On Integration-by-parts and the Itô Formula for Backwards Itô Integral
|
|
- Phebe Long
- 5 years ago
- Views:
Transcription
1 11 On Integration-by-parts and the Itô Formula for... On Integration-by-parts and the Itô Formula for Backwards Itô Integral Jayrold P. Arcede a, Emmanuel A. Cabral b a Caraga State University, Ampayon, Butuan City b Ateneo de Manila University, Quezon City a jayroldparcede@yahoo.com, b cabral@mathsci.math.admu.edu.ph Abstract: In this paper, we derive integration-by-parts formula using the generalized Riemann approach to stochastic calculus called the backwards Itô integral. Moreover, we use integration-by-parts formula to deduce the Itô formula for the backwards Itô integral. Keywords/phrases: Backwards Itô integral; backwards L - martingale; AC -property. 1 Introduction Itô Formula is the chain rule for stochastic calculus. It is one of the most important tools in stochastic calculus. The first version of this fundamental result was proved by Itô [1] in In this paper, we derived the Itô Formula by proving the integration-by-parts using the generalized Riemann approach to stochastic integrals which is called the backwards Itô integral [4, 3]. This approach is also called the Henstock approach and was discovered independently by J. Kurzweil in 195s and by R. Henstock in the 196s when studying the classical non-stochastic) integral. The reader is reminded that it is impossible to define stochastic integrals using the Riemann approach since the integrators have paths of unbounded variation and the integrands are highly oscillatory. Therefore, Henstock approach
2 J.P. Arcede, E.A. Cabral 113 has been used to define the Itô integral instead. See, for instance, [5], [8], [14], [15], [17], [18], and [] among others. These studies have shown that integrals defined by the generalized Riemann approach encompass the classical stochastic integral. Recently, Toh, T.L and Chew, T.S. [16, pp ], used the same approach to prove their integration-by-parts Formula for the Itô-Kurzweil-Henstock integral. However, their integral was defined using Riemann sums where the tags are always on the left endpoints of the subintervals. This integral is equivalent to the classical forward) Itô integral when the integrator is a Brownian motion. In this paper, backwards Itô integral [4] was defined using generalized Riemann approach, but the δ-fine division used to define our integral is backwards in the sense that the tags are the right endpoints of the disjoint left-open subintervals. The adaptedness property is preserved by using backwards filtration. Note that backwards δ-fine division is partial since a backwards δ-fine f ull division may not exist. By using Vitali s Covering theorem, we are assured that a partial backwards δ-fine division that covers almost the entire interval [, T ] exists, that is, except for a small part of [, T ] whose Lebesgue measure can be made small. Preliminaries We will assume familiarity with the definitions and basic properties which can be found in [3]. Throughout this note, R denotes the set of real numbers, R + the set of nonnegative real numbers, N the set of positive integers and Ω, G, P) denotes a probability space. Let {G s : s T } be a family of sub σ-algebras of G. Then {G s : s T } is called a backwards filtration if
3 114 On Integration-by-parts and the Itô Formula for... G t G s for all s < t T. If in addition, {G s : s T } satisfies the following condition: 1) G T contains all sets of P -measure zero in G; and ) for each s [, T ], G s = G s where G s = ε> Gs ε. Then {G s : s T } is called a standard backwards filtration. We often write {G s } instead of {G s : s T }. A stochastic process f or simply process is a function f : Ω [, T ] R, where [, T ] is an interval in R + and f, s) is G s -measurable for each s [, T ]. A process f = {f s : s [, T ]} is said to be adapted to the standard backwards filtration {G s } if f s is G s -measurable for each s [, T ]. Let B = { } B t : t R + be a standard Brownian motion BM). Let σb u : s u T ) be the smallest σ- algebra generated by {B u : s u T }. This is the smallest σ-algebra containing the information about the structure of BM on [s, T ]. Throughout this note, we assume that the standard backwards filtration {G s } is the family of σ-algebras σb u : s u T ). This family is then called the natural backwards filtration of B, see [1, pp. 39-4]). Let Ω, G, {G s }, P) be a standard backwards filtering space. We write L p Ω) for L p Ω, G, P) and f L p Ω) if Ef) p <. We also define f p = {E f p )} 1 p. For f L 1 Ω), let Ef) denote the expectation of f, that is, Ef) = fdp. The conditional Ω expectation of f given G s is the random variable Ef G s ). 3 Backwards Itô Integral In this section, we shall present the backwards Itô integral and some related results. The reader is refered to [4, 3] for proof. Let D = {u i, ξ i ], ξ i )} n be a finite collection of intervalpoint pairs of, T ]. Then D is said to be a partial division
4 J.P. Arcede, E.A. Cabral 115 of [, T ] if {u i, ξ i ]} n are disjoint subintervals of, T ]. In addition, if n u i, ξ i ] =, T ] then D is a division of [, T ]. Let δ be a positive function on, T ]. An interval-point pair u, ξ], ξ) is said to be backwards δ-fine if u, ξ] ξ δξ), ξ], whenever u, ξ] [, T ] and ξ, T ]. We call D a backwards δ-fine partial division of [, T ] if D is a partial division of [, T ] and for each i, u i, ξ i ], ξ i ) is backwards δ- fine. Given ε >, a backwards δ-fine partial division D is said to fail to cover, T ] by at most Lebesgue measure η if T n ξ i u i ) η. We remark that given any positive function δ, one may not be able to find a full) division that covers the entire interval, T ]. For example, take δξ) = ξ/. Then the interval, T ] is not covered by any finite collection of backwards δ-fine intervals. Definition 3.1 Let f = {f s : s [, T ]} be a process adapted to the standard backwards filtering space Ω, G, {G s }, P). Then f is said to be backwards Itô integrable on [, T ] if there exists an A L Ω) such that for every ε >, there exist a positive function δξ) on [, T ] and a positive number η such that for any backwards δ-fine partial division D = {u i, ξ i ], ξ i )} n of [, T ] that fails to cover [, T ] by at most Lebesgue measure η we have ) E f ξi B ξi B ui ) A ε. We call A the backwards Ito integral of f, that is, A = T f t db t. It is not difficult to check that the integral A is unique up to a set of P-measure zero. Example 3. The Brownian motion B is backwards Itô integrable on [a, b] with respect to itself, and b a B t db t = 1 B b Ba) 1 + b a).
