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Martingale Property of Exponential Semimartingales: A Note on Explicit Conditions and Applications to Financial Models

David Criens D. Criens - Technical University of Munich, Department of Mathematics, Germany david.criens@tum.de Kathrin Glau K. Glau - Technical University of Munich, Department of Mathematics, Germany kathrin.glau@tum.de  and  Zorana Grbac Z. Grbac - Université Paris Diderot, Laboratoire de Probabilités et Modèles Aléatoires, France grbac@math.univ-paris-diderot.fr
(Date: August 8, 2025)
Abstract.

We give a collection of explicit sufficient conditions for the true martingale property of a wide class of exponentials of semimartingales. We express the conditions in terms of semimartingale characteristics. This turns out to be very convenient in financial modeling in general. Especially it allows us to carefully discuss the question of well-definedness of semimartingale Libor models, whose construction crucially relies on a sequence of measure changes.

Key words and phrases:
Exponential semimartingale, martingale property, uniform integrability, semimartingale asset price model, Libor model
2010 Mathematics Subject Classification:
60G48, 91G30, 91B25
The authors thank Ernst Eberlein for useful discussions. The financial support from the DFG project EB66/9-3 and from the Entrepreneurial Program, Women for Math Science, TU Munich is gratefully acknowledged.

1. Introduction

Local martingales are the core object of stochastic integration. Thus they provide a natural access to time evolutionary stochastic modeling, which is a cornerstone of mathematical finance. The fundamental theorem of asset pricing states that the absence of arbitrage is essentially equivalent to the local martingale property of discounted asset prices under some equivalent probability measure. One important benefit of the true martingale property of discounted asset price processes is their use for density processes of a change of measure. In financial terms this corresponds to a change of numeraire. Since the seminal work of Geman et al. (1995) this concept became indispensable for both computational and modeling aspects. Often a change of numeraire facilitates option pricing by reducing complexity of computations. Moreover, it is a building stone of the construction of Libor market models introduced by Brace et al. (1997) and Miltersen et al. (1997). More fundamentally, a change of measure connects historical and risk-neutral probability measures. On the other hand if the discounted asset price process is a strict local martingale, i.e. a local martingale which is not a true martingale, this is sometimes interpreted as financial bubble. However, the definition and existence of financial bubbles critically depends on the specific notion of the market price, arbitrage and admissible strategies, see for example Cox and Hobson (2005) and Jarrow et al. (2010). In a typical modeling situation it is enjoyable to work with true martingales.

Usually price processes are non-negative and therefore are modeled as exponentials of semimartingales, which form a wide and flexible class of positive processes. One can characterize the local martingales in this class by a drift condition. It is, however, more involved to identify conditions for their true martingale property. In order to formulate the problem more precisely denote by XX an d{\mathbb{R}^{d}}-valued semimartingale and by λ\lambda an d{\mathbb{R}^{d}}-valued predictable process which is integrable with respect to XX. Then λX:=id0λidXi\lambda\cdot X:=\sum_{i\leq d}\int_{0}^{\cdot}\lambda^{i}\operatorname{d}\!X^{i} denotes the real-valued stochastic integral process of λ\lambda with respect to XX. Moreover, let VV be a predictable process with finite variation. We pose the following question: Under which conditions on the characteristics of XX is a real-valued semimartingale ZZ of the form

Z:=eλXVZ:=e^{\lambda\cdot X-V}

a (uniformly integrable) martingale?

If eλXe^{\lambda\cdot X} is a special semimartingale, there exists a unique predictable process of finite variation VV such that ZZ is a local martingale. In this case, VV is called the exponential compensator of λX\lambda\cdot X, see Section 2 for details. Various criteria for the more delicate true martingale property of ZZ have been proposed. The seminal paper by Novikov (1972) treats the continuous semimartingale case. Sufficient conditions for general semimartingales are provided for example in Lepingle and Mémin (1978), Kallsen and Shiryaev (2002), Jacod (1979), Cheridito et al. (2005) and Protter and Shimbo (2008), see also a recent paper by Larsson and Ruf (2014) for further generalizations of Novikov-Kazamaki type conditions based on convergence results for local supermartingales. Moreover, we refer to Section 1 and Section 3 of Kallsen and Shiryaev (2002) for an exhaustive literature overview. In the special case when XX is a process with independent increments and absolutely continuous characteristics and λ\lambda deterministic, Eberlein et al. (2005) show that if ZZ is a local martingale, it is also a true martingale. Deterministic conditions ensuring the martingale property of an exponential of an affine process are given in Kallsen and Muhle-Karbe (2010). The conditions for more general semimartingales are not as explicit.

Our contribution is to give explicit conditions for the martingale property of an exponential quasi-left continuous semimartingale in terms of its characteristics. In Section 2 we introduce the notation and describe the general semimartingale setting following Jacod and Shiryaev (2003). Section 3 contains the main results. The advantage of the explicit conditions is their convenience for applications. We illustrate this by investigating the true martingale property of asset prices in semimartingale stochastic volatility models in Section 4.1. Finally, in Section 4.2 we prove the well-definedness of the backward construction of Lévy Libor models. More precisely, we show that the candidate density processes for the measure changes are indeed true martingales which has not been rigorously proved earlier. Moreover, we present a natural extension to the semimartingale Libor model.

2. Semimartingale notation and preliminaries

In this section we introduce the notation and summarize the basic notions and facts from the semimartingale theory in order to keep the paper self-contained. Our main reference is Jacod and Shiryaev (2003), whose notation we use throughout the paper. Other standard references for stochastic calculus and semimartingales are e.g. Jacod (1979), Métivier (1982) and Protter (2004).

Let (Ω,,(t)t0,)(\Omega,{\mathcal{F}},({\mathcal{F}}_{t})_{t\geq 0},{\mathbb{P}}) denote a stochastic basis, i.e. a filtered probability space with right-continuous filtration. For a class of processes 𝒞\mathcal{C}, we say that a process XX is in the localized class 𝒞loc\mathcal{C}_{\textup{loc}} if there exits a sequence of stopping times (τn)n(\tau_{n})_{n\in\mathbb{N}} such that a.s. τn\tau_{n}\uparrow\infty as nn\to\infty and Xτn𝒞X^{\tau_{n}}\in\mathcal{C}. Denote by \mathcal{M} the class of càdlàg uniformly integrable martingales. The processes in the localized class loc{\mathcal{M}}_{{\mathrm{loc}}} are called local martingales. We denote by 𝒱+{\mathcal{V}}^{+} (resp. 𝒱{\mathcal{V}}) the set of all real-valued càdlàg processes starting from zero that have non-decreasing paths (resp. paths with finite variation over each finite interval [0,t][0,t]). Let 𝒜+{\mathcal{A}}^{+} denote the set of all processes A𝒱+A\in{\mathcal{V}}^{+} that are integrable, i.e. such that 𝔼[A]<{\mathbb{E}}[A_{\infty}]<\infty, where A(ω):=limtAt(ω)¯+A_{\infty}(\omega):=\lim_{t\to\infty}A_{t}(\omega)\in\overline{{\mathbb{R}}}_{+} for every ωΩ\omega\in\Omega. Moreover, let 𝒜{\mathcal{A}} denote the set of all A𝒱A\in{\mathcal{V}} that have integrable variation, i.e. Var(A)𝒜+\operatorname{Var}\,(A)\in{\mathcal{A}}^{+}, where for every t0t\geq 0 and every ωΩ\omega\in\Omega, Var(A)t(ω)\operatorname{Var}\,(A)_{t}(\omega) is defined as the total variation of the function sAs(ω)s\mapsto A_{s}(\omega) on [0,t][0,t]. A process XX is called a semimartingale if it has a decomposition of the form

X=X0+M+A,X=X_{0}+M+A, (2.1)

where X0X_{0} is finite-valued and 0{\mathcal{F}}_{0}-measurable, MlocM\in{\mathcal{M}}_{{\mathrm{loc}}} with M0=0M_{0}=0 and A𝒱A\in{\mathcal{V}}. If AA in decomposition (2.1) is predictable, XX is called a special semimartingale and the decomposition is unique. A semimartingale is called quasi-left continuous if a.s. ΔXτ=0\Delta X_{\tau}=0 on the set {τ<}\{\tau<\infty\} for all predictable times τ\tau.

