DIMENSIONAL REDUCTION IN NONLINEAR FILTERING: A HOMOGENIZATION APPROACH

Size: px
Start display at page:

Download "DIMENSIONAL REDUCTION IN NONLINEAR FILTERING: A HOMOGENIZATION APPROACH"

Transcription

1 DIMNSIONAL RDUCION IN NONLINAR FILRING: A HOMOGNIZAION APPROACH PR IMKLLR 1, N. SRI NAMACHCHIVAYA 2, NICOLAS PRKOWSKI 1, AND HOONG C. YONG 2 Abrac. We propoe a homogenized filer for mulicale ignal, which allow o reduce he dimenion of he yem. We prove ha he nonlinear filer converge o our homogenized filer wih rae. hi i achieved by a uiable aympoic expanion of he dual of he Zakai equaion, and by probabiliically repreening he correcion erm wih he help of BDSD. 1. Inroducion Filering heory i an eablihed field in applied probabiliy and deciion and conrol yem, which i imporan in many pracical applicaion from inerial guidance of aircraf and pacecraf o weaher and climae predicion. I provide a recurive algorihm for eimaing a ignal or ae of a random dynamical yem baed on noiy meauremen. More preciely, filering problem coni of an unobervable ignal proce X def = {X : } and an obervaion proce Y def = {Y : } ha i a funcion of X corruped by noie. he main objecive of filering heory i o ge he be eimae of X baed on he informaion Y = σ{y : }. def hi i given by he condiional diribuion π of X given Y or equivalenly, he condiional expecaion f(x ) Y for a rich enough cla of funcion. Since hi eimae minimize he mean quare error lo, we call π he opimal filer. he goal of filering heory i o characerize hi condiional diribuion effecively. In implified problem where he ignal and he obervaion model are linear and Gauian, he filering equaion i finie-dimenional, and he oluion i he well-known Kalman-Bucy filer. In more realiic problem, nonlineariie in he model lead o more complicaed equaion for π, defined by Zakai (1969) and Fujiaki e al. (1972), which decribe he evoluion of he condiional diribuion in he pace of probabiliy meaure (ee, for example, Bain and Crian (29), Kallianpur (198), Liper and Shiryaev (21)). I i impracical o implemen a numerical oluion o uch infinie dimenional ochaic evoluion equaion of he general nonlinear filering problem by finie difference or finie elemen approximaion. herefore, exended Kalman filer algorihm, which ue linear approximaion o he ignal dynamic and obervaion, have been ued exenively in everal applicaion. hee provide eenially a fir order approximaion o an infinie dimenional problem and can perform quie poorly in problem wih rong nonlineariie. Paricle filer have been well eablihed for he implemenaion of nonlinear filering in cience and engineering applicaion. Douce e al. (21) and Arulampalam e al. (22) provide comprehenive inigh ino paricle filering. However, due o dimenionaliy iue (ee, for example, Snyder e al. (28)) and compuaional complexiie ha arie in repreening he ignal deniy uing a high number of paricle, he problem of paricle filering in high dimenion i ill no compleely reolved. A a reul of hee difficulie, we have eablihed a novel paricle filering mehod Park e al. (211) for mulicale ignal and obervaion procee ha combine he homogenizaion wih filering echnique. he heoreical bai for hi new capabiliy i preened in hi paper. 21 Mahemaic Subjec Claificaion. 6G35, 35B27, 6H15, 6H35. Key word and phrae. nonlinear filering; dimenional reducion; homogenizaion; paricle filering; aympoic expanion; SPD; BDSD. 1

2 2 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG he reul preened here are e wihin he conex of low-fa dynamical yem, where he rae of change of differen variable differ by order of magniude. Muliple ime cale occur in model hroughou he cience and engineering field. For example, climae evoluion i governed by fa amopheric and low oceanic dynamic and ae dynamic in elecric power yem coni of fa- and lowly-varying elemen. hi paper addree he effec of he mulicale ignal and obervaion procee via he udy of he Zakai equaion. We conruc a lower dimenional Zakai equaion in a canonical way. hi problem ha alo been udied in Park e al. (21) uing a differen approach from wha i preened here. In moderae dimenional problem, paricle filer are an aracive alernaive o numerical approximaion of he ochaic parial differenial equaion (SPD) by finie difference or finie elemen mehod. For he reduced nonlinear model an appropriae form of paricle filer can be a viable and ueful cheme. Hence, Lingala e al. (212) preen he numerical oluion of he lower dimenional ochaic parial differenial equaion derived here, a i i applied o a chaoic high-dimenional mulicale yem. In general, hi paper provide rigorou mahemaical reul ha uppor he numerical algorihm baed on he idea ha ochaically averaged model provide qualiaively ueful reul which are poenially helpful in developing inexpenive lower-dimenional filering a demonraed by Park e al. (211) in he conex of homogenized paricle filer and by Harlim and Kang (212) in he conex of averaged enemble Kalman filer. he convergence of he opimal filer o he homogenized filer i hown uing backward ochaic differenial equaion (BSD) and aympoic echnique. Le u decribe he main reul. We aume he ignal i given a oluion of he wo ime cale ochaic differenial equaion (SD) dx = b(x, Z )d + σ(x, Z )dv dz = 1 f(x, Z )d + 1 g(x, Z )dw. Here X i he low componen and Z i he fa componen. We aume ha for every fixed x, he oluion Z x of dz x = f(x, Z x )d + g(x, Z x )dw i ergodic and converge rapidly o i unique aionary diribuion. In hi cae i i well known ha X converge in diribuion o a diffuion X which i governed by an SD dx = b(x )d + σ(x )dv. hi X i ued o conruc an averaged filer π. We denoe he opimal filer for he full yem by π. Define he x-marginal of π a π,x, i.e. ϕ(x)π,x (dx) = ϕ(x)π (dx, dz). Our main reul i hen heorem. Under he aumpion aed in heorem 3.1, for every p 1 and here exi C >, uch ha for every ϕ C 4 b ( Q π,x (ϕ) π (ϕ) p ) 1/p C ϕ 4,. In paricular, here exi a meric d on he pace of probabiliy meaure, uch ha d generae he opology of weak convergence, and uch ha for every here exi C > uch ha Q d(π,x, π ) C. We begin in Secion 2 by preening he general formulaion of he mulicale nonlinear filering problem. Here we decribe he meaure-valued Zakai equaion and inroduce he homogenized equaion ha we eek o derive for he reduced dimenion unnormalized filer. Secion 3 preen

3 DIMNSIONAL RDUCION IN NONLINAR FILRING 3 he formal aympoic expanion of he muli cale Zakai equaion ha reul in everal SPD. We alo preen he main reul of hi paper in hi ecion. Secion 4 provide he probabiliic repreenaion of he SPD, ha i, we decribe he oluion of he infinie dimenional SPD by finie dimenional backward doubly ochaic differenial equaion (BDSD). We reae ome of he reul in hi conex due o Rozovkii (199) and Pardoux and Peng (1994) a he end of hi ecion. We preen ome of he preliminary reul of Pardoux and Vereennikov (23) on convergence of he raniion funcion of Z x in ecion 5. hee eimae are ued in he proof of he main reul preened in ecion Formulaion of mulicale nonlinear filering problem Le (Ω, F, (F ), Q) be a filered probabiliy pace ha uppor a (k + l + d)-dimenional andard Brownian moion (V, W, B). Le he ignal (X, Z ) be a wo ime cale diffuion proce wih a fa componen Z and a low componen X : (1) dx = b(x, Z )d + σ(x, Z )dv dz = 1 f(x, Z )d + 1 g(x, Z )dw, where X R m, Z R n, W R l and V R k are independen andard Brownian moion, b : R m+n R m, σ : R m+n R m k, f : R m+n R n, g : R m+n R n l. All he funcion above are aumed o be Borel-meaurable. For fixed x R m, define (2) dz x = f(x, Z x )d + g(x, Z x )dw. Aume ha for all x R m, Z x i ergodic and converge rapidly oward i aionary meaure µ(x, ). We will make hi precie laer. he d-dimenional obervaion Y i given by Y = h(x, Z )d + B wih Borel-meaurable h : R m+n R d. B i aumed o be a d-dimenional andard Brownian moion ha i independen of W and V. Define Y = σ(y : ) N, where N are he Q-negligible e. For a finie meaure π on R m+n and for a bounded meaurable funcion ϕ on R m+n denoe π(ϕ) = ϕ(x, z)π(dx, dz). hen our aim i o calculae he meaure-valued proce (π, ) deermined by Define he Giranov ranform dp ( dq = D = exp F π (ϕ) = ϕ(x, Z ) Y. h(x, Z ) db 1 2 ) h(x, Z) 2 d. Under P, he obervaion proce, Y, i a Brownian moion and independen of (X, Z ). By he Kallianpur-Sriebel formula, P ϕ(x Q ϕ(x, Z ) Y, Z ) dq F dp Y = dq F P dp Y wih ( dq dp = D = exp F h(x, Z ) dy 1 2 ) h(x, Z) 2 d.

4 4 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG So if we define hen ρ (ϕ) = P ( ϕ(x, Z ) exp h(x, Z) dy 1 2 π (ϕ) = ρ (ϕ) ρ (1). ) h(x, Z) 2 d Y, Denoe by L = 1 L F + L S he differenial operaor aociaed o (X, Z ). ha i, n L F = f i (x, z) + 1 n (gg 2 ) ij (x, z) z i 2 z i z j L S = b i (x, z) x i (σσ 2 ) ij (x, z) x i x j where denoe he ranpoe of a marix or a vecor. hen he unnormalized meaure-valued proce, ρ, aifie he Zakai equaion: (3) dρ (ϕ) = ρ (L ϕ)d + ρ (hϕ)dy ρ (ϕ) = Q ϕ(x, Z) for every ϕ Cb 2(Rm+n, R) (ee, for example, Bain and Crian (29)). For k, Cb k i he pace of k ime coninuouly differeniable funcion f, uch ha f and all i parial derivaive up o order k are bounded. he heory of ochaic averaging (ee, for example, Papanicolaou e al. (1977)) ell u ha under uiable condiion, X converge in law o X a, where X i he oluion of an SD dx = b(x )d + σ(x )dw for uiably averaged b and σ. Denoe he generaor of X by L. We wan o how ha a long a we are only inereed in eimaing he low componen, we can ake advanage of hi fac. More preciely, we wan o find a homogenized (unnnormalized) filer ρ, uch ha for mall, ρ,x which i he x-marginal of ρ, i cloe o ρ. he x-marginal of ρ i defined a ρ,x (ϕ) = ϕ(x)ρ (dx, dz) R m+n for every meaurable bounded ϕ : R m R, and ρ i he oluion of (4) dρ (ϕ) = ρ ( Lϕ)d + ρ ( hϕ)dy ρ (ϕ) = Q ϕ(x ), where h i a uiably averaged verion of h. he meaure-valued procee π and π,x are hen defined in erm of ρ and ρ,x a π wa defined in erm of ρ : π (ϕ) = ρ (ϕ) ρ (1) and π,x (ϕ) = ρ,x (ϕ) ρ,x (ϕ). Noe ha he homogenized filer i ill driven by he real obervaion Y and no by a homogenized obervaion, which i pracical for implemenaion of he homogenized filer in applicaion ince uch homogenized obervaion i uually no available. However, hould uch homogenized obervaion be available, uing i would lead o lo of informaion for eimaing he ignal compared o uing he acual obervaion.

