Conditioned Martingales
|
|
- Allyson Tracey Bradley
- 5 years ago
- Views:
Transcription
1 Condiioned Maringales Nicolas Perkowski Insiu für Mahemaik Humbold-Universiä zu Berlin Johannes Ruf Oxford-Man Insiue of Quaniaive Finance Universiy of Oxford This draf: Ocober 8, 202 Absrac I is well known ha upward condiioned Brownian moion is a hree-dimensional Bessel process, and ha a downward condiioned Bessel process is a Brownian moion. We give a simple proof for his resul, which generalizes o any coninuous local maringale and clarifies he role of finie versus infinie ime in his seing. As a consequence, we can describe he law of regular diffusions ha are condiioned upward or downward. Keywords: Doob s h-ransform, change of measure; upward condiioning; downward condiioning; local maringale; diffusion; nullse; Bessel process. AMS MSC 200: 60G44; 60H99; 60J60. Inroducion We sudy he law Q of a coninuous nonnegaive P -local maringale X, if condiioned never o hi zero. The key sep in our analysis is he simple observaion ha he condiional measure Q, on he corresponding σ-algebra, is given by X T /X 0 dp, where T denoes he firs hiing ime of eiher 0 or anoher value y > X 0. This observaion relaes he change of measure over an infinie ime horizon hrough a condiioning argumen o he change of measure in finie ime via he Radon-Nikodym derivaive X T. Under he condiional measure Q, he process X diverges o, and /X is a local maringale. This insigh allows us o condiion X downwards, which corresponds o condiioning /X upwards and can herefore be reaed wih our previously developed argumens. In he case of a diffusion i is possible o wrie down he dynamics of he upward condiioned process explicily, defined via is scale funcion, - and similarly for downward condiioned diffusion. For example, if X is a P -Brownian moion sopped in 0, hen X is a Q-hree-dimensional Bessel process. This connecion of Brownian moion and Bessel process has been well known, a leas since he work of McKean [] building on Doob [4]. Following McKean, several differen proofs were given for his resul, mosly embedding his saemen in a more general resul such as he one abou pah decomposiions in Williams [9]. Mos of hese proofs are analyical and rely srongly on he Markov propery of Brownian moion and Bessel process - or even on he fac ha he ransiion densiies are known for hese processes. As he sudy of he law of upward and downward condiioned processes has usually no been he main focus of hese papers, resuls have, o he bes of our knowledge, no been proven in he full generaliy of his paper, and he underlying argumens were ofen only indirec. Our proof uses only elemenary argumens, i is probabilisic, and works for coninuous local maringales We hank Peer Carr, Peer Imkeller, and Kosas Kardaras for heir commens and suggesions. We are very graeful o Ioannis Karazas for careful reading an earlier version of his paper. We hank an anonymous referee for heir supporive remarks. N. P. is suppored by a Ph.D. scholarship of he Berlin Mahemaical School. Perkowsk@mahemaik.hu-berlin.de Johannes.Ruf@oxford-man.ox.ac.uk
2 and cerain jump processes. We show ha in finie ime i is no possible o obain a Bessel process by condiioning a Brownian moion no o hi zero and we poin ou ha condiioning a Brownian moion upward and condiioning a Bessel process downward can be undersood using he same resul. In Subsecion 2. we rea he case of upward condiioning of local maringales and in Subsecion 2.2 he case of downward condiioning. In Secion 3 we sudy he implicaions of hese resuls for diffusions. In Appendix A we illusrae ha condiioning on a nullse such as he Brownian moion never hiing zero is highly sensiive wih respec o he approximaing sequence of ses. Appendix B conains he slighly echnical proof of Proposiion 3.2, which describes he change of dynamics of a diffusion afer a change of measure. In Appendix C we sudy a class of jump processes ha can be reaed wih our mehods. Review of exising lieraure The connecion of Brownian moion and he hree-dimensional Bessel process has been sudied in several imporan and celebraed papers. Mos of hese sudies have focused on more general saemens han his connecion only. To provide a complee lis of references is beyond his noe. In he following paragraphs, we ry o give an overview of some of he mos relevan and influenial work in his area. For a Markov process X, Doob [4] sudies is h-ransform, where h denoes an excessive funcion such ha, in paricular, hx is a supermaringale. Using hx/hx 0 as a Radon- Nikodym densiy, a new sub-probabiliy measure is consruced. Doob shows, among many oher resuls, ha, if h is harmonic and addiionally minimal, as defined herein, he process X converges under he new measure o he poins on he exended real line where h akes he value infiniy. In his sense, changing he measure corresponds o condiioning he process o he even ha X converges o hese poins. For example, if X is Brownian moion sared in, hen hx = x is harmonic and leads o a probabiliy measure, under which X, now disribued as a Bessel process, ends o infiniy. Our resuls also yield his observaion; furhermore hey conain he case of non-markovian processes X ha are nonnegaive local maringales only. An analyic proof of he fac ha upward condiioned Brownian moion is a hree-dimensional Bessel process is given in McKean s work [] on Brownian excursions. He shows ha if W is a Brownian moion sared in, if B F s, where F s is he σ-algebra generaed by W up o ime s for some s > 0, and if T 0 is he hiing ime of 0, hen P W B T 0 > P X B as, where X is a hree-dimensional Bessel process. The proof is based on echniques from parial differenial equaions. In ha aricle, also a pah decomposiion is given for excursions of Brownian moion in erms of wo Bessel processes, one run forward in ime, and he oher one run backward. McKean already generalizes all hese resuls o regular diffusions. Knigh [0] compues he dynamics of Brownian moion condiioned o say eiher in he inerval [ a, a] or, a] for some a > 0 and hus, derives also he Bessel dynamics. To obain hese resuls, Knigh uses a very asue argumen based on invering Brownian local ime. He moreover illusraes he complicaions arising from condiioning on nullses by providing an insighful example; we shall give anoher example based on a direc argumen, wihou he necessiy of any compuaions, in Appendix A o illusrae his poin furher. In his seminal paper on pah decomposiions, Williams [9] shows ha Brownian moion condiioned no o hi zero corresponds o he Bessel process. His resuls exend o diffusions and reach far beyond his observaion. For example, he shows ha siching a Brownian moion up o a cerain sopping ime and a hree-dimensional Bessel process ogeher yields anoher Bessel process. In Piman and Yor [5] his approach is generalized o killed diffusions. A diffusion process is killed wih consan rae and condiioned o hi infiniy before he killing ime. This allows he inerpreaion of a wo-parameer Bessel process as an upward condiioned one-parameer Bessel process. Piman [4] proves essenially Lemma 2. of his paper in he Brownian case. This is achieved 2