Let XX be an d{\mathbb{R}^{d}}-valued semimartingale, i.e. each component of XX satisfies (2.1). Denoting by εa\varepsilon_{a} the Dirac measure at point aa, the random measure of jumps μX\mu^{X} of XX is an integer-valued random measure of the form

μX(ω;dt,dx):=s0𝟏{ΔXs(ω)0}ε(s,ΔXs(ω))(dt,dx).\mu^{X}(\omega;{\mathrm{d}}t,{\mathrm{d}}x):=\sum_{s\geq 0}{\mathbf{1}}_{\{\Delta X_{s}(\omega)\neq 0\}}\varepsilon_{(s,\Delta X_{s}(\omega))}({\mathrm{d}}t,{\mathrm{d}}x).

There is a version of the predictable compensator of μX\mu^{X}, denoted by ν\nu, such that the d\mathbb{R}^{d}-valued semimartingale XX is quasi-left continuous if and only if ν(ω,{t}×d)=0\nu(\omega,\{t\}\times\mathbb{R}^{d})=0 for all ωΩ\omega\in\Omega, c.f. Jacod and Shiryaev (2003), Corollary II.1.19.

In general, ν\nu satisfies

(|x|21)ν𝒜loc.(|x|^{2}\wedge 1)\ast\nu\in{\mathcal{A}}_{{\mathrm{loc}}}. (2.2)

The semimartingale XX admits a canonical representation

X=X0+B(h)+Xc+(xh(x))μX+h(x)(μXν),X=X_{0}+B(h)+X^{c}+(x-h(x))\ast\mu^{X}+h(x)\ast(\mu^{X}-\nu),

where h:ddh:{\mathbb{R}^{d}}\to{\mathbb{R}^{d}} is a truncation function, i.e. a function that is bounded and behaves like h(x)=xh(x)=x around 0, B(h)B(h) is a predictable d{\mathbb{R}^{d}}-valued process with components in 𝒱{\mathcal{V}}, and XcX^{c} is the continuous martingale part of XX.

Denote by CC the predictable dd{\mathbb{R}}^{d}\otimes\mathbb{R}^{d}-valued covariation process defined as Cij:=Xi,c,Xj,cC^{ij}:=\langle X^{i,c},X^{j,c}\rangle. Then the triplet (B(h),C,ν)(B(h),C,\nu) is called the triplet of predictable characteristics of XX (or simply the characteristics of XX). It can be shown (see Proposition II.2.9 in Jacod and Shiryaev (2003)) that there exists a predictable process A𝒜loc+A\in{\mathcal{A}}_{{\mathrm{loc}}}^{+} such that

B(h)=b(h)A,C=cA,ν=A×F,B(h)=b(h)\cdot A,\quad C=c\cdot A,\quad\nu=A\times F\,,

where b(h)b(h) is a dd-dimensional predictable process, cc is a predictable process taking values in the set of symmetric non-negative definite d×dd\times d-matrices and FF is a transition kernel from (Ω×+,𝒫)(\Omega\times{\mathbb{R}}_{+},{\mathcal{P}}) into (d,(d))({\mathbb{R}^{d}},{\mathcal{B}}({\mathbb{R}^{d}})). Here 𝒫{\mathcal{P}} denotes the predictable σ\sigma-field on Ω×+\Omega\times{\mathbb{R}}_{+}. We call (b(h),c,F;A)(b(h),c,F;A) the triplet of differential (or local) characteristics of XX. If XX admits the choice At=tA_{t}=t above, we say that XX has absolutely continuous characteristics (or shortly AC) and call XX an Itô semimartingale.

An important subclass of semimartingales is the class of Itô semimartingales with independent increments. These processes are known as time-inhomogeneous Lévy processes or as Processes with Independent Increments and Absolutely Continuous characteristics (PIIAC), see e.g. Section 2 in Eberlein et al. (2005). The differential characteristics (b(h),c,F)(b(h),c,F) of a PIIAC XX, for every truncation function hh, are deterministic and satisfy the following integrability assumption: For every T>0T>0

0T(|b(h)s|+cs+d(|x|21)Fs(dx))ds<,\displaystyle\int_{0}^{T}\bigg{(}|b(h)_{s}|+\|c_{s}\|+\int_{{\mathbb{R}^{d}}}(|x|^{2}\wedge 1)F_{s}(\operatorname{d}\!x)\bigg{)}\operatorname{d}\!s<\infty, (2.3)

where \|\cdot\| denotes any norm on the set of d×dd\times d-matrices. For every t>0t>0, the law of XtX_{t} is characterized by a Lévy-Khintchine type formula for its characteristic function, see again Section 2 in Eberlein et al. (2005). This property makes the class of PIIAC particularly suitable for applications. The following definition and results on exponentials of semimartingales are given in Definition 2.12, Lemma 2.13 and Lemma 2.15 in Kallsen and Shiryaev (2002).

Definition 2.1.

A real-valued semimartingale YY is called exponentially special if exp(YY0)\exp(Y-Y_{0}) is a special semimartingale.

Remark 2.2.

Let YY be a real-valued semimartingale and denote by νY\nu^{Y} the compensator of the random measure of jumps of YY and hh a truncation function.

  • (a)

    The following statements are equivalent:

    • (i)

      YY is an exponentially special semimartingale.

    • (ii)

      (ey1h(y))νY𝒱(e^{y}-1-h(y))\ast\nu^{Y}\in{\mathcal{V}}.

    • (iii)

      ey𝟏{y>1}νY𝒱e^{y}{\mathbf{1}}_{\{y>1\}}\ast\nu^{Y}\in{\mathcal{V}}.

  • (b)

    If YY is exponentially special, then it admits an exponential compensator, i.e. there exists a predictable process V𝒱V\in{\mathcal{V}} such that exp(YY0V)loc\exp(Y-Y_{0}-V)\in{\mathcal{M}}_{{\mathrm{loc}}}.