5 DIMNSIONAL RDUCION IN NONLINAR FILRING 5 In hi paper, we will prove L 1 -convergence of he acual filer o he homogenized filer, i.e. we will how ha for any >, lim d(π,x, π ) =, where d denoe a uiable diance on he pace of probabiliy meaure ha generae he opology of weak convergence. hi convergence reul i hown in Park e al. (21) for a wo-dimenional mulicale ignal proce wih no drif in he fa componen SD. Here, we exend he reul o an R m+n -dimenional ignal proce wih drif and diffuion coefficien of he fa and low componen dependen on boh componen. he proof of Park e al. (21) i baed on repreening he low componen a a ime-changed Brownian moion under a uiable meaure, which canno be exended eaily o he mulidimenional eing we aume here. Baed on (3) and (4), he filer convergence problem i a problem of homogenizaion of a SPD. In Papanicolaou e al. (1977), homogenizaion of diffuion procee wih periodic rucure i done uing he maringale problem approach. In Papanicolaou and Kohler (1975) and Chaper 2 of Benouan e al. (1978), limi behavior of ochaic procee i udied uing aympoic analyi. Benouan e al. (1978) udie linear SPD wih periodic coefficien and alo ued a probabiliic approach in Chaper 3. Homogenizaion in he nonlinear filering problem framework ha been udied in Benouan and Blankenhip (1986) and Ichihara (24) via aympoic analyi on a dual repreenaion of he nonlinear filering equaion. A far a we are aware, Ichihara (24) ha ued BSD for udying homogenizaion of Zakai-ype SPD for he fir ime. Our convergence proof applie BSD echnique by invoking he dual repreenaion of he filering equaion and uing aympoic analyi o deermine he limi behavior of he oluion of he backward equaion. Pardoux and Vereennikov (23) give precie eimae for he raniion funcion of an ergodic SD of he ype (2), and hee reul are ued in our proof. o our knowledge, uch mehod of homogenizaion for SPD combining BSD and aympoic mehod ha no been done before. o our knowledge, a reul preened in Chaper 6 of Kuhner (199) i he cloe o he reul preened in hi paper. In heorem of Kuhner (199) i i hown ha for a fixed e funcion, he difference of he unnormalized acual and homogenized filer for mulicale jumpdiffuion procee converge o zero in diribuion. Sandard reul hen give convergence in probabiliy of he fixed ime marginal. Kuhner (199) mehod of proof i by averaging he coefficien of he SD for he unnormalized filer and howing ha he limi of boh filer aify he ame SD ha poee a unique oluion. We obain L p convergence of he meaure valued proce, no ju for fixed e funcion, and we are able o quanify he rae of convergence, which, o he be of our knowledge, ha no been achieved before in homogenizaion of nonlinear filer.. In Klepina e al. (1997), convergence of he nonlinear filer i hown in a very general eing, baed on convergence in oal variaion diance of he law of (X, Y ). hi i hen applied o wo example. Since he diffuion marix of our low componen i allowed o depend on he fa componen, our reul are no a pecial cae. In he example of Klepina e al. (1997), X converge o X in probabiliy, which i no longer he cae in our eing. However i migh be poible o apply he oal variaion echnique developed in Klepina e al. (1997) o obain convergence in our eing. Only he rae of convergence canno be deermined wih hee echnique. For a given bounded e funcion ϕ and erminal ime, we follow Pardoux (1979) in inroducing he aociaed dual proce v,,ϕ (x, z), which i a dynamic verion of P ϕ(x ) D Y : v,,ϕ (x, z) = P,x,z ϕ(x ) D, Y, where P,x,z i he meaure under which X and Z are governed by he ame dynamic a under P, bu (X, Z ) ay in (x, z) unil ime, hen i ar o follow he SD dynamic. D, = D ( D ) 1 ; and Y, = σ(y r Y : r ) N (recall ha N denoe he

6 6 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Q-negligible e). From he Markov propery of (X, Z ) i follow ha for any, : ρ (v,,ϕ ) = ρ,x (ϕ). In paricular (becaue a ime, ρ i ju he aring diribuion of (X, Z )): ρ,x (ϕ) = v,,ϕ (x, z)q (X,Z ) (dx, dz). Similarly inroduce where v,,ϕ (x) = P,x ϕ(x ) D, Y,, ( D, = exp h(x r ) dyr 1 ) h(x r ) 2 dr 2 and P,x i he meaure under which X i governed by he ame dynamic a under P, bu ay in x unil ime. We can alo how ha for any, : ρ (v,,ϕ ) = ρ (ϕ), o ha ρ (ϕ) = v,,ϕ (x)q X (dx). Noe ha Q X = Q X, becaue he homogenized proce ha he ame aring diribuion a he unhomogenized one. Now fix and ϕ Cb 2(Rm, R) and wrie v = v,,ϕ and v = v,,ϕ. Our aim i o how ha for nice e funcion ϕ, and for he dual procee v and v defined above, v (x, z) v (x) p i mall (in a way ha will depend on x and z). hen ρ,x (ϕ) ρ (ϕ) p = (v(x, z) v(x))q p (X,Z ) (dx, dz) v(x, z) v(x) p Q (X,Z ) (dx, dz) = v(x, z) v(x) p Q (X,Z ) (dx, dz) will alo be mall a long a Q (X,Z ) i well behaved. 3. Formal expanion of he filering equaion and he main reul Before we coninue, le u change noaion: For large par of hi aricle we will only work under P, and he proce Y i a Brownian moion under P which i independen of (X, Z, X ). herefore from now on we wrie P inead of P and B inead of Y o faciliae he reading. he diribuion and noaion for he Markov procee (X, Z, X ) do no change. he key poin i now ha v and v olve backward SPD: (5) and (6) dv (x, z) = L v (x, z)d + h(x, z) v (x, z)db v (x, z) = ϕ(x) dv (x) = Lv (x, z)d + h(x) v (x)db v (x) = ϕ(x). Here and everywhere in hi aricle, d B denoe Iô backward inegral. We formally expand v a v (x, z) = u (x, z) + u 1 / (x, z) + 2 u 2 / (x, z). Noe ha rigorouly hi doe no make any ene, becaue:

7 DIMNSIONAL RDUCION IN NONLINAR FILRING 7 We work wih equaion wih erminal condiion. Bu when we end, hen / converge o infiniy. So for which ime hould he erminal condiion of e.g. u 1 be defined? he erm in hi expanion will all be ochaic. hen if u 1 i adaped o F B, he ochaic inegral u 1 / (x, z)d B a priori doe no make any ene for < 1. However if we do uch a formal aympoic expanion, and hen call v (, x) = u (, x), ψ 1 (, x, z) = u 1 / (x, z), R(, x, z) = 2 u 2 / (x, z) (of coure all erm excep v depend on, which we omi in he noaion o faciliae he reading), hen hee erm have o olve he following equaion: dv (x) = Lv (x, z)d + h(x) v (x)d B (7) (8) dψ 1 (x, z) = 1 L F ψ 1 (x, z)d + (L S L)v (x)d + ( h(x, z) h(x) ) v (x)d B dr (x, z) = L R (x, z)d + L S ψ 1 (x, z)d wih erminal condiion + h(x, z) ( ψ 1 (x, z) + R (x, z) ) d B v (, x) = ϕ(x), ψ 1 (, x, z) = R(, x, z) =. Noe ha he equaion for v i exacly he deired equaion (6). By exience and uniquene of he oluion o hee linear equaion, we can apply uperpoiion o obain ha hen indeed v (x, z) = v (x) + ψ 1 (x, z) + R (x, z). herefore he problem of howing L p -convergence of v o v reduce o howing L p -convergence of ψ 1 + R o. o achieve hi, we will give probabiliic repreenaion of ψ 1 and R in erm of backward doubly ochaic differenial equaion. hi will allow u o apply he exiing eimae for he raniion funcion of Z x from Pardoux and Vereennikov (23). I will be convenien for u o work wih funcion ha are mooher in heir x-componen han hey are in heir z-componen or vice vera. o do o, inroduce he funcion pace C k,l (R m R n, R d ): For θ : R m R n R d, θ = θ(x, z), wrie θ C k,l (R m R n, R d ), if θ i k ime coninuouly differeniable in i x-componen and l ime coninuouly differeniable in i z-componen. If θ a well a i parial derivaive up o order (k, l) are bounded, wrie θ C k,l b (Rm R n, R d ). Inroduce he following aumpion: (H a ) For he exience of a aionary diribuion µ(x, dz) for Z x, we uppoe ha here exi M >, α >, uch ha for all z M up f(x, z), z C z α. x For he uniquene of he aionary diribuion µ(x, dz) of Z x, we uppoe uniform ellipiciy, i.e. ha here are < λ Λ <, uch ha λi gg (x, y) ΛI in he ene of poiive emi-definie marice (I i he uni marix). (HF k,l ) he coefficien of he fa diffuion aify f C k,l b (Rm R n, R n ) and g C k,l b (Rm R n, R n k ). (HS k,l ) he coefficien of he low diffuion aify b C k,l b (Rm R n, R m ) and σ C k,l b (Rm R n, R m k ). (HO k,l ) he obervaion funcion h aifie h C k,l b (Rm R n, R d ).

8 8 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG We will uually wrie p (x, dz) inead of µ(x, dz). Alo inroduce he noaion p (z, θ; x) := θ(x, z )p (z, z ; x)dz := z θ(z x ) R n where z denoe he aring poin of Z x, and z p (z, z ; x) i he deniy of Z x if a ime i i ared in z. Noe ha he deniy exi for all > under he condiion (H a ), becaue of he uniform ellipiciy of gg. Similarly p (θ; x) = θ(x, z)p (x, dz). R n Le he differenial operaor L be defined a L = bi (x) + 1 x i 2 2 ā ij (x, z) x i x j where b(x) = p (b; x) and ā = p (σσ ; x). Alo define h(x) = p (h; x). We inroduce he following noaion: A muliindex α = (α 1,..., α m ) N n α = α α m. Given uch a muliindex, define he differenial operaor α D α = x α xαm m Finally inroduce he following norm for f Cb k(rm, R n ): f k, = D α f where i he uual upremum norm. Our main reul i α k i of order heorem 3.1. Aume (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ), and ha he iniial diribuion Q (X,Z ) ha finie momen of every order. hen for every p 1 and here exi C >, uch ha for every ϕ Cb 4 ( Q π,x (ϕ) π (ϕ) p ) 1/p C ϕ 4,. In paricular, here exi a meric d on he pace of probabiliy meaure, uch ha d generae he opology of weak convergence, and uch ha for every here exi C >, uch ha Q d(π,x, π ) C. hi reul will be proven in Secion 6. In paricular we can ue Borel-Canelli o conclude ha if ( n ) converge quickly enough o, hen π n will a.. converge weakly o π. he idea are raher imple: We repreen he backward SPD by finie-dimenional ochaic equaion (hi will be BDSD). he diffuion operaor ge replaced by he aociaed diffuion. We are able o olve hoe finie-dimenional equaion explicily, or a lea give explici eimae up o an applicaion of Gronwall. hi allow u o eimae ψ 1 and R in erm of he raniion funcion of he fa diffuion. Bu Pardoux and Vereennikov (23) proved very precie eimae for hi raniion funcion. hee eimae allow u o obain he convergence. While he idea are imple, he precie formulaion and he acual proof are quie echnical. We ar by decribing he probabiliic repreenaion.