3 by approximaing he coninuous processes by random walks, which can be couned. For he coninuous case, he saemen hen follows by a weak convergence argumen. The main resul of ha aricle is Piman s famous heorem ha 2W W is a Bessel process if W is a Brownian moion and W is running maximum. Baudoin [] akes a differen approach. Given a Brownian moion, a funcional Y of is pah and a disribuion ν, Baudoin consrucs a probabiliy measure under which Y is disribued as ν. The recen monograph by Roynee and Yor [7] sudies penalizaions of Brownian pahs, which can be undersood as a generalizaion of condiioned Brownian moion. Under he penalized measure, he coordinae process can have radically differen behavior han under he Wiener measure. In our example i does no hi zero. In Roynee and Yor [7] here is an example of a penalized measure under which he supremum process says almos surely bounded. 2 General case: coninuous local maringales Le Ω = C abs := C abs R +, [0, ] be he space of [0, ]-valued funcions ω ha are absorbed in 0 and, and ha are coninuous on [0, T ω, where T ω denoes he firs hiing ime of { } by ω, o be specified below. Le X be he coordinae process, ha is, X ω = ω. Define, for sake of noaional simpliciy, X := lim sup X lim inf X wih 0 :=. Denoe he canonical filraion by F 0 wih F = σx s : s, and wrie F = 0 F. For all a [0, ], define T a as he firs hiing ime of {a}, o wi, T a = inf{ [0, ] : X = a} 2. wih inf := T, represening a ime beyond infiniy. The inroducion of T allows for a unified approach o rea examples like geomeric Brownian moion. We shall exend he naural ordering o [0, ] {T} by < T for all [0, ]. For all sopping imes τ, define he σ-algebras F τ as F τ = {A F : A {τ } F [0, } = σx τ s : s < = σx τ T 0 s : s <, where X τ X τ T 0 is he process X sopped a he sopping ime τ. Le P be a probabiliy measure on Ω, F, such ha X is a nonnegaive local maringale wih P X 0 = =. 2. Upward condiioning In his secion, we sudy he law of he local maringale X condiioned never o hi zero. This even can be expressed as {T 0 = T} = {T a T 0 } {T a T 0 = T}. 2.2 a [0, a 0, ] The core of his aricle is he following simple observaion: Lemma 2. Upward condiioning. If P T a T 0 < T = for some a,, we have ha Proof. Noe ha X Ta which implies ha, for all A F, dp T a T 0 = X Ta dp. is bounded and hus a uniformly inegrable maringale. In paricular, P A T a T 0 = P A {T a T 0 } P T a T 0 yielding he saemen. = E P X Ta = ap T a T 0 + 0, = P A {T a T 0 } a = E P X T a A, The definiion of X is no furher relevan as X converges or diverges o infiniy almos surely under all measures ha we shall consider. We chose his definiion of X since i commues wih aking he reciprocal /X. 3
4 Three differen probabiliy measures Consider hree possible probabiliy measures:. The local maringale X inroduces an h-ransform Q of P. This is he unique probabiliy measure Q on Ω, F ha saisfies dq Fτ = X τ dp Fτ for all sopping imes τ for which X τ is a uniformly inegrable maringale. The probabiliy measure Q is called he Föllmer measure of X, see Föllmer [6] and Meyer [2]. 2 Noe ha he consrucion of his measure does no require he densiy process X o be he canonical process on Ω - he exension only relies on he opological srucure of Ω = C abs. This will be imporan laer, when we consider diffusions. We remark ha, in he case of X being a P -maringale, we could also use a sandard exension heorem, such as Theorem.3.5 in Sroock and Varadhan [8]. 2. If P T 0 = T = 0, Lemma 2. in conjuncion wih 2.2 direcly yields he consisency of he family of probabiliy measures {P T a T 0 } a> on he filraion F Ta a>. By Föllmer s consrucion again, here exiss a unique probabiliy measure Q on Ω, F, such ha Q FTa = P T a T 0 FTa. 3. If P T 0 = T > 0, we can define he probabiliy measure Q = P T 0 = T via he Radon-Nikodym derivaive {T0 =T}/P T 0 = T. Since in he case P T 0 = T = 0, we have {T a T 0 } = P a.s. {T a < T 0 } for all a 0, ], he measure Q is also called upward condiioned measure since i is consruced by ieraively condiioning he process X o hi any level a before hiing 0. Relaionship of probabiliy measures We are now ready o relae he hree probabiliy measures consruced above: Theorem 2.2 Ideniy of measures. Se b := P T 0 = T = P X > 0. If b = 0, hen Q = Q. If b > 0, hen Q = Q if and only if X is a uniformly inegrable maringale wih P X {0, /b} =. Proof. Firs, consider he case b = 0. Boh Q and Q saisfy, for all a >, d Q FTa = X Ta dp FTa = dq FTa. Thus Q and Q agree on a> F Ta = a> σx Ta : 0 = F. Nex, consider he case b > 0. Then, Q = Q and d Q/dP F /b imply ha X /b, yielding ha X is a uniformly inegrable maringale wih X = dq/dp {0, /b}. For he reverse direcion, observe ha X = {T0 =T}/b. This observaion ogeher wih is uniform inegrabiliy complees he proof. This heorem implies, in paricular, ha in finie ime he hree-dimensional Bessel process canno be obained from condiioning Brownian moion no o hi zero. However, over finie ime-horizons, a Bessel-process can be consruced via he h-ransform X T dp, when X is P - Brownian moion sared in and sopped in 0. Over infinie ime-horizons, one has wo choices; he firs one is using an exension heorem for he h-ransforms, he second one is condiioning X no o hi 0 by approximaing his nullse by he sequence of evens ha X his any a > 0 before i his 0. 2 See also Delbaen and Schachermayer [3] for a discussion of his measure, Pal and Proer [3] for he exension o infinie ime horizons and Carr, Fisher, and Ruf [2] for allowing nonnegaive local maringales. 4
