ype inegraor ineqaliies (3.3), (4.4)and (4.5), we have for each i {1,, 3, 4}: Fs 1 Us n a s dsξ J 1 (ξ) (c T,1,η ) ds Fs 1 Us n η η J 1 (ξ)

24 4 L. ACCARD*-W. AYED**-H. OUERDANE*** a + s F s U n s ds c T,,η a + s F 3 s U n s ab s ds c T,3,η F 4 s U n s ds c T,4,η η J (ξ) η J 3 (ξ) η J 4 (ξ) ds F s U n s η ds F 3 s U n s η ds F 4 s U n s η where c T,i,η, J i (ξ), i 1,, 3, 4 are defined as in (3.3), (4.4)and (4.5). Then U n ()ξ dm i 1 F i ( 1 )U n 1 1 ξ c T,ξ K T d 1 U n 1 1 ξ 1 where: c T,ξ K T ξ 1 J(ξ) d 1 ( 1 ξ 1 J(ξ) ) dm i F i U n ξ 1 c T,ξ 4 max c T,i,η ; J(ξ) J i (ξ), K T sp F s i {1,,3,4},η J(ξ) i s [,T ] becase of he condiions on F i, hen: U n ()ξ c T,ξ K T Using he same ineqaliy again c T,ξ K T J(ξ) ξ 1 J(ξ) ξ J(ξ) d 1 1 d 1 1 An n-fold ieraion of he same argmens gives s he esimae: U n ()ξ c n T,ξ Kn T J(ξ) n 1 ξ n J(ξ) ) dm i (F i U n ξ 1 d U n 1 ξ 1 d 1 d max η J(ξ) η. U c n T,ξ Kn T J(ξ) n n 1 n! n 1 d n U ξ n Therefore he series n U n converges in he srong opology on D MAD (C) niformly on bonded inervals of R +. This implies ha i defines a process U srongly coninos on D MAD (C). We show ha U is a solion of (5.5). By he inegraor of scalar ype esimae we have, for all n N, n FsU i s n dmsξ i dmsf i s i Us k ξ c T,ξ K T Us k η ds k hen, we obain for all s [, ], k N, η J(ξ) η J(ξ) U k s η max η J(ξ) η U J(ξ) k K k+1 T c k T,ξ k 1 k! kn+1 hen he series k U k (s)η converges in he srong opology on he Fock space niformly on bonded inervals of R +. follow from Lebesge heorem ha lim n dm i s ( kn Fs i k U k s ) dm i sf i su s