9 (9) DIMNSIONAL RDUCION IN NONLINAR FILRING 9 4. Probabiliic repreenaion of SPD In hi ecion, we derive probabiliic repreenaion for SPD of he form dψ(ω,, x) = Lψ(ω,, x)d + f(ω,, x)d ψ(, x) = ϕ(ω, x), + (g(ω,, x) + G(ω,, x)ψ(ω,, x))d B, where ψ : Ω, R m R, f : Ω, R m R, g : Ω, R m R 1 d, and G : Ω, R m R 1 d, ϕ : Ω R m R are all joinly meaurable, and (B :, ) i a d-dimenional andard Brownian moion under he meaure P. quaion (9) repreen he general form of he equaion (7) and (8) for he correcor ψ 1 (x, z) and error R (x, z), repecively. he differenial operaor L i given by L = b i (x) x i a ij (x) x i x j for meaurable b : R m R m and a : R m S m m (S m m denoe poiive emidefinie ymmeric marice). We will repreen hee equaion in erm of BDSD a inroduced by Pardoux and Peng (1994). Noe ha for hee linear equaion i i poible o give a Feynman-Kac ype repreenaion wihou uing BDSD. hi i done, for example, in Rozovkii (199) ( he Mehod of Sochaic Characeriic ). However he BDSD-repreenaion ha he advanage ha i permi u o apply Gronwall lemma. hi would no be poible wih he mehod of ochaic characeriic. A BDSD i an inegral equaion of he form Y = ξ + f(, Y, Z )d + g(, Y, Z )db Z dw where B and W are independen Brownian moion. he oluion (Y, Z ) will be F, B F W - meaurable. Saring from he noion of BDSD, we can define forward-backward doubly ochaic differenial equaion. Le σ = a 1/2 and X,x = x + b(x,x )d + X,x = x for We hen define he following BDSD dy,x Y,x = f(, X,x = ϕ(x,x ) )d + (g(, X,x )d + G(, X,x σ(x,x )dw for )Y,x )db Z,x dw I urn ou ha Y give a finie-dimenional probabiliic repreenaion for equaion (9), more preciely we have Y,x = ψ(, x). hi i no compleely covered by Pardoux and Peng (1994), becaue we have random unbounded coefficien, and becaue we do no aume he diffuion marix a o have a mooh quare roo. On he oher ide, he equaion i of a paricularly imple linear ype. In he remainder of hi ecion, we give he precie aemen and proof for hi repreenaion. hi can be kipped a fir reading. We will no be able o ge an exience reul for claical oluion of he above SPD from he heory of BDSD: hi i due o he fac ha for hi we would need moohne properie of a quare roo of a. Bu even when a i mooh, in he degenerae ellipic cae i doe no need o have a mooh quare roo (ee, for example, Sroock (28), Chaper 2.3). Inead we will ue he exience reul of Rozovkii (199) and only reprove he uniquene reul of Pardoux and Peng (1994) in our eing. hi will work under Lipchiz coninuiy of a 1/2.

10 1 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Define for F,B, = σ(b u B : u ) and F, B a he compleion of F,B, polynomial growh: under P. Inroduce he pace of adaped random field of Definiion. P (R m, R n ) i he pace of random field H : Ω, R m R n ha are joinly meaurable in (ω,, x), and for fixed (, x), ω H(ω,, x) i F, B -meaurable. Furher for fixed ω ouide a null e, H ha o be joinly coninuou in (, x), and i ha o aify he following inequaliy: For every p 1 here i C p >, q >, uch ha for all x R m up H(, x) p C p (1 + x q ) We make he following aumpion on he coefficien of he SPD: (S k ) f and g are k ime coninuouly differeniable and he parial derivaive up o order k are all in P. G i (k + 1) ime coninuouly differeniable and he parial derivaive up o order (k + 1) are all uniformly bounded in (ω,, x). ϕ i k ime coninuouly differeniable, and all parial derivae of order o k grow a mo polynomially. We make he following aumpion on he coefficien of he differenial operaor L: (D k ) b C k b (Rm, R m ), a C k b (Rm, S m m ), and a i degenerae ellipic: For every ξ R m and every x R m, hen we have he following reul: a(x)ξ, ξ = a ij (x)ξ i ξ j. Propoiion 4.1. Aume (S k ) and (D k ) for ome k 3. hen he equaion (9) ha a unique claical oluion ψ in he ene ha for every fixed ω ouide a null e, ψ(ω,, ) C,k 1 (, R d, R), ψ and i parial derivaive are in P (R m, R), and ψ olve he inegral equaion. If ψ i any oher oluion of he inegral equaion, hen ψ and ψ are indiinguihable. If furher f, g and ϕ a well a heir derivaive up o order k are uniformly bounded in (ω,, x), hen for any p > here exi C p, q > (only depending on p, he dimenion involved, he bound on a, b and G, and on ), uch ha for all α k 1 and x R m : up D α ψ(, x) p C(1 + x q ) ϕ p k, + up f(, ) p k, + up g(, ) p k, Proof. hi i a combinaion of heorem and Corollary of Rozovkii (199) (he claimed bound i only given for he equaion in unweighed Sobolev pace, in Corollary Bu from ha we can deduce he reul for he weighed Sobolev cae). he only hing we need o verify i ha our polynomial growh aumpion on he coefficien i compaible wih he Sobolev norm condiion here. Bu if θ P (R m, R n ), hen for any p 1 here cerainly i an.

11 DIMNSIONAL RDUCION IN NONLINAR FILRING 11 r < uch ha θ ake i value in he weighed L p -pace wih weigh (1 + x 2 ) r/2 : θ(, x) p (1 + x 2 ) r 2 dx up θ(, x) p (1 + x 2 ) r 2 dx up = up θ(, x) p (1 + x 2 ) r 2 dx C p (1 + x q )(1 + x 2 ) r 2 dx < for mall enough r. Now we combine hi reul wih he heory of BDSD: Le (W :, ) be an n-dimenional andard Brownian moion ha i independen of B. For, F W, i defined analogouly o F B,. For we e F = F B, F W. Noe ha hi i no a filraion, a i i neiher decreaing nor increaing in. Inroduce he following noaion: H 2 (Rm ) i he pace of meaurable R m -valued procee Y.. Y i F -meaurable and Y 2 d <. S 2 (Rm ) i he pace of coninuou adaped R m -valued procee Y.. Y F and A BDSD i an inegral equaion of he form (1) Y = ξ + f(,, Y, Z )d + up Y 2 <. g(,, Y, Z )db Z dw, where f :, Ω R R 1 n R, g :, Ω R R 1 n R 1 l, and for fixed y R, z R 1 n he procee (ω, ) f(, ω, x, z) and (ω, ) g(, ω, x, z) are (F B, F W ) B(R)-meaurable, and for every, f(,, x, z) and g(,, x, z) are F -meaurable. (Y, Z) will be called oluion of (1) if (Y, Z) S 2 (R) H2 (R1 n ) and if he couple olve he inegral equaion. We will alo wrie he equaion in differenial form: dy = f(, Y, Z )d + g(, Y, Z )d B Z dw. Oberve ha wih uiable adapaion, all of he following reul alo hold in he mulidimenional cae, i.e. for Y R m. We reric o one-dimenional Y for impliciy and becaue ulimaely we are only inereed in ha cae. Pardoux and Peng (1994) how ha under he following condiion, equaion (1) ha a unique oluion: ξ L 2 (Ω, F, P; R) for any (y, z) R R 1 n : f(,, y, z) H 2 (R) and g(,, y, z) H2 (R1 k ) f and g aify Lipchiz condiion and g i a conracion in z: here exi conan L > and < α < 1.. for any (ω, ) and y 1, y 2, z 1, z 2 : f(, ω, y 1, z 1 ) f(, ω, y 2, z 2 ) 2 L( y 1 y z 1 z 2 2 ) g(, ω, y 1, z 1 ) g(, ω, y 2, z 2 ) 2 L y 1 y α z 1 z 2 2. and

12 12 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Now we wan o aociae a diffuion X o he differenial operaor L. o do o, aume ha (D k ) i aified for ome k 2. hen σ := a 1/2 i Lipchiz coninuou by Lemma of Sroock (28). Hence for every (, x), R m, here exi a rong oluion of he SD X,x = x + b(x,x )d + X,x = x for. Aociae he following BDSD o (9): (11) dy,x Y,x = f(, X,x = ϕ(x,x ). )d + (g(, X,x ) + G(, X,x σ(x,x )dw for, )Y,x )db Z,x dw, Under he aumpion (S k ) and (D k ) for k 2, hi equaion ha a unique oluion. Propoiion 4.2. Aume (S k ) and (D k ) for ome k 3. hen he unique claical oluion ψ of he SPD (9) i given by ψ(, x) = Y,x, where (Y,x, Z,x ) i he unique oluion of he BDSD (11). We can give exacly he ame proof a in Pardoux and Peng (1994), heorem 3.1, aking advanage of he independence of B and W. For he reader convenience, we include i here. Proof. Le ψ be a claical oluion of (9). I uffice o how ha (ψ(, X,x ), Dψ(, X,x )σ(x,x ) : ) olve he BDSD (11). Here Dψ i he gradien of ψ. For hi purpoe, conider a pariion = < 1 < < n = of,. hen and ψ(, X,x n 1 ) = ψ(, X,x ) + (ψ( i, X,x ) ψ( i+1, X,x i+1 )) = ϕ(x,x i= i n 1 ) + (ψ( i, X,x ) ψ( i+1, X,x i+1 )) i= ψ( i,x,x i ) ψ( i+1, X,x i+1 ) = (ψ( i, X,x ) ψ( i, X,x i+1 )) + (ψ( i, X,x i+1 ) ψ( i+1, X,x = i ( i i i+1 i i+1 i Lψ( i, X,x )d + i i+1 (Lψ(, X,x i+1 ) + f(, X,x i+1 ))d i i+1 )) ) Dψ( i, X,x )σ(x,x )dw (g(, X,x i+1 ) + G(X,x i+1 )ψ(, X,x i+1 ))d B. hi i juified becaue X,x and ψ are independen and becaue ψ grow polynomially, hence we can apply Iô formula. We alo ued he fac ha ψ i a claical oluion o (9). If we le he meh ize end o, hen by coninuiy of X,x and ψ, he reul follow. 5. Preliminary eimae he noaion D α x indicae ha he differenial operaor D α i only acing on he x-variable. he following reul will help u o juify he BDSD-repreenaion on he deeper level. Recall ha p (z, θ; x) = θ(x, Z x ) Z x = z.

13 DIMNSIONAL RDUCION IN NONLINAR FILRING 13 Propoiion 5.1. Aume (HF k,l ). Le θ C k,l (R m R n, R) aify for ome C, p > Dx α Dz β θ(x, z) C(1 + x p + z p ). hen α k β l (, x, z) p (z, θ; x) C,k,l (R + R m R n, R) and here exi C 1, p 1 >, uch ha for all (, x, z), ) R m R n Dx α Dz β p (z, θ; x) C 1 e C1 (1 + x p 1 + z p 1 ). α k β l If he bound on he derivaive of θ can be choen uniformly in x, i.e. up Dx α Dz β θ(x, z) C(1 + z p ), x α k β l hen he bound on he derivaive of p (z, θ; x) i alo uniform in x: up Dx α Dz β p (z, θ; x) C 1 e C1 (1 + z p 1 ). x Proof. Noe ha α k β l p (z, θ; x) = θ(x, Z x ) Z x = z = (θ(x, Z ) (X, Z ) = (x, z) i he oluion of Kolmogorov backward equaion aociaed o (X, Z), where X = X, Z = Z + f(x, Z )d + g(x, Z )dw. In hi formulaion, he fir reul i andard. Cf. e.g. Sroock (28), Corollary he econd aemen can be proven in he ame way a Sroock (28), Corollary Some reul from Pardoux and Vereennikov (23) are colleced in he following Propoiion: Propoiion 5.2. Aume (H a ) and (HF k,3 ). Le θ C k, (R m R n, R) aify for ome C, p > : up Dx α θ(x, z) C(1 + z p ). x hen α k (1) x p (θ; x) C k b (Rm, R). (2) Aume addiionally ha θ aifie he cenering condiion R n θ(x, z)p (x, dz) = for all x, and ha θ C k,1 (R m R n, R) and up Dz β Dx α θ(x, z) C(1 + z p ). x hen α k β 1 (x, z) p (z, θ; x)d C k,1 (R m R n, R),