Let XX be an d{\mathbb{R}^{d}}-valued semimartingale with differential characteristics (b(h),c,F;A)(b(h),c,F;A) and λL(X)\lambda\in L(X), where L(X)L(X) denotes the set of predictable processes integrable with respect to XX, c.f. Jacod and Shiryaev (2003), page 207. Moreover, assume that λX\lambda\cdot X is exponentially special. Following Jacod and Shiryaev (2003), Section III.7.7a we define the Laplace cumulant process

K~X(λ)\displaystyle\widetilde{K}^{X}(\lambda) :=κ~X(λ)A,\displaystyle:=\widetilde{\kappa}^{X}(\lambda)\cdot A, (2.4)

where

κ~sX(λ)\displaystyle\widetilde{\kappa}^{X}_{s}(\lambda) :=λs,bs+12λs,csλs+(eλs,x1λs,h(x))Fs(dx),\displaystyle:=\langle\lambda_{s},b_{s}\rangle+\frac{1}{2}\langle\lambda_{s},c_{s}\lambda_{s}\rangle+\int\big{(}e^{\langle\lambda_{s},x\rangle}-1-\langle\lambda_{s},h(x)\rangle\big{)}F_{s}({\mathrm{d}}x), (2.5)

and the modified Laplace cumulant process KX(λ):=ln((K~X(λ)))K^{X}(\lambda):=\ln({\mathcal{E}}(\widetilde{K}^{X}(\lambda))), where {\mathcal{E}} denotes the stochastic exponential, and

KX(λ)\displaystyle K^{X}(\lambda) =\displaystyle= K~X(λ)+s(ln(1+ΔK~sX(λ))ΔK~sX(λ)).\displaystyle\widetilde{K}^{X}(\lambda)+\sum_{s\leq\cdot}(\ln(1+\Delta\widetilde{K}^{X}_{s}(\lambda))-\Delta\widetilde{K}^{X}_{s}(\lambda)). (2.6)

The following results are proved in Proposition III.7.14 and Theorem III.7.4 in Jacod and Shiryaev (2003):

Proposition 2.3.

Let XX be an d{\mathbb{R}^{d}}-valued semimartingale and λL(X)\lambda\in L(X) such that λX\lambda\cdot X is exponentially special.

  • (i)

    The modified Laplace cumulant process KX(λ)K^{X}(\lambda) is the exponential compensator of λX\lambda\cdot X, i.e. the process ZZ defined by

    Z:=exp(λXKX(λ))Z:=\exp(\lambda\cdot X-K^{X}(\lambda))

    is a local martingale.

  • (ii)

    If XX is quasi-left continuous, the Laplace cumulant process K~X(λ)\widetilde{K}^{X}(\lambda) and the modified Laplace cumulant process KX(λ)K^{X}(\lambda) coincide, i.e. KX(λ)=K~X(λ)K^{X}(\lambda)=\widetilde{K}^{X}(\lambda).

In the following section we give sufficient conditions for the martingale property of exponential semimartingales.

3. The Martingale Property of Exponential Semimartingales

Integrability conditions ensuring the (UI) martingale property of a non-negative or positive local martingale were studied from many perspectives and in various levels of generality. It started with the classical conditions of Novikov (1972) which applies to continuous exponential local martingales. A natural generalization included jumps was given in the seminal paper of Lepingle and Mémin (1978). Various related conditions are given by Kallsen and Shiryaev (2002). A profound overview on Novikov-type conditions as well as boundedness conditions is given in the monograph of Jacod (1979). In this section we collect conditions for exponential semimartingales and express them in terms of semimartingale characteristics. Thanks to these expression we usually call these type of conditions predictable conditions. Let us start with a Novikov-type integrability condition which is based on the main result of Lepingle and Mémin (1978). We follow its statement given by Jacod (1979) as Corollary 8.44.

Proposition 3.1.

Let YY be a real-valued quasi-left continuous semimartingale with characteristics (B(h),C,ν)(B(h),C,\nu). If

  1. (A1)

    𝔼(exp{12CT+((y1)ey+1)νT})<{\mathbb{E}}\left(\exp\left\{\frac{1}{2}C_{T}+((y-1)e^{y}+1)\ast\nu_{T}\right\}\right)<\infty for every T0T\geq 0,

the process M:=eYKY(1)M:=e^{Y-K^{Y}(1)} is a true martingale. Moreover, replacing condition (A1) with

  1. (A2)

    𝔼(exp{12C+((y1)ey+1)ν})<{\mathbb{E}}\left(\exp\left\{\frac{1}{2}C_{\infty}+((y-1)e^{y}+1)\ast\nu_{\infty}\right\}\right)<\infty,

MM is a UI martingale.

Proof: Note that the characteristics of XTX^{T}, for any T>0T>0, are given by (BT,CT,νT)(B^{T},C^{T},\nu^{T}), where νT(dt,dx):=𝟏[0,T]×dν(dt,dx)\nu^{T}({\mathrm{d}}t,{\mathrm{d}}x):={\mathbf{1}}_{[0,T]\times\mathbb{R}^{d}}\nu({\mathrm{d}}t,{\mathrm{d}}x). Now, since local martingales whose localizing sequence is deterministic are martingales, the first claim follows immediately from the second. Note that (A1) implies that XX is exponentially special and hence that MM is a local martingale. In view of Theorem 2.19 in Kallsen and Shiryaev (2002), the second claim follows from Jacod (1979), Corollary 8.44. \Box\hskip-1.42262pt

Remark 3.2.

If YY is continuous, i.e. ν=0\nu=0, then (A2) reduces to the classical Novikov condition as presented in Section 3.5.D in Karatzas and Shreve (1991).

As an immediate corollary we derive the follows sufficient conditions for the case where XX is given as a stochastic integral.

Corollary 3.3.

Let XX be an d{\mathbb{R}^{d}}-valued quasi-left continuous semimartingale with differential characteristics (b(h),c,F;A)(b(h),c,F;A) and λL(X)\lambda\in L(X). If

  1. (B1)

    for every T0T\geq 0,

    𝔼(exp{120Tλs,csλsdAs+0Td((λs,x1)eλs,x+1)Fs(dx)dAs})<\hskip-21.33955pt{\mathbb{E}}\big{(}\exp\big{\{}\frac{1}{2}\int_{0}^{T}\langle\lambda_{s},c_{s}\lambda_{s}\rangle{\mathrm{d}}A_{s}+\int_{0}^{T}\int_{{\mathbb{R}^{d}}}((\langle\lambda_{s},x\rangle-1)e^{\langle\lambda_{s},x\rangle}+1)F_{s}({\mathrm{d}}x){\mathrm{d}}A_{s}\big{\}}\big{)}<\infty

the process M:=eλXKX(λ)M:=e^{\lambda\cdot X-K^{X}(\lambda)} is a true martingale. Moreover, replacing (B1) with

  1. (B2)

    𝔼(exp{120λs,csλsdAs+0d((λs,x1)eλs,x+1)Fs(dx)dAs})<,{\mathbb{E}}\big{(}\exp\big{\{}\!\frac{1}{2}\!\int_{0}^{\infty}\langle\lambda_{s},c_{s}\lambda_{s}\rangle{\mathrm{d}}A_{s}\!+\int_{0}^{\infty}\int_{{\mathbb{R}^{d}}}((\langle\lambda_{s},x\rangle-1)e^{\langle\lambda_{s},x\rangle}\!+1)F_{s}({\mathrm{d}}x){\mathrm{d}}A_{s}\big{\}}\big{)}<\infty,

then MM is a UI martingale.