5 Remark 2.3 Condiioning on nullses. We remark ha he inerpreaion of he measure Q as P condiioned on a nullse requires specifying an approximaing sequence of ha nullse. In Appendix A we illusrae his suble bu imporan poin. Remark 2.4 The rans-infinie ime T. The inroducion of T in his subsecion allows us o inroduce he upward-condiioned measure Q and o show is equivalence o he h-ransform Q if X converges o zero bu no necessarily his zero in finie ime, such as P -geomeric Brownian moion. If one is only ineresed in processes as, say, sopped Brownian moion, hen one could formulae all resuls in his subsecion in he sandard way when inf := in 2.. One would hen need o exchange T by hroughou his subsecion; in paricular, one would have o assume in Lemma 2. ha P T a T 0 < = and replace he condiion P T 0 = T = 0 by P T 0 = = 0 for he consrucion of he upward-condiioned measure Q. We noe ha he argumens of his secion can be exended o cerain jump processes. In Appendix C we rea a simple random walk example o illusrae his observaion. 2.2 Downward condiioning In his subsecion, we consider he converse case of condiioning X downward insead of upward. Towards his end, we firs provide a well-known resul; see for example [2]. For sake of compleeness, we provide a direc proof: Lemma 2.5 Local maringaliy of /X. Under he h-ransformed measure Q, he process /X is a nonnegaive local maringale and QT = T = E P [X ]. Proof. Observe ha fe Q A X T /n +s = lim E Q = lim E P = lim E P = lim E Q = E Q A X T /n A {Tm>} A {Tm>} A {Tm>} A {Tm>} X T /n T m +s X T /n T m +s X T /n T m X T /n T m + E Q X Tm +s X Tm + E Q + E Q + E Q A {T } X T /n +s A {T } X T /n A {T } X T /n A {T } X T /n for all A F and s, 0, where in he hird equaliy we considered he wo evens {T /n } and {T /n > } separaely and used he P -maringaliy of X Tm afer condiioning on F and F T/n, respecively - noe ha A {T m > } {T /n > } F T/n. The local maringaliy of /X hen follows from Q lim T /n < = lim Q lim T /n < T m = lim E P {limn T n n /n <T m}x Tm = 0. Therefore, /X converges Q-almos surely o some random variable /X. We observe ha QT = T = lim QT m < = lim E P {Tm< }X Tm = lim E P {Tm }X = E P X, where we use ha X converges P -almos surely. 5
6 The las lemma direcly implies he following observaion: Corollary 2.6 Muual singulariy. We have P X = 0 = if and only if QX = =. This observaion is consisen wih our undersanding ha eiher condiion implies ha he wo measures are suppored on wo disjoin ses. Corollary 2.6 is also consisen wih Theorem 2.2, which yields ha P X = 0 = implies he ideniy Q = Q, where Q denoes he upward condiioned measure. Lemma 2.5 indicaes ha we can condiion X downward under Q, corresponding o condiioning /X upward. The proof of he nex resul is exacly along he lines of he argumens in Subsecion 2.; however, now wih he Q-local maringale /X aking he place of he P -local maringale X: Theorem 2.7 Downward condiioning. If b of Thereom 2.2 saisfies b = 0, hen dq T /a T = X T/a dq for all a >. In paricular, here exiss a unique probabiliy measure P, such ha P FT/a = Q T /a < T; in fac, P = P. 3 Diffusions In his secion, we apply Theorems 2.2 and 2.7 o diffusions. 3. Definiion and h-ransform for diffusions We call diffusion any ime-homogeneous srong Markov process Y : C abs [0, [l, r] wih coninuous pahs in a possibly infinie inerval [l, r] wih l < r. Noe ha we explicily allow Y o ake he values l and r; we sop Y once i his he boundary of [l, r]. We define τ a for all a [l, r] as in 2. wih X replaced by Y. We denoe he probabiliy measure under which Y 0 = y [l, r] by P y. Since Y is Markovian i has an infiniesimal generaor see page 6 in Ehier and Kurz [5]. As we do no assume any regulariy of he semigroup of Y, we find i convenien o work wih he following exended infiniesimal generaor: A coninuous funcion f : [l, r] R {, } wih f R R is in he domain of he exended infiniesimal generaor L of Y if here exiss a coninuous funcion g : [l, r] R {, } wih g R R, and an increasing sequence of sopping imes {ρ n } n N, such ha P y lim n ρ n τ l τ r = and ρn fy ρn fy gy s ds 0 is a P y -maringale for all y l, r. In ha case we wrie f doml and Lf = g. Throughou his secion we shall work wih a regular diffusion Y ; ha is, for all y, z l, r we have ha P y τ z < > 0. In ha case here always exiss a coninuous, sricly increasing funcion s : l, r R {, }, uniquely deermined up o an affine ransformaion, such ha sy is a local maringale see Proposiions VII.3.2 and VII.3.5 in Revuz and Yor [6]. We call every such s a scale funcion for Y, and we exend is domain o [l, r] by aking limis. The nex resul summarizes Proposiion VII.3.2 in [6] and describes he relaionship of he scale funcion s and he limiing behaviour of Y : Lemma 3. Scale funcion. We have ha. P y τ l = T = 0 for one and hen for all y l, r if and only if sl R and sr = ; 6
7 2. P y τ r = T = 0 for one and hen for all y l, r if and only if sl = and sr R; 3. P y τ l τ r = T = 0 and P y τ l < T 0, for one and hen for all y l, r if and only if sl R and sr R. Throughou his secion, we shall work wih he sanding assumpion ha he scale funcion s saisfies sl > Assumpion L or sr < Assumpion R. Wihou loss of generaliy, we shall assume ha hen sl = 0 or sr = 0, respecively, and ha F = F τl τ r. Since by assumpion sy is a local maringale, i defines, under each P y, a Föllmer measure Q y as in Secion 2, where we would se X := sy /sy, for all y [l, r] wih 0/0 := / :=. The nex proposiion illusraes how he exended infiniesimal generaors of Y under P y and Q y are relaed: Proposiion 3.2 h-ransform for diffusions. The process Y is a regular diffusion under he probabiliy measures {Q y } y [l,r]. Is exended infiniesimal generaor L s under {Q y } y [l,r] is given by doml s = {ϕ : sϕ doml} and L s ϕy = sy L[sϕ]y. The proof of his proposiion is echnical and herefore posponed o Appendix B. The following observaion is a direc consequence of Lemma 2.5 and he fac ha Y is a regular diffusion under he probabiliy measures {Q y } y [l,r] : Lemma 3.3 Scale funcion for h-ransform. Under {Q y } y [l,r], he funcion s = /s is, wih he appropriae definiion of /0, a scale funcion for Y wih sl =, sr R under Assumpion L and wih sr =, sl R under Assumpion R. 3.2 Condiioned diffusions We now are ready o formulae and prove a version of he saemens of Secion 2 for diffusions: Corollary 3.4 Condiioning of diffusions. Fix y l, r and make Assumpion L.. Suppose ha P y τ l = T = 0, which is equivalen o sr =. Then he family of probabiliy measures {P y τ a τ l Fτa } y<a<r is consisen and hus has an exension Q y on F. Moreover, he exension saisfies Q y = Q y. 2. Suppose ha P y τ l = T > 0, which is equivalen o sr <, and define Q y = P y τ l = T. Then Q y saisfies Q y = Q y. Furhermore, provided ha sr =, he family of probabiliy measures {Q y τ a τ r Fτa } l<a<y is consisen. Is unique exension is P y. Under Assumpion R, all saemens sill hold wih r exchanged by l and, implicily, y < a < r exchanged by l < a < y. Proof. We only consider he case of Assumpion L, as Assumpion R requires he same seps. We wrie X = sy /sy. The hiing imes T a of X are defined as in 2.. Since s is sricly increasing, we have ha, for all y < a < r, {τ a τ l } = {T sa/sy T 0 }. Since X is a nonnegaive local maringale wih P y X 0 = =, he saemens in. and 2. follow immediaely from Theorem 2.2 and Lemma 3., which shows ha sy akes exacly wo values. The remaining asserions follow from Lemma 3.3 and Theorem