25 This ogeher wih he ideniy WHTE NOSE APPROACH TO STOCHASTC NTEGRATON 5 kn+1 k U k ξ U ξ + dms i ( kn Fs i implies ha U verifies he sochasic differenial eqaion (5.5). ii)niqeness will be sfficien o prove ha all bonded coninos process Z, R + saisfying he following whie noise sochasic differenial eqaion: Z F i sz s dm i s ms be zero. n fac, for all ψ D MAD (C), applying or esimaes, we have: Z ψ c T,ψ K T Z s η ds η J(ψ) applying again he esimaes o he inegral in he righ-hand side (n - 1) imes and comping he ieraed inegral as we did before, we obain: k U k s ) ξ Z ψ sp st Z s max η J(ψ) η J(ψ) n KT n c n 1 T,ψ n n! Since his is re for all n N, i follows ha Z ψ for all [, T ]. References [1] L.Accardi, F.Fagnola and J.Qaegeber: A Represenaion Free Qanm Sochasic Calcls, A represenaion free Qanm Sochasic Calcls, Jorn. Fnc. Anal. 14 (1) (199) Volerra preprin N. 18 (199). [] L. Accardi, F. Fagnola: Sochasic negraion, in Qanm Probabiliy and Aplicaion, Lecre Noes in Mah, Vol. 133, pp, 6-19, Springer-Verlag, New York, (1988). [3] L.Accardi,.V.Vlovich and Y.G.L: A Whie Noise Approach o Classical and Qanm Sochasic Calcls, Volerra Preprin 375, Rome, Jly [4] L.Accardi: Qanm Probabiliy: An nrodcion o Some Basic deas and Trends, Modelos Esocasicos 16, Sociedad Mahemaica Mexicana, 1. [5] Accardi L., Qaegeber J.: o algebras of Gassian qanm fields, Jorn. Fnc. Anal. 85 (1988) [6] L.Accardi, Y.G.L.,.V.Volovich: Qanm heory and is sochasic limi. Springer Verlag () [7] Accardi L., L Y.G., Volovich.: Nonlinear exensions of classical and qanm sochasic calcls and essenially infinie dimensional analysis, in: Probabiliy Towards ; L. Accardi, Chris Heyde (eds.) Springer LN in Saisics 18 (1998) 1 33 Proceedings of he Symposim: Probabiliy owards wo hosand, Colmbia Universiy, New York, 6 Ocober (1995) [8] L. Accardi, W. Ayed and H. Oerdiane: Whie Noise Flows, in preparaion. [9] S. Aal and J. M. Lindsay: Qanm Sochasic Calcls wih maximal operaor domains.the annales of probabiliy, (4), Vol 3. [1] Ph. Biane: Calcl Sochasiqe non-commaif, Séminaire de Probabiliés XXX. Lecre Noe in Mah(168), Springer, Berlin. [11]. Gelfand and N. Vilenkin: Generelized fncions vol.1. Academic Press. [1] T. Hida: Brownian Moion. Springer, 199. [13] Hdson, R. L. and Parhasarahy, K. R.: Qanm ô s formla and sochasic evolion, Comm. Mah. Phys 93(1984), [14] H. Ko: Whie Noise Disribion Theory. C.R.C Press, Boca Raon, New York, London, Tokyo, (1996). [15] K. R. Parhasarahy: An nrodcion o Qanm Sochasic Calcls.(199)Birkhäser Verlag. Basel.Boson. Berlin. [16] P. A. Meyer: Qanm Probabiliy for Probabiliss, (1993), Springer, Berlin. [17] L. Schwarz: Theorie des disribions. Hermann, Paris. [18] K. Yosida: Fncional Analysis. Springer, (1978).

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

ON JENSEN S INEQUALITY FOR g-expectation

ON JENSEN S INEQUALITY FOR g-expectation Chin. Ann. Mah. 25B:3(2004),401 412. ON JENSEN S INEQUALITY FOR g-expectation JIANG Long CHEN Zengjing Absrac Briand e al. gave a conerexample showing ha given g, Jensen s ineqaliy for g-expecaion sally

More information

ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt

ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS. Cairo University, Orman, Giza 12221, Egypt a 1/α s)ds < Indian J. pre appl. Mah., 396): 491-507, December 2008 c Prined in India. ON THE OSCILLATION OF THIRD ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS SAID R. GRACE 1, RAVI P. AGARWAL 2 AND MUSTAFA

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

Compatible Versus Regular Well-Posed Linear Systems

Compatible Versus Regular Well-Posed Linear Systems Compaible Verss eglar Well-Posed Linear Sysems Olof J. Saffans Deparmen of Mahemaics Åbo Akademi Universiy FIN-25 Åbo, Finland Olof.Saffans@abo.fi hp://www.abo.fi/ saffans/ George Weiss Dep. of Elecr.

More information

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as

, u denotes uxt (,) and u. mean first partial derivatives of u with respect to x and t, respectively. Equation (1.1) can be simply written as Proceedings of he rd IMT-GT Regional Conference on Mahemaics Saisics and Applicaions Universii Sains Malaysia ANALYSIS ON () + () () = G( ( ) ()) Jessada Tanhanch School of Mahemaics Insie of Science Sranaree

More information

Chapter 2. First Order Scalar Equations

Chapter 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 information

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations

Applied Mathematics Letters. Oscillation results for fourth-order nonlinear dynamic equations Applied Mahemaics Leers 5 (0) 058 065 Conens liss available a SciVerse ScienceDirec Applied Mahemaics Leers jornal homepage: www.elsevier.com/locae/aml Oscillaion resls for forh-order nonlinear dynamic