Proof: The characteristics of λX\lambda\cdot X are given by Proposition IX.5.3 in Jacod and Shiryaev (2003). Now the claim follows by an application of Proposition 3.1. \Box\hskip-1.42262pt

Remark 3.4.

Obviously, by considering an real-valued semimartingale XX and λ=1\lambda=1 in Corollary 3.3 we recover Proposition 3.1.

For applications the following boundedness condition turns out to be useful, see for instance Corollary 4.1, Proposition 4.3 and 4.2 in the sections below.

Proposition 3.5.

Let XX be as in Corollary 3.3 and let λL(X)\lambda\in L(X). If

  1. (C1)

    for every T0T\geq 0, there exists a non-negative constant κ(T)\kappa(T) such that a.s.

    0Tλs,csλsdAs+0Td(1eλs,x)2Fs(dx)dAsκ(T)\displaystyle\int_{0}^{T}\langle\lambda_{s},c_{s}\lambda_{s}\rangle{\mathrm{d}}A_{s}+\int_{0}^{T}\int_{\mathbb{R}^{d}}\left(1-\sqrt{e^{\langle\lambda_{s},x\rangle}}\ \right)^{2}F_{s}({\mathrm{d}}x){\mathrm{d}}A_{s}\leq\kappa(T)

the process M:=eλXKX(λ)M:=e^{\lambda\cdot X-K^{X}(\lambda)} is a true martingale. Moreover, replacing (C1) with

  1. (C2)

    there exists a non-negative constant κ\kappa such that a.s.

    0λs,csλsdAs+0d(1eλs,x)2Fs(dx)dAsκ\displaystyle\int_{0}^{\infty}\langle\lambda_{s},c_{s}\lambda_{s}\rangle{\mathrm{d}}A_{s}+\int_{0}^{\infty}\int_{{\mathbb{R}^{d}}}\left(1-\sqrt{e^{\langle\lambda_{s},x\rangle}}\ \right)^{2}F_{s}({\mathrm{d}}x){\mathrm{d}}A_{s}\leq\kappa

then MM is a UI martingale.

Proof: Again, the first part is an immediate consequence of the second. Note that (C1) implies that λX\lambda\cdot X is exponentially special. Hence, we can deduce the claim from Theorem 2.19 in Kallsen and Shiryaev (2002) together with Lemma 8.8 and Theorem 8.25 in Jacod (1979). \Box\hskip-1.42262pt

Remark 3.6.

Clearly, thanks to Corollary 3.3, the condition (C1) could be replaced by the following condition: for every T0T\geq 0 there exists a constant κ(T)\kappa(T) such that a.s.

0Tλs,csλsdAs+0Td((λs,x1)eλs,x+1)Fs(dx)dAsκ(T).\displaystyle\int_{0}^{T}\langle\lambda_{s},c_{s}\lambda_{s}\rangle{\mathrm{d}}A_{s}+\int_{0}^{T}\int_{{\mathbb{R}^{d}}}\left((\langle\lambda_{s},x\rangle-1)e^{\langle\lambda_{s},x\rangle}+1\right)F_{s}({\mathrm{d}}x){\mathrm{d}}A_{s}\leq\kappa(T). (3.1)

The elementary inequality

0(1x)2xlog(x)(x1), for all x>0,\displaystyle 0\leq(1-\sqrt{x})^{2}\leq x\log(x)-(x-1),\textup{ for all }x>0,

as for instance noted in Esche (2004), Lemma 2.13, shows that condition (C1) is an improvement to (3.1).

Let us shortly turn to the subclass of semimartingales with independent increments (SII processes), for which the situation is slightly different than in the more general case. For exponential SII processes the local martingale property is equivalent to the true martingale property. From a mathematical finance perspective this interesting fact for instance implies that exponential SII models cannot include bubbles which are modeled as strict local martingales.

Let us formalize this observation and add some simple deterministic conditions for the martingale property. The main implication (ii)(i)(ii)\Rightarrow(i) is essentially thanks to Kallsen and Muhle-Karbe (2010), Proposition 3.12. Note that the assertion does not require quasi-left continuity.

Proposition 3.7.

Let XX be an d\mathbb{R}^{d}-valued semimartingale with deterministic characteristics (BX,CX,νX)(B^{X},C^{X},\nu^{X}), λL(X)\lambda\in L(X) be deterministic and M:=eλXKX(λ)M:=e^{\lambda\cdot X-K^{X}(\lambda)}. The following are equivalent

  1. (i)

    MM is a martingale.

  2. (ii)

    MM is a local martingale.

  3. (iii)

    λX\lambda\cdot X is exponentially special.

  4. (iv)

    (eλ,x1h(λ,x))νX𝒱(e^{\langle\lambda,x\rangle}-1-h(\langle\lambda,x\rangle))*\nu^{X}\in\mathcal{V}.

  5. (v)

    eλ,x𝟏{λ,x>1}νX𝒱e^{\langle\lambda,x\rangle}{\mathbf{1}}_{\{\langle\lambda,x\rangle>1\}}*\nu^{X}\in\mathcal{V}.

Proof: The implication (i)(i) \Rightarrow (ii)(ii) is trivial and equivalence (ii)(ii) \Leftrightarrow (iii)(iii) holds by definition. The equivalences of (iii),(iv)(iii),(iv) and (v)(v) are due to Remark 2.2 and Jacod and Shiryaev (2003), Proposition IX.5.3, which shows that λX\lambda\cdot X has deterministic characteristics with

νλX(A,ds)=d𝟏A(λs,x)νX(dx,ds),A(\{0}).\displaystyle\nu^{\lambda\cdot X}(A,{\mathrm{d}}s)=\int_{\mathbb{R}^{d}}{\mathbf{1}}_{A}\big{(}\langle\lambda_{s},x\rangle\big{)}\nu^{X}({\mathrm{d}}x,{\mathrm{d}}s),\quad A\in\mathcal{B}(\mathbb{R}\backslash\{0\}).

It is left to show the implication (iii)(iii) \Rightarrow (i)(i). In view of (2.6) and since λX\lambda\cdot X has deterministic characteristics, KX(λ)K^{X}(\lambda) is a deterministic process of finite variation and hence also has deterministic characteristics. Define f(x,y):=xyf(x,y):=x-y, then Y:=λXKX(λ)=f(λX,KX(λ))Y:=\lambda\cdot X-K^{X}(\lambda)=f(\lambda\cdot X,K^{X}(\lambda)). It follows from Goll and Kallsen (2000), Corollary 5.6 applied to f(λX,KX(λ))f(\lambda\cdot X,K^{X}(\lambda)) that YY has also deterministic characteristics. From the relationship of ordinary and stochastic exponentials given in Jacod and Shiryaev (2003), Theorem II.8.10, we obtain that M=eY=(Y¯),M=e^{Y}=\mathcal{E}(\overline{Y}), where Y¯\overline{Y} is a semimartingale with ΔY¯=(eΔY1)>1\Delta\overline{Y}=(e^{\Delta Y}-1)>-1. We deduce from Jacod and Shiryaev (2003), Equation II.8.14 that Y¯\overline{Y} inherits the property of deterministic characteristics from YY. Due to Remark 2.2(b), the condition eλ,x𝟏{λ,x>1}ν𝒱e^{\langle\lambda,x\rangle}{\mathbf{1}}_{\{\langle\lambda,x\rangle>1\}}*\nu\in\mathcal{V} yields that λX\lambda\cdot X is exponentially special. Thus, since KX(λ)K^{X}(\lambda) is the exponential compensator of λX\lambda\cdot X, c.f. Proposition 2.3 (i), MM is a local martingale. The claim now follows from Proposition 3.12 in Kallsen and Muhle-Karbe (2010). \Box\hskip-1.42262pt

4. Applications to Finanical Models

In this section we present two applications of the results from Section 3 to financial modeling. A detailed overview concerning applications of general semimartingales in finance is for instance provided by the monographs of Shiryaev (1999), Cont and Tankov (2003), Musiela and Rutkowski (2005) and Jeanblanc et al. (2009).

