1 Introduction
This paper is concerned with the study of multidimensional generalized backward stochastic differential equations (GBSDEs) with jumps in a general filtration. For convenience of the discussion, let us first make precise the notion of such equations, which is adopted from [9].
Let $T>0$ be a fixed time horizon and consider a filtered probability space $(\varOmega ,\mathcal{F},(\mathcal{F}_{t})_{t\le T},\mathbb{P})$ carrying a standard d-dimensional Brownian motion W and an independent compensated Poisson random measure $\widehat{\pi }$. The filtration $(\mathcal{F}_{t})_{0\le t\le T}$ is assumed to be complete and right continuous. Assume that we are given an ${\mathbb{R}}^{k}$-valued $\mathcal{F}_{T}$-measurable random variable ξ, a random function $f:\varOmega \times [0,T]\times {\mathbb{R}}^{k}\times {\mathbb{R}}^{k\times d}\times {\mathcal{L}_{\lambda }^{2}}\longrightarrow {\mathbb{R}}^{k}$ (see Section 2 for the definition of ${\mathcal{L}_{\lambda }^{2}}$) such that $f(\cdot ,y,z,v)$ is $(\mathcal{F}_{t})$-progressively measurable for each $(y,z,v)$, and an $(\mathcal{F}_{t})_{t\ge 0}$-progressively measurable càdlàg finite-variation process $(R_{t})_{t\in [0,T]}$ such that $R_{0}=0$. Roughly speaking, solving a GBSDE with jumps in a general filtration with terminal time T associated with terminal condition ξ and generator $f+dR$ amounts to finding the usual triple $(Y_{t},Z_{t},V_{t})$ (with Y adapted and Z and V predictable) and a càdlàg martingale $M=(M_{t})_{t\in [0,T]}$ that is orthogonal to W and $\widehat{\pi }$ (see Lemma 1) such that the following equation is satisfied $\mathbb{P}$-a.s.:
This equation is usually denoted by GBSDE$(\xi ,f+dR)$. Note that the reason behind adding the martingale M to the definition of GBSDE (1) is the fact that we do not assume that the underlying filtration is generated by W and $\widehat{\pi }$, and in such cases, the martingale representation property may fail.
(1)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle Y_{t}& \displaystyle =\xi +{\int _{t}^{T}}f(s,Y_{s},Z_{s},V_{s})ds+{\int _{t}^{T}}dR_{s}-{\int _{t}^{T}}Z_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}dM_{s},\hspace{1em}t\in [0,T].\end{array}\]Nonlinear BSDEs with jumps (i.e., the underlying filtration is generated by a Brownian motion and an independent Poisson random measure) were first introduced by Tang and Li [19]. They proved the existence and uniqueness of the solution under a Lipschitz continuity condition on the generator w.r.t. the variables. Since then, a lot of papers (see, e.g., [13, 1, 17, 20, 16, 12, 9], and the references therein) and books (see, e.g., [18] and [5]) studied BSDEs with jumps due to the connections of this subject with mathematical finance (see, e.g., [5]) (e.g., if the Brownian motion stands for the noise from a financial market, then the Poisson random measure can be interpreted as the randomness of the insurance claims), stochastic control (see, e.g., [10]), and partial differential equations (see, e.g., [1]), and so on. Since the work of Tang and Li [19], the attempts of generalization of their results have been made in several different directions. First of all, many papers aimed at relaxing the Lipschitz condition on the generator w.r.t. y. For example, Pardoux [13] considered a monotonicity condition on the generator w.r.t. y and a linear growth condition on y. Some efforts were devoted to weaken the square integrability on the coefficients, for example, $\mathbb{E}[|\xi {|}^{2}+{\int _{0}^{T}}|f(t,0,0,0){|}^{2}dt]<+\infty $. Yao [20] gave the existence and uniqueness results for ${\mathbb{L}}^{p}$-solutions ($p>1$) for BSDEs with jumps for a monotonic generator (not the same monotonicity condition considered in our paper) and ${\mathbb{L}}^{p}$ coefficients. Later, Li and Wei [12] analyzed fully coupled BSDEs with jumps and showed the existence and uniqueness of ${\mathbb{L}}^{p}$-solutions ($p\ge 2$) for such equations for a monotone generator and p-integrable data. Further, other settings of BSDEs with jumps have been introduced. Pardoux [13] studied a class of BSDEs with jumps called generalized BSDEs with jumps that involves an integral w.r.t. an increasing continuous process. The author shows the uniqueness and existence of the GBSDE with generator monotone in y and square-integrable data.
Recently, Kruse and Popier [9] considered another direction of generalization concerning the underlying filtration, which is no longer assumed to be generated by W and $\widehat{\pi }$. In fact, they studied multidimensional BSDEs in a general filtration of type (1) with $R\equiv 0$. The authors established the existence and uniqueness of ${\mathbb{L}}^{p}$-solutions ($p>1$) under a monotonicity assumption on the generator f w.r.t. y and under the condition that the data ξ and $f(t,0,0,0)$ are in ${\mathbb{L}}^{p}$, $p>1$, that is,
Moreover, they also considered the case of a random terminal time that is not necessarily bounded.
In our paper, we first investigate the existence and uniqueness of ${\mathbb{L}}^{p}(p\ge 2)$-solutions (see Definition 1) for GBSDEs (1) in a deterministic time horizon. We suppose that f is monotonic w.r.t. y (this condition is essential in the study of BSDEs with random terminal time), Lipschitz continuous w.r.t. to z and v, and satisfies a very general growth condition w.r.t. y considered earlier in the Brownian setting in [4] and recently in the case of jumps in [9]:
This condition seems to be the best possible growth condition on f w.r.t. y and is widely used in the theory of partial differential equations (see [2] and the references therein).
(3)
\[ \forall r>0,\hspace{1em}\underset{|y|\le r}{\sup }\big|f(\cdot ,y,0,0)-f(\cdot ,0,0,0)\big|\in {\mathbb{L}}^{1}\big(\varOmega \times [0,T]\big).\]Concerning the data, we assume that a p-integrability condition is satisfied (see assumption $(H1)$). Moreover, under an additional assumption on the jump component of f (see $(H{6^{\prime }})$ in Section 4), we provide a comparison principle in dimension one (see the counterexample in [1]). Then, we extend the results obtained in the case of deterministic time horizon to the case of a random terminal time that is not necessarily bounded.
Let us highlight the main contribution of the paper compared to the existing literature. On the one hand, our results extend the work of Kruse and Popier [9] to the case of generalized BSDEs. Furthermore, we strengthen their results even in the case $R=0$ since our p-integrability condition on $f(t,0,0,0)$ (see assumption $(H1)$) is weaker than the ${\mathbb{L}}^{p}$-integrability (2) assumed in their paper. It should be mentioned that, due to the p-integrability assumed on $f(t,0,0,0)$ and also to the process $dR$, some difficulties arise. Indeed, as in [4] and [9], to study the ${\mathbb{L}}^{p}$-solutions, a result on the existence and uniqueness in the classical ${\mathbb{L}}^{2}$ case (see Theorem 1) is first needed. To obtain such a result, the main trick is to truncate the coefficients with suitable truncation functions in order to have a bounded solution Y, which is a key tool in the proof in the ${\mathbb{L}}^{2}$ case (see [14, Prop. 2.4 and Thm. 2.2], Proposition 2.2 in [3] used in [4, Thm. 4.2] and [9, Lemma 4 and Thm. 1]). The approach followed in the papers mentioned to get this important estimate fails in our context. This is the reason why we give nonstandard estimates in Lemma 2, which allow us to overcome this problem.
On the other hand, we generalize the work of Pardoux [13] to the situation of a general filtration. Moreover, even in the case of a Wiener–Poisson filtration (filtration generated by W and π), compared to [13], we weaken the growth condition on f w.r.t. y stated in assumption (3), instead of the linear growth condition on the variable y, and derive the existence and uniqueness of ${\mathbb{L}}^{p}$-solutions of our GBSDE, whereas only the classical ${\mathbb{L}}^{2}$-solutions were studied in [13]. Note also that, in our case, GBSDE involves an integral w.r.t. a finite-variation càdlàg process unlike [13], where an integral w.r.t. a continuous increasing process is considered instead.
Our main motivation for writing this paper is because it is a first step in the study of our future work on the existence and uniqueness of ${\mathbb{L}}^{p}$-solutions for reflected GBSDEs. Note that since we solve that problem using a penalization method, the comparison principle obtained here is primordial. Finally, to the best of our knowledge, there is no such result in the literature.
The rest of the paper is organized as follows: in the following section, we give the mathematical setting of this paper and some basic identities. In Section 3, we study the existence and uniqueness of ${\mathbb{L}}^{p}$-solutions on a fixed time interval, which is done in three parts. First, we study the classical case of ${\mathbb{L}}^{2}$-solutions. The proof method follows the arguments and techniques (convolution, weak convergence, truncation technique) given in [8, 13, 14, 4, 9] with obvious modifications. Then, in the remaining parts, we extend the result to ${\mathbb{L}}^{p}$-solutions for any $p\ge 2$, using the right a priori estimate, the ${\mathbb{L}}^{2}$ case result, and a truncation technique. In Section 4, a comparison principle for GBSDEs with jumps in dimension 1 is provided. Finally, Section 5 is devoted to the case of a random terminal time.