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

Journal of Mathematical Analysis and Applications

Journal of Mathematical Analysis and Applications J. Mah. Anal. Appl. 411 2014 261 270 Conens liss available a ScienceDirec Jornal of Mahemaical Analysis and Applicaions www.elsevier.com/locae/jmaa On solions of Kolmogorov s eqaions for nonhomogeneos

More information

Srednicki Chapter 20

Srednicki Chapter 20 Srednicki Chaper QFT Problems & Solions. George Ocober 4, Srednicki.. Verify eqaion.7. Using eqaion.7,., and he fac ha m = in his limi, or ask is o evalae his inegral:! x x x dx dx dx x sx + x + x + x

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

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

Scalar Conservation Laws

Scalar Conservation Laws MATH-459 Nmerical Mehods for Conservaion Laws by Prof. Jan S. Heshaven Solion se : Scalar Conservaion Laws Eercise. The inegral form of he scalar conservaion law + f ) = is given in Eq. below. ˆ 2, 2 )

More information

4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be

4.2 Continuous-Time Systems and Processes Problem Definition Let the state variable representation of a linear system be 4 COVARIANCE ROAGAION 41 Inrodcion Now ha we have compleed or review of linear sysems and random processes, we wan o eamine he performance of linear sysems ecied by random processes he sandard approach

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

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

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

Kolmogorov s equations for jump Markov processes with unbounded jump rates

Kolmogorov s equations for jump Markov processes with unbounded jump rates DOI 10.1007/s10479-017-2538-8 FEINERG: PROAILITY Kolmogorov s eqaions for jmp Markov processes wih nbonded jmp raes Egene Feinberg 1 Manasa Mandava 2 Alber N. Shiryaev 3 Springer Science+siness Media New

More information

Finite-particle approximations for interacting Brownian particles with logarithmic potentials

Finite-particle approximations for interacting Brownian particles with logarithmic potentials c 218 The Mahemaical Sociey of Japan J. Mah. Soc. Japan Vol. 7, o. 3 (218) pp. 921 952 doi: 1.2969/jmsj/75717571 Finie-paricle approximaions for ineracing Brownian paricles wih logarihmic poenials By Yoske

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

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

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

L p -L q -Time decay estimate for solution of the Cauchy problem for hyperbolic partial differential equations of linear thermoelasticity ANNALES POLONICI MATHEMATICI LIV.2 99) L p -L q -Time decay esimae for soluion of he Cauchy problem for hyperbolic parial differenial equaions of linear hermoelasiciy by Jerzy Gawinecki Warszawa) Absrac.

More information

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

Stochastic delay differential equations driven by fractional Brownian motion with Hurst parameter H. 1 2

Stochastic delay differential equations driven by fractional Brownian motion with Hurst parameter H. 1 2 Bernolli 12(1), 26, 85 1 Sochasic delay differenial eqaions driven by fracional Brownian moion wih Hrs parameer H. 1 2 MARCO FERRANTE 1 and CARLES ROVIRA 2 1 Diparimeno di Maemaica Pra ed Applicaa, Universià

More information

Dispersive Systems. 1) Schrödinger equation 2) Cubic Schrödinger 3) KdV 4) Discreterised hyperbolic equation 5) Discrete systems.

Dispersive Systems. 1) Schrödinger equation 2) Cubic Schrödinger 3) KdV 4) Discreterised hyperbolic equation 5) Discrete systems. Dispersive Sysems 1) Schrödinger eqaion ) Cbic Schrödinger 3) KdV 4) Discreerised hyperbolic eqaion 5) Discree sysems KdV + + ε =, = ( ) ( ) d d + = d d =, =. ( ) = ( ) DISCONTINUITY, prescribed cri Collision

More information

Utility maximization in incomplete markets

Utility maximization in incomplete markets Uiliy maximizaion in incomplee markes Marcel Ladkau 27.1.29 Conens 1 Inroducion and general seings 2 1.1 Marke model....................................... 2 1.2 Trading sraegy.....................................