8 I is clear ha he measure Q under Assumpion L corresponds o he upward condiioned diffusion Y, while under Assumpion R i corresponds o he downward condiioned diffusion. Afer finishing his manuscrip we learned abou Kardaras [9]. Therein, by similar echniques i is shown ha Y under Q ends o infiniy if sr = ; see Secion 6.2 in [9]. In Secion 5 herein, a similar probabiliy measure is consruced for a Lévy process X ha drifs o. Afer a change of measure of he form sx for a harmonic funcion s, he process X under he new measure drifs now again o infiniy. 3.3 Explici generaors In his secion we formally derive he dynamics of upward condiioned and downward condiioned diffusions. For his purpose suppose ha Y is a diffusion wih exended infiniesimal generaor L, such ha doml C 2, where C 2 denoes he space of wice coninuously differeniable funcions on l, r, and Lϕy = byϕ y + 2 ayϕ y, ϕ C 2 for some locally bounded funcions b and a such ha ay > 0 for all y l, r. Finding he scale funcion hen a leas formally corresponds o solving he linear ordinary differenial equaion bys y + 2 ays y = This is for example done in Secion 5.5.B of Karazas and Shreve [8]. From now on, we coninue under eiher Assumpion L or Assumpion R wih s being eiher nonnegaive or nonposiive. We plug s ino he definiion of L s. Towards his end, le ϕ C 2. Then we have ha L s ϕy = sy Lsϕy = bysϕ y + sy 2 aysϕ y = bys yϕy + syϕ y + 2 ays yϕy + 2s yϕ y + syϕ y = sy by + ays y sy ϕ y + 2 ayϕ y since s = 2b/as due o 3.. Therefore, he upward or downward condiioned process has an addiional drif of as /s. This drif is always posiive or always negaive, as is o be expeced. Now, under Assumpion L upward condiioning wih l = 0, if b = 0, hen sy = y; herefore he addiional drif of he upward condiioned process is ay/y. Under Assumpion R downward condiioning wih r =, if by = ay/y, hen 3. yields sy = y and hus an addiional drif of ay/y = by. These observaions lead o he well-known fac: Corollary 3.5 Geomeric Brownian moion. A Brownian moion condiioned on hiing before hiing 0 is a hree-dimensional Bessel process. Vice versa, a hree-dimensional Bessel process condiioned o hi 0 is a Brownian moion. Moreover, a geomeric Brownian moion condiioned on hiing before hiing 0 is a geomeric Brownian moion wih uni drif. A Condiioning on nullses Before Theorem 2.2, we consruced a probabiliy measure Q by condiioning P on he nullse {T 0 = T} = a [0, {T a T 0 } using an exension heorem. I is imporan o poin ou ha he choice of he approximaing sequence of evens, necessary for his consrucion, is highly 8
9 relevan. We remark ha his has been illusraed before by Knigh [0] wih anoher example, which, in our opinion, is slighly more involved han he one presened in he following. To illusrae he issue, consider he coninuous maringale X, defined as X = X + X {T3/4 } + 8 X 2 {T3/4 < T /4 }; he process X moves wice as much as X unil X his 3/4, hen i moves half as much as X unil X caches up, which occurs when X his /4. Wih his undersanding, i is clear ha X his zero exacly when X his zero. Therefore, we have ha {T 0 = T} = a [0, { T a T 0 }, where T a is defined exacly like T a wih X replaced by X in 2.. Now, i is easy o see ha P T a T 0 defines a consisen family of probabiliy measures on he filraion F T0 T a a> ; namely he one defined hrough he Radon-Nikodym derivaives X Ta. Since P X Ta X Ta > 0, he induced measure differs from he one in Theorem 2.2. Therefore, alhough in he limi we condiion on he same even, he induced probabiliy measures srongly depend on he approximaing sequence of evens. B Proof of Proposiion 3.2 We only discuss he case sl = 0 since he case sr = 0 follows in he same way. In order o show he Markov propery of Y under Q y, we need o prove ha E Qy fy ρ+ F ρ = E Qy fy ρ+ Y ρ for all 0, for all bounded and coninuous funcions f : [l, r] R, and for all finie sopping imes ρ. On he even {ρ τ r }, he equaliy holds rivially as Y ges absorbed in l and r. On he even {ρ < τ r }, observe ha E Qy fy ρ+ F ρ = lim E Qy fyρ+ τa F ρ = lim E Qy fy τa τa ρ+ Yρ = E Qy fy ρ+ Y ρ, a r a r where he second equaliy follows from he generalized Bayes formula in Proposiion C.2 in [2] and he Markov propery of Y τa under P y. Therefore, Y is srongly Markovian under Q y. Since Y is also ime-homogeneous under any of he measures Q y, we have shown ha Y is a diffusion under {Q y } y [l,r]. As for he regulariy, fix a l, y and b y, r. Observe ha Q y is equivalen o P y on F τa τb. This fac in conjuncion wih he regulariy of Y under P and Proposiion VII.3.2 in [6] yields ha Q y τ a < > 0 as well as Q y τ b < > 0. Denoe now he exended infiniesimal generaor of Y under {Q y } y [l,r] by G, le ϕ domg wih localizing sequence {ρ n } n N, and fix y l, r. Fix wo sequences {a n } n N and {b n } n N wih a n l and b n r as n. We may assume, wihou loss of generaliy, ha ρ n τ an τ bn. By definiion of he exended infiniesimal generaor, ϕy ρn ϕy ρn 0 GϕY s ds is a Q y -maringale. Since ϕ and Gϕ are bounded on [a n, b n ] his fac, in conjuncion wih Fubini s heorem, yields ha ρn ϕy ρn sy ρn ϕysy GϕYu ρn syu ρn du sy is a P y -maringale. Since {ρ n } n N converges P y -almos surely o τ l τ r for all y l, r his implies ha ϕs doml and L[sϕ]y = Gϕysy. The oher inclusion can be shown in he same manner, which complees he proof. 9 0
10 C Jumps Here we illusrae on a simple example ha our resuls abou upward condiioning can be exended o cerain jump processes. Towards his end, we consider he canonical space of pahs ω aking values in [0, ], geing absorbed in eiher 0 or, and being càdlàg on [0, T ω. The measure P is chosen in such a way ha he canonical process X is a purely disconinuous maringale saring in, whose semimaringale characerisics under he runcaion funcion hx = x x are given by 0, 0, ν. Here ν is a predicable random measure, he compensaor of he jump measure of X. We assume ha νω, ds, dx = ν in ω, ds 2 δ /N + δ /N dx, for some N N, where ν in denoes he jump inensiy, and ha ν in ω, ds X s ων in ω, ds; o wi, X only has jumps of size ±/N and ges absorbed when hiing 0. We furhermore assume ha ν is bounded away from and 0; ha is, ha for all 0 here exis wo nonnegaive funcions c and C ending o infiniy as increases such ha {X ω>0}c ν in ω, ds C. [0,] For example, X could be a compound Poisson process wih jumps of size ±/N, geing absorbed in 0. The condiions on X guaranee ha P T 0 < = since a one-dimensional random walk is recurren; furhermore, X saisfies P T n/n < > 0 for all n N. Therefore, he asserion of Lemma 2. holds for a = n/n for all n N wih n N; hence, he h-ransform Q, defined by dq F = X dp F, equals he upward condiioned measure Q, defined as he exension of he measures {P T n/n T 0 } n N. Girsanov s heorem Theorem III.3.24 in Jacod and Shiryaev [7] implies ha, under he probabiliy measure Q = Q, he process X has semimaringale characerisics 0, 0, ν, where ν ω, ds, dx = ν in ω, ds 2 Xs ω N X s ω δ /N + X s ω + N X s ω δ /N dx. These compuaions show ha we canno expec /X o be a Q-local maringale; indeed, in our example, he process /X is bounded by N and a rue Q-supermaringale. Thus, we canno obain P hrough condiioning X downward as we did for he coninuous case in Subsecion 2.2. Consider now he case of deerminisic jump imes wih ν in ω, ds = {Xs ω>0}δ nδ ds, n= where δ := /N 2. Wih a sligh misuse of noaion allowing X 0 o ake he value x = n/n for some n N, observe ha, for all C 2 -funcions f, δ E Q[fX δ X 0 = x] fx = [ E P fx δ X ] δ δ x X 0 = x fx [ = N 2 2 f x + x + /N + N x 2 f x ] x /N fx N x = [f 2 N 2 x + + f x ] 2fx N N 0