2 Preliminaries
Throughout this paper, $T>0$ is a fixed time horizon, $(\varOmega ,\mathcal{F},(\mathcal{F}_{t})_{t\le T},\mathbb{P})$ is a filtered probability space. The filtration $(\mathcal{F}_{t},0\le t\le T)$ is assumed to be complete and right continuous. We suppose that $(\varOmega ,\mathcal{F},(\mathcal{F}_{t})_{t\le T},\mathbb{P})$ supports a d-dimensional Wiener process $(W_{t},0\le t\le T)$ and a random Poisson measure π on ${\mathbb{R}}^{+}\times U$, where $U:={\mathbb{R}}^{n}\setminus \{0\}$ is equipped with its Borel field $\mathcal{U}$, with the compensator $\nu (dt,de)=dt\lambda (de)$ such that $\{\widehat{\pi }([0,t]\times A)=(\pi -\nu )([0,t]\times A)\}_{t\le T}$ is a martingale for all $A\in \mathcal{U}$ satisfying $\lambda (A)<+\infty $. Here, λ is assumed to be a σ-finite Lévy measure on $(U,\mathcal{U})$ such that
Let $\mathcal{P}$ denote the σ-algebra of predictable sets on $\varOmega \times [0,T]$, and let us introduce the following notation:
For a given process $R\in \mathcal{V}$, we denote by $|R|_{t}$ the variation of R on $[0,t]$ and by $dR$ the random measure generated by its trajectories. By $\mathcal{T}$ we denote the set of all stopping times with values in $[0,T]$ and by $\mathcal{T}_{t}$ the set of all stopping times with values in $[t,T]$. We say that a sequence $(\tau _{k})_{k\in \mathbb{N}}\subset T$ is stationary if $\mathbb{P}(\liminf _{k\to +\infty }\{\tau _{k}=T\})=1$. For $X\in \mathcal{S}$, we set $X_{t-}=\lim _{s\nearrow t}X_{s}$ and $\Delta X_{t}=X_{t}-X_{t-}$ with the convention that $X_{0-}=0$.
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• $\mathcal{S}$ is the set of all adapted càdlàg processes.
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• $\mathbb{M}_{\mathit{loc}}$ is the set of càdlàg local martingales orthogonal to W and $\widehat{\pi }$. If $M\in \mathbb{M}_{\mathit{loc}}$, then
(4)
\[ \big[M,{W}^{i}\big]_{t}=0,\hspace{2.5pt}1\le i\le d,\hspace{1em}\text{and}\hspace{1em}\big[M,\widehat{\pi }(A,\cdot )\big]_{t}=0,\] -
• $\mathbb{M}$ is the subspace of $\mathbb{M}_{\mathit{loc}}$ of martingales.
-
• $\mathcal{V}$ is the set of all càdlàg progressively measurable processes R of finite variation such that $R_{0}=0$.
Now, since we are dealing with a general filtration, we recall Lemma III.4.24 in [7], which gives the representation property of a local martingale in our context.
The Euclidean norm of a vector $y\in {\mathbb{R}}^{k}$ will be defined by $|y|=\sqrt{{\sum _{i=1}^{k}}|y_{i}{|}^{2}}$, and for any $k\times d$ matrix z, we define $|z|=\sqrt{\operatorname{Trace}(z{z}^{t})}$, where ${z}^{t}$ stands for the transpose of z. The quadratic variation of a martingale $M\in {\mathbb{R}}^{k}$ is defined by $[M]_{t}={\sum _{i=1}^{k}}[{M}^{i}]_{t}$. By ${[M]}^{c}$ we denote the continuous part of the quadratic variation $[M]$. Let us introduce the following spaces of processes for any real constant $p\ge 2$:
In what follows, let ξ be an ${\mathbb{R}}^{k}$-valued and $\mathcal{F}_{T}$-measurable random variable, and let R be a process in $\mathcal{V}$. Finally, let us consider a random function $f:[0,T]\times \varOmega \times {\mathbb{R}}^{k}\times {\mathbb{R}}^{k\times d}\times {\mathcal{L}_{\lambda }^{2}}\longrightarrow {\mathbb{R}}^{k}$ measurable with respect to $\mathcal{P}\otimes \mathcal{B}({\mathbb{R}}^{k})\otimes \mathcal{B}({\mathbb{R}}^{k\times d})\otimes \mathcal{B}({\mathcal{L}_{\lambda }^{2}})$. In the paper, we consider the following hypotheses:
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• ${\mathbb{M}}^{p}$ is the set of all ${\mathbb{R}}^{k}$-valued martingales $M\in \mathbb{M}$ such that $\mathbb{E}{([M]_{T})}^{\frac{p}{2}}<+\infty $.
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• ${\mathcal{L}}^{p}$ is the set of $\mathcal{P}\otimes \mathcal{U}$-measurable mappings $V:\varOmega \times [0,T]\times U\to {\mathbb{R}}^{k}$ such that
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• ${\varXi }^{p}$ is the space ${\mathcal{S}}^{p}\times {\mathcal{M}}^{p}\times {\mathcal{L}}^{p}\times {\mathbb{M}}^{p}$.
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• ${\mathcal{V}}^{p}$ is the set of all processes $R\in \mathcal{V}$ such that $\| R\| _{{\mathcal{V}}^{p}}:=\mathbb{E}{(|R{|_{T}^{p}})}^{1/p}<\infty $, where $|R|_{T}$ denotes the total variation of R on $[0,T]$.
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$(H1)$ $\mathbb{E}[|\xi {|}^{p}+{({\int _{0}^{T}}|f(t,0,0,0)|dt)}^{p}+|R{|_{T}^{p}}]<+\infty $.
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$(H2)$ For every $(t,z,v)\in [0,T]\times {\mathbb{R}}^{k\times d}\times {\mathcal{L}_{\lambda }^{2}}$, the mapping $y\in {\mathbb{R}}^{k}\to f(t,y,z,v)$ is continuous.
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$(H4)$ For every $r>0$, the mapping $t\in [0,T]\to \sup _{|y|\le r}|f(t,y,0,0)-f(t,0,0,0)|$ belongs to ${\mathbb{L}}^{1}(\varOmega \times [0,T])$.
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$(H5)$ f is Lipschitz continuous w.r.t. z, that is, there exists a constant $L>0$ such that for all $t\in [0,T],y\in {\mathbb{R}}^{k},z,{z^{\prime }}\in {\mathbb{R}}^{k\times d},v\in {\mathcal{L}_{\lambda }^{2}}$.
-
$(H6)$ f is Lipschitz continuous w.r.t. v, that is, there exists a constant $L>0$ such that\[ \big|f(t,y,z,v)-f\big(t,y,z,{v^{\prime }}\big)\big|\le L\big\| v-{v^{\prime }}\big\| _{{\mathcal{L}_{\lambda }^{2}}},\]for all $t\in [0,T],y\in {\mathbb{R}}^{k},z\in {\mathbb{R}}^{k\times d},v,{v^{\prime }}\in {\mathcal{L}_{\lambda }^{2}}$.
To begin with, let us make precise the notion of ${\mathbb{L}}^{p}$-solutions of the GBSDE (1), which we consider throughout this paper.
3 Generalized BSDEs with constant terminal time
3.1 ${\mathbb{L}}^{2}$-solutions
In this subsection, we study the classical case of ${\mathbb{L}}^{2}$-solutions of GBSDE (1). The results given here generalize those of [13] and [9]. Note that the integrability condition $(H1)_{p=2}$ made on $f(\cdot ,0,0,0)$ is weaker than the assumption $E{\int _{0}^{T}}|f(t,0,0,0){|}^{2}dt<+\infty $, $t\in [0,T]$, made in those papers, which means that our assumption is weaker than that of [9] even in the case $R\equiv 0$.
Let us begin by giving nonstandard a priori estimates on the solution, which will play a primordial role in the proof of Theorem 1. Let us first make the following assumption:
Now, we give the main result of this subsection.
Remark 1.
Note that $(A)$ is not a new assumption, but a direct consequence of assumptions $(H3)$, $(H5)$, and $(H6)$ with $f_{t}=|f(t,0,0,0)|$. In fact, three assumptions $(H3)$, $(H5)$, and $(H6)$ are reduced to a single one (assumption $(A)$) for simplicity.
Lemma 2.
Let assumption $(A)$ hold, and let $(Y,Z,V,M)$ be a solution of GBSDE (1). If $Y\in {\mathcal{S}}^{2}$ and
then, $(Z,V,M)$ belongs to ${\mathcal{M}}^{2}\times {\mathcal{L}}^{2}\times {\mathbb{M}}^{2}$, and for some $a\ge \mu +2{L}^{2}$, there is a constant $C>0$ such that, for all $0\le q\le t\le T$,
(5)
\[ \mathbb{E}|\xi {|}^{2}+\mathbb{E}{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{2}+\mathbb{E}|R{|_{T}^{2}}<+\infty ,\](6)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{s\in [t,T]}{\sup }{e}^{2as}|Y_{s}{|}^{2}+{\int _{t}^{T}}{e}^{2as}|Z_{s}{|}^{2}ds+{\int _{t}^{T}}\int _{U}{e}^{2as}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\\{} & \displaystyle \hspace{2em}+{e}^{2aT}[M]_{T}-{e}^{2at}[M]_{t}\Big|\mathcal{F}_{q}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg[{e}^{2aT}|\xi {|}^{2}+{\Bigg({\int _{t}^{T}}{e}^{as}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{t}^{T}}{e}^{as}d|R|_{s}\Bigg)}^{2}\Big|\mathcal{F}_{q}\Bigg].\end{array}\]Proof.