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

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

PH2130 Mathematical Methods Lab 3. z x

PH2130 Mathematical Methods Lab 3. z x PH130 Mahemaical Mehods Lab 3 This scrip shold keep yo bsy for he ne wo weeks. Yo shold aim o creae a idy and well-srcred Mahemaica Noebook. Do inclde plenifl annoaions o show ha yo know wha yo are doing,

More information

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004 ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform

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

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

Conservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations

Conservation Laws and Hamiltonian Symmetries of Whitham-Broer-Kaup Equations Indian Jornal of Science and Technology Vol 8( 78 84 Janary 05 ISSN (Prin : 0974-84 ISSN (Online : 0974-545 DOI : 0.7485/ijs/05/8i/47809 Conseraion Laws and Hamilonian Symmeries of Whiham-Broer-Kap Eqaions

More information

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT Inerna J Mah & Mah Sci Vol 4, No 7 000) 48 49 S0670000970 Hindawi Publishing Corp GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT RUMEN L MISHKOV Received

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

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

Generalized Chebyshev polynomials

Generalized 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 information

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations

A Sharp Existence and Uniqueness Theorem for Linear Fuchsian Partial Differential Equations A Sharp Exisence and Uniqueness Theorem for Linear Fuchsian Parial Differenial Equaions Jose Ernie C. LOPE Absrac This paper considers he equaion Pu = f, where P is he linear Fuchsian parial differenial

More information

t 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...

t 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 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

On a Fractional Stochastic Landau-Ginzburg Equation

On a Fractional Stochastic Landau-Ginzburg Equation Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn

More information

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

An impact of noise on invariant manifolds in nonlinear dynamical systems

An impact of noise on invariant manifolds in nonlinear dynamical systems JOURNAL OF MATHEMATICAL PHYSICS 51, 4272 21 An impac of noise on invarian manifolds in nonlinear dynamical sysems X Sn, a Jinqiao Dan, and Xiaofan Li Deparmen of Applied Mahemaics, Illinois Insie of Technology,

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

6. Stochastic calculus with jump processes

6. 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 information

Singular control of SPDEs and backward stochastic partial diffe. reflection

Singular control of SPDEs and backward stochastic partial diffe. reflection Singular conrol of SPDEs and backward sochasic parial differenial equaions wih reflecion Universiy of Mancheser Join work wih Bern Øksendal and Agnès Sulem Singular conrol of SPDEs and backward sochasic

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

Operators related to the Jacobi setting, for all admissible parameter values

Operators 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 information

Chapter 6. Systems of First Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations Chaper 6 Sysems of Firs Order Linear Differenial Equaions We will only discuss firs order sysems However higher order sysems may be made ino firs order sysems by a rick shown below We will have a sligh

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

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial

More information

arxiv:math/ v1 [math.nt] 3 Nov 2005

arxiv:math/ v1 [math.nt] 3 Nov 2005 arxiv:mah/0511092v1 [mah.nt] 3 Nov 2005 A NOTE ON S AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION D. A. GOLDSTON AND S. M. GONEK Absrac. Le πs denoe he argumen of he Riemann zea-funcion a he poin 1 + i. Assuming

More information

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

MATH 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 information

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

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n

More information

DESIGN OF TENSION MEMBERS

DESIGN OF TENSION MEMBERS CHAPTER Srcral Seel Design LRFD Mehod DESIGN OF TENSION MEMBERS Third Ediion A. J. Clark School of Engineering Deparmen of Civil and Environmenal Engineering Par II Srcral Seel Design and Analysis 4 FALL

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

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

STABILITY 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 information

Dual Representation as Stochastic Differential Games of Backward Stochastic Differential Equations and Dynamic Evaluations

Dual Representation as Stochastic Differential Games of Backward Stochastic Differential Equations and Dynamic Evaluations arxiv:mah/0602323v1 [mah.pr] 15 Feb 2006 Dual Represenaion as Sochasic Differenial Games of Backward Sochasic Differenial Equaions and Dynamic Evaluaions Shanjian Tang Absrac In his Noe, assuming ha he

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

Intuitionistic Fuzzy 2-norm

Intuitionistic Fuzzy 2-norm In. Journal of Mah. Analysis, Vol. 5, 2011, no. 14, 651-659 Inuiionisic Fuzzy 2-norm B. Surender Reddy Deparmen of Mahemaics, PGCS, Saifabad, Osmania Universiy Hyderabad - 500004, A.P., India bsrmahou@yahoo.com

