A family of martingales generated by a process with independent increments

An explicit procedure to construct a family of martingales generated by a process with independent increments is presented. The main tools are the polynomials that give the relationship between the moments and cumulants, and a set of martingales related to the jumps of the process called Teugels mar...

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Datum:2008
Hauptverfasser: Sole, J.L., Utzet, F.
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Zitieren:A family of martingales generated by a process with independent increments / J.L. Sole, F. Utzet // Theory of Stochastic Processes. — 2008. — Т. 14 (30), № 2. — С. 139–144. — Бібліогр.: 9 назв.— англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Sole, J.L.
Utzet, F.
author_facet Sole, J.L.
Utzet, F.
citation_txt A family of martingales generated by a process with independent increments / J.L. Sole, F. Utzet // Theory of Stochastic Processes. — 2008. — Т. 14 (30), № 2. — С. 139–144. — Бібліогр.: 9 назв.— англ.
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description An explicit procedure to construct a family of martingales generated by a process with independent increments is presented. The main tools are the polynomials that give the relationship between the moments and cumulants, and a set of martingales related to the jumps of the process called Teugels martingales.
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fulltext Theory of Stochastic Processes Vol. 14 (30), no. 2, 2008, pp. 139–144 UDC 519.21 JOSEP LLUÍS SOLÉ AND FREDERIC UTZET A FAMILY OF MARTINGALES GENERATED BY A PROCESS WITH INDEPENDENT INCREMENTS An explicit procedure to construct a family of martingales generated by a process with independent increments is presented. The main tools are the polynomials that give the relationship between the moments and cumulants, and a set of martingales related to the jumps of the process called Teugels martingales. 1. Introduction In this work, we present an explicit procedure to generate a family of martingales from a process X = {Xt, t ≥ 0} with independent increments and continuous in probability. We extend our results exposed in [8], where we dealt with Lévy processes (independent and stationary increments); in that case, the martingales obtained were of the form Mt = P (Xt, t), where P (x, t) is a polynomial in x and t, and then they are time–space harmonic polynomials relative to X . Here, the martingales constructed are polynomials on Xt but, in general, not in t. Part of the paper is devoted to define the Teugels martingales of a process with independent increments; such martingales, introduced by Nualart and Schoutens [5] for Lévy processes, are a building block of the stochastic calculus with that type of processes. 2. Independent increment processes and their Teugels martingales Let X = {Xt, t ≥ 0} be a process with independent increments, X0 = 0, continuous in probability and cadlag; such processes are also called additive processes, and we will indistinctly use both names. Moreover, assume that Xt is centered and has moments of all orders. It is well known that the law of Xt is infinitely divisible for all t ≥ 0. Let σ2 t be the variance of the Gaussian part of Xt, and let νt be its Lévy measure; for all these notions, we refer to Sato [6] or Skorohod [7]. Denote, by ν̃, the (unique) measure on B((0,∞) × R0) defined by ν̃((0, t] ×B) = νt(B), B ∈ B(R0), where R0 = R − {0}. By the standard approximation argument, we have that, for a measurable function f : R0 → R and for every t > 0,∫∫ (0,t]×R0 |f(x)| ν̃(ds, dx) <∞ ⇐⇒ ∫ R0 |f(x)| νt(dx) <∞, and, in this case, ∫∫ (0,t]×R0 f(x) ν̃(ds, dx) = ∫ R0 f(x) νt(dx). 2000 AMS Mathematics Subject Classification. Primary 60G51, 60G44. Key words and phrases. Process with independent increments, Cumulants, Teugels martingales. This research was supported by grant BFM2006-06247 of the Ministerio de Educación y Ciencia and FEDER. 