The proof is performed in two steps. For simplicity, we can assume w.l.o.g. that $a=0$. Indeed, let us fix $a\ge \mu +2{L}^{2}$ and define $\widetilde{Y}_{t}={e}^{at}Y_{t}$, $\widetilde{Z}={e}^{at}Z_{t}$, $\widetilde{V}_{t}={e}^{at}V_{t}$, $d\widetilde{M}_{t}={e}^{at}dM_{t}$. Observe that $(\widetilde{Y},\widetilde{Z},\widetilde{V},\widetilde{M})$ solves the following GBSDE:
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \widetilde{Y}_{t}& \displaystyle =\widetilde{\xi }+{\int _{t}^{T}}\widetilde{f}(s,\widetilde{Y}_{s},\widetilde{Z}_{s},\widetilde{V}_{s})ds+{\int _{t}^{T}}d\widetilde{R}_{s}-{\int _{t}^{T}}\widetilde{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}\widetilde{V}_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}d\widetilde{M}_{s},\hspace{1em}t\in [0,T],\end{array}\]
where $\widetilde{\xi }={e}^{aT}\xi $, $\widetilde{f}(t,y,z,v)={e}^{at}f(t,{e}^{-at}y,{e}^{-at}z,{e}^{-at}v)-ay$, and $d\widetilde{R}_{t}={e}^{at}dR_{t}$. Notice that $\widetilde{f}$ satisfies assumption $(A)$ with $\widetilde{f}_{t}={e}^{at}f_{t}$, $\widetilde{\mu }=\mu -a$, $\widetilde{L}=L$. Since we are working on a compact time interval, the integrability conditions are equivalent with or without the superscript ~. Thus, with this change of variable, we reduce to the case $a=0$ and $\mu +2{L}^{2}\le 0$. We omit the superscript ~ for notational convenience.
Step 1. First, we show that there exists a constant $C>0$ such that, for all $0\le q\le t\le T$,
Since there is a lack of integrability of the processes $(Z,V,M)$, we are proceeding by localization. For $n\in \mathbb{N}$, we set
But from $(A)$, the basic inequality $2ab\le 2{a}^{2}+\frac{{b}^{2}}{2}$, and the fact that $\mu +2{L}^{2}\le 0$ we have that
Then, plugging the last inequality into (8), we deduce
Note that since $Y\in {\mathcal{S}}^{2}$, by the definition of the stopping time $\tau _{n}$ it follows by the BDG inequality that ${\int _{0}^{t\wedge \tau _{n}}}Y_{s}Z_{s}dW_{s}$, ${\int _{0}^{t\wedge \tau _{n}}}\hspace{-0.1667em}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)$ and ${\int _{0}^{t\wedge \tau _{n}}}Y_{s-}dM_{s}$ are uniformly integrable martingales. Consequently, taking the conditional expectation w.r.t. $\mathcal{F}_{q}$, $0\le q\le t\le T$, in both sides of (10) yields
(7)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg({\int _{t}^{T}}|Z_{s}{|}^{2}ds+{\int _{t}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+{\int _{t}^{T}}d[M]_{s}\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}+{\Bigg({\int _{t}^{T}}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{t}^{T}}d|R|_{s}\Bigg)}^{2}\Big|\mathcal{F}_{q}\Bigg).\end{array}\]
\[ \tau _{n}=\inf \Bigg\{t>0;{\int _{0}^{t}}|Z_{s}{|}^{2}ds+{\int _{0}^{t}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+[M]_{t}>n\Bigg\}\wedge T.\]
By Itô’s formula (see [15, Thm. II.32]),
(8)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle |Y_{t\wedge \tau _{n}}{|}^{2}+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}|Z_{s}{|}^{2}ds+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}d[M]_{s}\\{} & \displaystyle \hspace{1em}=|Y_{\tau _{n}}{|}^{2}+2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s}f(s,Y_{s},Z_{s},V_{s})ds+2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s-}dR_{s}\\{} & \displaystyle \hspace{2em}-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s-}dM_{s}.\end{array}\](9)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle 2Y_{s}f(s,Y_{s},Z_{s},V_{s})& \displaystyle \le 2L|Y_{s}||Z_{s}|+2L|Y_{s}|\big\| V_{s}(e)\big\| _{{\mathcal{L}_{\lambda }^{2}}}+2\mu |Y_{s}{|}^{2}+2|Y_{s}|f_{s}\\{} & \displaystyle \le 2\big(\mu +2{L}^{2}\big)|Y_{s}{|}^{2}+2|Y_{s}|f_{s}+\frac{1}{2}|Z_{s}{|}^{2}+\frac{1}{2}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)\\{} & \displaystyle \le 2|Y_{s}|f_{s}+\frac{1}{2}|Z_{s}{|}^{2}+\frac{1}{2}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de).\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \frac{1}{2}{\int _{t\wedge \tau _{n}}^{\tau _{n}}}|Z_{s}{|}^{2}ds+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\\{} & \displaystyle \hspace{2em}-\frac{1}{2}{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}d[M]_{s}\\{} & \displaystyle \hspace{1em}\le \underset{s\in [t\wedge \tau _{n},T]}{\sup }|Y_{s}{|}^{2}+2\underset{s\in [t\wedge \tau _{n},T]}{\sup }|Y_{s}|\Bigg({\int _{t\wedge \tau _{n}}^{T}}f_{s}ds\Bigg)\\{} & \displaystyle \hspace{2em}+2\underset{s\in [t\wedge \tau _{n},T]}{\sup }|Y_{s}|\Bigg({\int _{t\wedge \tau _{n}}^{T}}d|R|_{s}\Bigg)-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s-}dM_{s}.\end{array}\]
Hence, using the inequality $2ab\le {a}^{2}+{b}^{2}$, we obtain
(10)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \frac{1}{2}{\int _{t\wedge \tau _{n}}^{\tau _{n}}}|Z_{s}{|}^{2}ds+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\\{} & \displaystyle \hspace{2em}-\frac{1}{2}{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}d[M]_{s}\\{} & \displaystyle \hspace{1em}\le 3\underset{u\in [t\wedge \tau _{n},T]}{\sup }|Y_{u}{|}^{2}+{\Bigg({\int _{t\wedge \tau _{n}}^{T}}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{t\wedge \tau _{n}}^{T}}d|R|_{s}\Bigg)}^{2}\\{} & \displaystyle \hspace{2em}-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)-2{\int _{t\wedge \tau _{n}}^{\tau _{n}}}Y_{s-}dM_{s}.\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg(\frac{1}{2}{\int _{t\wedge \tau _{n}}^{\tau _{n}}}|Z_{s}{|}^{2}ds+\frac{1}{2}{\int _{t\wedge \tau _{n}}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+{\int _{t\wedge \tau _{n}}^{\tau _{n}}}d[M]_{s}\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le \mathbb{E}\Bigg(3\underset{u\in [t\wedge \tau _{n},T]}{\sup }|Y_{u}{|}^{2}+{\Bigg({\int _{t\wedge \tau _{n}}^{T}}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{t\wedge \tau _{n}}^{T}}d|R|_{s}\Bigg)}^{2}\Big|\mathcal{F}_{q}\Bigg).\end{array}\]
Therefore, letting n to infinity and using Fatou’s lemma, we obtain (7).
Step 2. In this step, we will estimate $\mathbb{E}(\sup _{u\in [t,T]}|Y_{u}{|}^{2}|\mathcal{F}_{q})$, $0\le q\le t\le T$. Applying Itô’s formula to $|Y_{t}{|}^{2}$ for each $t\in [0,T]$, we get
but in view of (9), we deduce
Recalling that $Y\in {\mathcal{S}}^{2}$, thanks to the first step (estimate (7)), it follows that $Z\in {\mathcal{M}}^{2}$, $V\in {\mathcal{L}}^{2}$, and $M\in {\mathbb{M}}^{2}$. Therefore, by the BDG inequality we deduce that ${\int _{0}^{t}}Y_{s}Z_{s}dW_{s}$, ${\int _{0}^{t}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)$, and ${\int _{0}^{t}}Y_{s-}dM_{s}$ are uniformly integrable martingales. Therefore, taking the conditional expectation in (12) w.r.t. $\mathcal{F}_{q}$, it follows that, for all $0\le q\le t\le T$,
where $\varsigma =|\xi {|}^{2}+2{\int _{t}^{T}}|Y_{s}|f_{s}ds+2{\int _{t}^{T}}|Y_{s-}|d|R|_{s}$.