11 + x N [ f x + + f x ] 2 N N 2 f x + x f x. Using argumens based on he maringale problem, we obain he weak convergence of X under Q o a Bessel process as N ends o infiniy see Corollary in [5]. On he oher side, Donsker s heorem implies ha X converges weakly o a Brownian moion under P. We hus recover Piman s proof ha upward condiioned Brownian moion is a Bessel process; see Piman [4]. References [] Fabrice Baudoin, Condiioned sochasic differenial equaions: heory, examples and applicaion o finance, Sochasic Process. Appl , MR 9960 [2] Peer Carr, Travis Fisher, and Johannes Ruf, On he hedging of opions on exploding exchange raes, Preprin, arxiv: , 202. [3] Freddy Delbaen and Waler Schachermayer, Arbirage possibiliies in Bessel processes and heir relaions o local maringales, Probab. Theory Relaed Fields , no. 3, MR [4] Joseph L. Doob, Condiional Brownian moion and he boundary limis of harmonic funcions, Bull. Soc. Mah. France , MR [5] Sewar N. Ehier and Thomas G. Kurz, Markov processes: Characerizaion and convergence, John Wiley & Sons, Hoboken, NJ, 986. MR [6] Hans Föllmer, The exi measure of a supermaringale, Z. Wahrscheinlichkeisheorie und Verw. Gebiee 2 972, MR [7] Jean Jacod and Alber N. Shiryaev, Limi heorems for sochasic processes, 2nd ed., Springer, Berlin, MR [8] Ioannis Karazas and Seven E. Shreve, Brownian moion and sochasic calculus, 2nd ed., Springer, Berlin, 99. MR 2940 [9] Consaninos Kardaras, On he sochasic behavior of opional processes up o random imes, Preprin, arxiv:007.24, 202. [0] Frank B. Knigh, Brownian local imes and aboo processes, Trans. Amer. Mah. Soc , MR [] Henry P. McKean, Excursions of a non-singular diffusion, Z. Wahrscheinlichkeisheorie und Verw. Gebiee 963, MR [2] Paul A. Meyer, La mesure de H. Föllmer en héorie de surmaringales, Séminaire de Probabiliés, VI, Springer, Berlin, 972, pp MR [3] Soumik Pal and Philip E. Proer, Analysis of coninuous sric local maringales via h- ransforms, Sochasic Process. Appl , no. 8, MR [4] James W. Piman, One-dimensional Brownian moion and he hree-dimensional Bessel process, Adv. in Appl. Probab , no. 3, MR [5] Jim Piman and Marc Yor, Bessel processes and infiniely divisible laws, Sochasic Inegrals, LMS Durham Symposium 980, 98, pp MR
12 [6] Daniel Revuz and Marc Yor, Coninuous maringales and Brownian moion, 3rd ed., Springer, Berlin, 999. MR [7] Bernard Roynee and Marc Yor, Penalising Brownian pahs, Springer, Berlin, MR [8] Daniel W. Sroock and S. R. Srinivasa Varadhan, Mulidimensional Diffusion Processes, Springer, Berlin, Berlin, 2006, Reprin of he 997 ediion. MR [9] David Williams, Pah decomposiion and coninuiy of local ime for one-dimensional diffusions, I., Proc. Lond. Mah. Soc , MR
arxiv: v1 [math.pr] 6 Oct 2008
MEASURIN THE NON-STOPPIN TIMENESS OF ENDS OF PREVISIBLE SETS arxiv:8.59v [mah.pr] 6 Oc 8 JU-YI YEN ),) AND MARC YOR 3),4) Absrac. In his paper, we propose several measuremens of he nonsopping imeness of
More informationarxiv: v1 [math.pr] 19 Feb 2011
A NOTE ON FELLER SEMIGROUPS AND RESOLVENTS VADIM KOSTRYKIN, JÜRGEN POTTHOFF, AND ROBERT SCHRADER ABSTRACT. Various equivalen condiions for a semigroup or a resolven generaed by a Markov process o be of
More informationLECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS
LECTURE : GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS We will work wih a coninuous ime reversible Markov chain X on a finie conneced sae space, wih generaor Lf(x = y q x,yf(y. (Recall ha q
More informationAn 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 informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More information6. Stochastic calculus with jump processes
A) Trading sraegies (1/3) Marke wih d asses S = (S 1,, S d ) A rading sraegy can be modelled wih a vecor φ describing he quaniies invesed in each asse a each insan : φ = (φ 1,, φ d ) The value a of a porfolio
More informationMatrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality
Marix Versions of Some Refinemens of he Arihmeic-Geomeric Mean Inequaliy Bao Qi Feng and Andrew Tonge Absrac. We esablish marix versions of refinemens due o Alzer ], Carwrigh and Field 4], and Mercer 5]
More informationA 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 informationHamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:
M ah 5 7 Fall 9 L ecure O c. 4, 9 ) Hamilon- J acobi Equaion: Weak S oluion We coninue he sudy of he Hamilon-Jacobi equaion: We have shown ha u + H D u) = R n, ) ; u = g R n { = }. ). In general we canno
More information2. Nonlinear Conservation Law Equations
. Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear
More informationThe Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions
More informationMATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence
MATH 433/533, Fourier Analysis Secion 6, Proof of Fourier s Theorem for Poinwise Convergence Firs, some commens abou inegraing periodic funcions. If g is a periodic funcion, g(x + ) g(x) for all real x,
More informationON SCHRÖDINGER S EQUATION, 3-DIMENSIONAL BESSEL BRIDGES, AND PASSAGE TIME PROBLEMS
ON SCHRÖDINGER S EQUATION, 3-DIMENSIONAL BESSEL BRIDGES, AND PASSAGE TIME PROBLEMS GERARDO HERNÁNDEZ-DEL-VALLE Absrac. We obain explici soluions for he densiy ϕ T of he firs-ime T ha a one-dimensional
More information23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes
Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion
More informationEXERCISES FOR SECTION 1.5
1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler
More information11!Hí MATHEMATICS : ERDŐS AND ULAM PROC. N. A. S. of decomposiion, properly speaking) conradics he possibiliy of defining a counably addiive real-valu
ON EQUATIONS WITH SETS AS UNKNOWNS BY PAUL ERDŐS AND S. ULAM DEPARTMENT OF MATHEMATICS, UNIVERSITY OF COLORADO, BOULDER Communicaed May 27, 1968 We shall presen here a number of resuls in se heory concerning
More informationChapter 2. First Order Scalar Equations
Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.
More informationHamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t
M ah 5 2 7 Fall 2 0 0 9 L ecure 1 0 O c. 7, 2 0 0 9 Hamilon- J acobi Equaion: Explici Formulas In his lecure we ry o apply he mehod of characerisics o he Hamilon-Jacobi equaion: u + H D u, x = 0 in R n
More informationThe Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite
American Journal of Operaions Research, 08, 8, 8-9 hp://wwwscirporg/journal/ajor ISSN Online: 60-8849 ISSN Prin: 60-8830 The Opimal Sopping Time for Selling an Asse When I Is Uncerain Wheher he Price Process
More informationOn a Fractional Stochastic Landau-Ginzburg Equation
Applied Mahemaical Sciences, Vol. 4, 1, no. 7, 317-35 On a Fracional Sochasic Landau-Ginzburg Equaion Nguyen Tien Dung Deparmen of Mahemaics, FPT Universiy 15B Pham Hung Sree, Hanoi, Vienam dungn@fp.edu.vn
More informationBackward 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 informationarxiv: v1 [math.fa] 9 Dec 2018
AN INVERSE FUNCTION THEOREM CONVERSE arxiv:1812.03561v1 [mah.fa] 9 Dec 2018 JIMMIE LAWSON Absrac. We esablish he following converse of he well-known inverse funcion heorem. Le g : U V and f : V U be inverse
More information23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes
Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals
More informationarxiv: v1 [math.pr] 21 May 2010
ON SCHRÖDINGER S EQUATION, 3-DIMENSIONAL BESSEL BRIDGES, AND PASSAGE TIME PROBLEMS arxiv:15.498v1 [mah.pr 21 May 21 GERARDO HERNÁNDEZ-DEL-VALLE Absrac. In his work we relae he densiy of he firs-passage
More informationDOOB S MAXIMAL IDENTITY, MULTIPLICATIVE DECOMPOSITIONS AND ENLARGEMENTS OF FILTRATIONS
Illinois Journal of Mahemaics Volume 5, Number 4, Winer 26, Pages 791 814 S 19-282 DOOB S MAXIMAL IDENTITY, MULTIPLICATIVE DECOMPOSITIONS AND ENLARGEMENTS OF FILTRATIONS ASHKAN NIKEGHBALI AND MARC YOR
More informationCash 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 informationQuasi-sure Stochastic Analysis through Aggregation
E l e c r o n i c J o u r n a l o f P r o b a b i l i y Vol. 16 (211), Paper no. 67, pages 1844 1879. Journal URL hp://www.mah.washingon.edu/~ejpecp/ Quasi-sure Sochasic Analysis hrough Aggregaion H. Mee
More informationExplicit construction of a dynamic Bessel bridge of dimension 3
Explici consrucion of a dynamic Bessel bridge of dimension 3 Luciano Campi Umu Çein Albina Danilova February 25, 23 Absrac Given a deerminisically ime-changed Brownian moion Z saring from, whose imechange
More informationMODULE 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 informationPhysics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle
Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,
More informationVehicle Arrival Models : Headway
Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where
More informationRepresentation of Stochastic Process by Means of Stochastic Integrals
Inernaional Journal of Mahemaics Research. ISSN 0976-5840 Volume 5, Number 4 (2013), pp. 385-397 Inernaional Research Publicaion House hp://www.irphouse.com Represenaion of Sochasic Process by Means of
More informationNotes for Lecture 17-18
U.C. Berkeley CS278: Compuaional Complexiy Handou N7-8 Professor Luca Trevisan April 3-8, 2008 Noes for Lecure 7-8 In hese wo lecures we prove he firs half of he PCP Theorem, he Amplificaion Lemma, up
More informationOn 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 informationGeneralized 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 informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationClass Meeting # 10: Introduction to the Wave Equation
MATH 8.5 COURSE NOTES - CLASS MEETING # 0 8.5 Inroducion o PDEs, Fall 0 Professor: Jared Speck Class Meeing # 0: Inroducion o he Wave Equaion. Wha is he wave equaion? The sandard wave equaion for a funcion
More informationFinish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!