14 14 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG and for every q > here exi C 1, q 1 >, uch ha for every z R n up Dz β Dx α p (z, θ; x) q d C 1 (1 + z q 1 ). x α k β 1 Proof. he aemen in he Propoiion are aken from heorem 1, heorem 2 and Propoiion 1 of Pardoux and Vereennikov (23): (1) We ge from heorem 1 of Pardoux and Vereennikov (23), ha for any q > here exi C q >, uch ha for any (x, z, z ) R m R n R n : α k up x D x α p (z ; x) C q 1 + z q. So if we chooe q large enough and differeniae p (θ; x) under he inegral ign, hen we obain he fir claim. (Of coure here we have o ue he growh conrain on θ and i derivaive). (2) hi follow from he bound on he derivaive of p (z, θ; x) ha are given in Pardoux and Vereennikov (23), heorem 2, formulae (14) and (15): For any k > here exi C k, m k >, uch ha for any (, x, z) 1, ) R m R n Dz β Dx α 1 + z m k p (z, θ; x) C k (1 + ) k. α k β 1 We combine hi eimae wih Propoiion 5.1, from where we obain for (, x, z) R + R m R n up Dx α Dz β p (z, θ; x) C 1 e C1 (1 + z p 1 ). x α k β l We chooe k uch ha qk > 1 and ue he fir eimae on 1, ) and he econd eimae on, 1). he reul follow. We will alo need ome momen bound for he diffuion X and Z. Propoiion 5.3. Aume (H a ) and ha he coefficien b and σ and f and g of he fa and low moion are bounded and globally Lipchiz coninuou. hen for any p 1 here exi C p >, uch ha up Z p (X, Z) = (x, z) C p (1 + z p ). (,,x), ),1 R m Alo, for every > and every p 1 here exi C(p, ), q >, uch ha up X p (X, Z) = (x, z) C(p, )(1 + x p ). (,),,1 Proof. he fir claim can be proven exacly a in Vereennikov (1997): Fir wrie Z := Z 2. hen d Z = f(x 2, Z )d + g(x 2, Z )d W where W := 1/W 2 i a Wiener proce. Nex, inroduce he ame ime change a in Pardoux and Vereennikov, page 163: κ(x, z) := g(x, z) z / z, γ () := Define Z := Z τ (). hen, κ 2 (X 2, Z )d, τ () := (γ ) 1 (). d Z = κ 2 (X 2, Z )f(x 2, Z )d + κ 1 (X 2, Z )g(x 2, Z )d W

15 DIMNSIONAL RDUCION IN NONLINAR FILRING 15 wih a new andard Brownian moion W. Now we are in a poiion o ju copy he proof of Lemma 1 in Vereennikov (1997) (which we do no do here) o ge he fir reul. he econd claim i obviou, becaue he coefficien of X are bounded. Now we we are able o impoe condiion on he coefficien of he diffuion ha guaranee moohne of he coefficien of L. Recall ha L wa defined a L = bi (x) ā ij (x, z) x i 2 x i x j where b = p (b; x) and ā = p (σσ ; x). Propoiion 5.4. Aume (HF k,3 ), (HS k, ), and (HO k, ). hen b C k b (R m, R m ), ā C k b (Rm, S m m ), h C k b (Rm, R k ) Proof. All he erm of b, ā and h are of he form p (θ; x). So by Propoiion 5.2, we only need o verify ha he repecive θ are in C k, and aify he polynomial bound up Dx α θ(x, z) C(1 + z p ) x α k for ome C, p >. Bu we even aumed hem o be in C k, b, o he reul follow. 6. Proof of he main reul We will find convergence rae for he correcor and remainder erm ha are expreed in erm of v and i derivaive. So now we give bound on v and i derivaive in erm of he e funcion ϕ. hi i neceary, becaue we do no only wan o how convergence of he filer inegraing fixed e funcion, bu wih repec o a uiable diance on he pace of probabiliy meaure. Lemma 6.1. Le k 2 and aume b, ā, ϕ C k+1 b, and h C k+2 b. hen v C,k (, R m, R), and for any p 1 here exi C p, q >, independen of ϕ, uch ha for all x R m : up D α v (x) p C p (1 + x q ) ϕ p k,. α k In paricular, v and all i parial derivaive up o order (, k) are in P (R m, R). Proof. hi i a imple applicaion of Propoiion 4.1, noing ha he equaion (6) for v i of he ype (9) wih f =, g =, and G = h. We will prove L p -convergence of ψ 1 and R eparaely: Lemma 6.2. Le k, l 2. Aume (H a ), (HF k+1,l+1 ), (HS k+1,l+1 ), and (HO k+1,l+1 ). Alo aume v C,k+1 (, R m, R), and ha all i parial derivaive in x up o order k + 1 are in P (R m, R). Finally aume ā, b, h Cb k. hen ψ1 C,k,l (, R m R n, R), and ψ 1 a well a i parial derivaive up o order (, k, l) are in P (R m R n, R). For any p 1 here exi C p, q >, independen of ϕ, uch ha for any (x, z) R m+n and any (, 1) up Dx α ψ 1 (x, z) p α k 1 p 2 Cp (1 + z q ) α k+1 up D α x v (x) p.

16 16 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Proof. ψ 1 (x, z) olve he BSPD (12) dψ 1 (x, z) = ψ 1 (x, z) =. 1 L F ψ 1 (x, z) + (L S L)v (x) d + h(x, z) h(x) v (x)d B, xience of he oluion ψ 1 and i derivaive a well a he polynomial growh all follow from Propoiion 4.1. Wrie Z,x,(,z) for he oluion of he SD dz,x,(,z) = 1 Z,x,(,z) = z,. f(x, Z,x,(,z) )d + 1 g(x, Z,x,(,z) )dw, We conider (x, Z,x,(,z) ) a a join diffuion, ju a in he proof of Propoiion 5.1 (x ha generaor ). By Propoiion 4.2, he oluion of (12) i given by θ (,x,z)(1), he unique oluion o he BDSD dθ (,x,z)(1) θ (,x,z)(1) =. We will drop upercrip (, x, z) for θ (,x,z)(1) inead of Z,x,(,z) θ 1 F B, = (L S (, Z,x,(,z) ) L)v (x)d ( + h(x, Z,x,(,z) ) h(x) ) v (x)db + γ,x,z dw, and wrie θ 1 inead. Similarly, we wrie Z,x. ψ 1 (x, z) i F, B -meaurable, hence, o i θ1. We can hen wrie θ 1 =, where θ 1 F, B = (L S L)v (x)d F, B + h(x, Z,x ) h(x) v (x)db F, B γ,x,z dw F, B. W and B are independen, herefore W i a Brownian moion in he large filraion (F W F, B :, ), hence γ,x,z dw F W F, B =, and by he ower propery γ,x,z dw F, B =. v i F B, -meaurable and L ha deerminiic coefficien. hu = = Lv (x)d F B, Lv (x) F, B d p (b i ; x) x i v (x) + p ((σσ 2 ) ij ; x) v x i x (x) j d.

17 Since Z,x i independen of B, DIMNSIONAL RDUCION IN NONLINAR FILRING 17 = = L S (, Z,x { m { m )v(x)d F, B = b i (x, Z,x ) x i v (x) (σσ ) ij (x, Z,x ) p (z, b i ; x) v x (x) i p L S (, Z,x )v (x) F B, d 2 v x i x (x) j d (z, (σσ 2 ) ij ; x) v x i x (x) j d, o (L S L)v (x)d F, B { m = p (z, b i p (b i ; x); x) v x (x) i + 1 p (z, (σσ ) ij p ((σσ 2 ) ij ; x); x) v 2 x i x (x) j d (he p (.; x) erm have been brough inide he inegral p (z, ; x) ince hey no depend on z) p u (z, b i p (b i ; x); x) v x u+(x)du i + 2 p u (z, (σσ ) ij p ((σσ 2 ) ij ; x); x) v x i x u+(x)du j p u (z, b i p (b i ; x); x) du up v x (x) i + p u (z, (σσ ) ij p ((σσ ) ij ; x); x) du up 2 2 v x i x (x) j (f p (f; x) i cenered, o by Propoiion 5.2, (2):) C 1 (1 + z q 1 ) up v x (x) m i + up 2 v x i x (x) j

18 18 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG and herefore finally p (13) (L S L)v (x)d F, B p C 2 (1 + z q 2 ) v x (x) i up p + up Nex, uing again v F, B and ha Z,x i independen of B, h(x, Z,x ) h(x) v (x)db F, B = = h(x, Z,x ) h(x) v (x) F B, d B p (z, h h; x) v(x)d B. For r, r r p ime i run backward. Hence by he Burkholder-Davi-Gundy inequaliy, where 2 p v x i x (x) j. (z, h h; x) v (x)d B, i a maringale w.r.. (F B r, p (z, h h; x) v(x)d B p C p p (z, h h; x) v(x)d B = p (z, h h; x) v(x)d B p 2 p, (z, h h; x) v(x) 2 d p u (z, h h; x) 2 du up C 3 (1 + z q 3 ) up v (x) 2, v (x) 2 where he la inequaliy i by Propoiion 5.2, (2), ince h h i cenered. herefore, p (z, h h; x) v(x)d p B p 2 C4 (1 + z q 4 ) up v (x) (14) p. Combining (13) and (14), θ 1 p p C 4 (1 + z q 4 ) α 2 Nex, conider a fir order x-derivaive of θ 1 : x k θ 1 = x k + x k L S L v (x)d up Dx α v(x) p. h(x, Z,x ) h(x) v (x)d B. : r, ) if A before, he forward Ió inegral erm vanihed afer aking he (condiional) expecaion.

19 DIMNSIONAL RDUCION IN NONLINAR FILRING 19 Inerchanging order of differeniaion and inegraion, L S x L v (x)d k { p u (z, b i p (b i ; x); x) v x k x u+(x) i 2 } +p u (z, b i p (b i ; x); x) v x k x u+(x) du i + { p 2 u (z, (σσ ) ij p ((σσ 2 ) ij ; x); x) v x k x i x u+(x) j +p u (z, (σσ ) ij p ((σσ 3 } ) ij ; x); x) v x i x j x u+(x) du k { p u (z, b i p (b i ; x); x) x k du up v x (x) i + p u (z, b i p (b i ; x); x) du up 2 } v x k x (x) i { + 2 p u (z, (σσ ) ij p ((σσ ) ij ; x); x) x k du up 2 v x i x (x) j + p u (z, (σσ ) ij p ((σσ ) ij ; x); x) du up 3 } v x i x j x (x) k. hen, from Propoiion 5.2, (2) again, x k L S L v(x)d C 5(1 + z q 5 ) up 1 β 3 Dxv β (x). ince he quaniie b b and σσ σσ are cenered. aking expecaion, (15) x k L S L v(x)d p p C 6 (1 + z q 6 ) 1 β 3 up Dxv β (x) p.

20 2 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Nex, by (HO k,l ), we can inerchange he order of ordinary differeniaion and ochaic inegraion (cf. Karandikar (1983)): ( h(x, Z,x ) x h(x) ) v (x)d p B k ( = h(x, Z,x ) x h(x) v (x) ) db p k ( C p ( h(x, Z,x ) x h(x) v (x) ) ) 2 p/2 d, k where ( h(x, Z,x ) x h(x) v (x) ) 2 d k = p u (z, h x h; x)vu+(x) + p u (z, h h; x) v k x u+(x) k { 2 p u (z, h x h; x) 2 vu+(x) 2 du k + pu (z, h h; x) } 2 v 2 x u+(x) k du { C 7 (1 + z q 7 ) up v (x) 2 + up v 2} x (x). k he la ep follow once again from Propoiion 5.2, (2). So, ( h(x, Z,x ) x h(x) ) v (x)d p (16) B k { p 2 C8 (1 + z q 8 ) up v (x) p + Combining (15) and (16) θ 1 p x k p 2 C9 (1 + z q 9 ) α 3 up up Ieraing hee argumen for he higher order derivaive of θ 1, D x α θ 1 p p 2 C1 (1 + z q 1 ) α k 1 α k+1 2 v p} x (x). k D x α v(x) p. up du D x α v(x) p. Lemma 6.3. Le k, l 3. Aume (HF k,l ), (HS k,l ), and (HO k+1,l+1 ). Alo aume ψ 1 C,k+2,l (, R m R n, R) and ha all i parial derivaive up o order (, k + 2, l) are in P (, R m, R). hen for any p 1 here exi C p >, independen of ϕ, uch ha for any (x, z) R m+n, any (, 1), and any, R (x, z) p C p D x α ψ(x 1, z ) p d. α 2 (x,z )=(X,(,x),Z,(,z) )

21 Proof. R (x, z) olve he BSPD DIMNSIONAL RDUCION IN NONLINAR FILRING 21 (17) dr (x, z) = ( L R (x, z) + L S ψ 1 (x, z) ) d R (x, z) =. + h(x, z) ( ψ 1 (x, z) + R (x, z) ) d B, xience of he oluion R and i derivaive, a well a he polynomial growh all follow from Propoiion 4.1. By Propoiion 4.2, he oluion of (17) i given by θ (,x,z)(2), he oluion o he BDSD dθ (,x,z)(2) θ (,x,z)(2) =. = L S ψ 1 (X,(,x) + h(x,(,x) + h(x,(,x), Z,(,z) )d, Z,(,z), Z,(,z) ) ψ 1 (X,(,x) ) θ (,x,z)(2), Z,(,z) )db d B γ,x,z dw δ,x,z dv We will drop upercrip (, x, z) for θ (,x,z)(2), (, z) for Z,(,z), and (, x) for X,(,x). R (x, z) i F B, -meaurable, hence, o i θ2. A before, he ochaic inegral over dv and dw vanih when we ake condiional expecaion wih repec o F B,. hu (18) θ 2 = L S ψ(x 1, Z)d F, B + h(x, Z) ψ(x 1, Z)d B F, B + h(x, Z) θd 2 B F, B. Conider each erm eparaely: L S ψ(x 1, Z)d p p F, B L S ψ(x 1, Z)d ( m ( ) p 1 b i (X, Z) x i + 1 p (σσ ) ij (X 2, Z) 2 ψ 1 x i x (X, Z) i d ( m C 1 b ψ 1 x (X, Z) p i C σσ m 1 α 2 2 p ψ 1 x i x (X, Z) d i D α x ψ 1 (X, Z ) p d.