(11)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle |Y_{t}{|}^{2}+{\int _{t}^{T}}|Z_{s}{|}^{2}ds+{\int _{t}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)+{\int _{t}^{T}}d[M]_{s}\\{} & \displaystyle \hspace{1em}=|\xi {|}^{2}+2{\int _{t}^{T}}Y_{s}f(s,Y_{s},Z_{s},V_{s})ds+2{\int _{t}^{T}}Y_{s-}dR_{s}\\{} & \displaystyle \hspace{2em}-2{\int _{t}^{T}}Y_{s}Z_{s}dW_{s}-2{\int _{t}^{T}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)-2{\int _{t}^{T}}Y_{s-}dM_{s},\end{array}\](12)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle |Y_{t}{|}^{2}+\frac{1}{2}{\int _{t}^{T}}|Z_{s}{|}^{2}ds+{\int _{t}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)+{\int _{t}^{T}}d[M]_{s}\\{} & \displaystyle \hspace{1em}\le |\xi {|}^{2}+2{\int _{t}^{T}}|Y_{s}|f_{s}ds+2{\int _{t}^{T}}|Y_{s-}|d|R|_{s}+\frac{1}{2}{\int _{t}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\\{} & \displaystyle \hspace{2em}-2{\int _{t}^{T}}Y_{s}Z_{s}dW_{s}-2{\int _{t}^{T}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)-2{\int _{t}^{T}}Y_{s-}dM_{s}.\end{array}\](13)
\[ \mathbb{E}\Bigg(\frac{1}{2}{\int _{t}^{T}}|Z_{s}{|}^{2}\hspace{0.1667em}ds+\frac{1}{2}{\int _{t}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+{\int _{t}^{T}}d[M]_{s}\Big|\mathcal{F}_{q}\Bigg)\le \mathbb{E}(\varsigma \mid \mathcal{F}_{q}),\]Next, we deduce from (12) that
Consequently, taking the conditional expectation w.r.t. $\mathcal{F}_{q}$, $0\le q\le t\le T$, we obtain from (13) that
Next, applying the BDG inequality to the martingale terms implies that there exists a constant $C_{1}>0$ such that
and
Hence, plugging estimates (16)–(18) into (15) implies in view of (13) that there exits a constant $C_{2}>0$ such that
from which we deduce, coming back to the definition of ς, that there exists $C_{4}>0$ such that
(14)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}& \displaystyle \le \varsigma +\frac{1}{2}{\int _{t}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+2\underset{u\in [t,T]}{\sup }\Bigg|{\int _{u}^{T}}Y_{s}Z_{s}dW_{s}\Bigg|\\{} & \displaystyle \hspace{1em}+2\underset{u\in [t,T]}{\sup }\Bigg|{\int _{u}^{T}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)\Bigg|+2\underset{u\in [t,T]}{\sup }\Bigg|{\int _{u}^{T}}Y_{{s}^{-}}dM_{s}\Bigg|.\end{array}\](15)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\mid \mathcal{F}_{q}\big)\\{} & \displaystyle \hspace{1em}\le \mathbb{E}\Bigg(2\varsigma +2\underset{u\in [t,T]}{\sup }\bigg|{\int _{u}^{T}}Y_{s}Z_{s}dW_{s}\bigg|+2\underset{u\in [t,T]}{\sup }\bigg|{\int _{u}^{T}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)\bigg|\\{} & \displaystyle \hspace{2em}+2\underset{u\in [t,T]}{\sup }\bigg|{\int _{u}^{T}}Y_{{s}^{-}}dM_{s}\bigg|\Big|\mathcal{F}_{q}\Bigg).\end{array}\](16)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle 2\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }\Bigg|{\int _{u}^{T}}Y_{s}Z_{s}dW_{s}\Bigg|\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le 2C_{1}\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }|Y_{u}|{\Bigg({\int _{t}^{T}}|Z_{s}{|}^{2}ds\Bigg)}^{1/2}\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\Big|\mathcal{F}_{q}\big)+2{C_{1}^{2}}\mathbb{E}\Bigg({\int _{t}^{T}}|Z_{s}{|}^{2}ds\Big|\mathcal{F}_{q}\Bigg),\end{array}\](17)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle 2\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }\Bigg|{\int _{u}^{T}}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)\Bigg|\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le 2C_{1}\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }|Y_{u}|{\Bigg({\int _{t}^{T}}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{1/2}\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\Big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\Big|\mathcal{F}_{q}\Big)+2{C_{1}^{2}}\mathbb{E}\Bigg({\int _{t}^{T}}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Big|\mathcal{F}_{q}\Bigg),\end{array}\](18)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle 2\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }\Bigg|{\int _{u}^{T}}Y_{s-}dM_{s}\Bigg|\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le 2C_{1}\mathbb{E}\Bigg(\underset{u\in [t,T]}{\sup }|Y_{u}|{\Bigg({\int _{t}^{T}}d[M]_{s}\Bigg)}^{1/2}\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\Big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\Big|\mathcal{F}_{q}\Big)+2{C_{1}^{2}}\mathbb{E}\Bigg({\int _{t}^{T}}d[M]_{s}\Big|\mathcal{F}_{q}\Bigg).\end{array}\]
\[ \mathbb{E}\Big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\Big|\mathcal{F}_{q}\Big)\le C_{2}\mathbb{E}(\varsigma \mid \mathcal{F}_{q}).\]
Applying Young’s inequality yields
(19)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle C_{2}\mathbb{E}\Bigg({\int _{t}^{T}}|Y_{s}|f_{s}ds+{\int _{t}^{T}}|Y_{s-}|d|R|_{s}\Big|\mathcal{F}_{q}\Bigg)\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\Big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\Big|\mathcal{F}_{q}\Big)+C_{3}\mathbb{E}\Bigg[{\Bigg({\int _{t}^{T}}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{t}^{T}}d|R|_{s}\Bigg)}^{2}\Big|\mathcal{F}_{q}\Bigg],\end{array}\]
\[ \mathbb{E}\Big(\underset{u\in [t,T]}{\sup }|Y_{u}{|}^{2}\Big|\mathcal{F}_{q}\Big)\le C_{4}\mathbb{E}\Bigg(|\xi {|}^{2}+{\Bigg({\int _{t}^{T}}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{t}^{T}}d|R|_{s}\Bigg)}^{2}\Big|\mathcal{F}_{q}\Bigg).\]
Finally, combining this with (7), the desired result follows, which ends the proof. □Theorem 1.
$({L}^{2}$-solutions) Assume that $(H1)_{p=2}$–$(H6)$ are in force. Then, there exists a unique ${\mathbb{L}}^{2}$-solution $(Y,Z,V,M)$ for the GBSDE (1).
Proof.
Uniqueness. Let $(Y,Z,V,M)$ and $({Y^{\prime }},{Z^{\prime }},{V^{\prime }},{M^{\prime }})$ denote respectively two ${\mathbb{L}}^{2}$-solutions of GRBSDE (1). Define $(\bar{Y},\bar{Z},\bar{V},\bar{M})=(Y-{Y^{\prime }},Z-{Z^{\prime }},V-{V^{\prime }},M-{M^{\prime }})$. Then, $(\bar{Y},\bar{Z},\bar{V},\bar{M})$ solves the following GBSDE in ${\varXi }^{2}$:
It follows from $(H3)$, $(H5)$, and $(H6)$ that
(20)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \bar{Y}_{t}& \displaystyle ={\int _{t}^{T}}\big(f(s,Y_{s},Z_{s},V_{s})-f\big(s,{Y^{\prime }_{s}},{Z^{\prime }_{s}},{V^{\prime }_{s}}\big)\big)ds-{\int _{t}^{T}}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}\bar{V}_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}d\bar{M}_{s},\hspace{1em}t\in [0,T].\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \widehat{\operatorname{sgn}}(\bar{y})\big(f(t,y,z,v)-f\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\big)\\{} & \displaystyle \hspace{1em}=\widehat{\operatorname{sgn}}(\bar{y})\big[f(t,y,z,v)-f\big(t,{y^{\prime }},z,v\big)+f\big(t,{y^{\prime }},z,v\big)-f\big(t,{y^{\prime }},{z^{\prime }},v\big)\\{} & \displaystyle \hspace{2em}+f\big(t,{y^{\prime }},{z^{\prime }},v\big)-f\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\big]\\{} & \displaystyle \hspace{1em}\le \mu |y|+L|z|+L\| v\| _{{\mathcal{L}_{\lambda }^{2}}},\end{array}\]
which means that assumption $(A)$ is satisfied for the generator of GBSDE (20) with $f_{t}\equiv 0$. By Lemma 2 with $q=t=0$ we obtain immediately that $(\bar{Y},\bar{Z},\bar{V},\bar{M})=(0,0,0,0)$. The proof of the uniqueness is then complete.
Existence. Before giving the proof of the existence part, we will talk a little bit about it, but let us first give the following assumption, the so-called general growth condition, which will be needed later:
where $\gamma :{\mathbb{R}}^{+}\to {\mathbb{R}}^{+}$ is a deterministic continuous increasing function.
(21)
\[ (H_{gg})\hspace{1em}\text{For every}\hspace{2.5pt}(t,y)\in [0,T]\times \mathbb{R},\hspace{1em}\big|f(t,y,0,0)\big|\le \big|f(t,0,0,0)\big|+\gamma \big(|y|\big),\]The proof method of Theorem 1 is enlightened by [8, 13, 14, 4, 9], but of course with some obvious changes. More precisely, the first step uses arguments given in [8, 13, 9], whereas the techniques used in the second step, the convolution and weak convergence, are borrowed from [13]. The truncation techniques applied in the third and fourth steps are taken partly from [4, 9, 8]. However, it should be mentioned that since we have changed, compared to [9], the ${\mathbb{L}}^{2}$-integrability condition of $f(t,0,0,0)$ from $\mathbb{E}{\int _{0}^{T}}|f(t,0,0,0){|}^{2}dt<+\infty $ to the one given in $(H1)_{p=2}$ and due also to the finite-variation part $dR$, some new troubles come up, especially, when we want to prove an analogous result of [9, Lemma 4], which says that whenever the data is bounded, so is the solution of the GBSDE. Their approach fails in our context. This is the reason why we give nonstandard estimates in Lemma 2, which allows us to overcome this problem (see, e.g., estimates (26) and (28)). Additionally, in order to prove the existence part of Theorem 1, we first need an existence result under the assumptions of this theorem but with $(H4)$ replaced with $(H_{gg})$, which extends results given in [13] and [9].