5 116 On Integration-by-parts and the Itô Formula for... The following definitions and theorems can be found in [4, 3]. Definition 3.3 [, p.59] Let F = {F s : s [, T ]} be a stochastic process. Then the process F is said to have an AC - property if for each ε >, there exists η > such that E F u i, v i ) ) ε, for any finite collection of disjoint subintervals {u i, v i ]} n of [, T ] for which v i u i η. Theorem 3.4 Let f be backwards Itô integrable on [, T ]. Let Φξ, T ) = f ξ tdb t. Then Φ has AC -property. Theorem 3.5 Let f and F be stochastic processes on [, T ]. Then f is backwards Itô integrable to F on [, T ] if and only if i) F satisfies AC -property and ii) for every ε >, there exists a positive function δ on [, T ] such that for every backwards δ-fine partial division D = {u, ξ], ξ)} of [, T ] we have, E D) B ξi B ui ) F u i, ξ i ) ) ε. Definition 3.6 An adapted process f = {f s : s [, T ]} on Ω, G, {G s }, P) is called backwards L - martingale if i) E f s ) <, for all s [, T ]; ii) Ef t G s ) = f s whenever t s T ; and
6 J.P. Arcede, E.A. Cabral 117 iii) sup t [,T ] Ω f t dp <. Theorem 3.7 Let f be backwards Itô integrable on any subinterval [, T ] of [, ) with F s, T ) = f s t db t. Then the process {F s : s [, T ]} is backwards L -martingale with respect to its natural backwards filtration {G s }. We restate Definition 3.1 in the light of Theorem 3.4 and Theorem 3.5 as follows. Definition 3.8 Let f = {f t } t [,T ] be backwards adapted process on Ω, G, {G t }, P). Then f is said to be backwards Itô integrable on [, T ] if there exists a backwards L -martingale process F = {F t } t [,T ] that satisfies the AC -property on [, T ] such that for every ε >, there exists a positive function δξ) > such that for every backwards δ-fine partial division D = {u i, ξ i ], ξ i )} n of [, T ] we have ) E f ξi B ξi B ui ) F ξi F ui ) ε. In brief, we denote F ξi F ui by F u i, ξ i ). 4 Integration-By-Parts for the Backwards Itô Integral In this section, we shall establish the integration-by-parts and prove some results relating to it. Definition 4.1 Let G = {G t : t [, T ]} be a backwards process. For every backwards δ-fine partial division D = {u i, ξ i ], ξ i )} n of [, T ], we define G[u, ξ] := G ξ G u = Gu, ξ) 1)
7 118 On Integration-by-parts and the Itô Formula for... and V G) = inf δ sup D )) E Gu i, ξ i ) where sup is taken over all possible backwards δ-fine partial division D of [, T ] and inf is taken over all possible positive function δξ) on [, T ]. Definition 4. Let f = {f t } t [,T ] be backwards adapted process on Ω, G, {G t }, P). In Definition 3.8, replacing B by a backwards adapted process X = {X t } t [,T ], an integral fdx is defined, which is also called the backwards Itô integral with respect to X. The stochastic process F t, T ) = t fdx is not necessarily backwards L -martingale. Remark 4.3 V G) = if and only if for every ε >, there is a δξ) > on [, T ] such that for every backwards δ-fine partial division D = {u i, ξ i ], ξ i )} n of [, T ] we have D) E G u i, ξ i )) ε. The following result is very crucial in proving the Itô s Formula. Theorem 4.4 Integration-By-Parts). Let f and X be backwards adapted defined on a standard backwards filtering space Ω, G, {G t }, P). Assume that f is backwards Itô integrable with respect to X on [, T ]. Then there exists a backwards adapted process H such that V f X H) = if and only if X is backwards Itô integrable with respect to f on [, T ]. Moreover, fs)dxs) + Xs)dfs) = ft )XT ) f)x) + HT ) H)).
8 J.P. Arcede, E.A. Cabral 119 Proof : Here, we denote fξ) = f ξ, Xξ) = X ξ and Hξ) = H ξ. Suppose a backwards adapted process H exists. Let F ξ, T ) = ft)dxt) and define ξ Gξ, T ) = ft )XT ) fξ)xξ) + HT ) Hξ)) ξ ft)dxt) = ft )XT ) fξ)xξ)) F ξ, T ) + Hξ, T ). Given any ε >, there exists a positive function δ 1 on [, T ] such that for every backwards δ 1 -fine partial division D 1 = {u i, ξ i ], ξ i )} n 1 of [, T ] we have, n 1 ) E f ξi X ξi X ui ) F u i, ξ i ) ε 4. Since V f X H) = it follows by Remark 4.3, that there exists a positive function δ on [, T ] such that for every backwards δ -fine partial division D = {u i, ξ i ], ξ i )} n of [, T ] we have, n ) ε E f ξi f ui )X ξi X ui ) Hu i, ξ i ) 4. Define δξ) = min{δ 1 ξ), δ ξ)} for all ξ [, T ]. Let D = {u i, ξ i ], ξ i )} n be a backwards δ-fine partial division of [, T ]. Then we have, E X ξi f ξi f ui ) Gu i, ξ i )) < ε. Hence, X is backwards Itô integrable with respect to f on [, T ].
9 1 On Integration-by-parts and the Itô Formula for... Conversely, suppose that X is backwards Itô integrable with respect to f on [, T ] with Kt, T ) = Xs)dfs). t We follow the idea above by letting Hξ, T ) = ξ ft)dxt) + ξ Xt)dft) [ft )XT ) fξ)xξ)]. 3) Then given any ε >, there exists a positive function δ 1 on [, T ] such that for every D 1 = {u i, ξ i ], ξ i )} n 1 backwards δ 1 -fine partial division of [, T ] we have, n 1 ) E X ξi f ξi f ui ) K ξi K ui ) ε 4. Note that f is backwards Itô integrable to F t, T ) = t fs)dxs) with respect to X on [, T ]. For each ε >, there exists a positive function δ on [, T ] such that for every D = {u i, ξ i ], ξ i )} n backwards δ -fine partial division of [, T ] we have, n ) E f ξi X ξi X ui ) F ξi F ui ) ε 4. We will show that V f X H) =, that is, for each ε >, there exists a positive function δ on [, T ] such that for every backwards δ-fine partial division D = {u i, ξ i ], ξ i )} n of [, T ] we have, ) ε E f ξi f ui )X ξi X ui ) H ξi H ui ) 4.
10 J.P. Arcede, E.A. Cabral 11 Now, define δξ) = min{δ 1 ξ), δ ξ)} for all ξ [, T ]. Let D = {u i, ξ i ], ξ i )} n be a backwards δ-fine partial division of [, T ]. Then we have, E f ξi f ui )X ξi X ui ) Hu i, ξ i )) ε. The proof is now complete. The following corollary is a special case of Theorem 4.4 by putting Ht). Corollary 4.5 Let f and X be backwards adapted processes defined on Ω, G, {G t }, P). If f backwards Itô integrable with respect to X on [, T ] and V f X) =, then X is backwards Itô integrable with respect to f on [, T ]. Furthermore, fs)dxs) + Xs)dfs) = ft )XT ) f)x). Also, by letting f = X, the next corollary follows. Corollary 4.6 Let X be backwards adapted processes defined on the standard backward filtering space Ω, G, {G t }, P) such that V X) =. Then X is backwards Itô integrable with respect to X and Xs)dXs) = 1 XT ) 1 X). The next result follows from Theorem 4.4 by setting f = X and H = G.