22 22 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Noe ha Z and X are F W independen. hu o ha (19) F V -meaurable, ψ 1 i F, B -meaurable, and B and (V, W ) are D x α ψ(x 1, Z) p = Dx α ψ(x 1, Z) p F V = D α x ψ(x 1, z ) p L S ψ(x 1, Z)d p F, B C 2 1 α 2 F W (x,z )=(X,Z ), D x α ψ(x 1, z ) p (x z )=(X,Z ) d. Nex, by Jenen inequaliy, he ower propery, and he Burkholder-Davi-Gundy inequaliy, h(x, Z) ψ(x 1, Z)d B p F, B C p h(x, Z ) ψ 1 (X, Z )d B p h(x, Z ) ψ 1 (X, Z )d B p 2 where by Hölder inequaliy and he Cauchy-Schwarz inequaliy h(x, Z,x ) ψ 1 (X, Z )d B p 2 = ( h(x, Z,x, ) ψ 1 (X, Z ) 2 d C 3 h(x, Z) p ψ(x 1, Z) p d. So by he ame argumen a for he fir erm, h(x, Z) ψ(x 1, Z)d B p (2) F, B C 4 ψ(x 1, z ) p d. (x,z )=(X,Z ) Finally, uing Burkholder-Davi-Gundy in he econd line, and Cauchy-Schwarz in he hird line h(x, Z) θd 2 B p F, B h(x, Z) θd 2 B p ( ) p C p h(x, Z) θ d (21) C p ( C 5 h p ) p h(x, Z) 2 θ d θ 2 p d. ) p 2

23 DIMNSIONAL RDUCION IN NONLINAR FILRING 23 Combining (18) wih (19), (2), and (21) By Gronwall, θ 2 p C6 θ 2 p C 6 α 2 C 7 α 2 α 2 + C 5 h p D α x ψ(x 1, z ) p (x,z )=(X,Z ) d θ 2 p d. D x α ψ(x 1, z ) p (x,z )=(X,Z ) D x α ψ(x 1, z ) p (x,z )=(X,Z ) d e ( )C 5 h p d. where we chooe C 7 o ha he inequaliy hold for every, (replace e ( )C 5 h e C 5 h ). by Now we can collec all hee reul, o obain he fir ep oward heorem 3.1. Lemma 6.4. Aume (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ), and ha ϕ C 7 b (Rm, R). hen for every p 1 here exi C, q 1, q 2 >, independen of ϕ, uch ha up v (x, z) v (x) p p/2 C (1 + x q 1 + z q 2 ) ϕ p 4,. Proof of heorem 3.1. We rack he neceary condiion backward from Lemma For he oluion R given in Lemma 6.3 o exi and aify he aed bound, we need (HF 3,3 ), (HS 3,3 ), (HO 4,4 ), and ψ 1 C,5,3 (, R m R n, R). he polynomial growh condiion will be aified anyway. 2. For ψ 1 o be in C,5,3 (, R m R n, R), we need (H a ), (HF 6,4 ), (HS 6,4 ), (HO 6,4 ) and ā, b, h Cb 5. We alo need v C,6 (, R m, R). Again, he polynomial growh condiion will be aified. 3. For v o be in C,6 (, R m, R) we need ā, b, ϕ Cb 7 and h Cb For ā, b o be in Cb 7 we need (HF 7,3) a well a (HS 7, ) by Propoiion 5.4. Similarly we need (HF 8,3 ) a well a (HO 8, ) for h o be in Cb So ufficien condiion are (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ). In ha cae we obain from Lemma 6.1 (22) α 2 α 4 up D α v (x) p C 1 (1 + x q 1 ) ϕ p 4,. From Lemma 6.2 we obain up Dx α ψ 1 (x, z) p p 2 C2 (1 + z q 2 ) (23) From Lemma 6.3 we ge (24) R (x, z) p C 3 α 2 α 4 D x α ψ(x 1, z ) p up D x α v (x) p. (x,z )=(X,(,x),Z,(,z) ) d.

24 24 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Combining (22), (24), (24), we ge for any, (by ime-homogeneiy of X and Z ) R (x, z) p + ψ 1 (x, z) p ) (25) p/2 C 4 (1 + up From Propoiion 5.3 we obain X q 1 + Z,x q 2 (X, Z) = (x, z) ϕ p 4,. up X q 1 + Z,x q 2 (X, Z) = (x, z) C 5 (1 + x q 3 + z q 4 ). Noing ha he righ hand ide in (25) doe no depend on,, up R (x, z) p + up ψ 1 (x, z) p Finally which complee he proof. p/2 C 6 (1 + x q 3 + z q 4 ) ϕ p 4,. up v (x, z) v (x) p ( C 7 up R (x, z) p + up ψ 1 (x, z) p) p/2 C 8 (1 + x q 3 + z q 4 ) ϕ p 4,, Now we recall ha all he calculaion up unil now were under he changed meaure P. We only wroe P and B o faciliae he reading. So le u ranfer he reul o he original meaure Q. Lemma 6.5. Aume (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ), and ha ϕ C 7 b (Rm, R). hen for every p 1 here exi C, q 1, q 2 >, independen of ϕ, uch ha up Q v (x, z) v (x) p p/2 C (1 + x q 1 + z q 2 ) ϕ p 4,. Proof. hi i a imple applicaion of he Cauchy-Schwarz inequaliy in combinaion wih Gronwall lemma: Q v (x, z) v (x) p = P v (x, z) v (x) p dq dp ( ) dq 2 1/2 P v (x, z) v (x) 2p 1/2 P dp, o we ee ha he reul i rue by Lemma 6.4 a long a he econd expecaion i finie. Recall ha we had defined he noaion ( dq dp = D = exp h(x, Z) dy 1 ) h(x F 2, Z) 2 d. So D aifie he SD d D = D h(x, Z ) dy, D = 1. Since under P, Y i a Brownian moion, we ge by Iô-iomery P ( D ) 2 = P ( D ) 2 h(x, Z) 2 d h 2 P ( D ) 2 d, o ha by Gronwall P ( D )2 <

25 DIMNSIONAL RDUCION IN NONLINAR FILRING 25 Lemma 6.6. Aume (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ), ha ϕ Cb 7, and ha he iniial diribuion Q (X,Z ) ha finie momen of every order. hen for every p 1 here exi C >, independen of ϕ, uch ha Q ρ,x (ϕ) ρ (ϕ) p p/2 C ϕ p 4,. Proof. A we already decribed in he inroducion, we obain from Lemma 6.5 Q ρ,x (ϕ) ρ (ϕ) p = Q (v(x, z) v(x))q p (X,Z ) (dx, dz) Q v(x, z) v(x) p Q (X,Z ) (dx, dz) p/2 C 1 (1 + x q 1 + z q 2 ) Q (X,Z ) (dx, dz) ϕ p 4, p/2 C 2 ϕ p 4,. he convergence of he acual filer, i.e. of π,x o π, now follow exacly a in Chaper 9.4 of Bain and Crian (29). For he ake of compleene, we include he argumen. Lemma 6.7. Le p 1. hen a long a h i bounded. up (,1,, { Q ρ,x (1) p + Q ρ (1) p } < Proof. We give he argumen for Q ρ,x (1) p, Q ρ (1) p being compleely analogue. We have Q ρ,x (1) p = P ρ,x p dq (1) P dp ρ,x (1) 2p 1/2 P ( ) dq 2 1/2 dp We howed in he proof of Lemma 6.5 ha he econd expecaion i finie. Noe ha x x 2p i convex. herefore by Jenen inequaliy, P ρ,x (1) 2p ( = P P exp h(x, Z) dy 1 ) 2p h(x 2, Z) 2 d Y ( P exp h(x, Z) dy 1 ) 2p h(x 2, Z) 2 d dq 2p P dp 2p+1 dp = Q. dq he reul now follow exacly a in he proof of Lemma 6.5, becaue for D = dp /dq F have dd = h(x, Z ) db, D = 1 and B i a Brownian moion under Q. we

26 26 P. IMKLLR, N.S. NAMACHCHIVAYA, N. PRKOWSKI, AND H.C. YONG Define for any meaurable and bounded e funcion ϕ : R m R Recall ha π,x π (ϕ) = ρ (ϕ) ρ (1). wa defined analogouly wih ρ,x inead of ρ. We hen have Lemma 6.8. Aume (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ), and ha he iniial diribuion Q (X,Z ) ha finie momen of every order. Le p 1. hen here exi C > uch ha for every ϕ Cb 7 Q π,x (ϕ) π (ϕ) p p/2 C ϕ p 4,. Proof. In he hird line we ue ha π,x i a.. equal o a probabiliy meaure. Q π,x (ϕ) π (ϕ) p ρ,x = (ϕ) Q ρ,x (1) ρ (ϕ) p ρ (1) ρ,x = (ϕ) ρ (ϕ) Q ρ (1) π,x (ϕ)ρ,x (1) ρ (1) p ρ (1) ( ρ,x C p (ϕ) ρ (ϕ) p Q ρ (1) + ϕ p ρ,x (1) ρ (1) p) Q ρ (1) ( C p Q ρ (1) 2p ) ( 1/2 Q ρ,x (ϕ) ρ (ϕ) 2p 1/2 p/2 C 1 ϕ 4,, where he la ep follow from Lemma 6.6 and Lemma ϕ p Q ρ,x (1) ρ (1) ) 2p 1/2 Since he bound only depend on ϕ 4,, we can replace he aumpion ϕ Cb 7 by ϕ C4 b : Ju approximae ϕ Cb 4 by ϕn Cb 7 in he 4, -norm, and ake advanage of he fac ha and π are a.. equal o probabiliy meaure. herefore we have π,x Corollary 6.9. Aume (H a ), (HF 8,4 ), (HS 7,4 ), (HO 8,4 ), and ha he iniial diribuion Q (X,Z ) ha finie momen of every order. Le p 1. hen here exi C > uch ha for every ϕ C 4 b, Q π,x (ϕ) π (ϕ) p p/2 C ϕ p 4,. Now noe ha here exi a counable algebra (ϕ i ) i N of Cb 4 funcion ha rongly eparae poin in R m. ha i, for every x R m and δ >, here exi i N, uch ha inf y: x y >δ ϕ i (x) ϕ i (y) >. ake e.g. all funcion of he form n exp q j (x x j ) 2 j=1 wih n N, q j Q +, x j Q m. By heorem of hier and Kurz (1986), he equence (ϕ i ) i convergence deermining for he opology of weak convergence of probabiliy meaure. ha i, if µ n and µ are probabiliy meaure on R m, uch ha lim n µ n (ϕ i ) = µ(ϕ i ) for every i N, hen µ n converge weakly o µ. Define he following meric on he pace of probabiliy meaure on R m : d(ν, µ) = d (ϕi )(ν, µ) = ν(ϕ i ) µ(ϕ i ) 2 i.