The proof is divided into five steps as follows. Note that we will frequently apply Lemma 2. For simplicity, we will assume w.l.o.g. that $a=0$, which means that, in this case, $\mu <0$ (since $\mu +2{L}^{2}\le a=0$, i.e., $\mu \le -2{L}^{2}<0$). In the rest of the proof, we will assume that $\mu <0$.
Step 1. We first assume additionally that there exists a constant $l>0$ such that
for $t\in [0,T],y,{y^{\prime }}\in {\mathbb{R}}^{k},z\in {\mathbb{R}}^{k\times d},v\in {\mathcal{L}_{\lambda }^{2}}$. Moreover, we assume also that there exists a constant $\epsilon >0$ such that
For $(\varGamma ,\varUpsilon ,\varPsi ,N)\in {\varXi }^{2}$, in view of the assumptions made on ξ, f, and R, define the processes $(Y,Z,V,M)$ as follows:
Moreover, from the conditions on ξ, f and R it is easy to prove that $(Y,Z,V,M)\in {\varXi }^{2}$.
\[\begin{array}{r@{\hskip0pt}l}\displaystyle Y_{t}& \displaystyle =\mathbb{E}\Bigg[\xi +{\int _{0}^{T}}f(s,\varGamma _{s},\varUpsilon _{s},\varPsi _{s})ds+{\int _{0}^{T}}dR_{s}\bigg|\mathcal{F}_{t}\Bigg]\\{} & \displaystyle \hspace{1em}-{\int _{0}^{t}}f(s,\varGamma _{s},\varUpsilon _{s},\varPsi _{s})ds-{\int _{0}^{t}}dR_{s},\end{array}\]
and the local martingale
\[ \mathbb{E}\Bigg[\xi +{\int _{0}^{T}}f(s,\varGamma _{s},\varUpsilon _{s},\varPsi _{s})ds+{\int _{0}^{T}}dR_{s}\bigg|\mathcal{F}_{t}\Bigg]-Y_{0},\]
which thanks to the martingale representation theorem (see Lemma 1), can be decomposed as follows:
where Z, V, and M belong respectively to ${\mathbb{L}_{\mathit{loc}}^{2}}(W)$, $G_{\mathit{loc}}(\pi )$, and $\mathbb{M}_{\mathit{loc}}$. Therefore, $(Y,Z,V,M)$ is the unique solution of the GBSDE
(24)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle Y_{t}& \displaystyle =\xi +{\int _{t}^{T}}f(s,\varGamma _{s},\varUpsilon _{s},\varPsi _{s})ds+{\int _{t}^{T}}dR_{s}-{\int _{t}^{T}}Z_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}dM_{s},\hspace{1em}t\in [0,T].\end{array}\]As a by-product, we may define the mapping $\varPhi :{\varXi }^{2}\to {\varXi }^{2}$ that associates $(\varGamma ,\varUpsilon ,\varPsi ,N)$ with $\varPhi ((\varGamma ,\varUpsilon ,\varPsi ,N))=(Y,Z,V,M)$. By standard arguments (see, e.g., the proof of [13, Thm. 55.1]) it can be shown that Φ is contractive on the Banach space ${\varXi }^{2}$ endowed with the norm
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \big\| (Y,Z,V,M)\big\| _{\beta }& \displaystyle =\mathbb{E}\Bigg\{\underset{t\in [0,T]}{\sup }{e}^{\beta t}|Y_{t}{|}^{2}+{\int _{0}^{T}}{e}^{\beta t}|Z_{t}{|}^{2}dt\\{} & \displaystyle \hspace{1em}+{\int _{0}^{T}}\int _{U}{e}^{\beta t}{\big|V_{t}(e)\big|}^{2}\lambda (de)dt+\Bigg[{\int _{0}^{.}}{e}^{\beta t}dM_{t}\Bigg]_{T}\Bigg\}{}^{\frac{1}{2}},\end{array}\]
for a suitably chosen constant $\beta >0$. Consequently, Φ has a fixed point $(Y,Z,V,M)\in {\varXi }^{2}$. Therefore, clearly, $(Y,Z,V,M)$ is the unique solution of GBSDE (1) under the assumptions made so far.
Step 2. In this step, we will show how to dispense with assumption (22). We state and prove the following lemma.
Lemma 3.
Assume that $(H1)_{p=2}$, $(H2)$, $(H3)$, $(H_{gg})$, $(H5)$, $(H6)$, and (23) hold. For given $(\varUpsilon ,\varPsi )\in {\mathcal{M}}^{2}\times {\mathcal{L}}^{2}$, there exists a unique quadruple of processes $(Y,Z,V,M)\in {\varXi }^{2}$ such that
(25)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle Y_{t}& \displaystyle =\xi +{\int _{t}^{T}}f(s,Y_{s},\varUpsilon _{s},\varPsi _{s})ds+{\int _{t}^{T}}dR_{s}-{\int _{t}^{T}}Z_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}dM_{s}.\end{array}\]For notational convenience, we set $f(t,y)=f(t,y,\varUpsilon _{t},\varPsi _{t})$ for each $y\in {\mathbb{R}}^{k}$.
Proof.
Uniqueness is proved by arguing as for uniqueness in Theorem 1. The result follows immediately. For the existence part, we follow the line of the proof of [14, Prop. 2.4]. Now, let us assume that (23) holds and define $f_{n}(t,y)=(\rho _{n}\ast f(t,\cdot ))(y)$, where $\rho _{n}:\mathbb{R}\to {\mathbb{R}}^{+}$ is a sequence of smooth functions with compact support that approximate the Dirac measure at 0 and satisfy $\int \rho _{n}(z)dz=1$. Moreover, they are defined such that ϖ satisfying $\varpi (r)=\sup _{n}\sup _{|y|\le r}\int _{\mathbb{R}}\gamma (|y|)\rho _{n}(y-z)dz$ is finite for all $r\in {\mathbb{R}}^{+}$. Note that f satisfies the following assumptions:
Thus, it is elementary to check that $f_{n}$ satisfies (i)–(iv) with the same constant L and ϖ instead of γ. However, we cannot apply step 1 of the proof since $f_{n}$ is not necessarily globally Lipschitz continuous in y but only locally Lipschitz. Hence, to overcome this problem, we add a truncation function $T_{p}$ in $f_{n}$. Indeed, define, for each $p\in \mathbb{N}$,
Hence, for any $p>r$, the sequence $({Y}^{n,p},{Z}^{n,p},{V}^{n,p},{M}^{n,p})$ does not depend on p. Then we denote it by $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$, and it is a solution to GBSDE (25) associated with $(\xi ,f_{n}+dR)$. Moreover, now $f_{n}$ satisfies the conditions of Lemma 2 with a constant independent of n, and thus the sequence $({Y}^{n},{U}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is uniformly bounded, that is,
Let us set ${U_{t}^{n}}=f_{n}(t,{Y_{t}^{n}})$ for $t\in [0,T]$. Using the previous uniform estimate of the sequence $\{({Y}^{n},{Z}^{n},{V}^{n},{U}^{n},)\}_{n}$ and the Hilbert structure of ${\mathbb{L}}^{2}(\varOmega \times [0,T])\times {\mathcal{M}}^{2}\times {\mathcal{L}}^{2}\times {\mathfrak{H}}^{2}$, we deduce that we can extract subsequences, still denoted $\{n\}$, that weakly converge to some process $(Y,Z,V,U)$ in ${\mathbb{L}}^{2}(\varOmega \times [0,T])\times {\mathcal{M}}^{2}\times {\mathcal{L}}^{2}\times {\mathfrak{H}}^{2}$, where ${\mathfrak{H}}^{2}$ denotes the set of $\mathcal{F}_{t}$-progressively measurable ${\mathbb{R}}^{k}$-valued processes $(U_{t})_{t\in [0,T]}$ such that
\[ f_{n,p}(t,y)=f_{n}\big(t,T_{p}(y)\big)\hspace{1em}\text{such that}\hspace{2.5pt}T_{p}(y)=\frac{py}{|y|\vee p}.\]
Notice that, for all $n,p\in \mathbb{N}$, $y\to f_{n,p}(t,y)$ is globally Lipschitz and satisfies the conditions of Step 1. Therefore, for all $n,p\in \mathbb{N}$, according to what has already been proved in Step 1, there exists a unique solution $({Y}^{n,p},{Z}^{n,p},{V}^{n,p},{M}^{n,p})$ to GBSDE (25) associated with $(\xi ,f_{n,p}+dR)$. Furthermore, it follows from (23) and Lemma 2 with $a=0$ and $q=t$ that there exists a universal constant $C_{1}>0$ such that, for all $n,p\in \mathbb{N}$ and $t\in [0,T]$,