More information

On R d -valued peacocks

On R d -valued peacocks On R d -valued peacocks Francis HIRSCH 1), Bernard ROYNETTE 2) July 26, 211 1) Laboraoire d Analyse e Probabiliés, Universié d Évry - Val d Essonne, Boulevard F. Mierrand, F-9125 Évry Cedex e-mail: francis.hirsch@univ-evry.fr

More information

OBJECTIVES OF TIME SERIES ANALYSIS

OBJECTIVES OF TIME SERIES ANALYSIS OBJECTIVES OF TIME SERIES ANALYSIS Undersanding he dynamic or imedependen srucure of he observaions of a single series (univariae analysis) Forecasing of fuure observaions Asceraining he leading, lagging

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

Omega-limit sets and bounded solutions

Omega-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 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

Math 334 Fall 2011 Homework 11 Solutions

Math 334 Fall 2011 Homework 11 Solutions Dec. 2, 2 Mah 334 Fall 2 Homework Soluions Basic Problem. Transform he following iniial value problem ino an iniial value problem for a sysem: u + p()u + q() u g(), u() u, u () v. () Soluion. Le v u. Then

More information

Emmanuel Cépa 1 and Dominique Lépingle 1

Emmanuel Cépa 1 and Dominique Lépingle 1 ESAIM: Probabiliy and Saisics December 1, Vol. 5, 3 4 URL: hp://www.emah.fr/ps/ BROWNIAN PARTICLES WITH ELECTROSTATIC REPULSION ON THE CIRCLE: DYSON S MODEL FOR UNITARY RANDOM MATRICES REVISITED Emmanel

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

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 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 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

EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE

EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Version April 30, 2004.Submied o CTU Repors. EXPLICIT TIME INTEGRATORS FOR NONLINEAR DYNAMICS DERIVED FROM THE MIDPOINT RULE Per Krysl Universiy of California, San Diego La Jolla, California 92093-0085,

More information

Elements of Stochastic Processes Lecture II Hamid R. Rabiee

Elements of Stochastic Processes Lecture II Hamid R. Rabiee Sochasic Processes Elemens of Sochasic Processes Lecure II Hamid R. Rabiee Overview Reading Assignmen Chaper 9 of exbook Furher Resources MIT Open Course Ware S. Karlin and H. M. Taylor, A Firs Course

More information

Math 10B: Mock Mid II. April 13, 2016

Math 10B: Mock Mid II. April 13, 2016 Name: Soluions Mah 10B: Mock Mid II April 13, 016 1. ( poins) Sae, wih jusificaion, wheher he following saemens are rue or false. (a) If a 3 3 marix A saisfies A 3 A = 0, hen i canno be inverible. True.

More information

Lecture 10: The Poincaré Inequality in Euclidean space

Lecture 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 information

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples

A Direct Method for Solving Nonlinear PDEs and. New Exact Solutions for Some Examples In. J. Conemp. Mah. Sciences, Vol. 6, 011, no. 46, 83-90 A Direc Mehod for Solving Nonlinear PDEs and New Eac Solions for Some Eamples Ameina S. Nseir Jordan Universiy of Science and Technology Deparmen

More information

Computers and Mathematics with Applications

Computers and Mathematics with Applications Compers and Mahemaics wih Applicaions 59 (00) 80 809 Conens liss available a ScienceDirec Compers and Mahemaics wih Applicaions jornal homepage: www.elsevier.com/locae/camwa Solving fracional bondary vale

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

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

Backward stochastic dynamics on a filtered probability space

Backward stochastic dynamics on a filtered probability space Backward sochasic dynamics on a filered probabiliy space Gechun Liang Oxford-Man Insiue, Universiy of Oxford based on join work wih Terry Lyons and Zhongmin Qian Page 1 of 15 gliang@oxford-man.ox.ac.uk

More information

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k Challenge Problems DIS 03 and 0 March 6, 05 Choose one of he following problems, and work on i in your group. Your goal is o convince me ha your answer is correc. Even if your answer isn compleely correc,