11 1 On Integration-by-parts and the Itô Formula for... Corollary 4.7 Let X be backwards adapted processes defined on the standard backward filtering space Ω, G, {G t }, P) such that there exists a process G with V X) G) =. Then X is backwards Itô integrable with respect to X and Xs)dXs) = 1 XT ) 1 X) + 1 GT ) G)). Lemma 4.8 The following are true; i) V B) G) =, where Gu, ξ) = ξ u, and ii.) For each ε >, there exists a positive function δ on [, T ] such that for every backwards δ-fine partial division D = {u i, ξ i ], ξ i )} n of [, T ], we have [ E B ξi B ui ) ξ i u i ) ) 4 ] 1 ε. Proof : To prove i), let ε > be given and choose δξ) = ε so that for any backwards δ-fine partial division D = T {u i, ξ i ], ξ i )} n of [, T ] we have E B ξi B ui ) Gu, ξ) ) ε. In proving ii), we need to use the fact that p E B ξi B ξi )) = Cp ξ i u i ) p, 4) for some constant C p, p > see [19, p.83]). The proof is similar to that of i).
12 J.P. Arcede, E.A. Cabral 13 Example 4.9 Let X be a Brownian motion B which is by definition is backwards adapted to standard backwards filtering space Ω, G, {G t }, P). By applying the Theorem 4.7 and Lemma 4.8i), B is backwards Itô integrable with respect to itself. Moreover, by definition of G in Lemma 4.8i) we have Bs)dBs) = 1 BT ) 1 B) + 1 T 5) Observe that there is one extra term, the 1 T. This is because the Brownian motion is of unbounded variation. 5 The Itô Formula The integration-by-parts formula that is developed earlier is the main tool in proving the Itô Formula. It asserts that, if F : R R is a real valued function which is at least twice continuously differentiable on R and that the following condition ) holds: 1) F Bt))dBt), and; ) F Bt))dBt) both exist in terms of L -convergence. The goal is to show that F Bt))dBt) = F BT )) F B)) + 1 F Bt))dt 6)
13 14 On Integration-by-parts and the Itô Formula for... Note that in [11, pp ], the Itô Formula is shown using convergence in probability but we do not impose such a condition here. Lemma 5.1 Let F : R R be at least twice continuously differentiable with the condition ) above. Then there exists a backwards adapted process H such that V F B H) = if and only if the backwards adapted process Bt) is backwards Itô integrable with respect to F Bt)) on [, T ]. Furthermore, F Bt))dBt) + Bt)dF Bt)) = F BT ))BT ) F B))B) + H1) H)). Proof : Let ft) = F Bt)) and X = B, and by applying integration-by-parts, the result follows. Lemma 5. Let f be backwards Itô integrable with respect to B with the primitive process Φt, T ) = fs)dbs). t Let G = {G t : t [, T ]} be backwards adapted process. If V G Φ) =, then for every ε > there exists a positive function δ on [, T ] such that for every backwards δ- fine partial division D = {u i, ξ i ], ξ i )} n of [, T ], we have E f ξi B ξi B ui ) Gu i, ξ i )) ε. That is, Φu i, ξ i ) can be replaced by f ξi B ξi B ui ) in V G Φ) =. Proof : Let ε >. Since f is backwards Itô integrable with respect to B with the primitive process Φt, T ) =
14 J.P. Arcede, E.A. Cabral 15 t fs)dbs), it follows that there exists a positive function δ 1 on [, T ] such that for every backwards δ 1 -fine partial division D 1 = {u i, ξ i ], ξ i )} n 1 of [, T ], we have n 1 ) ε D 1 ) E f ξi B ξi B ui ) Φu i, ξ i ) 4. Since V G Φ) =, it follows from Remark 4.3 that there exists a positive function δ on [, T ] such that for every backwards δ -fine partial division D = {u i, ξ i ], ξ i )} n of [, T ], we have n ) ε D ) E Gu i, ξ i ) Φu i, ξ i ) 4. Define δξ) = min{δ 1 ξ), δ ξ)} for all ξ [, T ]. Let D = {u i, ξ i ], ξ i )} n be a backwards δ-fine partial division of [, T ], then we have D) E f ξ B ξi B ui ) Gu i, ξ i )) ε, thereby completing the proof. Theorem 5.3 Let F be a backwards adapted process that is at least twice continuously differentiable with and F Bt))dBt) F Bt))dBt), both exist in terms of L -convergence. Furthermore, we assume that lim EF Bs)) F Bt))) 4 =. t s
15 16 On Integration-by-parts and the Itô Formula for... If H is the backwards adapted process given in Lemma 5.1. Then H equals Ht, T ) = [F BT ))BT ) F Bt))Bt)] + [F BT )) F Bt))] + 1 t F Bs))ds + The following results are needed. t Bs)dF Bs)). Lemma 5.4 Let F be a backwards adapted process that is at least twice continuously differentiable. Then for every ε > given, there exists a positive function δ on [, T ] small enough such that when θ u, ξ] ξ δξ), ξ], E F Bξ)) F Bθ))) 4 ε. Proof : Observe that F is continuous and Brownian motion B has continuous sample paths. Therefore, F B is uniformly continuous on [, T ]. Thus, for every ε > there exists a positive function δξ) on [, T ] small enough such that when θ, ξ u, ξ] ξ δξ), ξ], we have By taking p = 4 we have, and the result follows. F Bξ)) F Bθ)) p ε. F Bξ)) F Bθ)) 4 ε, Lemma 5.5 Let F be a backwards adapted process that is at least twice continuously differentiable. Let D = {u i, ξ i ], ξ i )} n be a backwards δ-fine partial division of [, T ]. Then for every ε >, there exists a positive function δξ) such that D) E F Bξ i ) F Bθ i ))) Bξ i ) Bu i )) ) ε.