(26)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {\big|{Y_{t}^{n,p}}\big|}^{2}+\mathbb{E}\Bigg({\int _{t}^{T}}{\big|{Z_{s}^{n,p}}\big|}^{2}ds+{\int _{t}^{T}}\int _{U}{\big|{V_{s}^{n,p}}(e)\big|}^{2}\lambda (de)ds+{\int _{t}^{T}}d\big[{M}^{n,p}\big]_{s}\bigg|\mathcal{F}_{t}\Bigg)\\{} & \displaystyle \hspace{1em}\le C_{1}\mathbb{E}\Bigg[|\xi {|}^{2}+{\Bigg({\int _{t}^{T}}\big|f(s,0,0,0)\big|ds\Bigg)}^{2}+{\Bigg({\int _{t}^{T}}d|R|_{s}\Bigg)}^{2}\bigg|\mathcal{F}_{t}\Bigg]\\{} & \displaystyle \hspace{1em}\le C_{1}{\epsilon }^{2}\big(2+{T}^{2}\big):={r}^{2}.\end{array}\](27)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \underset{n\in \mathbb{N}}{\sup }\mathbb{E}\Bigg[{\int _{0}^{T}}{\big|{Y_{t}^{n}}\big|}^{2}dt+{\Bigg({\int _{0}^{T}}f_{n}\big(t,{Y_{t}^{n}}\big)dt\Bigg)}^{2}+{\int _{0}^{T}}{\big|{Z_{t}^{n}}\big|}^{2}dt\\{} & \displaystyle \hspace{1em}+{\int _{0}^{T}}\int _{U}{\big|{V_{t}^{n}}(e)\big|}^{2}\lambda (de)dt+\big[{M}^{n}\big]_{T}\Bigg]\le C.\end{array}\]
\[ \| U\| _{{\mathfrak{H}}^{2}}:={\Bigg\{\mathbb{E}\Bigg[{\Bigg({\int _{0}^{T}}|U_{t}|dt\Bigg)}^{2}\Bigg]\Bigg\}}^{\frac{1}{2}}<+\infty .\]
Now we deal with the convergence of the martingale ${M}^{n}$. By estimate (27) it follows that $\sup _{n\ge 1}\mathbb{E}|{M_{T}^{n}}{|}^{2}<\infty $. Thus, there exists a subsequence, still denoted $\{n\}$, such that ${M_{T}^{n}}$ converges weakly to some random variable $M_{T}$ in ${\mathbb{L}}^{2}(\varOmega )$. Let $M_{t}$ denote the martingale with terminal value $M_{T}$.Next, following [14, Prop. 2.4], we deduce, by using the martingale representation theorem (see Lemma 1) and orthogonality that the following weak convergence hold for the martingales in ${\mathbb{L}}^{2}(\varOmega )$: for each $t\in [0,T]$,
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {\int _{t}^{T}}{Z_{s}^{n}}dW_{s}\to {\int _{t}^{T}}Z_{s}dW_{s},\hspace{2.5pt}{\int _{t}^{T}}\int _{U}{V_{s}^{n}}(e)\hat{\pi }(de,ds)\to {\int _{t}^{T}}\int _{U}V_{s}(e)\hat{\pi }(de,ds),\\{} & \displaystyle \hspace{1em}\text{and}\hspace{1em}{M_{t}^{n}}\to M_{t}.\end{array}\]
Therefore, taking weak limits in the approximating equation, we get that $(Y,Z,V,M)$ satisfies the GBSDE
\[ Y_{t}=\xi +{\int _{t}^{T}}U_{s}ds+{\int _{t}^{T}}dR_{s}-{\int _{t}^{T}}Z_{s}dW_{s}-{\int _{t}^{T}}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}dM_{s}.\]
Finally, as in [14, Prop. 2.4], we can show that $U_{t}=f(t,Y_{t})$. This implies that $(Y,Z,V,M)$ solves GBSDE (25) under the assumptions made so far in this step, which completes the proof of Lemma 3.
Step 3. In this step, we will show that assumption $(H_{gg})$ assumed so far can be weakened to $(H4)$. In fact, by the mean of truncation technique we will show that, for given $(\varUpsilon ,\varPsi )\in {\mathcal{M}}^{2}\times {\mathcal{L}}^{2}$ and provided that $(H1)_{p=2}$–$(H6)$ and (23) hold, GBSDE (25) has a solution in ${\varXi }^{2}$. The idea behind the proof is to approximate f by a sequence of functions $f_{n}$ satisfying assumption $(H_{gg})$. Indeed, let $\theta _{r}$ be a smooth function such that $0\le \theta _{r}\le 1$ and satisfies for r large enough:
As a by-product, $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a solution to the GBSDE (25) associated with the data $(\xi ,f_{n}+dR)$. Next, we show as in [9, Thm. 1] (see also [4, Thm. 4.2]) by using similar arguments that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence in ${\varXi }^{2}$, and its limit is $(Y,Z,V,M)\in {\varXi }^{2}$.
\[ \theta _{r}(y)=\bigg\{\begin{array}{l}1\hspace{1em}\text{for}\hspace{1em}|y|\le r,\\{} 0\hspace{1em}\text{for}\hspace{1em}|y|\ge r+1.\end{array}\]
Let $\varphi _{r}(t)=\sup _{|y|\le r}|f(t,y,0,0)-f(t,0,0,0)|\in {\mathbb{L}}^{1}([0,T])$ and, for $n\in {\mathbb{N}}^{\ast }$, denote $T_{n}(x)=\frac{xn}{|x|\vee n}$. The approximation sequence $f_{n}$ is defined by
\[\begin{array}{r@{\hskip0pt}l}\displaystyle f_{n}(t,y,\varUpsilon ,\varPsi )& \displaystyle =\big(f\big(t,y,T_{n}(\varUpsilon _{t}),T_{n}(\varPsi _{t})\big)-f(t,0,\varUpsilon _{t},\varPsi _{t})\big)\frac{n}{\varphi _{r+1}(t)\vee n}\\{} & \displaystyle \hspace{1em}+f(t,0,\varUpsilon _{t},\varPsi _{t}).\end{array}\]
We also define a sequence $h_{n}$ that truncates $f_{n}$ for $|y|\ge r+1$:
\[\begin{array}{r@{\hskip0pt}l}\displaystyle h_{n}(t,y,\varUpsilon _{t},\varPsi _{t})& \displaystyle =\theta _{r}(y)\big(f\big(t,y,T_{n}(\varUpsilon _{t}),T_{n}(\varPsi _{t})\big)-f(t,0,\varUpsilon _{t},\varPsi _{t})\big)\frac{n}{\varphi _{r+1}(t)\vee n}\\{} & \displaystyle \hspace{1em}+f(t,0,\varUpsilon _{t},\varPsi _{t}).\end{array}\]
Following the same reasoning as in the proof of [4, Thm. 4.2], it can be shown that $h_{n}$ still satisfies the monotonicity condition $(H3)$ but with a positive constant $C(r,k,n)$ depending on $r,k$, and n. Then, the conditions of Lemma 3 of the previous step are fulfilled by the data $(\xi ,h_{n}+dR)$. Consequently, for each $n\in {\mathbb{N}}^{\ast }$, the GBSDE (25) associated with $(\xi ,h_{n}+dR)$, admits a unique solution $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})\in {\varXi }^{2}$. Moreover, since $yh_{n}(t,y,\varUpsilon ,\varPsi )\le |y|\| f(t,0,0,0)\| _{\infty }+k|y|(|\varUpsilon |+\| \varPsi \| _{{\mathcal{L}_{\lambda }^{2}}})$, $h_{n}$ satisfies the condition of Lemma 2. Consequently, applying Lemma 2 with $a=0$ and $q=t=0$, in view of the boundedness assumption (23), we get similarly as in (26) that, for each $n\in \mathbb{N}$, the following estimates hold $d\mathbb{P}\times dt$-a.e.:
(28)
\[ \big|{Y_{t}^{n}}\big|\le r\hspace{1em}\text{and}\hspace{1em}\mathbb{E}\Bigg({\int _{0}^{T}}{\big|{Z_{s}^{n}}\big|}^{2}ds+{\int _{0}^{T}}\int _{U}{\big|{V_{s}^{n}}(e)\big|}^{2}\lambda (de)ds+\big[{M}^{n}\big]_{T}\Bigg)\le {r}^{2}.\]
Step 4. We now treat the general case. We want to get rid of the boundedness condition (23) used so far. To this end, a truncation procedure. Indeed, under assumptions $(H1)_{p=2}$–$(H6)$, we first set, for each $n\in {\mathbb{N}}^{\ast }$,
Thanks to $(H3)$, $(H5)$, and $(H6)$, the generator of GBSDE (29) satisfies assumption $(A)$ with $f_{t}\equiv T_{m}(f(t,0))-T_{n}(f(t,0))$ and $L=0$. Therefore, applying Lemma 2 with $a=0$ and $q=t=0$ yields, for all $n,m\in \mathbb{N}$,
Obviously, the right-hand side of (30) tends to 0 as $n,m\to \infty $. Therefore, $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence in ${\varXi }^{2}$, and its limit $(Y,Z,V,M)\in {\varXi }^{2}$ is an ${L}^{2}$-solution of GBSDE (25).