MAT 257, Handou 6: Ocober 7-2, 20. I. Assignmen. Finish reading Chaper 2 of Spiva, rereading earlier secions as necessary. handou and fill in some missing deails! II. Higher derivaives. Also, read his
More informationExpert Advice for Amateurs
Exper Advice for Amaeurs Ernes K. Lai Online Appendix - Exisence of Equilibria The analysis in his secion is performed under more general payoff funcions. Wihou aking an explici form, he payoffs of he
More informationA New Perturbative Approach in Nonlinear Singularity Analysis
Journal of Mahemaics and Saisics 7 (: 49-54, ISSN 549-644 Science Publicaions A New Perurbaive Approach in Nonlinear Singulariy Analysis Ta-Leung Yee Deparmen of Mahemaics and Informaion Technology, The
More informationarxiv: v1 [math.pr] 28 Nov 2016
Backward Sochasic Differenial Equaions wih Nonmarkovian Singular Terminal Values Ali Devin Sezer, Thomas Kruse, Alexandre Popier Ocober 15, 2018 arxiv:1611.09022v1 mah.pr 28 Nov 2016 Absrac We solve a
More informationarxiv:math/ v2 [math.pr] 2 Aug 2007
arxiv:mah/53386v2 [mah.pr] 2 Aug 27 DOOB S MAXIMAL IDENTITY, MULTIPLICATIVE DECOMPOSITIONS AND ENLARGEMENTS OF FILTRATIONS ASHKAN NIKEGHBALI AND MARC YOR In he memory of J.L. Doob Absrac. In he heory of
More informationOptimality Conditions for Unconstrained Problems
62 CHAPTER 6 Opimaliy Condiions for Unconsrained Problems 1 Unconsrained Opimizaion 11 Exisence Consider he problem of minimizing he funcion f : R n R where f is coninuous on all of R n : P min f(x) x
More informationHomogenization of random Hamilton Jacobi Bellman Equations
Probabiliy, Geomery and Inegrable Sysems MSRI Publicaions Volume 55, 28 Homogenizaion of random Hamilon Jacobi Bellman Equaions S. R. SRINIVASA VARADHAN ABSTRACT. We consider nonlinear parabolic equaions
More informationOn Boundedness of Q-Learning Iterates for Stochastic Shortest Path Problems
MATHEMATICS OF OPERATIONS RESEARCH Vol. 38, No. 2, May 2013, pp. 209 227 ISSN 0364-765X (prin) ISSN 1526-5471 (online) hp://dx.doi.org/10.1287/moor.1120.0562 2013 INFORMS On Boundedness of Q-Learning Ieraes
More information4 Sequences of measurable functions
4 Sequences of measurable funcions 1. Le (Ω, A, µ) be a measure space (complee, afer a possible applicaion of he compleion heorem). In his chaper we invesigae relaions beween various (nonequivalen) convergences
More informationSolutions to Assignment 1
MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we
More informationarxiv: 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 informationarxiv: v1 [math.pr] 23 Jan 2019
Consrucion of Liouville Brownian moion via Dirichle form heory Jiyong Shin arxiv:90.07753v [mah.pr] 23 Jan 209 Absrac. The Liouville Brownian moion which was inroduced in [3] is a naural diffusion process
More informationLecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.
Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in
More informationMarkov Processes and Stochastic Calculus
Markov Processes and Sochasic Calculus René Caldeney In his noes we revise he basic noions of Brownian moions, coninuous ime Markov processes and sochasic differenial equaions in he Iô sense. 1 Inroducion
More informationf(s)dw Solution 1. Approximate f by piece-wise constant left-continuous non-random functions f n such that (f(s) f n (s)) 2 ds 0.
Advanced Financial Models Example shee 3 - Michaelmas 217 Michael Tehranchi Problem 1. Le f : [, R be a coninuous (non-random funcion and W a Brownian moion, and le σ 2 = f(s 2 ds and assume σ 2
More informationInternational Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN
Inernaional Journal of Scienific & Engineering Research, Volume 4, Issue 10, Ocober-2013 900 FUZZY MEAN RESIDUAL LIFE ORDERING OF FUZZY RANDOM VARIABLES J. EARNEST LAZARUS PIRIYAKUMAR 1, A. YAMUNA 2 1.
More informationUtility 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 informationt is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...
Mah 228- Fri Mar 24 5.6 Marix exponenials and linear sysems: The analogy beween firs order sysems of linear differenial equaions (Chaper 5) and scalar linear differenial equaions (Chaper ) is much sronger
More informationA FAMILY OF MARTINGALES GENERATED BY A PROCESS WITH INDEPENDENT INCREMENTS
Theory of Sochasic Processes Vol. 14 3), no. 2, 28, pp. 139 144 UDC 519.21 JOSEP LLUÍS SOLÉ AND FREDERIC UTZET A FAMILY OF MARTINGALES GENERATED BY A PROCESS WITH INDEPENDENT INCREMENTS An explici procedure
More informationOn the Timing Option in a Futures Contract
On he Timing Opion in a Fuures Conrac Francesca Biagini, Mahemaics Insiue Universiy of Munich Theresiensr. 39 D-80333 Munich, Germany phone: +39-051-2094459 Francesca.Biagini@mahemaik.uni-muenchen.de Tomas
More informationIMPLICIT AND INVERSE FUNCTION THEOREMS PAUL SCHRIMPF 1 OCTOBER 25, 2013
IMPLICI AND INVERSE FUNCION HEOREMS PAUL SCHRIMPF 1 OCOBER 25, 213 UNIVERSIY OF BRIISH COLUMBIA ECONOMICS 526 We have exensively sudied how o solve sysems of linear equaions. We know how o check wheher
More informationLecture 20: Riccati Equations and Least Squares Feedback Control
34-5 LINEAR SYSTEMS Lecure : Riccai Equaions and Leas Squares Feedback Conrol 5.6.4 Sae Feedback via Riccai Equaions A recursive approach in generaing he marix-valued funcion W ( ) equaion for i for he
More informationA 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 informationA Note on Lando s Formula and Conditional Independence
A Noe on Lando s Formula and Condiional Independence Xin Guo Rober A. Jarrow Chrisian Menn May 29, 2007 Absrac We exend Lando s formula for pricing credi risky derivaives o models where a firm s characerisics
More informationPositive 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 informationVanishing 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 informationLecture 4 Notes (Little s Theorem)
Lecure 4 Noes (Lile s Theorem) This lecure concerns one of he mos imporan (and simples) heorems in Queuing Theory, Lile s Theorem. More informaion can be found in he course book, Bersekas & Gallagher,
More informationThe Strong Law of Large Numbers
Lecure 9 The Srong Law of Large Numbers Reading: Grimme-Sirzaker 7.2; David Williams Probabiliy wih Maringales 7.2 Furher reading: Grimme-Sirzaker 7.1, 7.3-7.5 Wih he Convergence Theorem (Theorem 54) and
More informationExistence of positive solution for a third-order three-point BVP with sign-changing Green s function
Elecronic Journal of Qualiaive Theory of Differenial Equaions 13, No. 3, 1-11; hp://www.mah.u-szeged.hu/ejqde/ Exisence of posiive soluion for a hird-order hree-poin BVP wih sign-changing Green s funcion
More informationRisk assessment for uncertain cash flows: Model ambiguity, discounting ambiguity, and the role of bubbles
Finance and Sochasics manuscrip No. (will be insered by he edior) Risk assessmen for uncerain cash flows: Model ambiguiy, discouning ambiguiy, and he role of bubbles Bearice Acciaio Hans Föllmer Irina
More information10. State Space Methods
. Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he
More informationLINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS
LINEAR INVARIANCE AND INTEGRAL OPERATORS OF UNIVALENT FUNCTIONS MICHAEL DORFF AND J. SZYNAL Absrac. Differen mehods have been used in sudying he univalence of he inegral ) α ) f) ) J α, f)z) = f ) d, α,
More informationFinal Spring 2007
.615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o
More informationOn Oscillation of a Generalized Logistic Equation with Several Delays
Journal of Mahemaical Analysis and Applicaions 253, 389 45 (21) doi:1.16/jmaa.2.714, available online a hp://www.idealibrary.com on On Oscillaion of a Generalized Logisic Equaion wih Several Delays Leonid
More informationDifferential Harnack Estimates for Parabolic Equations
Differenial Harnack Esimaes for Parabolic Equaions Xiaodong Cao and Zhou Zhang Absrac Le M,g be a soluion o he Ricci flow on a closed Riemannian manifold In his paper, we prove differenial Harnack inequaliies
More informationA Note on the Equivalence of Fractional Relaxation Equations to Differential Equations with Varying Coefficients
mahemaics Aricle A Noe on he Equivalence of Fracional Relaxaion Equaions o Differenial Equaions wih Varying Coefficiens Francesco Mainardi Deparmen of Physics and Asronomy, Universiy of Bologna, and he
More informationEXISTENCE AND UNIQUENESS OF SOLUTIONS TO THE BACKWARD STOCHASTIC LORENZ SYSTEM
Communicaions on Sochasic Analysis Vol. 1, No. 3 (27) 473-483 EXISTENCE AND UNIQUENESS OF SOLUTIONS TO THE BACKWARD STOCHASTIC LORENZ SYSTEM P. SUNDAR AND HONG YIN Absrac. The backward sochasic Lorenz
More informationT 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 informationPrediction for Risk Processes
Predicion for Risk Processes Egber Deweiler Universiä übingen Absrac A risk process is defined as a marked poin process (( n, X n )) n 1 on a cerain probabiliy space (Ω, F, P), where he ime poins 1 < 2
More informationOptimal Consumption and Investment Portfolio in Jump markets. Optimal Consumption and Portfolio of Investment in a Financial Market with Jumps
Opimal Consumpion and Invesmen Porfolio in Jump markes Opimal Consumpion and Porfolio of Invesmen in a Financial Marke wih Jumps Gan Jin Lingnan (Universiy) College, China Insiue of Economic ransformaion
More informationSMT 2014 Calculus Test Solutions February 15, 2014 = 3 5 = 15.
SMT Calculus Tes Soluions February 5,. Le f() = and le g() =. Compue f ()g (). Answer: 5 Soluion: We noe ha f () = and g () = 6. Then f ()g () =. Plugging in = we ge f ()g () = 6 = 3 5 = 5.. There is a
More informationStochastic Modelling in Finance - Solutions to sheet 8
Sochasic Modelling in Finance - Soluions o shee 8 8.1 The price of a defaulable asse can be modeled as ds S = µ d + σ dw dn where µ, σ are consans, (W ) is a sandard Brownian moion and (N ) is a one jump
More informationResearch Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations
Hindawi Publishing Corporaion Boundary Value Problems Volume 11, Aricle ID 19156, 11 pages doi:1.1155/11/19156 Research Aricle Exisence and Uniqueness of Periodic Soluion for Nonlinear Second-Order Ordinary
More information1 Review of Zero-Sum Games
COS 5: heoreical Machine Learning Lecurer: Rob Schapire Lecure #23 Scribe: Eugene Brevdo April 30, 2008 Review of Zero-Sum Games Las ime we inroduced a mahemaical model for wo player zero-sum games. Any
More informationTHE 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 informationFractional Method of Characteristics for Fractional Partial Differential Equations
Fracional Mehod of Characerisics for Fracional Parial Differenial Equaions Guo-cheng Wu* Modern Teile Insiue, Donghua Universiy, 188 Yan-an ilu Road, Shanghai 51, PR China Absrac The mehod of characerisics
More informationMath 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 informationHeavy Tails of Discounted Aggregate Claims in the Continuous-time Renewal Model
Heavy Tails of Discouned Aggregae Claims in he Coninuous-ime Renewal Model Qihe Tang Deparmen of Saisics and Acuarial Science The Universiy of Iowa 24 Schae er Hall, Iowa Ciy, IA 52242, USA E-mail: qang@sa.uiowa.edu
More informationLecture 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 informationTwo 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 informationMean-Variance Hedging for General Claims
Projekbereich B Discussion Paper No. B 167 Mean-Variance Hedging for General Claims by Marin Schweizer ) Ocober 199 ) Financial suppor by Deusche Forschungsgemeinschaf, Sonderforschungsbereich 33 a he
More informationStochastic Model for Cancer Cell Growth through Single Forward Mutation
Journal of Modern Applied Saisical Mehods Volume 16 Issue 1 Aricle 31 5-1-2017 Sochasic Model for Cancer Cell Growh hrough Single Forward Muaion Jayabharahiraj Jayabalan Pondicherry Universiy, jayabharahi8@gmail.com
More informationAnn. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:
Ann. Func. Anal. 2 2011, no. 2, 34 41 A nnals of F uncional A nalysis ISSN: 2008-8752 elecronic URL: www.emis.de/journals/afa/ CLASSIFICAION OF POSIIVE SOLUIONS OF NONLINEAR SYSEMS OF VOLERRA INEGRAL EQUAIONS
More informationNEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS
QUANTUM PROBABILITY BANACH CENTER PUBLICATIONS, VOLUME 43 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 998 NEW EXAMPLES OF CONVOLUTIONS AND NON-COMMUTATIVE CENTRAL LIMIT THEOREMS MAREK
More information18 Biological models with discrete time
8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so
More informationElectrical and current self-induction
Elecrical and curren self-inducion F. F. Mende hp://fmnauka.narod.ru/works.hml mende_fedor@mail.ru Absrac The aricle considers he self-inducance of reacive elemens. Elecrical self-inducion To he laws of
More informationarxiv: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 informationDiebold, 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 informationMATH 5720: Gradient Methods Hung Phan, UMass Lowell October 4, 2018
MATH 5720: Gradien Mehods Hung Phan, UMass Lowell Ocober 4, 208 Descen Direcion Mehods Consider he problem min { f(x) x R n}. The general descen direcions mehod is x k+ = x k + k d k where x k is he curren
More informationMath 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 informationThe Arcsine Distribution
The Arcsine Disribuion Chris H. Rycrof Ocober 6, 006 A common heme of he class has been ha he saisics of single walker are ofen very differen from hose of an ensemble of walkers. On he firs homework, we
More informationConvergence of the Neumann series in higher norms
Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann
More informationLecture 10: The Poincaré Inequality in Euclidean space
Deparmens of Mahemaics Monana Sae Universiy Fall 215 Prof. Kevin Wildrick n inroducion o non-smooh analysis and geomery Lecure 1: The Poincaré Inequaliy in Euclidean space 1. Wha is he Poincaré inequaliy?
More information