16 J.P. Arcede, E.A. Cabral 17 Proof : Use the fact that EBξ i ) Bu i )) 8 = βξ i u i ) 4 for some constant β and using Lemma 5.5 the result follows. We are now ready to prove the Itô formula. Proof : Observe that Hu, ξ) = F Bu))Bu) F Bξ))Bξ) + F Bξ)) F Bu)) + 1 ξ F Bs))ds + ξ u u In view of Lemma 5., in Hu, ξ), Bs)dF Bs)). 7) and ξ ξ u u F Bs))ds Bs)dF Bs)) can be replaced by F Bξ))ξ u) and Bξ)F Bξ)) F Bu))) respectively. Therefore, [ E [Hu, ξ)] = E F Bu))Bu) F Bξ))Bξ) + F Bξ)) F Bu)) + 1 F Bξ))ξ u) + Bξ) F Bξ)) F Bu)))]. On the other hand, apply the Taylor s expansion to F at Bu) up to just second order we get, F Bu)) = F Bξ)) + F Bξ)) Bu) Bξ)) + 1 F Bθ))Bξ) Bu)) 8) where θ u, ξ] and equation 8) holds pathwise. Observe that there exists α between Bu) and Bξ) such that equation 8) holds with Bθ) replaced by α. Note also that B
17 18 On Integration-by-parts and the Itô Formula for... is continuous on u, ξ], so there exist θ such that Bθ) = α Furthermore, note that Bξ) is in fact Bω, ξ), that is, Bξ) depends on ω Ω, so θ also depends on ω Ω. Now by equation 8) we get { E [Hu, ξ)] = E F Bu)) [Bu) Bξ)] + F Bξ)) { F Bξ)) + F Bξ))Bu) Bξ)) Thus, + 1 F Bθ))Bξ) Bu)) }+ 1 }. F Bξ))ξ u) E [F Bξ)) F Bu))) Bξ) Bu)) Hu, ξ)] 1 = E[ F Bθ)) Bξ) Bu)) 9) ] 1. F Bξ))ξ u) Observe that in equation 9) we assume that Bθ) be replaced by Bξ). Now, by Lemma 5.5, D) E F Bξ i ) F Bθ i ))) Bξ i ) Bu i )) ) ε, whenever D = {u i, ξ i ], ξ i )} n is a backwards δ-fine partial division of [, T ]. Now going back to equation 9), we have E [F Bξ)) F Bu)))Bξ) Bu)) Hu, ξ)] [ 1 = E F Bξ)) [ Bξ) Bu)) ξ u) ] ] 1) Let Γ k = {ξ [, T ] : EF Bξ))) 4 [k 1, k)}, k N. Then for every ε > and k N by Lemma 4.8ii) there
18 J.P. Arcede, E.A. Cabral 19 exists a positive function δ k on Γ k such that [ E Bξ) Bu)) ξ u) ) 4 ] 1 ε k k) for any backwards δ k -fine partial division D = {u i, ξ i ], ξ i )} n with ξ i Γ k. Clearly, we have [, T ] = k=1 Γ k. Define δξ) = δ k ξ), if ξ Γ k, for k = 1,, 3,.... Let D = {u i, ξ i ], ξ i )} n be any backwards δ-fine partial division of [, T ], and D k = {u i, ξ i ], ξ i ) D : ξ i Γ k }. Then D) D k ) i E F Bξ i ))) B ξi B ui ) ) ) ξ i u i [E F B ξ i ))) 4] [ E Bξi B ui ) ξ i u i ) 4] 1 = kdk ) E[B ξi B ui ) ξ i u i ) 4 ] 1 ε k k k) ε k = ε. i 11) Hence, by equation 1), we have D) E F Bξ)) F Bu)) ) Bξ) Bu)) Hu, ξ) ) = 1 4 D) E F Bξ i )) ) B ξi B ui ) ξ i u i ) )) ε
19 13 On Integration-by-parts and the Itô Formula for... and the proof is done. By substituting Hξ, T ) of Theorem 5.3 to Lemma 5.1, the Itô Formula follows. Theorem 5.6 Itô Formula) Let F : R R be a twice continuously differentiable function with additional condition and lim t s EF Bs)) F Bt))) 4 =. If F Bt)) is backwards Itô integrable with respect to Bt). Then we have s F Bt))dBt) = F Bs)) F B))+ 1 References s F Bt))dt. [1] Applebaum, David. Lévy Processes and Stochastic Calculus. Cambridge University Press, 4. [] T. S. Chew, J.Y. Tay and T. L. Toh, The non-uniform Riemann approach to Itô s integral. Real Anal. Exchange 7 1/), [3] J.P. Arcede and E.A. Cabral, An Equivalent Definition for the Backwards Itô Integral, Thai, Vol. 9 11) No. 3, [4] J.P. Arcede and E.A. Cabral, The Backwards Itô Integral, Taiwanese, submitted. [5] E. J. McShane, Stochastic Calculus and Stochastic Models, Academic Press, New York, [6] R. Henstock, Lectures on the Theory on integration, World Scientific Singapore, 1988.
20 J.P. Arcede, E.A. Cabral 131 [7] R. Henstock, The efficiency of convergence of factors for functions of a continuous real variable, Journal London Math. Soc.,Vol ), [8] R. Henstock: The General Theory of Integration. Oxford Science, [9] R. Henstock, Stochastic and other functional integrals, Real Anal. Exchange, /1991), [1] K. Itô. On a formula concerning stochastic differentials. Nagoya Math J.31951), [11] Klebaner, Fima. Introduction to Stochastic Calculus with Applications. Imperial College Press, [1] J. Kurzweil, Generalized ordinary differential equations and continuous dependence on a parameter, Czechoslovak Math. Journal, 71957), [13] P.Y. Lee, and R. Výborný, The Integral: An Easy Approach after Kurzwiel and Henstock, Cambridge University Press,. [14] T.L. Toh and T.S Chew. A variational Approach to Itô s integral, Proceedings of SAP s 98, Taiwan World Scientific, Singapore, [15] T. L. Toh and T. S. Chew, The Riemann approach to stochastic integration using non-uniform meshes, Journal of Mathematical Analysis and Application, 8 3), [16] T.L.Toh and T.S. Chew, On Itô-Kurzweil-Henstock integral and integration-by-part formula, Czechoslovak Mathematical Journal, 55 13) 5),
21 13 On Integration-by-parts and the Itô Formula for... [17] Z. R. Pop-Stojanovic, On McShanes belated stochastic integral, SIAM J. Appl. Math., 197), 899 [18] T. L. Toh et. al., The Non-Uniform Riemann Approach to Itô s Integral, Real Analysis Exchange Vol 7 No. 1/), [19] K.R. Stromberg, Probability for Analysts. 1st ed. Chapman and Hall/CRC, [] J. G. Xu and P. Y. Lee, Stochastic integrals of Itô and Henstock, Real Anal. Exchange, /1993),
Transformation and Differentiation of Henstock-Wiener Integrals (Transformasi dan Pembezaan Kamiran Henstock-Wiener)
Sains Malaysiana 46(12)(2017): 2549 2554 http://dx.doi.org/10.17576/jsm-2017-4612-33 Transformation Differentiation of Henstock-Wiener Integrals (Transformasi dan Pembezaan Kamiran Henstock-Wiener) VARAYU
More informationInner Variation and the SLi-Functions
International Journal of Mathematical Analysis Vol. 9, 2015, no. 3, 141-150 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ijma.2015.411343 Inner Variation and the SLi-Functions Julius V. Benitez
More informationDedicated to Prof. Jaroslav Kurzweil on the occasion of his 80th birthday
131 (2006) MATHEMATICA BOHEMICA No. 4, 365 378 ON MCSHANE-TYPE INTEGRALS WITH RESPECT TO SOME DERIVATION BASES Valentin A. Skvortsov, Piotr Sworowski, Bydgoszcz (Received November 11, 2005) Dedicated to
More informationStochastic Calculus (Lecture #3)
Stochastic Calculus (Lecture #3) Siegfried Hörmann Université libre de Bruxelles (ULB) Spring 2014 Outline of the course 1. Stochastic processes in continuous time. 2. Brownian motion. 3. Itô integral:
More informationLecture 21 Representations of Martingales
Lecture 21: Representations of Martingales 1 of 11 Course: Theory of Probability II Term: Spring 215 Instructor: Gordan Zitkovic Lecture 21 Representations of Martingales Right-continuous inverses Let
More information(B(t i+1 ) B(t i )) 2
ltcc5.tex Week 5 29 October 213 Ch. V. ITÔ (STOCHASTIC) CALCULUS. WEAK CONVERGENCE. 1. Quadratic Variation. A partition π n of [, t] is a finite set of points t ni such that = t n < t n1
More informationBernardo D Auria Stochastic Processes /12. Notes. March 29 th, 2012
1 Stochastic Calculus Notes March 9 th, 1 In 19, Bachelier proposed for the Paris stock exchange a model for the fluctuations affecting the price X(t) of an asset that was given by the Brownian motion.