27 DIMNSIONAL RDUCION IN NONLINAR FILRING 27 Becaue (ϕ i ) i convergence deermining, he meric d generae he opology of weak convergence. herefore he proof of heorem 3.1 i complee. 7. Concluion and fuure direcion hi paper preened he heoreical bai for he developmen of a lower-dimenional paricle filering algorihm for he ae eimaion in complex mulicale yem. o hi end, we combined ochaic homogenizaion wih nonlinear filering heory o conruc a homogenized SPD which i he approximaion of a lower-dimeional nonlinear filer for he coare-grained proce. he convergence of he opimal filer of he coare-grained proce o he oluion of he homogenized filer i hown uing BSD and aympoic echnique. hi homogenized SPD can be ued a he bai for an efficien muli-cale paricle filering algorihm for eimaing he low dynamic of he yem, wihou direcly accouning for he fa dynamic. In Lingala e al. (212) we preen a numerical algorihm baed on hi cheme, ha enable efficien incorporaion of obervaion daa for eimaion of he coare-grained ( low ) dynamic, and we apply he algorihm o a high-dimenional chaoic mulicale yem. ven hough hi paper deal wih ju one widely eparaed characeriic ime cale, one can exend hi work o incorporae a more realiic eing where he ignal ha more han one ime cale eparaion. A before we le be a mall parameer ha meaure he raio of low and fa ime cale. Conider he ignal and obervaion procee governed by: dz = 1 2 f(z, X ) + 1 g(z, X ) dw, Z = z, (26) dx = 1 bi (Z, X ) + b(z, X ) + σ(z, X ) dv, X = x, dy = h(z, X ) d + db, Y =, where W, V and B are independen Wiener procee and x and z are random iniial condiion which are independen of W, V and B. I i imporan o realize ha here are everal cale in (26), even he low proce X ha a fa varying componen. hi cae i imporan, in paricular, for applicaion in geophyical flow and climae dynamic. he drif erm b and he diffuion σ caue flucuaion of order order 1, and he drif erm f and he diffuion g caue flucuaion of order order 2, wherea he drif erm b I caue flucuaion a an inermediae order 1. I wa found ha when he average of b I wih repec o he invarian meaure of he fa componen Z (for he fixed low componen) i zero, he limi diribuion of he low componen (away from he iniial layer) can alo be obained in erm of he oluion of ome auxiliary Poion equaion in he homogenizaion heory. However, a unified framework o deal wih 1 erm in developing a lower-dimenional nonlinear filer for he coare-grained proce i ill no available. Our condiion on he coefficien are very rericive and exclude for example linear model. hi i due o he fac ha we are uing homogenizaion of SPD o obain convergence of he filer, and ha for exience of oluion o he SPD, he coefficien need o be bounded and ufficienly mooh. Working wih weak oluion in place of claical oluion would no improve he condiion much. Uing vicoiy oluion or enirely relying on probabiliic argumen migh be a way o ge le rericive condiion, however wih hee mehod we do no expec ha a rae of convergence can be obained. While we were able o obain he explici rae of convergence, he conan C in heorem 3.1 depend on he erminal ime. I would be inereing o find condiion under which hi can be avoided. hi migh be achieved by building on abiliy reul for nonlinear filer, ee e.g. Crian and Rozovkii (211), Chaper 4, Sabiliy and aympoic analyi.

ESTIMATES FOR THE DERIVATIVE OF DIFFUSION SEMIGROUPS

ESTIMATES FOR THE DERIVATIVE OF DIFFUSION SEMIGROUPS Elec. Comm. in Probab. 3 (998) 65 74 ELECTRONIC COMMUNICATIONS in PROBABILITY ESTIMATES FOR THE DERIVATIVE OF DIFFUSION SEMIGROUPS L.A. RINCON Deparmen of Mahemaic Univeriy of Wale Swanea Singleon Par

More information

Generalized Orlicz Spaces and Wasserstein Distances for Convex-Concave Scale Functions

Generalized Orlicz Spaces and Wasserstein Distances for Convex-Concave Scale Functions Generalized Orlicz Space and Waerein Diance for Convex-Concave Scale Funcion Karl-Theodor Surm Abrac Given a ricly increaing, coninuou funcion ϑ : R + R +, baed on he co funcional ϑ (d(x, y dq(x, y, we

More information

Introduction to SLE Lecture Notes

Introduction to SLE Lecture Notes Inroducion o SLE Lecure Noe May 13, 16 - The goal of hi ecion i o find a ufficien condiion of λ for he hull K o be generaed by a imple cure. I urn ou if λ 1 < 4 hen K i generaed by a imple curve. We will

More information

, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max

, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max ecure 8 7. Sabiliy Analyi For an n dimenional vecor R n, he and he vecor norm are defined a: = T = i n i (7.) I i eay o how ha hee wo norm aify he following relaion: n (7.) If a vecor i ime-dependen, hen

More information

To become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship

To become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship Laplace Tranform (Lin & DeCarlo: Ch 3) ENSC30 Elecric Circui II The Laplace ranform i an inegral ranformaion. I ranform: f ( ) F( ) ime variable complex variable From Euler > Lagrange > Laplace. Hence,

More information

Fractional Ornstein-Uhlenbeck Bridge

Fractional Ornstein-Uhlenbeck Bridge WDS'1 Proceeding of Conribued Paper, Par I, 21 26, 21. ISBN 978-8-7378-139-2 MATFYZPRESS Fracional Ornein-Uhlenbeck Bridge J. Janák Charle Univeriy, Faculy of Mahemaic and Phyic, Prague, Czech Republic.

More information

Mathematische Annalen

Mathematische Annalen Mah. Ann. 39, 33 339 (997) Mahemaiche Annalen c Springer-Verlag 997 Inegraion by par in loop pace Elon P. Hu Deparmen of Mahemaic, Norhweern Univeriy, Evanon, IL 628, USA (e-mail: elon@@mah.nwu.edu) Received:

More information

EE Control Systems LECTURE 2

EE Control Systems LECTURE 2 Copyrigh F.L. Lewi 999 All righ reerved EE 434 - Conrol Syem LECTURE REVIEW OF LAPLACE TRANSFORM LAPLACE TRANSFORM The Laplace ranform i very ueful in analyi and deign for yem ha are linear and ime-invarian

More information

Stability in Distribution for Backward Uncertain Differential Equation

Stability in Distribution for Backward Uncertain Differential Equation Sabiliy in Diribuion for Backward Uncerain Differenial Equaion Yuhong Sheng 1, Dan A. Ralecu 2 1. College of Mahemaical and Syem Science, Xinjiang Univeriy, Urumqi 8346, China heng-yh12@mail.inghua.edu.cn

More information

6.8 Laplace Transform: General Formulas

6.8 Laplace Transform: General Formulas 48 HAP. 6 Laplace Tranform 6.8 Laplace Tranform: General Formula Formula Name, ommen Sec. F() l{ f ()} e f () d f () l {F()} Definiion of Tranform Invere Tranform 6. l{af () bg()} al{f ()} bl{g()} Lineariy

More information

CHAPTER 7: SECOND-ORDER CIRCUITS

CHAPTER 7: SECOND-ORDER CIRCUITS EEE5: CI RCUI T THEORY CHAPTER 7: SECOND-ORDER CIRCUITS 7. Inroducion Thi chaper conider circui wih wo orage elemen. Known a econd-order circui becaue heir repone are decribed by differenial equaion ha

More information

Laplace Transform. Inverse Laplace Transform. e st f(t)dt. (2)

Laplace Transform. Inverse Laplace Transform. e st f(t)dt. (2) Laplace Tranform Maoud Malek The Laplace ranform i an inegral ranform named in honor of mahemaician and aronomer Pierre-Simon Laplace, who ued he ranform in hi work on probabiliy heory. I i a powerful

More information

Rough Paths and its Applications in Machine Learning

Rough Paths and its Applications in Machine Learning Pah ignaure Machine learning applicaion Rough Pah and i Applicaion in Machine Learning July 20, 2017 Rough Pah and i Applicaion in Machine Learning Pah ignaure Machine learning applicaion Hiory and moivaion

More information

Research Article Existence and Uniqueness of Solutions for a Class of Nonlinear Stochastic Differential Equations

Research Article Existence and Uniqueness of Solutions for a Class of Nonlinear Stochastic Differential Equations Hindawi Publihing Corporaion Abrac and Applied Analyi Volume 03, Aricle ID 56809, 7 page hp://dx.doi.org/0.55/03/56809 Reearch Aricle Exience and Uniquene of Soluion for a Cla of Nonlinear Sochaic Differenial

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual

More information

Randomized Perfect Bipartite Matching

Randomized Perfect Bipartite Matching Inenive Algorihm Lecure 24 Randomized Perfec Biparie Maching Lecurer: Daniel A. Spielman April 9, 208 24. Inroducion We explain a randomized algorihm by Ahih Goel, Michael Kapralov and Sanjeev Khanna for

More information

Notes on cointegration of real interest rates and real exchange rates. ρ (2)

Notes on cointegration of real interest rates and real exchange rates. ρ (2) Noe on coinegraion of real inere rae and real exchange rae Charle ngel, Univeriy of Wiconin Le me ar wih he obervaion ha while he lieraure (mo prominenly Meee and Rogoff (988) and dion and Paul (993))

More information

An introduction to the (local) martingale problem

An introduction to the (local) martingale problem An inroducion o he (local) maringale problem Chri Janjigian Ocober 14, 214 Abrac Thee are my preenaion noe for a alk in he Univeriy of Wiconin - Madion graduae probabiliy eminar. Thee noe are primarily

More information

Let. x y. denote a bivariate time series with zero mean.

Let. x y. denote a bivariate time series with zero mean. Linear Filer Le x y : T denoe a bivariae ime erie wih zero mean. Suppoe ha he ime erie {y : T} i conruced a follow: y a x The ime erie {y : T} i aid o be conruced from {x : T} by mean of a Linear Filer.

More information

ARTIFICIAL INTELLIGENCE. Markov decision processes

ARTIFICIAL INTELLIGENCE. Markov decision processes INFOB2KI 2017-2018 Urech Univeriy The Neherland ARTIFICIAL INTELLIGENCE Markov deciion procee Lecurer: Silja Renooij Thee lide are par of he INFOB2KI Coure Noe available from www.c.uu.nl/doc/vakken/b2ki/chema.hml

More information

An Introduction to Malliavin calculus and its applications

An Introduction to Malliavin calculus and its applications An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214

More information

Chapter 6. Laplace Transforms

Chapter 6. Laplace Transforms Chaper 6. Laplace Tranform Kreyzig by YHLee;45; 6- An ODE i reduced o an algebraic problem by operaional calculu. The equaion i olved by algebraic manipulaion. The reul i ranformed back for he oluion of

More information

Explicit form of global solution to stochastic logistic differential equation and related topics

Explicit form of global solution to stochastic logistic differential equation and related topics SAISICS, OPIMIZAION AND INFOMAION COMPUING Sa., Opim. Inf. Compu., Vol. 5, March 17, pp 58 64. Publihed online in Inernaional Academic Pre (www.iapre.org) Explici form of global oluion o ochaic logiic

More information

18.03SC Unit 3 Practice Exam and Solutions

18.03SC Unit 3 Practice Exam and Solutions Sudy Guide on Sep, Dela, Convoluion, Laplace You can hink of he ep funcion u() a any nice mooh funcion which i for < a and for > a, where a i a poiive number which i much maller han any ime cale we care

More information

u(t) Figure 1. Open loop control system

u(t) Figure 1. Open loop control system Open loop conrol v cloed loop feedbac conrol The nex wo figure preen he rucure of open loop and feedbac conrol yem Figure how an open loop conrol yem whoe funcion i o caue he oupu y o follow he reference