139 140 JOSEP LLUÍS SOLÉ AND FREDERIC UTZET Note that since, for every t ≥ 0, νt is a Lévy measure, ν̃ is σ–finite. To prove this, we observe that νt({|x| > 1}) <∞, νt((1/(n+ 1), 1/n]) <∞, and νt([−1/n,−1/(n+ 1))) < ∞, n ≥ 1. So there is a numerable partition of R0 with sets of finite νt measure, ∀t > 0. Then, we can construct a numerable partition of (0,∞) × R0, each set being with finite ν̃-measure. Write N(C) = #{t : (t,ΔXt) ∈ C}, C ∈ B((0,∞) × R0), the jump measure of the process, where ΔXt = Xt − Xt−. It is a Poisson random measure on (0,∞) × R0 with intensity measure ν̃ (Sato [6, Theorem 19.2]). Define the compensated jump measure dÑ(t, x) = dN(t, x) − dν̃(t, x). The process admits the Lévy–Itô representation Xt = Gt + ∫∫ (0,t]×R0 xdÑ (t, x), (2) where {Gt, t ≥ 0} is a centered continuous Gaussian process with independent increments and variance E[G2 t ] = σ2 t . The relationship between the moments of an infinitely divisible law and the moments of its Lévy measure is also well known (see Sato [6,Theorem 25.4]). In our case, as the process has moments of all orders, for all t ≥ 0,∫ {|x|>1} |x| νt(dx) <∞ and ∫ R0 |x|n νt(dx) <∞, ∀n ≥ 2. Write F2(t) = σ2 t + ∫ R0 x2 νt(dx) and Fn(t) = ∫ R0 xn νt(dx), n ≥ 3. (1) Since ∫ {|x|>1} |x| νt(dx) < ∞ and E[Xt] = 0, the characteristic function of Xt can be written as φt(u) = exp { − 1 2 σ2 t u 2 + ∫ R0 ( eiux − 1 − iux ) νt(dx) } . It is deduced that, for n ≥ 2, Fn(t) is the cumulant of order n of Xt (for n = 2, E[X2 t ] = F2(t)). Also σ2 t is continuous and increasing (Sato [6, Theorem 9.8]). Proposition 1. The functions Fn(t), n ≥ 2, are continuous and have finite variation on finite intervals, and, for n even, they are increasing. Proof. Consider 0 < u < t < v, and write U = [u, v]. From the continuity in probability of X , lim s→t, s∈U Xn s = Xn t , in probability. Moreover, ∀s ∈ U, |Xs| ≤ supr∈U |Xr|, and since X is a martingale, by Doob’s inequality, E [ sup r∈U |Xr|n ] ≤ C sup r∈U E[|Xr|n] ≤ CE[|Xv|n] <∞. So it follows by dominated convergence that the function t !→ E[Xn t ] is continuous. Since the cumulants are polynomials of the moments, the continuity of all functions Fn(t) is deduced. MARTINGALES AND INDEPENDENT INCREMENT PROCESSES 141 To prove that Fn(t) has finite variation on finite intervals, consider a partition of [0, t]: 0 < t0 < · · · < tk = t. Then k∑ j=1 ∣∣Fn(tj) − Fn(tj−1) ∣∣ = k∑ j=1 ∣∣ ∫∫ (tj−1,tj ]×R0 xnν̃(ds, dx) ∣∣ ≤ k∑ j=1 ∫∫ (tj−1,tj ]×R0 |x|n ν̃(ds, dx) = ∫∫ (0,t]×R0 |x|n ν̃(ds, dx) <∞. � Consider the variations of the process X (see Meyer [4]): X (1) t = Xt, X (2) t = [X,X ]t = σ2 t + ∑ 0<s≤t ( ΔXs )2 X (n) t = ∑ 0<s≤t ( ΔXs )n , n ≥ 3. By Kyprianou [2, Theorem 2.7], for n ≥ 3 (the case n = 2 is similar), the characteristic function of X(n) is exp {∫∫ (0,t]×R0 ( eiuxn − 1 ) ν̃(ds, dx) } = exp {∫ R0 ( eiux − 1 ) ν (n) t (dx) } , where ν(n) t is the measure image of νt by the function x !→ xn which is a Lévy measure. So X(n) has independent increments. Also by Kyprianou [2, Theorem 2.7], for n ≥ 2, E[X(n) t ] = Fn(t) and E [( X (n) t )2] = F2n(t) + ( Fn(t) )2 . Therefore, combining the independence of the increments and the continuity of Fn(t), it is deduced that X(n) is continuous in probability. By Proposition 1, Fn(t) has finite variation on finite intervals. Hence, the process X (n) t = Fn(t) + ( X (n) t − Fn(t) ) is a semimartingale. The Teugels martingales introduced by Nualart and Schoutens [5] for Lévy processes can be extended to additive processes. In the same way as in [5], these martingales are obtained centering the processes X(n): Y (1) t = Xt, Y (n) t = X(n) − Fn(t), n ≥ 2, They are square integrable martingales with optional quadratic covariation [Y (n), Y (m)]t = X(n+m), and, since F2n(t) is increasing, the predictable quadratic variation of Y (n) is 〈Y (n)〉t = F2n(t). 