More informationUPPER AND LOWER HENSTOCK INTEGRALS
RESEARCH Real Analysis Exchange Vol. 22(2), 1996-97, pp. 734 739 Lee Peng Yee and Zhao ongsheng, ivision of Mathematics, School of Science, National Institute of Education, Singapore 259756 e-mail: zhaod@am.nie.ac.sg
More informationACG M and ACG H Functions
International Journal of Mathematical Analysis Vol. 8, 2014, no. 51, 2539-2545 HIKARI Ltd, www.m-hiari.com http://dx.doi.org/10.12988/ijma.2014.410302 ACG M and ACG H Functions Julius V. Benitez Department
More informationComparison between some Kurzweil-Henstock type integrals for Riesz-space-valued functions
Comparison between some Kurzweil-Henstock type integrals for Riesz-space-valued functions A. Boccuto V. A. Skvortsov ABSTRACT. Some kinds of integral, like variational, Kurzweil-Henstock and (SL)-integral
More informationFinal. due May 8, 2012
Final due May 8, 2012 Write your solutions clearly in complete sentences. All notation used must be properly introduced. Your arguments besides being correct should be also complete. Pay close attention
More informationLecture 17 Brownian motion as a Markov process
Lecture 17: Brownian motion as a Markov process 1 of 14 Course: Theory of Probability II Term: Spring 2015 Instructor: Gordan Zitkovic Lecture 17 Brownian motion as a Markov process Brownian motion is
More informationStochastic Calculus February 11, / 33
Martingale Transform M n martingale with respect to F n, n =, 1, 2,... σ n F n (σ M) n = n 1 i= σ i(m i+1 M i ) is a Martingale E[(σ M) n F n 1 ] n 1 = E[ σ i (M i+1 M i ) F n 1 ] i= n 2 = σ i (M i+1 M
More informationFrom Random Variables to Random Processes. From Random Variables to Random Processes
Random Processes In probability theory we study spaces (Ω, F, P) where Ω is the space, F are all the sets to which we can measure its probability and P is the probability. Example: Toss a die twice. Ω
More informationThe McShane and the weak McShane integrals of Banach space-valued functions dened on R m. Guoju Ye and Stefan Schwabik
Miskolc Mathematical Notes HU e-issn 1787-2413 Vol. 2 (2001), No 2, pp. 127-136 DOI: 10.18514/MMN.2001.43 The McShane and the weak McShane integrals of Banach space-valued functions dened on R m Guoju
More informationTools from Lebesgue integration
Tools from Lebesgue integration E.P. van den Ban Fall 2005 Introduction In these notes we describe some of the basic tools from the theory of Lebesgue integration. Definitions and results will be given
More informationNotes on uniform convergence
Notes on uniform convergence Erik Wahlén erik.wahlen@math.lu.se January 17, 2012 1 Numerical sequences We begin by recalling some properties of numerical sequences. By a numerical sequence we simply mean
More informationAPPROXIMATING BOCHNER INTEGRALS BY RIEMANN SUMS
APPROXIMATING BOCHNER INTEGRALS BY RIEMANN SUMS J.M.A.M. VAN NEERVEN Abstract. Let µ be a tight Borel measure on a metric space, let X be a Banach space, and let f : (, µ) X be Bochner integrable. We show
More informationLecture 19 L 2 -Stochastic integration
Lecture 19: L 2 -Stochastic integration 1 of 12 Course: Theory of Probability II Term: Spring 215 Instructor: Gordan Zitkovic Lecture 19 L 2 -Stochastic integration The stochastic integral for processes
More informationconvergence theorem in abstract set up. Our proof produces a positive integrable function required unlike other known
https://sites.google.com/site/anilpedgaonkar/ profanilp@gmail.com 218 Chapter 5 Convergence and Integration In this chapter we obtain convergence theorems. Convergence theorems will apply to various types
More informationBrownian Motion and Stochastic Calculus
ETHZ, Spring 17 D-MATH Prof Dr Martin Larsson Coordinator A Sepúlveda Brownian Motion and Stochastic Calculus Exercise sheet 6 Please hand in your solutions during exercise class or in your assistant s
More informationExistence Theorem for Abstract Measure. Differential Equations Involving. the Distributional Henstock-Kurzweil Integral
Journal of Applied Mathematics & Bioinformatics, vol.4, no.1, 2014, 11-20 ISSN: 1792-6602 (print), 1792-6939 (online) Scienpress Ltd, 2014 Existence Theorem for Abstract Measure Differential Equations
More informationBOUNDEDNESS OF SET-VALUED STOCHASTIC INTEGRALS
Discussiones Mathematicae Differential Inclusions, Control and Optimization 35 (2015) 197 207 doi:10.7151/dmdico.1173 BOUNDEDNESS OF SET-VALUED STOCHASTIC INTEGRALS Micha l Kisielewicz Faculty of Mathematics,
More informationI forgot to mention last time: in the Ito formula for two standard processes, putting
I forgot to mention last time: in the Ito formula for two standard processes, putting dx t = a t dt + b t db t dy t = α t dt + β t db t, and taking f(x, y = xy, one has f x = y, f y = x, and f xx = f yy
More informationEULER MARUYAMA APPROXIMATION FOR SDES WITH JUMPS AND NON-LIPSCHITZ COEFFICIENTS
Qiao, H. Osaka J. Math. 51 (14), 47 66 EULER MARUYAMA APPROXIMATION FOR SDES WITH JUMPS AND NON-LIPSCHITZ COEFFICIENTS HUIJIE QIAO (Received May 6, 11, revised May 1, 1) Abstract In this paper we show
More informationLecture 12. F o s, (1.1) F t := s>t
Lecture 12 1 Brownian motion: the Markov property Let C := C(0, ), R) be the space of continuous functions mapping from 0, ) to R, in which a Brownian motion (B t ) t 0 almost surely takes its value. Let
More informationOn pathwise stochastic integration
On pathwise stochastic integration Rafa l Marcin Lochowski Afican Institute for Mathematical Sciences, Warsaw School of Economics UWC seminar Rafa l Marcin Lochowski (AIMS, WSE) On pathwise stochastic
More informationBernardo D Auria Stochastic Processes /10. Notes. Abril 13 th, 2010
1 Stochastic Calculus Notes Abril 13 th, 1 As we have seen in previous lessons, the stochastic integral with respect to the Brownian motion shows a behavior different from the classical Riemann-Stieltjes
More informationNumerical methods for solving stochastic differential equations
Mathematical Communications 4(1999), 251-256 251 Numerical methods for solving stochastic differential equations Rózsa Horváth Bokor Abstract. This paper provides an introduction to stochastic calculus
More informationStochastic Processes II/ Wahrscheinlichkeitstheorie III. Lecture Notes
BMS Basic Course Stochastic Processes II/ Wahrscheinlichkeitstheorie III Michael Scheutzow Lecture Notes Technische Universität Berlin Sommersemester 218 preliminary version October 12th 218 Contents
More informationOPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS
APPLICATIONES MATHEMATICAE 29,4 (22), pp. 387 398 Mariusz Michta (Zielona Góra) OPTIMAL SOLUTIONS TO STOCHASTIC DIFFERENTIAL INCLUSIONS Abstract. A martingale problem approach is used first to analyze
More informationStochastic Processes
Stochastic Processes A very simple introduction Péter Medvegyev 2009, January Medvegyev (CEU) Stochastic Processes 2009, January 1 / 54 Summary from measure theory De nition (X, A) is a measurable space
More informationON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS
PORTUGALIAE MATHEMATICA Vol. 55 Fasc. 4 1998 ON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS C. Sonoc Abstract: A sufficient condition for uniqueness of solutions of ordinary
More informationLee Peng Yee. Received December 18, 2007
Scientiae Mathematicae Japonicae Online, e-2007, 763 771 763 THE INTEGRAL À LA HENSTOCK Lee Peng Yee Received December 18, 2007 Abstract. Henstock provided a unified approach to many integrals in use.