More information

Introduction to Congestion Games

Introduction to Congestion Games Algorihmic Game Theory, Summer 2017 Inroducion o Congeion Game Lecure 1 (5 page) Inrucor: Thoma Keelheim In hi lecure, we ge o know congeion game, which will be our running example for many concep in game

More information

Chapter 7: Inverse-Response Systems

Chapter 7: Inverse-Response Systems Chaper 7: Invere-Repone Syem Normal Syem Invere-Repone Syem Baic Sar ou in he wrong direcion End up in he original eady-ae gain value Two or more yem wih differen magniude and cale in parallel Main yem

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

FIXED POINTS AND STABILITY IN NEUTRAL DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

FIXED POINTS AND STABILITY IN NEUTRAL DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 136, Number 3, March 28, Page 99 918 S 2-9939(7)989-2 Aricle elecronically publihed on November 3, 27 FIXED POINTS AND STABILITY IN NEUTRAL DIFFERENTIAL

More information

FULLY COUPLED FBSDE WITH BROWNIAN MOTION AND POISSON PROCESS IN STOPPING TIME DURATION

FULLY COUPLED FBSDE WITH BROWNIAN MOTION AND POISSON PROCESS IN STOPPING TIME DURATION J. Au. Mah. Soc. 74 (23), 249 266 FULLY COUPLED FBSDE WITH BROWNIAN MOTION AND POISSON PROCESS IN STOPPING TIME DURATION HEN WU (Received 7 Ocober 2; revied 18 January 22) Communicaed by V. Sefanov Abrac

More information

Stochastic Optimal Control in Infinite Dimensions: Dynamic Programming and HJB Equations

Stochastic Optimal Control in Infinite Dimensions: Dynamic Programming and HJB Equations Sochaic Opimal Conrol in Infinie Dimenion: Dynamic Programming and HJB Equaion G. Fabbri 1 F. Gozzi 2 and A. Świe ch3 wih Chaper 6 by M. Fuhrman 4 and G. Teiore 5 1 Aix-Mareille Univeriy (Aix-Mareille

More information

1 Motivation and Basic Definitions

1 Motivation and Basic Definitions CSCE : Deign and Analyi of Algorihm Noe on Max Flow Fall 20 (Baed on he preenaion in Chaper 26 of Inroducion o Algorihm, 3rd Ed. by Cormen, Leieron, Rive and Sein.) Moivaion and Baic Definiion Conider

More information

Problem Set If all directed edges in a network have distinct capacities, then there is a unique maximum flow.

Problem Set If all directed edges in a network have distinct capacities, then there is a unique maximum flow. CSE 202: Deign and Analyi of Algorihm Winer 2013 Problem Se 3 Inrucor: Kamalika Chaudhuri Due on: Tue. Feb 26, 2013 Inrucion For your proof, you may ue any lower bound, algorihm or daa rucure from he ex

More information

Network Flows: Introduction & Maximum Flow

Network Flows: Introduction & Maximum Flow CSC 373 - lgorihm Deign, nalyi, and Complexiy Summer 2016 Lalla Mouaadid Nework Flow: Inroducion & Maximum Flow We now urn our aenion o anoher powerful algorihmic echnique: Local Search. In a local earch

More information

Additional Methods for Solving DSGE Models

Additional Methods for Solving DSGE Models Addiional Mehod for Solving DSGE Model Karel Meren, Cornell Univeriy Reference King, R. G., Ploer, C. I. & Rebelo, S. T. (1988), Producion, growh and buine cycle: I. he baic neoclaical model, Journal of

More information

Mon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5

Mon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5 Mah 225-4 Week 2 April 2-6 coninue.-.3; alo cover par of.4-.5, EP 7.6 Mon Apr 2:.-.3 Laplace ranform and iniial value problem like we udied in Chaper 5 Announcemen: Warm-up Exercie: Recall, The Laplace

More information

NECESSARY AND SUFFICIENT CONDITIONS FOR LATENT SEPARABILITY

NECESSARY AND SUFFICIENT CONDITIONS FOR LATENT SEPARABILITY NECESSARY AND SUFFICIENT CONDITIONS FOR LATENT SEPARABILITY Ian Crawford THE INSTITUTE FOR FISCAL STUDIES DEPARTMENT OF ECONOMICS, UCL cemmap working paper CWP02/04 Neceary and Sufficien Condiion for Laen

More information

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution Physics 7b: Saisical Mechanics Fokker-Planck Equaion The Langevin equaion approach o he evoluion of he velociy disribuion for he Brownian paricle migh leave you uncomforable. A more formal reamen of his

More information

On the Benney Lin and Kawahara Equations

On the Benney Lin and Kawahara Equations JOURNAL OF MATEMATICAL ANALYSIS AND APPLICATIONS 11, 13115 1997 ARTICLE NO AY975438 On he BenneyLin and Kawahara Equaion A Biagioni* Deparmen of Mahemaic, UNICAMP, 1381-97, Campina, Brazil and F Linare

More information

Multidimensional Markovian FBSDEs with superquadratic

Multidimensional Markovian FBSDEs with superquadratic Mulidimenional Markovian FBSDE wih uperquadraic growh Michael Kupper a,1, Peng Luo b,, Ludovic angpi c,3 December 14, 17 ABSRAC We give local and global exience and uniquene reul for mulidimenional coupled

More information

CONTROL SYSTEMS. Chapter 10 : State Space Response

CONTROL SYSTEMS. Chapter 10 : State Space Response CONTROL SYSTEMS Chaper : Sae Space Repone GATE Objecive & Numerical Type Soluion Queion 5 [GATE EE 99 IIT-Bombay : Mark] Conider a econd order yem whoe ae pace repreenaion i of he form A Bu. If () (),

More information

Chapter 6. Laplace Transforms

Chapter 6. Laplace Transforms 6- Chaper 6. Laplace Tranform 6.4 Shor Impule. Dirac Dela Funcion. Parial Fracion 6.5 Convoluion. Inegral Equaion 6.6 Differeniaion and Inegraion of Tranform 6.7 Syem of ODE 6.4 Shor Impule. Dirac Dela

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More 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

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance.

An Introduction to Backward Stochastic Differential Equations (BSDEs) PIMS Summer School 2016 in Mathematical Finance. 1 An Inroducion o Backward Sochasic Differenial Equaions (BSDEs) PIMS Summer School 2016 in Mahemaical Finance June 25, 2016 Chrisoph Frei cfrei@ualbera.ca This inroducion is based on Touzi [14], Bouchard

More information

The Residual Graph. 11 Augmenting Path Algorithms. Augmenting Path Algorithm. Augmenting Path Algorithm

The Residual Graph. 11 Augmenting Path Algorithms. Augmenting Path Algorithm. Augmenting Path Algorithm Augmening Pah Algorihm Greedy-algorihm: ar wih f (e) = everywhere find an - pah wih f (e) < c(e) on every edge augmen flow along he pah repea a long a poible The Reidual Graph From he graph G = (V, E,

More information

arxiv: v1 [math.oc] 2 Jan 2019

arxiv: v1 [math.oc] 2 Jan 2019 ASYMTOTIC ROERTIES OF LINEAR FILTER FOR NOISE FREE DYNAMICAL SYSTEM ANUGU SUMITH REDDY, AMIT ATE, AND SREEKAR VADLAMANI arxiv:191.37v1 [mah.oc] 2 Jan 219 Abrac. I i known ha Kalman-Bucy filer i able wih

More information

Algorithmic Discrete Mathematics 6. Exercise Sheet

Algorithmic Discrete Mathematics 6. Exercise Sheet Algorihmic Dicree Mahemaic. Exercie Shee Deparmen of Mahemaic SS 0 PD Dr. Ulf Lorenz 7. and 8. Juni 0 Dipl.-Mah. David Meffer Verion of June, 0 Groupwork Exercie G (Heap-Sor) Ue Heap-Sor wih a min-heap

More information

Backward Stochastic Differential Equations and Applications in Finance

Backward Stochastic Differential Equations and Applications in Finance Backward Sochaic Differenial Equaion and Applicaion in Finance Ying Hu Augu 1, 213 1 Inroducion The aim of hi hor cae i o preen he baic heory of BSDE and o give ome applicaion in 2 differen domain: mahemaical

More information

ON FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES

ON FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES Communicaion on Sochaic Analyi Vol. 5, No. 1 211 121-133 Serial Publicaion www.erialpublicaion.com ON FRACTIONAL ORNSTEIN-UHLENBECK PROCESSES TERHI KAARAKKA AND PAAVO SALMINEN Abrac. In hi paper we udy

More information

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems Sample Final Exam Covering Chaper 9 (final04) Sample Final Exam (final03) Covering Chaper 9 of Fundamenal of Signal & Syem Problem (0 mar) Conider he caual opamp circui iniially a re depiced below. I LI

More information

Systems of nonlinear ODEs with a time singularity in the right-hand side

Systems of nonlinear ODEs with a time singularity in the right-hand side Syem of nonlinear ODE wih a ime ingulariy in he righ-hand ide Jana Burkoová a,, Irena Rachůnková a, Svaolav Saněk a, Ewa B. Weinmüller b, Sefan Wurm b a Deparmen of Mahemaical Analyi and Applicaion of

More information

Physics 240: Worksheet 16 Name

Physics 240: Worksheet 16 Name Phyic 4: Workhee 16 Nae Non-unifor circular oion Each of hee proble involve non-unifor circular oion wih a conan α. (1) Obain each of he equaion of oion for non-unifor circular oion under a conan acceleraion,

More information

On the Exponential Operator Functions on Time Scales

On the Exponential Operator Functions on Time Scales dvance in Dynamical Syem pplicaion ISSN 973-5321, Volume 7, Number 1, pp. 57 8 (212) hp://campu.m.edu/ada On he Exponenial Operaor Funcion on Time Scale laa E. Hamza Cairo Univeriy Deparmen of Mahemaic

More information

Coupling Homogenization and Large Deviations. Principle in a Parabolic PDE

Coupling Homogenization and Large Deviations. Principle in a Parabolic PDE Applied Mahemaical Science, Vol. 9, 215, no. 41, 219-23 HIKARI Ld, www.m-hikari.com hp://dx.doi.org/1.12988/am.215.5169 Coupling Homogenizaion and Large Deviaion Principle in a Parabolic PDE Alioune Coulibaly,

More information

Backward stochastic differential equations and integral partial differential equations

Backward stochastic differential equations and integral partial differential equations Backward ochaic differenial equaion and inegral parial differenial equaion Guy BARLS, Rainer BUCKDAHN 1 and ienne PARDOUX 2 June 30, 2009 Abrac We conider a backward ochaic differenial equaion, whoe he

More information

NEUTRON DIFFUSION THEORY

NEUTRON DIFFUSION THEORY NEUTRON DIFFUSION THEORY M. Ragheb 4//7. INTRODUCTION The diffuion heory model of neuron ranpor play a crucial role in reacor heory ince i i imple enough o allow cienific inigh, and i i ufficienly realiic

More information

Approximation for Option Prices under Uncertain Volatility

Approximation for Option Prices under Uncertain Volatility Approximaion for Opion Price under Uncerain Volailiy Jean-Pierre Fouque Bin Ren February, 3 Abrac In hi paper, we udy he aympoic behavior of he wor cae cenario opion price a he volailiy inerval in an uncerain

More information

ANSWERS TO ODD NUMBERED EXERCISES IN CHAPTER

ANSWERS TO ODD NUMBERED EXERCISES IN CHAPTER John Riley 6 December 200 NWER TO ODD NUMBERED EXERCIE IN CHPTER 7 ecion 7 Exercie 7-: m m uppoe ˆ, m=,, M (a For M = 2, i i eay o how ha I implie I From I, for any probabiliy vecor ( p, p 2, 2 2 ˆ ( p,

More information

The Residual Graph. 12 Augmenting Path Algorithms. Augmenting Path Algorithm. Augmenting Path Algorithm

The Residual Graph. 12 Augmenting Path Algorithms. Augmenting Path Algorithm. Augmenting Path Algorithm Augmening Pah Algorihm Greedy-algorihm: ar wih f (e) = everywhere find an - pah wih f (e) < c(e) on every edge augmen flow along he pah repea a long a poible The Reidual Graph From he graph G = (V, E,