142 JOSEP LLUÍS SOLÉ AND FREDERIC UTZET 3. The polynomials of cumulants The formal expression exp { ∞∑ n=1 κn un n! } = ∞∑ n=0 μn un n! . (3) relates the sequences of numbers {κn, n ≥ 1} and {μn, n ≥ 0}. When we consider a random variable Z with moment generating function in some open interval containing 0, then both series converge in a neighborhood of 0, and (3) is the relationship between the moment generating function, ψ(u) = E[euZ ], and the cumulant generating function, logψ(u). Moreover, μn (respectively, κn) is the moment (respectively, the cumulant) of order n of Z, and the well-known relations between moments and cumulants can be deduced from (3). The first three ones are μ1 = κ1, μ2 = κ2 1 + κ2, μ3 = κ3 1 + 3κ1κ2 + κ3, . . . If the random variable Z has only finite moments up to order n, the corresponding relationship is true up to this order. There is a general explicit expression of the moments in terms of cumulants in Kendall and Stuart [1], or formulas involving the partitions of a set, see McCullagh [3]. In general, μn is a polynomial of κ1, . . . , κn, called Kendall polynomial. Denote, by Γn(x1, . . . , xn), n ≥ 1, this polynomial, that is, we have μn = Γn(κ1, . . . , κn). Also write Γ0 = 1. These polynomials enjoy very interesting properties, as the recurrence formula that follows from Stanley [9, Proposition 5.1.7]: Γn+1(x1, . . . , xn+1) = n∑ j=0 ( n j ) Γj(x1, . . . , xj)xn+1−j . (4) We also have ∂Γn(x1, . . . , xn) ∂xj = ( n j ) Γn−j(x1, . . . , xn−j), j = 1, . . . , n. (5) Computing the Taylor expansion of Γn(x1 + y, x2, . . . , xn) at y = 0, we get the following expression we will need later: Γn(x1 + y, x2, . . . , xn) = n∑ j=0 ( n j ) Γn−j(x1, . . . , xn−j) yj . (6) Interchanging the roles of x1 and y and evaluating the function at 0, we obtain Γn(x1, x2, . . . , xn) = n∑ j=0 ( n j ) Γn−j(0, x2, . . . , xn−j)xj 1. (7) 4. A family of martingales relative to the additive process The main result of the paper is the following Theorem: Theorem 1. Let X be a centered additive process with finite moments of all orders. Then the process M (n) t = Γn ( Xt,−F2(t), . . . ,−Fn(t) ) MARTINGALES AND INDEPENDENT INCREMENT PROCESSES 143 is a martingale. Proof. Let n ≥ 2. We apply the multidimensional Itô formula to the semimartingales Xt, F2(t), . . . , Fn(t). By Proposition 1, the functions F2(t), . . . , Fn(t) and σ2 t are contin- uous and of finite variation. From (5) and the fact that [X,X ]ct = σ2 t and [Fj , Fj ]ct = 0, we have M (n) t = n ∫ t 0 M (n−1) s− dXs − n∑ j=2 ( n j )∫ t 0 M (n−j) s dFj(s) + 1 2 n(n− 1) ∫ t 0 M (n−2) s d(σ2 s) + ∑ 0<s≤t ( Γn ( Xs− + ΔXs,−F2(s), . . . ,−Fn(s) ) − Γn ( Xs−,−F2(s), . . . ,−Fn(s) ) − nΔXs Γn−1 ( Xs−,−F2(s), . . . ,−Fn(s) )) . Applying (6), Γn ( Xs− + ΔXs,−F2(s), . . . ,−Fn(s) ) = n∑ j=0 ( n j ) M (n−j) s− ( ΔXs )j . Then, the jumps part given in the expression of M (n) t is∑ 0<s≤t n∑ j=2 ( n j ) M (n−j) s− ( ΔXs )j = n∑ j=2 ( n j )∫ t 0 M (n−j) s− dX(j) s − ( n 2 )∫ t 0 M (n−2) s d(σ2 s) = n∑ j=2 ( n j )∫ t 0 M (n−j) s− d ( Y (j) s + Fj(s) ) − ( n 2 )∫ t 0 M (n−2) s d(σ2 s). Therefore, M (n) t = n∑ j=1 ( n j )∫ t 0 M (n−j) s− dY (j) s . (8) Moreover, ( M (k) t )2 is a polynomial inXt, F2(t), . . . , Fk(t). Taking expectations and using the relations between moments and cumulants, as well as the fact that the cumulants of Xt are Fn(t), n ≥ 2, we obtain that E [( M (k) t )2] = P (F2(t), . . . , F2k(t)), for a suitable polynomial P . Then, for every t ≥ 0, we have E [ ∫ t 0 ( M (k) s− )2 d〈Y (j)〉s ] = ∫ t 0 E [( M (k) s− )2 ] dF2j(s) = ∫ t 0 P (F2(s), . . . , F2k(s)) dF2j(s) <∞, So all the stochastic integrals on the right-hand side of (8) are martingales. � Remark 1. It is worth to note that the preceding Theorem implies that the function gn(x, t) = Γn ( x,−F2(t), . . . ,−Fn(t) ) is a time–space harmonic function with respect to Xt. By (7), gn(x, t) = n∑ j=0 Γn−j(0,−F2(t), . . . , Fn(t))xj . 