More information1. Stochastic Processes and filtrations
1. Stochastic Processes and 1. Stoch. pr., A stochastic process (X t ) t T is a collection of random variables on (Ω, F) with values in a measurable space (S, S), i.e., for all t, In our case X t : Ω S
More informationElementary Analysis Math 140D Fall 2007
Elementary Analysis Math 140D Fall 2007 Bernard Russo Contents 1 Friday September 28, 2007 1 1.1 Course information............................ 1 1.2 Outline of the course........................... 1
More informationON WEAK SOLUTION OF A HYPERBOLIC DIFFERENTIAL INCLUSION WITH NONMONOTONE DISCONTINUOUS NONLINEAR TERM
Internat. J. Math. & Math. Sci. Vol. 22, No. 3 (999 587 595 S 6-72 9922587-2 Electronic Publishing House ON WEAK SOLUTION OF A HYPERBOLIC DIFFERENTIAL INCLUSION WITH NONMONOTONE DISCONTINUOUS NONLINEAR
More informationRepresentations of Gaussian measures that are equivalent to Wiener measure
Representations of Gaussian measures that are equivalent to Wiener measure Patrick Cheridito Departement für Mathematik, ETHZ, 89 Zürich, Switzerland. E-mail: dito@math.ethz.ch Summary. We summarize results
More informationOn the martingales obtained by an extension due to Saisho, Tanemura and Yor of Pitman s theorem
On the martingales obtained by an extension due to Saisho, Tanemura and Yor of Pitman s theorem Koichiro TAKAOKA Dept of Applied Physics, Tokyo Institute of Technology Abstract M Yor constructed a family
More informationJae Gil Choi and Young Seo Park
Kangweon-Kyungki Math. Jour. 11 (23), No. 1, pp. 17 3 TRANSLATION THEOREM ON FUNCTION SPACE Jae Gil Choi and Young Seo Park Abstract. In this paper, we use a generalized Brownian motion process to define
More informationFiltrations, Markov Processes and Martingales. Lectures on Lévy Processes and Stochastic Calculus, Braunschweig, Lecture 3: The Lévy-Itô Decomposition
Filtrations, Markov Processes and Martingales Lectures on Lévy Processes and Stochastic Calculus, Braunschweig, Lecture 3: The Lévy-Itô Decomposition David pplebaum Probability and Statistics Department,
More informationAn essay on the general theory of stochastic processes
Probability Surveys Vol. 3 (26) 345 412 ISSN: 1549-5787 DOI: 1.1214/1549578614 An essay on the general theory of stochastic processes Ashkan Nikeghbali ETHZ Departement Mathematik, Rämistrasse 11, HG G16
More informationTHEOREMS, ETC., FOR MATH 515
THEOREMS, ETC., FOR MATH 515 Proposition 1 (=comment on page 17). If A is an algebra, then any finite union or finite intersection of sets in A is also in A. Proposition 2 (=Proposition 1.1). For every
More information1 Definition of the Riemann integral
MAT337H1, Introduction to Real Analysis: notes on Riemann integration 1 Definition of the Riemann integral Definition 1.1. Let [a, b] R be a closed interval. A partition P of [a, b] is a finite set of
More informationDOOB S DECOMPOSITION THEOREM FOR NEAR-SUBMARTINGALES
Communications on Stochastic Analysis Vol. 9, No. 4 (215) 467-476 Serials Publications www.serialspublications.com DOOB S DECOMPOSITION THEOREM FOR NEAR-SUBMARTINGALES HUI-HSIUNG KUO AND KIMIAKI SAITÔ*
More informationConvergence of Banach valued stochastic processes of Pettis and McShane integrable functions
Convergence of Banach valued stochastic processes of Pettis and McShane integrable functions V. Marraffa Department of Mathematics, Via rchirafi 34, 90123 Palermo, Italy bstract It is shown that if (X
More informationarxiv:math/ v1 [math.dg] 6 Jul 1998
arxiv:math/9807024v [math.dg] 6 Jul 998 The Fundamental Theorem of Geometric Calculus via a Generalized Riemann Integral Alan Macdonald Department of Mathematics Luther College, Decorah, IA 520, U.S.A.
More informationA NOTE ON STOCHASTIC INTEGRALS AS L 2 -CURVES
A NOTE ON STOCHASTIC INTEGRALS AS L 2 -CURVES STEFAN TAPPE Abstract. In a work of van Gaans (25a) stochastic integrals are regarded as L 2 -curves. In Filipović and Tappe (28) we have shown the connection
More information( f ^ M _ M 0 )dµ (5.1)
47 5. LEBESGUE INTEGRAL: GENERAL CASE Although the Lebesgue integral defined in the previous chapter is in many ways much better behaved than the Riemann integral, it shares its restriction to bounded
More informationNONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS. Shouchuan Hu Nikolas S. Papageorgiou. 1. Introduction
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 34, 29, 327 338 NONTRIVIAL SOLUTIONS FOR SUPERQUADRATIC NONAUTONOMOUS PERIODIC SYSTEMS Shouchuan Hu Nikolas S. Papageorgiou
More informationAn Analysis of the Henstock-Kurzweil Integral
An Analysis of the Henstock-Kurzweil Integral A Thesis Submitted to the Graduate School in Partial Fulfillment for the degree of Masters of Science by Joshua L. Turner Advisor: Dr. Ahmed Mohammed Ball
More informationHardy-Stein identity and Square functions
Hardy-Stein identity and Square functions Daesung Kim (joint work with Rodrigo Bañuelos) Department of Mathematics Purdue University March 28, 217 Daesung Kim (Purdue) Hardy-Stein identity UIUC 217 1 /
More informationLecture 10. Riemann-Stieltjes Integration
Lecture 10 Riemann-Stieltjes Integration In this section we will develop the basic definitions and some of the properties of the Riemann-Stieltjes Integral. The development will follow that of the Darboux
More informationRegularity of the density for the stochastic heat equation
Regularity of the density for the stochastic heat equation Carl Mueller 1 Department of Mathematics University of Rochester Rochester, NY 15627 USA email: cmlr@math.rochester.edu David Nualart 2 Department
More informationA Concise Course on Stochastic Partial Differential Equations
A Concise Course on Stochastic Partial Differential Equations Michael Röckner Reference: C. Prevot, M. Röckner: Springer LN in Math. 1905, Berlin (2007) And see the references therein for the original
More informationExercises. T 2T. e ita φ(t)dt.