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

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

1 First Order Partial Differential Equations

1 First Order Partial Differential Equations Firs Order Parial Differenial Eqaions The profond sdy of nare is he mos ferile sorce of mahemaical discoveries. - Joseph Forier (768-830). Inrodcion We begin or sdy of parial differenial eqaions wih firs

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

STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES

STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES Novi Sad J. Mah. Vol. 46, No. 1, 2016, 15-25 STABILITY OF PEXIDERIZED QUADRATIC FUNCTIONAL EQUATION IN NON-ARCHIMEDEAN FUZZY NORMED SPASES N. Eghbali 1 Absrac. We deermine some sabiliy resuls concerning

More information

THE BERNOULLI NUMBERS. t k. = lim. = lim = 1, d t B 1 = lim. 1+e t te t = lim t 0 (e t 1) 2. = lim = 1 2.

THE BERNOULLI NUMBERS. t k. = lim. = lim = 1, d t B 1 = lim. 1+e t te t = lim t 0 (e t 1) 2. = lim = 1 2. THE BERNOULLI NUMBERS The Bernoulli numbers are defined here by he exponenial generaing funcion ( e The firs one is easy o compue: (2 and (3 B 0 lim 0 e lim, 0 e ( d B lim 0 d e +e e lim 0 (e 2 lim 0 2(e

More information

Engineering Letter, 16:4, EL_16_4_03

Engineering 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 information

DISCRETE GRONWALL LEMMA AND APPLICATIONS

DISCRETE GRONWALL LEMMA AND APPLICATIONS DISCRETE GRONWALL LEMMA AND APPLICATIONS JOHN M. HOLTE MAA NORTH CENTRAL SECTION MEETING AT UND 24 OCTOBER 29 Gronwall s lemma saes an inequaliy ha is useful in he heory of differenial equaions. Here is

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

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

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

GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS

GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS GCD AND LCM-LIKE IDENTITIES FOR IDEALS IN COMMUTATIVE RINGS D. D. ANDERSON, SHUZO IZUMI, YASUO OHNO, AND MANABU OZAKI Absrac. Le A 1,..., A n n 2 be ideals of a commuaive ring R. Le Gk resp., Lk denoe

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

The L p -Version of the Generalized Bohl Perron Principle for Vector Equations with Infinite Delay

The 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 information

A proof of Ito's formula using a di Title formula. Author(s) Fujita, Takahiko; Kawanishi, Yasuhi. Studia scientiarum mathematicarum H Citation

A proof of Ito's formula using a di Title formula. Author(s) Fujita, Takahiko; Kawanishi, Yasuhi. Studia scientiarum mathematicarum H Citation A proof of Io's formula using a di Tile formula Auhor(s) Fujia, Takahiko; Kawanishi, Yasuhi Sudia scieniarum mahemaicarum H Ciaion 15-134 Issue 8-3 Dae Type Journal Aricle Tex Version auhor URL hp://hdl.handle.ne/186/15878

More information

EXISTENCE OF S 2 -ALMOST PERIODIC SOLUTIONS TO A CLASS OF NONAUTONOMOUS STOCHASTIC EVOLUTION EQUATIONS

EXISTENCE OF S 2 -ALMOST PERIODIC SOLUTIONS TO A CLASS OF NONAUTONOMOUS STOCHASTIC EVOLUTION EQUATIONS Elecronic Journal of Qualiaive Theory of Differenial Equaions 8, No. 35, 1-19; hp://www.mah.u-szeged.hu/ejqde/ EXISTENCE OF S -ALMOST PERIODIC SOLUTIONS TO A CLASS OF NONAUTONOMOUS STOCHASTIC EVOLUTION

More information

EXERCISES FOR SECTION 1.5

EXERCISES 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 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

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method

A Mathematical model to Solve Reaction Diffusion Equation using Differential Transformation Method Inernaional Jornal of Mahemaics Trends and Technology- Volme Isse- A Mahemaical model o Solve Reacion Diffsion Eqaion sing Differenial Transformaion Mehod Rahl Bhadaria # A.K. Singh * D.P Singh # #Deparmen

More information