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \xi _{n}& \displaystyle =T_{n}(\xi ),\hspace{2em}f_{n}(t,y)=f_{n}(t,y,\varUpsilon _{t},\varPsi _{t})=f(t,y)-f(t,0)+T_{n}\big(f(t,0)\big),\\{} \displaystyle {R_{t}^{n}}& \displaystyle ={\int _{0}^{t}}\mathbb{1}_{\{|R|_{s}\le n\}}dR_{s}.\end{array}\]
Then, according to the previous step, for each $n\in {\mathbb{N}}^{\ast }$, GBSDE (25) associated with $(\xi _{n},f_{n}+d{R}^{n})$ has a unique solution $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})\in {\varXi }^{2}$. Our goal now is to show that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence in ${\varXi }^{2}$. Set $(\bar{Y},\bar{Z},\bar{V},\bar{M})=({Y}^{m}-{Y}^{n},{Z}^{m}-{Z}^{n},{V}^{m}-{V}^{n},{M}^{m}-{M}^{n})$. Then $(\bar{Y},\bar{Z},\bar{V},\bar{M})$ is solution to the GBSDE
(29)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \bar{Y}_{t}& \displaystyle =\xi _{m}-\xi _{n}+{\int _{t}^{T}}d\big({R_{s}^{m}}-{R_{s}^{n}}\big)+{\int _{t}^{T}}\big(f_{m}\big(s,{Y_{s}^{m}}\big)-f_{n}\big(s,{Y_{s}^{n}}\big)\big)ds\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\bar{Z}_{s}dW_{s}-{\int _{t}^{T}}\int _{U}\bar{V}_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}d\bar{M}_{s},\hspace{1em}t\in [0,T].\end{array}\](30)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }|\bar{Y}_{t}{|}^{2}+{\int _{0}^{T}}|\bar{Z}_{t}{|}^{2}dt+{\int _{0}^{T}}\int _{U}{\big|\bar{V}_{t}(e)\big|}^{2}\lambda (de)dt+[\bar{M}]_{T}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg[|\xi _{m}-\xi _{n}{|}^{2}+{\Bigg({\int _{0}^{T}}\big|T_{m}\big(f(t,0)\big)-T_{n}\big(f(t,0)\big)\big|dt\Bigg)}^{2}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{T}}d\big|{R}^{m}-{R}^{n}\big|_{s}\Bigg)}^{2}\Bigg].\end{array}\]
Step 5. In this step, we will finally complete the proof of the existence part of Theorem 1. To this end, we consider a Picard’s iteration procedure. Set $({Y}^{0},{Z}^{0},{V}^{0},{M}^{0})\hspace{0.1667em}=\hspace{0.1667em}(0,0,0,0)$ and define $\{({Y_{t}^{n}},{Z_{t}^{n}},{V_{t}^{n}},{M_{t}^{n}})_{t\in [0,T]}\}_{n\ge 1}$ recursively in view of Step 4, for all $n\ge 0$ and $t\in [0,T]$,
From the previous step it follows that, under assumptions $(H1)_{p=2}$–$(H6)$, for each $n\ge 0$, there exists a solution of GBSDE (31). Let us set $\delta {Y}^{n}:={Y}^{n+1}-{Y}^{n}$, $\delta {Z}^{n}:={Z}^{n+1}-{Z}^{n}$, $\delta {V}^{n}:={V}^{n+1}-{V}^{n}$, and $\delta {M}^{n}:={M}^{n+1}-{M}^{n}$. $(\delta {Y}^{n},\delta {Z}^{n},\delta {V}^{n},\delta {M}^{n})$ solves the GBSDE
(31)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle {Y_{t}^{n+1}}& \displaystyle =\xi +{\int _{t}^{T}}f\big(s,{Y_{s}^{n+1}},{Z_{s}^{n}},{V_{s}^{n}}\big)ds+{\int _{t}^{T}}dR_{s}-{\int _{t}^{T}}{Z_{s}^{n+1}}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}{V_{s}^{n+1}}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}d{M_{s}^{n+1}}.\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \delta {Y_{t}^{n}}& \displaystyle ={\int _{t}^{T}}\big[f\big(s,{Y_{s}^{n+1}},{Z_{s}^{n}},{V_{s}^{n}}\big)-f\big(s,{Y_{s}^{n}},{Z_{s}^{n-1}},{V_{s}^{n-1}}\big)\big]ds-{\int _{t}^{T}}\delta {Z_{s}^{n}}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}\delta {V_{s}^{n}}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}d\delta {M_{s}^{n}},\hspace{1em}t\in [0,T].\end{array}\]
By assumptions $(H3)$, $(H5)$, and $(H6)$ we have that
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \widehat{\operatorname{sgn}}\big(\delta {y}^{n}\big)\big(f\big(t,{y}^{n+1},{z}^{n},{v}^{n}\big)-f\big(t,{y}^{n},{z}^{n-1},{v}^{n-1}\big)\big)\\{} & \displaystyle \hspace{1em}=\widehat{\operatorname{sgn}}\big(\delta {y}^{n}\big)\big[\big(f\big(t,{y}^{n+1},{z}^{n},{v}^{n}\big)-f\big(t,{y}^{n},{z}^{n},{v}^{n}\big)\big)\\{} & \displaystyle \hspace{2em}+\big(f\big(t,{y}^{n},{z}^{n},{v}^{n}\big)-f\big(t,{y}^{n},{z}^{n-1},{v}^{n-1}\big)\big)\big]\\{} & \displaystyle \hspace{1em}\le \mu \big|\delta {y}^{n}\big|+L\big|\delta {z}^{n-1}\big|+L\big\| \delta {v}^{n-1}\big\| _{{\mathcal{L}_{\lambda }^{2}}},\end{array}\]
which is assumption $(A)$ with $f_{t}=L|\delta {z}^{n-1}|+L\| \delta {v}^{n-1}\| _{{\mathcal{L}_{\lambda }^{2}}}$ and $L\equiv 0$. Thus, it follows from Lemma 2 with $a=q=t=0$ and Hölder’s inequality that there exists a constant $C>0$ such that
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }{\big|\delta {Y_{t}^{n}}\big|}^{2}+{\int _{0}^{T}}{\big|\delta {Z_{s}^{n}}\big|}^{2}ds+{\int _{0}^{T}}\int _{U}{\big|\delta {V_{s}^{n}}(e)\big|}^{2}\lambda (de)ds+\big[\delta {M}^{n}\big]_{T}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}{\Bigg[{\int _{0}^{T}}L\big(\big|\delta {Z_{t}^{n-1}}\big|+\big\| \delta {V_{t}^{n-1}}(e)\big\| _{{\mathcal{L}_{\lambda }^{2}}}\big)dt\Bigg]}^{2}\\{} & \displaystyle \hspace{1em}\le C{L}^{2}T\mathbb{E}\Bigg[{\int _{0}^{T}}\big({\big|\delta {Z_{t}^{n-1}}\big|}^{2}+\big\| \delta {V_{t}^{n-1}}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}\big)dt\Bigg].\end{array}\]
Consequently, by induction we deduce that, for $n\ge 2$,
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }{\big|\delta {Y_{t}^{n}}\big|}^{2}+{\int _{0}^{T}}{\big|\delta {Z_{t}^{n}}\big|}^{2}dt+{\int _{0}^{T}}\int _{U}{\big|\delta {V_{t}^{n}}(e)\big|}^{2}\lambda (de)dt+\big[\delta {M}^{n}\big]_{T}\Bigg]\\{} & \displaystyle \hspace{1em}\le {c}^{n-1}\mathbb{E}\Bigg[{\int _{0}^{T}}{\big|\delta {Z_{t}^{1}}\big|}^{2}dt+{\int _{0}^{T}}\int _{U}{\big|\delta {V_{t}^{1}}(e)\big|}^{2}\lambda (de)dt\Bigg],\end{array}\]
where $c=C{L}^{2}T$. Let us first assume, for a sufficiently small T, that $c<1$. Then, since the remaining term of the right-hand side of the last inequality is finite, we deduce that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence in ${\varXi }^{2}$, and the limit process $(Y,Z,V,M)$ is a solution to GBSDE (1) in ${\varXi }^{2}$.For the general case, it suffices to subdivide the interval time $[0,T]$ into a finite number of small intervals, and using the standard arguments, we can prove the existence of a solution $(Y,Z,V,M)$ of GBSDE (1) in ${\varXi }^{2}$ on the whole interval $[0,T]$. This completes the proof of this step and thus of the whole proof of Theorem 1. □
3.2 Case $p\ge 2$
In this subsection, we study the issue of existence and uniqueness of ${\mathbb{L}}^{p}$-solutions of GBSDE (1) in the case $p\ge 2$. Let us first give a priori estimates for the solution and their variations induced by a variation of the data.
Lemma 4.