Exercises. Set #. Construct an example of a sequence of probability measures P n on R which converge weakly to a probability measure P but so that the first moments m,n = xdp n do not converge to m = xdp.
More informationDoléans measures. Appendix C. C.1 Introduction
Appendix C Doléans measures C.1 Introduction Once again all random processes will live on a fixed probability space (Ω, F, P equipped with a filtration {F t : 0 t 1}. We should probably assume the filtration
More information2 Statement of the problem and assumptions
Mathematical Notes, 25, vol. 78, no. 4, pp. 466 48. Existence Theorem for Optimal Control Problems on an Infinite Time Interval A.V. Dmitruk and N.V. Kuz kina We consider an optimal control problem on
More informationThe Gauge Integral of Denjoy, Luzin, Perron, Henstock and Kurzweil
The Gauge Integral of Denjoy, Luzin, Perron, Henstock and Kurzweil Tim Sullivan tjs@caltech.edu California Institute of Technology Ortiz Group Meeting Caltech, California, U.S.A. 12 August 2011 Sullivan
More informationFE610 Stochastic Calculus for Financial Engineers. Stevens Institute of Technology
FE610 Stochastic Calculus for Financial Engineers Lecture 3. Calculaus in Deterministic and Stochastic Environments Steve Yang Stevens Institute of Technology 01/31/2012 Outline 1 Modeling Random Behavior
More informationFirst-Return Integrals
First-Return ntegrals Marianna Csörnyei, Udayan B. Darji, Michael J. Evans, Paul D. Humke Abstract Properties of first-return integrals of real functions defined on the unit interval are explored. n particular,
More informationThe Wiener Itô Chaos Expansion
1 The Wiener Itô Chaos Expansion The celebrated Wiener Itô chaos expansion is fundamental in stochastic analysis. In particular, it plays a crucial role in the Malliavin calculus as it is presented in
More informationPanAmerican Mathematical Journal
International Publications (USA PanAmerican Mathematical Journal Volume 16(2006, Number 4, 63 79 he Kurzweil-Henstock Integral for Riesz Space-Valued Maps Defined in Abstract opological Spaces and Convergence
More informationJournal of Inequalities in Pure and Applied Mathematics
Journal of Inequalities in Pure and Applied Mathematics ON A HYBRID FAMILY OF SUMMATION INTEGRAL TYPE OPERATORS VIJAY GUPTA AND ESRA ERKUŞ School of Applied Sciences Netaji Subhas Institute of Technology
More informationBrownian Motion. 1 Definition Brownian Motion Wiener measure... 3
Brownian Motion Contents 1 Definition 2 1.1 Brownian Motion................................. 2 1.2 Wiener measure.................................. 3 2 Construction 4 2.1 Gaussian process.................................
More informationWeak solutions of mean-field stochastic differential equations
Weak solutions of mean-field stochastic differential equations Juan Li School of Mathematics and Statistics, Shandong University (Weihai), Weihai 26429, China. Email: juanli@sdu.edu.cn Based on joint works
More informationIntroduction to numerical simulations for Stochastic ODEs
Introduction to numerical simulations for Stochastic ODEs Xingye Kan Illinois Institute of Technology Department of Applied Mathematics Chicago, IL 60616 August 9, 2010 Outline 1 Preliminaries 2 Numerical
More informationfor all f satisfying E[ f(x) ] <.
. Let (Ω, F, P ) be a probability space and D be a sub-σ-algebra of F. An (H, H)-valued random variable X is independent of D if and only if P ({X Γ} D) = P {X Γ}P (D) for all Γ H and D D. Prove that if
More informationMA8109 Stochastic Processes in Systems Theory Autumn 2013
Norwegian University of Science and Technology Department of Mathematical Sciences MA819 Stochastic Processes in Systems Theory Autumn 213 1 MA819 Exam 23, problem 3b This is a linear equation of the form
More informationStochastic Differential Equations.
Chapter 3 Stochastic Differential Equations. 3.1 Existence and Uniqueness. One of the ways of constructing a Diffusion process is to solve the stochastic differential equation dx(t) = σ(t, x(t)) dβ(t)
More informationRiemann Integrable Functions
Riemann Integrable Functions MATH 464/506, Real Analysis J. Robert Buchanan Department of Mathematics Summer 2007 Cauchy Criterion Theorem (Cauchy Criterion) A function f : [a, b] R belongs to R[a, b]
More informationCourse 212: Academic Year Section 1: Metric Spaces
Course 212: Academic Year 1991-2 Section 1: Metric Spaces D. R. Wilkins Contents 1 Metric Spaces 3 1.1 Distance Functions and Metric Spaces............. 3 1.2 Convergence and Continuity in Metric Spaces.........