4.1. Stochastic Volatility Asset Price Model

Here, we illustrate how the conditions of Section 3 can be used to facilitate pricing in arbitrage-free models driven by semimartingales. Let (Ω,,(t)0tT,)(\Omega,{\mathcal{F}},({\mathcal{F}}_{t})_{0\leq t\leq T},{\mathbb{P}}) be a stochastic basis, where T>0T>0 denotes a finite time horizon. We model the asset price SS and a bank account BB with stochastic interest rate rr by

S:=S0eσSXSV,B:=eσrXrS:=S_{0}e^{\sigma^{S}\cdot X^{S}-V},\qquad B:=e^{\sigma^{r}\cdot X^{r}} (4.1)

with S0>0S_{0}>0, a dd-dimensional semimartingale X:=(XS,Xr)X:=(X^{S},X^{r}) with XSX^{S} d1d_{1}-dimensional and XrX^{r} d2d_{2}-dimensional such that d1+d2=dd_{1}+d_{2}=d, and a dd-dimensional predictable process σ:=(σS,σr)\sigma:=(\sigma^{S},-\sigma^{r}) with σSL(XS)\sigma^{S}\in L(X^{S}) and σrL(Xr)\sigma^{r}\in L(X^{r}) such that σX\sigma\cdot X is exponentially special. We assume that the process VV is the exponential compensator of σSXSσrXr\sigma^{S}\cdot X^{S}-\sigma^{r}\cdot X^{r}, c.f. Proposition 2.3. Thanks to this assumption, the discounted stock price S~:=B1S\widetilde{S}:=B^{-1}S is a local martingales, i.e. in other words {\mathbb{P}} is a risk-neutral probability measure. According to the fundamental theorem of asset pricing for general semimartingales in Delbaen and Schachermayer (1998), the No Free Lunch With Vanishing Risk (NFLVR) holds is this case.

Note that in general the risk-neutral probability measure may not be unique and the model is incomplete. Let us now consider a European call option with strike K>0K>0 with payoff (STK)+(S_{T}-K)^{+} at maturity T>0T>0. Its fundamental price under {\mathbb{P}}, denoted by CtC^{\ast}_{t} for any t[0,T]t\in[0,T], is given by

Ct:=Bt𝔼(BT1(STK)+|t)Bt𝔼(S~T|t)BtS~t=St<,C^{\ast}_{t}:=B_{t}{\mathbb{E}}_{{\mathbb{P}}}\big{(}B_{T}^{-1}(S_{T}-K)^{+}\big{|}{\mathcal{F}}_{t}\big{)}\leq B_{t}{\mathbb{E}}_{{\mathbb{P}}}\big{(}\widetilde{S}_{T}\big{|}{\mathcal{F}}_{t}\big{)}\leq B_{t}\widetilde{S}_{t}=S_{t}<\infty, (4.2)

which is well-defined and finite a.s. The inequality 𝔼(S~T|t)S~t{\mathbb{E}}(\widetilde{S}_{T}|{\mathcal{F}}_{t})\leq\widetilde{S}_{t} is a consequence of S~\widetilde{S} being a positive local martingale and hence a supermartingale. The price CC^{\ast} is an arbitrage-free price, which – even in the case of a complete model – might be non-unique. This subtle issue is closely related to financial bubbles, see for example Definition 3.6 in Jarrow et al. (2010) and Definition 2.10 in Biagini et al. (2014). For a detailed mathematical treatment we refer to Protter (2013).

When S~\widetilde{S} is a true martingale, these delicate issues do not appear: The asset price has no bubble and the market prices coincide with the fundamental prices – this was proved for example in the setting of Jarrow et al. (2010). Thus, our Section 3 provides convenient conditions to exclude ambiguities in the pricing due to the possible presence of bubbles.

To illustrate a further benefit of the explicit martingale conditions from Section 3 we use the true martingale property of the discounted asset price to perform a change of numeraire which reduces the complexity of a pricing problem at hand. Considering for example a call option as above, in order to compute the expectation in (4.2) directly, information on the joint distribution of SS and BB is required. Here the true martingale property of S~\widetilde{S} allows to facilitate the computation of the expectation by a change of numeraire. More precisely, we can express the call price as a conditional expectation of a function of the asset value STS_{T} solely. Defining a probability measure ~\widetilde{{\mathbb{P}}} via d~d|t:=S01S~t\frac{\operatorname{d}\!\widetilde{{\mathbb{P}}}}{\operatorname{d}\!{\mathbb{P}}}|_{{\mathcal{F}}_{t}}:=S_{0}^{-1}\widetilde{S}_{t} for 0tT0\leq t\leq T, and denoting by 𝔼~{\mathbb{E}}_{\widetilde{{\mathbb{P}}}} the expectation under ~\widetilde{{\mathbb{P}}}, Bayes formula yields

Ct=St𝔼~((1KST1)+|t).C_{t}=S_{t}{\mathbb{E}}_{\widetilde{{\mathbb{P}}}}\big{(}(1-KS_{T}^{-1})^{+}\big{|}{\mathcal{F}}_{t}\big{)}. (4.3)

Compared with the original pricing formula Ct=Bt𝔼(BT1(STK)+|t)C_{t}=B_{t}{\mathbb{E}}_{{\mathbb{P}}}\big{(}B_{T}^{-1}(S_{T}-K)^{+}\big{|}{\mathcal{F}}_{t}\big{)}, the random variable BTB_{T} does not appear in the conditional expectation in (4.3). This typically facilitates the computation since the semimartingale characteristics of SS are known under the new probability measure.

By combining Corollary 3.3 and Proposition 3.5 the following characterization of the true martingale property for the semimartingale asset price model defined above.

Corollary 4.1.

Assume that XX is quasi-left continuous and denote its local characteristics by (b,c,F;A)(b,c,F;A). If (b,c,F;A)(b,c,F;A) and σ\sigma satisfy (B1) of Corollary 3.3, resp. condition (C1) of Proposition 3.5, the discounted asset price process S~\widetilde{S} is a true martingale.

Under the conditions of Corollary 4.1 the fair price at time tt of the call option with maturity TT and strike KK is therefore given by CtC_{t} in (4.3).

4.2. Semimartingale Libor model

In this subsection we apply the results from Section 3 to Libor models. These are models for discretely compounded forward interest rates known as Libor rates, where the term Libor stems from the London Interbank Offered Rate. The Libor models were introduced in Brace et al. (1997) and Miltersen et al. (1997) and later further developed and studied by many authors. We refer to Musiela and Rutkowski (2005), Section 12.4, for a detailed overview.