144 JOSEP LLUÍS SOLÉ AND FREDERIC UTZET In general, gn(x, t) is a polynomial in x. If Fn(t), n ≥ 2, are polynomials in t, then gn(x, t) is a time–space harmonic polynomial; this happens for all Lévy processes with moments of all orders and for some additive process; see the example below. Example. Let Λ(t) : R+ −→ R+ be a continuous increasing function, and let J be a Poisson random measure on R+ with intensity measure μ(A) = ∫ A Λ(dt), A ∈ B(R+). Then the process X = {Xt, t ≥ 0} defined pathwise, Xt(ω) = ∫ t 0 J(ds, ω) − Λ(t) , is an additive process; it is a Cox process with deterministic hazard function Λ(t). From the characteristic function of Xt, we deduce that the Lévy measure is νt(dx) = Λ(t)δ1(dx), where δ1 is a Dirac delta measure concentrated in the point 1. Hence, Fn(t) = Λ(t), n ≥ 2. Note that the conditions we have assumed on Λ are necessary to obtain an additive process, but it is not necessary (though not very restrictive) to assume that Λ is absolutely continuous with respect to the Lebesgue measure. The function defined in Remark 1 is gn(x, t) = Γn ( x,−Λ(t), . . . ,−Λ(t) ) . Hence, when Λ(t) is a polynomial, gn(x, t) is a time–space harmonic polynomial. Denote, by Cn(x, t), the Charlier polynomial with leading coefficient equal to 1. Then (see [8]) gn(x, t) = n∑ j=1 λ (n) j Cj(x,Λ(t)), where λ(n) 1 = 1 and λ (n) k+1 = n−1∑ j=k ( n j ) λ (j) k , k = 1, . . . , n− 1. Bibliography 1. M.Kendall and A.Stuart, The Advanced Theory of Statistics, Vol. 1, 4th edition, MacMillan, New York, 1977. 2. A.E.Kyprianou, Introductory Lectures on Fluctuations of Lévy Processes with Applications, Springer, Berlin, 2006. 3. P.McCullagh, Tensor Methods in Statistics, Chapman and Hall, London, 1987. 4. P.A.Meyer, Un cours sur les integrales stochastiques, Séminaire de Probabilités X, Springer, New York, 1976, pp. 245–400. (French) 5. D.Nualart and W.Schoutens, Chaotic and predictable representation for Lévy processes, Sto- chastic Process. Appl. 90 (2000), 109–122. 6. K.Sato, Lévy Processes and Infinitely Divisible Distributions, Cambridge University Press, Cambridge, 1999. 7. A.V.Skorohod, Random Processes with Independent Increments, Kluwer Academic Publ., Dor- drecht, Boston, London, 1986. 8. J.L.Solé and F.Utzet, Time-space harmonic polynomials relative to a Lévy process, Bernoulli (2007). 9. R.P.Stanley, Enumerative Combinatorics, Vol. 2, Cambridge University Press, Cambridge, 1999. 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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
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publishDate 2008
publisher Інститут математики НАН України
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spelling Sole, J.L.
Utzet, F.
2009-12-03T16:42:16Z
2009-12-03T16:42:16Z
2008
A family of martingales generated by a process with independent increments / J.L. Sole, F. Utzet // Theory of Stochastic Processes. — 2008. — Т. 14 (30), № 2. — С. 139–144. — Бібліогр.: 9 назв.— англ.
0321-3900
https://nasplib.isofts.kiev.ua/handle/123456789/4559
519.21
An explicit procedure to construct a family of martingales generated by a process with independent increments is presented. The main tools are the polynomials that give the relationship between the moments and cumulants, and a set of martingales related to the jumps of the process called Teugels martingales.
This research was supported by grant BFM2006-06247 of the Ministerio de Educacion y Ciencia and FEDER.
en
Інститут математики НАН України
A family of martingales generated by a process with independent increments
Article
published earlier
spellingShingle A family of martingales generated by a process with independent increments
Sole, J.L.
Utzet, F.
title A family of martingales generated by a process with independent increments
title_full A family of martingales generated by a process with independent increments
title_fullStr A family of martingales generated by a process with independent increments
title_full_unstemmed A family of martingales generated by a process with independent increments
title_short A family of martingales generated by a process with independent increments
title_sort family of martingales generated by a process with independent increments
url https://nasplib.isofts.kiev.ua/handle/123456789/4559
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