More informationEquiintegrability and Controlled Convergence for the Henstock-Kurzweil Integral
International Mathematical Forum, Vol. 8, 2013, no. 19, 913-919 HIKARI Ltd, www.m-hiari.com Equiintegrability and Controlled Convergence for the Henstoc-Kurzweil Integral Esterina Mema University of Elbasan,
More informationVariational Stability for Kurzweil Equations associated with Quantum Stochastic Differential Equations}
Australian Journal of Basic Applied Sciences, 7(7): 787-798, 2013 ISSN 1991-8178 Variational Stability for Kurzweil Equations associated with Quantum Stochastic Differential Equations} 1 S.A. Bishop, 2
More informationPreliminary Exam: Probability 9:00am 2:00pm, Friday, January 6, 2012
Preliminary Exam: Probability 9:00am 2:00pm, Friday, January 6, 202 The exam lasts from 9:00am until 2:00pm, with a walking break every hour. Your goal on this exam should be to demonstrate mastery of
More informationThe Uniform Integrability of Martingales. On a Question by Alexander Cherny
The Uniform Integrability of Martingales. On a Question by Alexander Cherny Johannes Ruf Department of Mathematics University College London May 1, 2015 Abstract Let X be a progressively measurable, almost
More informationMetric Spaces Lecture 17
Metric Spaces Lecture 17 Homeomorphisms At the end of last lecture an example was given of a bijective continuous function f such that f 1 is not continuous. For another example, consider the sets T =
More informationPathwise Construction of Stochastic Integrals
Pathwise Construction of Stochastic Integrals Marcel Nutz First version: August 14, 211. This version: June 12, 212. Abstract We propose a method to construct the stochastic integral simultaneously under
More informationTopics in fractional Brownian motion
Topics in fractional Brownian motion Esko Valkeila Spring School, Jena 25.3. 2011 We plan to discuss the following items during these lectures: Fractional Brownian motion and its properties. Topics in
More informationFundamental Inequalities, Convergence and the Optional Stopping Theorem for Continuous-Time Martingales
Fundamental Inequalities, Convergence and the Optional Stopping Theorem for Continuous-Time Martingales Prakash Balachandran Department of Mathematics Duke University April 2, 2008 1 Review of Discrete-Time
More informationAdditive Summable Processes and their Stochastic Integral
Additive Summable Processes and their Stochastic Integral August 19, 2005 Abstract We define and study a class of summable processes,called additive summable processes, that is larger than the class used
More informationWeak convergence and Brownian Motion. (telegram style notes) P.J.C. Spreij
Weak convergence and Brownian Motion (telegram style notes) P.J.C. Spreij this version: December 8, 2006 1 The space C[0, ) In this section we summarize some facts concerning the space C[0, ) of real
More informationA CAUCHY PROBLEM ON TIME SCALES WITH APPLICATIONS
ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I. CUZA DIN IAŞI (S.N.) MATEMATICĂ, Tomul LVII, 211, Supliment A CAUCHY PROBLEM ON TIME SCALES WITH APPLICATIONS BY BIANCA SATCO Abstract. We obtain the existence
More informationA Short Introduction to Diffusion Processes and Ito Calculus
A Short Introduction to Diffusion Processes and Ito Calculus Cédric Archambeau University College, London Center for Computational Statistics and Machine Learning c.archambeau@cs.ucl.ac.uk January 24,
More informationThe multidimensional Ito Integral and the multidimensional Ito Formula. Eric Mu ller June 1, 2015 Seminar on Stochastic Geometry and its applications
The multidimensional Ito Integral and the multidimensional Ito Formula Eric Mu ller June 1, 215 Seminar on Stochastic Geometry and its applications page 2 Seminar on Stochastic Geometry and its applications
More informationOn Mean-Square and Asymptotic Stability for Numerical Approximations of Stochastic Ordinary Differential Equations
On Mean-Square and Asymptotic Stability for Numerical Approximations of Stochastic Ordinary Differential Equations Rózsa Horváth Bokor and Taketomo Mitsui Abstract This note tries to connect the stochastic
More informationStochastic Calculus and Black-Scholes Theory MTH772P Exercises Sheet 1
Stochastic Calculus and Black-Scholes Theory MTH772P Exercises Sheet. For ξ, ξ 2, i.i.d. with P(ξ i = ± = /2 define the discrete-time random walk W =, W n = ξ +... + ξ n. (i Formulate and prove the property
More informationarxiv: v1 [math.ca] 26 Apr 2017
Existence theorems for a nonlinear second-order distributional differential equation Wei Liu a, Guoju Ye a, Dafang Zhao a,b, Delfim F. M. Torres c,d, arxiv:174.89v1 [math.ca] 6 Apr 17 Abstract a College
More informationn E(X t T n = lim X s Tn = X s
Stochastic Calculus Example sheet - Lent 15 Michael Tehranchi Problem 1. Let X be a local martingale. Prove that X is a uniformly integrable martingale if and only X is of class D. Solution 1. If If direction:
More informationSome Background Math Notes on Limsups, Sets, and Convexity
EE599 STOCHASTIC NETWORK OPTIMIZATION, MICHAEL J. NEELY, FALL 2008 1 Some Background Math Notes on Limsups, Sets, and Convexity I. LIMITS Let f(t) be a real valued function of time. Suppose f(t) converges
More informationSTOCHASTIC CALCULUS JASON MILLER AND VITTORIA SILVESTRI
STOCHASTIC CALCULUS JASON MILLER AND VITTORIA SILVESTRI Contents Preface 1 1. Introduction 1 2. Preliminaries 4 3. Local martingales 1 4. The stochastic integral 16 5. Stochastic calculus 36 6. Applications
More informationDedicated to Prof. J. Kurzweil on the occasion of his 80th birthday
131 (2006) MATHEMATCA BOHEMCA No. 2, 211 223 KURZWEL-HENSTOCK AND KURZWEL-HENSTOCK-PETTS NTEGRABLTY OF STRONGLY MEASURABLE FUNCTONS B. Bongiorno, Palermo, L. Di Piazza, Palermo, K. Musia l, Wroc law (Received
More informationGENERALITY OF HENSTOCK-KURZWEIL TYPE INTEGRAL ON A COMPACT ZERO-DIMENSIONAL METRIC SPACE
Ø Ñ Å Ø Ñ Ø Ð ÈÙ Ð Ø ÓÒ DOI: 10.2478/v10127-011-0027-z Tatra Mt. Math. Publ. 49 (2011), 81 88 GENERALITY OF HENSTOCK-KURZWEIL TYPE INTEGRAL ON A COMPACT ZERO-DIMENSIONAL METRIC SPACE Francesco Tulone ABSTRACT.
More informationA NEW PROOF OF THE WIENER HOPF FACTORIZATION VIA BASU S THEOREM
J. Appl. Prob. 49, 876 882 (2012 Printed in England Applied Probability Trust 2012 A NEW PROOF OF THE WIENER HOPF FACTORIZATION VIA BASU S THEOREM BRIAN FRALIX and COLIN GALLAGHER, Clemson University Abstract
More information1 Brownian Local Time
1 Brownian Local Time We first begin by defining the space and variables for Brownian local time. Let W t be a standard 1-D Wiener process. We know that for the set, {t : W t = } P (µ{t : W t = } = ) =
More informationAn Integral-type Constraint Qualification for Optimal Control Problems with State Constraints
An Integral-type Constraint Qualification for Optimal Control Problems with State Constraints S. Lopes, F. A. C. C. Fontes and M. d. R. de Pinho Officina Mathematica report, April 4, 27 Abstract Standard
More informationThe Generalised Riemann Integral
Bachelorproject Mathemetics: The Generalised Riemann ntegral Vrije Universiteit Amsterdam Author: Menno Kos Supervisor: Prof. dr. R.C.A.M. Vandervorst August 11th, 2009 Contents 1 ntroduction 1 2 Basic
More informationMeasure and integration
Chapter 5 Measure and integration In calculus you have learned how to calculate the size of different kinds of sets: the length of a curve, the area of a region or a surface, the volume or mass of a solid.
More informationApplications of Ito s Formula
CHAPTER 4 Applications of Ito s Formula In this chapter, we discuss several basic theorems in stochastic analysis. Their proofs are good examples of applications of Itô s formula. 1. Lévy s martingale
More informationOn distribution functions of ξ(3/2) n mod 1
ACTA ARITHMETICA LXXXI. (997) On distribution functions of ξ(3/2) n mod by Oto Strauch (Bratislava). Preliminary remarks. The question about distribution of (3/2) n mod is most difficult. We present a
More information