The challenge in modeling Libor rates is to simultaneously define the rates for different maturities as local martingales under different equivalent measures which ensures the absence of arbitrage. These measures are in fact forward measures and they are interconnected via the Libor rates themselves. A convenient way to obtain such a model is by backward construction, following the pioneering work of Musiela and Rutkowski (1997). This construction relies on the martingale property of Libor rates (under the corresponding forward measures), which allows to define changes of measure. In the backward construction the Libor rates thus have to be not only local, but true martingales under their corresponding forward measures. When the model is driven by a continuous semimartingale this is standard by using Novikov type conditions, but verifying that the Libor rates are true martingales in general semimartingale models including jumps is more involved and has not been properly addressed in the financial literature. Using explicit conditions from Section 3, we study this issue in detail below to close this gap.

Let us begin by describing a general semimartingale Libor model. Assume that T>0T^{*}>0 is a fixed finite time horizon and we are given a pre-determined collection of maturities 0=T0<T1<<Tn=T0=T_{0}<T_{1}<\ldots<T_{n}=T^{*}, with δk:=Tk+1Tk\delta_{k}:=T_{k+1}-T_{k} for k=0,,n1k=0,\ldots,n-1. Moreover, let (Ω,T,(t)0tT,T)(\Omega,{\mathcal{F}}_{T^{*}},({\mathcal{F}}_{t})_{0\leq t\leq T^{*}},{\mathbb{P}}_{T^{*}}) be a stochastic basis. A general semimartingale Libor model consists of a family of semimartingales modeling the Libor rates (L(,Tk))1kn1(L(\cdot,T_{k}))_{1\leq k\leq n-1} for lending periods ([Tk,Tk+1])1kn1([T_{k},T_{k+1}])_{1\leq k\leq n-1} and a family of probability measures (Tk)1kn({\mathbb{P}}_{T_{k}})_{1\leq k\leq n}, where L(,Tk)L(\cdot,T_{k}) and Tk{\mathbb{P}}_{T_{k}} are defined on (Ω,Tk,(t)0tTk)(\Omega,\mathcal{F}_{T_{k}},(\mathcal{F}_{t})_{0\leq t\leq T_{k}}) and Tn=T{\mathbb{P}}_{T_{n}}={\mathbb{P}}_{T^{*}}, such that

  1. (SML1)

    L(,Tk)L(\cdot,T_{k}) is a Tk+1{\mathbb{P}}_{T_{k+1}}-martingale for all k=1,,n1k=1,\ldots,n-1.

  2. (SML2)

    For k=n1,,1k=n-1,\ldots,1

    dTkdTk+1=1+δkL(Tk,Tk)1+δkL(0,Tk).\displaystyle\frac{{\mathrm{d}}{\mathbb{P}}_{T_{k}}}{{\mathrm{d}}{\mathbb{P}}_{T_{k+1}}}=\frac{1+\delta_{k}L(T_{k},T_{k})}{1+\delta_{k}L(0,T_{k})}.

For each kk the probability measure Tk{\mathbb{P}}_{T_{k}} is called the forward Libor measure for maturity TkT_{k}, cf. Musiela and Rutkowski (2005), Definition 12.4.1. The measure Tk{\mathbb{P}}_{T_{k}} is in fact the forward martingale measure associated with maturity TkT_{k} and the density process above is a forward price process. This can be seen from the link between forward Libor rates and zero-coupon bond prices, see Musiela and Rutkowski (2005), Sections 12.1.1 and 12.4.4.

Below we present the main ideas of the backward construction of the Libor model in a semimartingale framework. We start by modeling the Libor rate with the most distant maturity under a given probability measure and then proceed backwards. We define in each step the next forward measure via a density process based on the previously modeled Libor rates and model the next Libor rate under this measure.

Let XX be an d{\mathbb{R}^{d}}-valued semimartingale on the stochastic basis (Ω,T,(t)0tT,T)(\Omega,{\mathcal{F}}_{T^{*}},({\mathcal{F}}_{t})_{0\leq t\leq T^{*}},{\mathbb{P}}_{T^{*}}). We start by modeling the Libor rate L(,Tn1)L(\cdot,T_{n-1}) for maturity Tn1T_{n-1} by

L(t,Tn1):=L(0,Tn1)exp{λ(,Tn1)XtKtX(T,λ(,Tn1))},\displaystyle L(t,T_{n-1}):=L(0,T_{n-1})\exp\big{\{}\lambda(\cdot,T_{n-1})\cdot X_{t}-K^{X}_{t}({\mathbb{P}}_{T^{*}},\lambda(\cdot,T_{n-1}))\big{\}}, (4.4)

for tTn1t\leq T_{n-1}, where L(0,Tn1)>0L(0,T_{n-1})>0 and λ(,Tn1)L(X)\lambda(\cdot,T_{n-1})\in L(X) is a volatility process such that the stochastic integral λ(,Tn1)X\lambda(\cdot,T_{n-1})\cdot X is T{\mathbb{P}}_{T^{*}}-exponentially special with KX(T,λ(,Tn1))K^{X}({\mathbb{P}}_{T^{*}},\lambda(\cdot,T_{n-1})) its T{\mathbb{P}}_{T^{*}}-exponential compensator. Hence, L(,Tn1)L(\cdot,T_{n-1}) is a T{\mathbb{P}}_{T^{*}}-local martingale. Assuming that L(,Tn1)L(\cdot,T_{n-1}) is a true T{\mathbb{P}}_{T^{*}}-martingale, we can define the probability measure Tn1{\mathbb{P}}_{T_{n-1}} on (Ω,Tn1)(\Omega,\mathcal{F}_{T_{n-1}}) by the Radon-Nikodym derivative

dTn1dT=1+δn1L(Tn1,Tn1)1+δn1L(0,Tn1).\displaystyle\frac{{\mathrm{d}}{\mathbb{P}}_{T_{n-1}}}{{\mathrm{d}}{\mathbb{P}}_{T^{*}}}=\frac{1+\delta_{n-1}L(T_{n-1},T_{n-1})}{1+\delta_{n-1}L(0,T_{n-1})}. (4.5)

Moreover, we obtain for tTn1t\leq T_{n-1}

dTn1dT|t=1+δn1L(t,Tn1)1+δn1L(0,Tn1).\displaystyle\frac{{\mathrm{d}}{\mathbb{P}}_{T_{n-1}}}{{\mathrm{d}}{\mathbb{P}}_{T^{*}}}\bigg{|}_{\mathcal{F}_{t}}=\frac{1+\delta_{n-1}L(t,T_{n-1})}{1+\delta_{n-1}L(0,T_{n-1})}. (4.6)

Now we recursively model the Libor rates L(,Tk)L(\cdot,T_{k}) for k=n2,,1k=n-2,\ldots,1 by