More information

FLAT CYCLOTOMIC POLYNOMIALS OF ORDER FOUR AND HIGHER

FLAT CYCLOTOMIC POLYNOMIALS OF ORDER FOUR AND HIGHER #A30 INTEGERS 10 (010), 357-363 FLAT CYCLOTOMIC POLYNOMIALS OF ORDER FOUR AND HIGHER Nahan Kaplan Deparmen of Mahemaic, Harvard Univeriy, Cambridge, MA nkaplan@mah.harvard.edu Received: 7/15/09, Revied:

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

U T,0. t = X t t T X T. (1)

U T,0. t = X t t T X T. (1) Gauian bridge Dario Gabarra 1, ommi Soinen 2, and Eko Valkeila 3 1 Deparmen of Mahemaic and Saiic, PO Box 68, 14 Univeriy of Helinki,Finland dariogabarra@rnihelinkifi 2 Deparmen of Mahemaic and Saiic,

More information

Measure-valued Diffusions and Stochastic Equations with Poisson Process 1

Measure-valued Diffusions and Stochastic Equations with Poisson Process 1 Publihed in: Oaka Journal of Mahemaic 41 (24), 3: 727 744 Meaure-valued Diffuion and Sochaic quaion wih Poion Proce 1 Zongfei FU and Zenghu LI 2 Running head: Meaure-valued Diffuion and Sochaic quaion

More information

Modeling the Evolution of Demand Forecasts with Application to Safety Stock Analysis in Production/Distribution Systems

Modeling the Evolution of Demand Forecasts with Application to Safety Stock Analysis in Production/Distribution Systems Modeling he Evoluion of Demand oreca wih Applicaion o Safey Sock Analyi in Producion/Diribuion Syem David Heah and Peer Jackon Preened by Kai Jiang Thi ummary preenaion baed on: Heah, D.C., and P.L. Jackon.

More information

Optimal State-Feedback Control Under Sparsity and Delay Constraints

Optimal State-Feedback Control Under Sparsity and Delay Constraints Opimal Sae-Feedback Conrol Under Spariy and Delay Conrain Andrew Lamperki Lauren Leard 2 3 rd IFAC Workhop on Diribued Eimaion and Conrol in Neworked Syem NecSy pp. 24 29, 22 Abrac Thi paper preen he oluion

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

Backward Stochastic Partial Differential Equations with Jumps and Application to Optimal Control of Random Jump Fields

Backward Stochastic Partial Differential Equations with Jumps and Application to Optimal Control of Random Jump Fields Backward Sochaic Parial Differenial Equaion wih Jump and Applicaion o Opimal Conrol of Random Jump Field Bern Økendal 1,2, Frank Proke 1, Tuheng Zhang 1,3 June 7, 25 Abrac We prove an exience and uniquene

More information

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB

T L. t=1. Proof of Lemma 1. Using the marginal cost accounting in Equation(4) and standard arguments. t )+Π RB. t )+K 1(Q RB Elecronic Companion EC.1. Proofs of Technical Lemmas and Theorems LEMMA 1. Le C(RB) be he oal cos incurred by he RB policy. Then we have, T L E[C(RB)] 3 E[Z RB ]. (EC.1) Proof of Lemma 1. Using he marginal

More information

13.1 Accelerating Objects

13.1 Accelerating Objects 13.1 Acceleraing Objec A you learned in Chaper 12, when you are ravelling a a conan peed in a raigh line, you have uniform moion. However, mo objec do no ravel a conan peed in a raigh line o hey do no

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

Admin MAX FLOW APPLICATIONS. Flow graph/networks. Flow constraints 4/30/13. CS lunch today Grading. in-flow = out-flow for every vertex (except s, t)

Admin MAX FLOW APPLICATIONS. Flow graph/networks. Flow constraints 4/30/13. CS lunch today Grading. in-flow = out-flow for every vertex (except s, t) /0/ dmin lunch oday rading MX LOW PPLIION 0, pring avid Kauchak low graph/nework low nework direced, weighed graph (V, ) poiive edge weigh indicaing he capaciy (generally, aume ineger) conain a ingle ource

More information

Semi-discrete semi-linear parabolic SPDEs

Semi-discrete semi-linear parabolic SPDEs Semi-dicree emi-linear parabolic SPDE Nico Georgiou Univeriy of Suex Davar Khohnevian Univeriy of Uah Mahew Joeph Univeriy of Sheffield Shang-Yuan Shiu Naional Cenral Univeriy La Updae: November 2, 213

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

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information

Pathwise description of dynamic pitchfork bifurcations with additive noise

Pathwise description of dynamic pitchfork bifurcations with additive noise Pahwie decripion of dynamic pichfork bifurcaion wih addiive noie Nil Berglund and Barbara Genz Abrac The low drif (wih peed ) of a parameer hrough a pichfork bifurcaion poin, known a he dynamic pichfork

More information

5.2 GRAPHICAL VELOCITY ANALYSIS Polygon Method

5.2 GRAPHICAL VELOCITY ANALYSIS Polygon Method ME 352 GRHICL VELCITY NLYSIS 52 GRHICL VELCITY NLYSIS olygon Mehod Velociy analyi form he hear of kinemaic and dynamic of mechanical yem Velociy analyi i uually performed following a poiion analyi; ie,

More information

Class Meeting # 10: Introduction to the Wave Equation

Class Meeting # 10: Introduction to the Wave Equation MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion

More information

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles Diebold, Chaper 7 Francis X. Diebold, Elemens of Forecasing, 4h Ediion (Mason, Ohio: Cengage Learning, 006). Chaper 7. Characerizing Cycles Afer compleing his reading you should be able o: Define covariance

More information

EE202 Circuit Theory II

EE202 Circuit Theory II EE202 Circui Theory II 2017-2018, Spring Dr. Yılmaz KALKAN I. Inroducion & eview of Fir Order Circui (Chaper 7 of Nilon - 3 Hr. Inroducion, C and L Circui, Naural and Sep epone of Serie and Parallel L/C

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

18 Extensions of Maximum Flow

18 Extensions of Maximum Flow Who are you?" aid Lunkwill, riing angrily from hi ea. Wha do you wan?" I am Majikhie!" announced he older one. And I demand ha I am Vroomfondel!" houed he younger one. Majikhie urned on Vroomfondel. I

More information

arxiv: v1 [math.pr] 23 Apr 2018

arxiv: v1 [math.pr] 23 Apr 2018 arxiv:184.8469v1 [mah.pr] 23 Apr 218 The Neumann Boundary Problem for Ellipic Parial ifferenial Equaion wih Nonlinear ivergence Term Xue YANG Tianjin Univeriy e-mail: xyang213@ju.edu.cn Jing ZHANG Fudan

More information

6.302 Feedback Systems Recitation : Phase-locked Loops Prof. Joel L. Dawson

6.302 Feedback Systems Recitation : Phase-locked Loops Prof. Joel L. Dawson 6.32 Feedback Syem Phae-locked loop are a foundaional building block for analog circui deign, paricularly for communicaion circui. They provide a good example yem for hi cla becaue hey are an excellen

More information

Buckling of a structure means failure due to excessive displacements (loss of structural stiffness), and/or

Buckling of a structure means failure due to excessive displacements (loss of structural stiffness), and/or Buckling Buckling of a rucure mean failure due o exceive diplacemen (lo of rucural iffne), and/or lo of abiliy of an equilibrium configuraion of he rucure The rule of humb i ha buckling i conidered a mode

More information

LECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS

LECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS LECTURE : GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS We will work wih a coninuous ime reversible Markov chain X on a finie conneced sae space, wih generaor Lf(x = y q x,yf(y. (Recall ha q

More information

Discussion Session 2 Constant Acceleration/Relative Motion Week 03

Discussion Session 2 Constant Acceleration/Relative Motion Week 03 PHYS 100 Dicuion Seion Conan Acceleraion/Relaive Moion Week 03 The Plan Today you will work wih your group explore he idea of reference frame (i.e. relaive moion) and moion wih conan acceleraion. You ll

More information

MALLIAVIN CALCULUS FOR BACKWARD STOCHASTIC DIFFERENTIAL EQUATIONS AND APPLICATION TO NUMERICAL SOLUTIONS

MALLIAVIN CALCULUS FOR BACKWARD STOCHASTIC DIFFERENTIAL EQUATIONS AND APPLICATION TO NUMERICAL SOLUTIONS The Annal of Applied Probabiliy 211, Vol. 21, No. 6, 2379 2423 DOI: 1.1214/11-AAP762 Iniue of Mahemaical Saiic, 211 MALLIAVIN CALCULUS FOR BACKWARD STOCHASTIC DIFFERENTIAL EQUATIONS AND APPLICATION TO

More information

Flow networks. Flow Networks. A flow on a network. Flow networks. The maximum-flow problem. Introduction to Algorithms, Lecture 22 December 5, 2001

Flow networks. Flow Networks. A flow on a network. Flow networks. The maximum-flow problem. Introduction to Algorithms, Lecture 22 December 5, 2001 CS 545 Flow Nework lon Efra Slide courey of Charle Leieron wih mall change by Carola Wenk Flow nework Definiion. flow nework i a direced graph G = (V, E) wih wo diinguihed verice: a ource and a ink. Each

More information

BSDE's, Clark-Ocone formula, and Feynman-Kac formula for Lévy processes Nualart, D.; Schoutens, W.

BSDE's, Clark-Ocone formula, and Feynman-Kac formula for Lévy processes Nualart, D.; Schoutens, W. BSD', Clark-Ocone formula, and Feynman-Kac formula for Lévy procee Nualar, D.; Schouen, W. Publihed: 1/1/ Documen Verion Publiher PDF, alo known a Verion of ecord (include final page, iue and volume number)

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

The expectation value of the field operator.

The expectation value of the field operator. The expecaion value of he field operaor. Dan Solomon Universiy of Illinois Chicago, IL dsolom@uic.edu June, 04 Absrac. Much of he mahemaical developmen of quanum field heory has been in suppor of deermining

More information

14 Autoregressive Moving Average Models

14 Autoregressive Moving Average Models 14 Auoregressive Moving Average Models In his chaper an imporan parameric family of saionary ime series is inroduced, he family of he auoregressive moving average, or ARMA, processes. For a large class

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

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

Time Varying Multiserver Queues. W. A. Massey. Murray Hill, NJ Abstract

Time Varying Multiserver Queues. W. A. Massey. Murray Hill, NJ Abstract Waiing Time Aympoic for Time Varying Mulierver ueue wih Abonmen Rerial A. Melbaum Technion Iniue Haifa, 3 ISRAEL avim@x.echnion.ac.il M. I. Reiman Bell Lab, Lucen Technologie Murray Hill, NJ 7974 U.S.A.

More information

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law Vanishing Viscosiy Mehod. There are anoher insrucive and perhaps more naural disconinuous soluions of he conservaion law (1 u +(q(u x 0, he so called vanishing viscosiy mehod. This mehod consiss in viewing

More information

Parameter Estimation for Fractional Ornstein-Uhlenbeck Processes: Non-Ergodic Case

Parameter Estimation for Fractional Ornstein-Uhlenbeck Processes: Non-Ergodic Case Parameer Eimaion for Fracional Ornein-Uhlenbeck Procee: Non-Ergodic Cae R. Belfadli 1, K. E-Sebaiy and Y. Ouknine 3 1 Polydiciplinary Faculy of Taroudan, Univeriy Ibn Zohr, Taroudan, Morocco. Iniu de Mahémaique

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

CSC 364S Notes University of Toronto, Spring, The networks we will consider are directed graphs, where each edge has associated with it

CSC 364S Notes University of Toronto, Spring, The networks we will consider are directed graphs, where each edge has associated with it CSC 36S Noe Univeriy of Torono, Spring, 2003 Flow Algorihm The nework we will conider are direced graph, where each edge ha aociaed wih i a nonnegaive capaciy. The inuiion i ha if edge (u; v) ha capaciy

More information