L(t,Tk):=L(0,Tk)exp{λ(,Tk)XtKtX(Tk+1,λ(,Tk))},\displaystyle L(t,T_{k}):=L(0,T_{k})\exp\big{\{}\lambda(\cdot,T_{k})\cdot X_{t}-K^{X}_{t}({\mathbb{P}}_{T_{k+1}},\lambda(\cdot,T_{k}))\big{\}}, (4.7)

for tTkt\leq T_{k}, where L(0,Tk)>0L(0,T_{k})>0 and λ(,Tk)L(X)\lambda(\cdot,T_{k})\in L(X) is a volatility process such that λ(,Tk)X\lambda(\cdot,T_{k})\cdot X is Tk+1{\mathbb{P}}_{T_{k+1}}-exponentially special with Tk+1{\mathbb{P}}_{T_{k+1}}-exponential compensator KX(Tk+1,λ(,Tk))K^{X}({\mathbb{P}}_{T_{k+1}},\lambda(\cdot,T_{k})). As above, this means that L(,Tk)L(\cdot,T_{k}) is a Tk+1{\mathbb{P}}_{T_{k+1}}-local martingale. Note that the Libor rate for the interval starting at T0=0T_{0}=0 and ending at T1T_{1} is simply the given spot Libor rate L(0,T0)>0L(0,T_{0})>0. The probability measure Tk{\mathbb{P}}_{T_{k}} is defined on (Ω,Tk)(\Omega,\mathcal{F}_{T_{k}}) by the Radon-Nikodym derivative

dTkdTk+1=1+δkL(Tk,Tk)1+δkL(0,Tk),\displaystyle\frac{{\mathrm{d}}{\mathbb{P}}_{T_{k}}}{{\mathrm{d}}{\mathbb{P}}_{T_{k+1}}}=\frac{1+\delta_{k}L(T_{k},T_{k})}{1+\delta_{k}L(0,T_{k})}, (4.8)

where it has to be assumed that L(,Tk)L(\cdot,T_{k}) is a true Tk+1{\mathbb{P}}_{T_{k+1}}-martingale. Then we have for tTkt\leq T_{k}

dTkdTk+1|t=1+δkL(t,Tk)1+δkL(0,Tk).\displaystyle\frac{{\mathrm{d}}{\mathbb{P}}_{T_{k}}}{{\mathrm{d}}{\mathbb{P}}_{T_{k+1}}}\bigg{|}_{\mathcal{F}_{t}}=\frac{1+\delta_{k}L(t,T_{k})}{1+\delta_{k}L(0,T_{k})}. (4.9)

Furthermore, we obtain that the probability measure Tk+1{\mathbb{P}}_{T_{k+1}} is related to T{\mathbb{P}}_{T^{*}} via

dTk+1dT|t\displaystyle\frac{\operatorname{d}\!{\mathbb{P}}_{T_{k+1}}}{\operatorname{d}\!{\mathbb{P}}_{T^{*}}}\bigg{|}_{{\mathcal{F}}_{t}} =\displaystyle= i=k+1n11+δiL(t,Ti)1+δiL(0,Ti),tTk+1.\displaystyle\prod_{i=k+1}^{n-1}\frac{1+\delta_{i}L(t,T_{i})}{1+\delta_{i}L(0,T_{i})},\quad t\leq T_{k+1}. (4.10)

Note that the construction is well-defined if the Libor rates L(,Tk)L(\cdot,T_{k}) are Tk+1{\mathbb{P}}_{T_{k+1}}-martingales for all k=1,,n1k=1,\ldots,n-1.

To justify the backward construction (4.4) – (4.10) of the measures (Tk)1kn1({\mathbb{P}}_{T_{k}})_{1\leq k\leq n-1}, we prove the required martingale property of the Libor rates in the proposition below.

Proposition 4.2.

Let XX in equation (4.7) be an d{\mathbb{R}^{d}}-valued quasi-left continuous semimartingale with differential characteristics (bT,c,FT;A)(b^{T^{\ast}},c,F^{T^{\ast}};A) with respect to PTP_{T^{\ast}}, and non-negative λ(,Tk)L(X)\lambda(\cdot,T_{k})\in L(X). Assume

  • (SL)

    for all i=1,,n1i=1,\ldots,n-1 there exists a non-negative constant κ\kappa such that a.s.

    0T\displaystyle\int_{0}^{T^{*}}\langle λ(t,Ti),ctλ(t,Ti)dAt\displaystyle\lambda(t,T_{i}),c_{t}\lambda(t,T_{i})\rangle{\mathrm{d}}A_{t}
    +0Td(1eλ(t,Ti),x)2ek=i+1n1λ(t,Tk),xFtT(dx)dAtκ,\displaystyle+\int_{0}^{T^{*}}\int_{{\mathbb{R}^{d}}}\left(1-\sqrt{e^{\langle\lambda(t,T_{i}),x\rangle}}\ \right)^{2}e^{\langle\sum_{k=i+1}^{n-1}\lambda(t,T_{k}),x\rangle}\ F^{T^{\ast}}_{t}(\operatorname{d}\!x){\mathrm{d}}A_{t}\leq\kappa,

    where we use the convention =0\sum_{\emptyset}=0.

Then for each k=1,,n1k=1,\ldots,n-1, the process L(,Tk)L(\cdot,T_{k}) from (4.7) is a martingale with respect to Tk+1{\mathbb{P}}_{T_{k+1}} given by (4.10).

Proof: For k=n1k=n-1, the assertion follows directly from assumption (SL) and Proposition 3.5.

For kn2k\leq n-2, denote the semimartingale characteristics of XX with respect to Tk+1{\mathbb{P}}_{T_{k+1}} by (BTk+1,CTk+1,νTk+1)(B^{T_{k+1}},C^{T_{k+1}},\nu^{T_{k+1}}). Next we compute these characteristics by backward induction and Girsanov’s theorem as given by Theorem III.3.24 in Jacod and Shiryaev (2003). We shortly give some details on the application of Girsanov’s theorem. Denote dTn1/dT|=:ZTn1{\mathrm{d}}{\mathbb{P}}_{T_{n-1}}/{\mathrm{d}}{\mathbb{P}}_{T^{*}}|_{\mathcal{F}_{\cdot}}=:Z^{T_{n-1}} and note that

L(,T)=L(0,Tn1)(λ(,Tn1)Xc,T+(eλ(,Tn1),x1)(μXνT)),L(\cdot,T^{*})=L(0,T_{n-1})\mathcal{E}\left(\lambda(\cdot,T_{n-1})\cdot X^{c,T^{*}}+\left(e^{\langle\lambda(\cdot,T_{n-1}),x\rangle}-1\right)*\left(\mu^{X}-\nu^{T^{*}}\right)\right),

where Xc,TX^{c,T^{*}} denotes the continuous local T{\mathbb{P}}_{T^{*}}-martingale part of XX. We have

MμXT(ZTn1|𝒫~)\displaystyle M^{{\mathbb{P}}_{T^{*}}}_{\mu^{X}}(Z^{T_{n-1}}|\widetilde{\mathcal{P}}) =ZTn1+δn1L(,Tn1)1+δn1L(0,Tn1)(eλ(,Tn1,x1).\displaystyle=Z^{T^{n-1}}_{-}+\frac{\delta_{n-1}L(\cdot-,T_{n-1})}{1+\delta_{n-1}L(0,T_{n-1})}\left(e^{\langle\lambda(\cdot,T_{n-1},x\rangle}-1\right).

Now Girsanov’s theorem yields that

CTn1=C,νTn1(dt,dx)=β(t,x,Tn1)FtT(dx)dAt,\displaystyle C^{T_{n-1}}=C,\quad\nu^{T_{n-1}}({\mathrm{d}}t,{\mathrm{d}}x)=\beta(t,x,T_{n-1})F^{T^{*}}_{t}({\mathrm{d}}x){\mathrm{d}}A_{t},

with

β(t,x,Tl):=δlL(t,Tl)1+δlL(t,Tl)(eλ(t,Tl),x1)+1,\beta(t,x,T_{l}):=\frac{\delta_{l}L(t-,T_{l})}{1+\delta_{l}L(t-,T_{l})}\left(e^{\langle\lambda(t,T_{l}),x\rangle}-1\right)+1,

for l=1,,n1l=1,\ldots,n-1. Repeating these steps, by backward induction we obtain

CTk+1=C,νTk+1(dt,dx)=l=k+1n1β(t,x,Tl)FtT(dx)dAt.\displaystyle C^{T_{k+1}}=C,\quad\nu^{T_{k+1}}({\mathrm{d}}t,{\mathrm{d}}x)=\prod_{l=k+1}^{n-1}\beta(t,x,T_{l})F^{T^{*}}_{t}({\mathrm{d}}x){\mathrm{d}}A_{t}.

Noting that β(t,x,Tl)eλ(t,Tl),x\beta(t,x,T_{l})\leq e^{\langle\lambda(t,T_{l}),x\rangle}, the claim follows from Proposition 3.5. \Box\hskip-1.42262pt

Let us link our discussion to the Lévy Libor model of Eberlein and Özkan (2005) in which the driving process XX is assumed to be an d{\mathbb{R}^{d}}-valued PIIAC with differential characteristic (0,c,FT)(0,c,F^{T^{*}}) under T{\mathbb{P}}_{T^{*}}. Eberlein and Özkan impose the following assumptions: For some M,ε>0M,\varepsilon>0 and every k=1,,n1k=1,\ldots,n-1 we have

  1. (L1)

    0T|x|>1eu,xFtT(dx)dt<\int_{0}^{T^{*}}\int_{|x|>1}e^{\langle u,x\rangle}F^{T^{*}}_{t}({\mathrm{d}}x){\mathrm{d}}t<\infty for every u[(1+ε)M,(1+ε)M]du\in[-(1+\varepsilon)M,(1+\varepsilon)M]^{d},

  2. (L2)

    λ(,Tk):[0,T]+d\lambda(\cdot,T_{k}):[0,T^{*}]\to{\mathbb{R}}^{d}_{+} is a bounded, nonnegative function such that for t>Tkt>T_{k}, λ(t,Tk)=0\lambda(t,T_{k})=0 and k=1n1λj(t,Tk)M,\sum_{k=1}^{n-1}\lambda^{j}(t,T_{k})\leq M, for all t[0,T]t\in[0,T^{*}] and every coordinate j{1,,d}j\in\{1,\ldots,d\},

  3. (L3)

    λ(,Tk):[0,T]+d\lambda(\cdot,T_{k}):[0,T^{*}]\to{\mathbb{R}}^{d}_{+} is deterministic.

Let us point that even when the driving process has deterministic characteristics under T{\mathbb{P}}_{T^{*}} and λ\lambda is deterministic (as in the case above), the characteristics of XX under Tk{\mathbb{P}}_{T_{k}} for k=1,,n1k=1,\ldots,n-1 are stochastic.

We obtain the following sufficient conditions for the Lévy Libor model, where we also allow λ\lambda to be stochastic.

Corollary 4.3.

Assume that j=1n|λ(,Tj)|N\sum_{j=1}^{n}|\lambda(\cdot,T^{j})|\leq N for a non-negative constant NN, and that there exists a non-negative constant κ\kappa such that

0T|x|>1eN|x|FtT(dx)dtκ.\int_{0}^{T^{*}}\int_{|x|>1}e^{N|x|}F^{T^{*}}_{t}({\mathrm{d}}x){\mathrm{d}}t\leq\kappa.

Then for each k=1,,n1k=1,\ldots,n-1 the process L(,Tk)L(\cdot,T_{k}) defined in (4.7) is a martingale with respect to Tk+1{\mathbb{P}}_{T_{k+1}} given by (4.10).

Proof: It suffices to show that (SL) is satisfied. Note that we find a non-negative constant KK^{*} such that for any i=1,,n1i=1,...,n-1 for all xdx\in\mathbb{R}^{d} with |x|1|x|\leq 1

(1eλ(t,Ti),x)2\displaystyle\left(1-\sqrt{e^{\langle\lambda(t,T_{i}),x\rangle}}\ \right)^{2} ek=i+1n1λ(t,Tk),xK|x|2.\displaystyle e^{\langle\sum_{k=i+1}^{n-1}\lambda(t,T_{k}),x\rangle}\leq K^{*}|x|^{2}.

Next we bound the large jumps. Using the fact that (1x)21+x(1-\sqrt{x})^{2}\leq 1+x for x>0x>0 and some non-negative constant KK, and the Cauchy-Schwarz inequality, we obtain

0T|x|>1\displaystyle\int_{0}^{T^{*}}\int_{|x|>1} (1eλ(t,Ti),x)2ek=i+1n1λ(t,Tk),xFtT(dx)dt\displaystyle\left(1-\sqrt{e^{\langle\lambda(t,T_{i}),x\rangle}}\ \right)^{2}e^{\langle\sum_{k=i+1}^{n-1}\lambda(t,T_{k}),x\rangle}\ F^{T^{\ast}}_{t}(\operatorname{d}\!x){\mathrm{d}}t
0T|x|>1(ek=i+1n1λ(t,Tk),x+ek=in1λ(t,Tk),x)FtT(dx)dt\displaystyle\leq\int_{0}^{T^{*}}\int_{|x|>1}\left(e^{\langle\sum_{k=i+1}^{n-1}\lambda(t,T_{k}),x\rangle}+e^{\langle\sum_{k=i}^{n-1}\lambda(t,T_{k}),x\rangle}\right)F^{T^{*}}_{t}({\mathrm{d}}x){\mathrm{d}}t
20T|x|>1eN|x|FtT(dx)dt.\displaystyle\leq 2\int_{0}^{T^{*}}\int_{|x|>1}e^{N|x|}F^{T^{*}}_{t}({\mathrm{d}}x){\mathrm{d}}t.

Finally, since

0Tλ(t,Ti),ctλ(t,Ti)dtN20Tctdt,\displaystyle\int_{0}^{T^{*}}\langle\lambda(t,T_{i}),c_{t}\lambda(t,T_{i})\rangle{\mathrm{d}}t\leq N^{2}\int_{0}^{T^{*}}\|c_{t}\|{\mathrm{d}}t,

where \|\cdot\| denotes the operator norm of cc, we conclude that (SL) holds. This concludes the proof. \Box\hskip-1.42262pt

As mentioned in the introduction of the section, the martingale property of Libor rates under their corresponding measures is crucial for the validity of the backward construction of Libor models. Therefore, Proposition 4.2 and Corollary 4.3 provide a theoretical justification of the construction of the Lévy Libor model by Eberlein and Özkan (2005), and more generally of Libor models driven by quasi-left continuous semimartingales.

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