Let assumption $(A)$ hold, and let $(Y,Z,V,M)$ be a solution of GBSDE (1). Let us assume moreover that
If $Y\in {S}^{p}$, then there exists a constant $C_{p}>0$, depending only on p and T, such that, for every $a\ge \mu +2{L}^{2}$,
(32)
\[ \mathbb{E}\Bigg[|\xi {|}^{p}+{\Bigg({\int _{0}^{T}}f_{t}dt\Bigg)}^{p}+|R{|_{T}^{p}}\Bigg]<+\infty .\](33)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }{e}^{apt}|Y_{t}{|}^{p}+{\Bigg({\int _{0}^{T}}{e}^{2at}|Z_{t}{|}^{2}dt\Bigg)}^{p/2}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{T}}\int _{U}{e}^{2at}{\big|V_{t}(e)\big|}^{2}\lambda (de)dt\Bigg)}^{p/2}+{e}^{apT}{[M]_{T}^{p/2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg[{e}^{apT}|\xi {|}^{p}+{\Bigg({\int _{0}^{T}}{e}^{at}f_{t}dt\Bigg)}^{p}+{\Bigg({\int _{0}^{T}}{e}^{at}d|R|_{t}\Bigg)}^{p}\Bigg].\end{array}\]Proof.
The proof is divided into two steps. By an already used argument (see Lemma (2)) we can assume w.l.o.g. that $\mu +2{L}^{2}\le 0$ and take $a=0$.
Step 1. First, we show that
Indeed, define the sequence of stopping times $\tau _{n}$ for $n\in \mathbb{N}$:
Thus, since $\tau _{n}\le T$, we deduce that
Since $\frac{p}{2}\ge 1$, we can apply the BDG inequality to obtain
and
Plugging estimates (37)–(39) into (36) and then taking the expectation, we get
Thus, choosing ϵ small enough and depending only on p, we deduce that
(34)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{\Bigg({\int _{0}^{T}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{T}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{T}}d[M]_{s}\Bigg)}^{\frac{p}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C(p,T)\Bigg[\mathbb{E}\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}+{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{p}+{\Bigg({\int _{0}^{T}}d|R|_{s}\Bigg)}^{p}\Bigg].\end{array}\]
\[ \tau _{n}=\inf \Bigg\{t>0;{\int _{0}^{t}}|Z_{s}{|}^{2}ds+{\int _{0}^{t}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda de(ds)+[M]_{t}>n\Bigg\}\wedge T.\]
By Itô’s formula on $|Y_{t}{|}^{2}$,
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle |Y_{0}{|}^{2}+{\int _{0}^{\tau _{n}}}|Z_{s}{|}^{2}ds+{\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)+{\int _{0}^{\tau _{n}}}d[M]_{s}\\{} & \displaystyle \hspace{1em}=|Y_{\tau _{n}}{|}^{2}+2{\int _{0}^{\tau _{n}}}Y_{s}f(s,Y_{s},Z_{s},V_{s})ds+2{\int _{0}^{\tau _{n}}}Y_{s-}dR_{s}-2{\int _{0}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-2{\int _{0}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)-2{\int _{0}^{\tau _{n}}}Y_{s-}dM_{s}.\end{array}\]
But from assumption $(A)$, combined with the inequality $2ab\le \frac{1}{\varepsilon }{a}^{2}+\varepsilon {b}^{2}$ for $\varepsilon >0$, since $\mu +2{L}^{2}<0$, we have
(35)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle 2Y_{s}f(s,Y_{s},Z_{s},V_{s})& \displaystyle \le 2\mu |Y_{s}{|}^{2}+2|Y_{s}||f_{s}|+2L|Y_{s}||Z_{s}|+2L|Y_{s}|\big\| V_{s}(e)\big\| _{{\mathcal{L}_{\lambda }^{2}}}\\{} & \displaystyle \le \bigg(\frac{1}{\varepsilon }+2\big(\mu +{L}^{2}\big)\bigg)|Y_{s}|+2|Y_{s}|f_{s}+\frac{1}{2}|Z_{s}{|}^{2}+\varepsilon \big\| V_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}\\{} & \displaystyle \le \frac{1}{\varepsilon }|Y_{s}{|}^{2}+2|Y_{s}|f_{s}+\frac{1}{2}|Z_{s}{|}^{2}+\varepsilon \big\| V_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}.\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \frac{1}{2}{\int _{0}^{\tau _{n}}}|Z_{s}{|}^{2}ds+{\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)+{\int _{0}^{\tau _{n}}}d[M]_{s}\\{} & \displaystyle \hspace{1em}\le \underset{t\in [0,T]}{\sup }|Y_{t}{|}^{2}+\frac{1}{\varepsilon }{\int _{0}^{T}}|Y_{s}{|}^{2}ds+2\underset{t\in [0,T]}{\sup }|Y_{t}|{\int _{0}^{T}}f_{s}ds\\{} & \displaystyle \hspace{2em}+2\underset{t\in [0,T]}{\sup }|Y_{t}|{\int _{0}^{T}}d|R|_{s}+\varepsilon {\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+2\Bigg|{\int _{0}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}\Bigg|\\{} & \displaystyle \hspace{2em}+2\Bigg|{\int _{0}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}{(e)}^{2}\widehat{\pi }(de,ds)\Bigg|+2\Bigg|{\int _{0}^{\tau _{n}}}Y_{s-}dM_{s}\Bigg|\\{} & \displaystyle \hspace{1em}\le \bigg(3+\frac{T}{\epsilon }\bigg)\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{2}+{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{2}+{\Bigg({\int _{0}^{T}}d|R|_{s}\Bigg)}^{2}\\{} & \displaystyle \hspace{2em}+\varepsilon {\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds+\Bigg|{\int _{0}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}\Bigg|\\{} & \displaystyle \hspace{2em}+\Bigg|{\int _{0}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}{(e)}^{2}\widehat{\pi }(de,ds)\Bigg|+\Bigg|{\int _{0}^{\tau _{n}}}Y_{s-}dM_{s}\Bigg|.\end{array}\]
It follows that there exists a constant $c_{p}>0$, depending only on p, such that
(36)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {\Bigg({\int _{0}^{\tau _{n}}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau _{n}}}d[M]_{s}\Bigg)}^{\frac{p}{2}}\\{} & \displaystyle \hspace{1em}\le c_{p}\Bigg[{\bigg(3+\frac{T}{\epsilon }\bigg)}^{\frac{p}{2}}\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}+{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{p}+{\Bigg({\int _{0}^{\tau _{n}}}d|R|_{s}\Bigg)}^{p}\\{} & \displaystyle \hspace{2em}+{\epsilon }^{\frac{p}{2}}{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}+{\Bigg|{\int _{0}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}\Bigg|}^{\frac{p}{2}}\\{} & \displaystyle \hspace{2em}+{\Bigg|{\int _{0}^{\tau _{n}}}\int _{U}Y_{s-}V_{s}{(e)}^{2}\widehat{\pi }(de,ds)\Bigg|}^{\frac{p}{2}}+{\Bigg|{\int _{0}^{\tau _{n}}}Y_{s-}dM_{s}\Bigg|}^{\frac{p}{2}}\Bigg].\end{array}\](37)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle c_{p}\mathbb{E}{\Bigg|{\int _{0}^{\tau _{n}}}Y_{s}Z_{s}dW_{s}\Bigg|}^{\frac{p}{2}}& \displaystyle \le d_{p}\mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau _{n}}}|Y_{s}{|}^{2}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{4}}\Bigg]\\{} & \displaystyle \le \frac{{d_{p}^{2}}}{4}\mathbb{E}\Big(\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\Big)+\frac{1}{2}\mathbb{E}{\Bigg({\int _{0}^{\tau _{n}}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}},\end{array}\](38)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle c_{p}\mathbb{E}{\Bigg|{\int _{0}^{\tau _{n}}}Y_{s-}dM_{s}\Bigg|}^{\frac{p}{2}}& \displaystyle \le d_{p}\mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau _{n}}}|Y_{s-}{|}^{2}d[M]_{s}\Bigg)}^{\frac{p}{4}}\Bigg]\\{} & \displaystyle \le \frac{{d_{p}^{2}}}{4}\mathbb{E}\Big(\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\Big)+\frac{1}{2}\mathbb{E}{[M]_{\tau _{n}}^{\frac{p}{2}}},\end{array}\](39)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle c_{p}\mathbb{E}{\Bigg|{\int _{0}^{T}}\int _{U}Y_{s-}V_{s}(e)\widehat{\pi }(de,ds)\Bigg|}^{\frac{p}{2}}\\{} & \displaystyle \hspace{1em}\le d_{p}\mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau _{n}}}|Y_{s}{|}^{2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{p}{4}}\Bigg]\\{} & \displaystyle \hspace{1em}\le \frac{{d_{p}^{2}}}{4}\mathbb{E}\Big(\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\Big)+\frac{1}{2}\mathbb{E}{\Bigg({\int _{0}^{\tau _{n}}}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{p}{2}}.\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \frac{1}{2}\mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau _{n}}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau _{n}}}d[M]_{s}\Bigg)}^{\frac{p}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C(p,T,\epsilon )\mathbb{E}\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}+c_{p}\mathbb{E}{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{p}+c_{p}\mathbb{E}{\Bigg({\int _{0}^{\tau _{n}}}d|R|_{s}\Bigg)}^{p}\\{} & \displaystyle \hspace{2em}+c_{p}{\epsilon }^{\frac{p}{2}}\mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}\Bigg].\end{array}\]
By [11, Section 4] or [6, Lemma 2.1] we have that, for some constant $\eta _{p}>0$,
(40)
\[ \mathbb{E}{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}\le \eta _{p}\mathbb{E}{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{p}{2}}.\]
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau _{n}}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau _{n}}}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau _{n}}}d[M]_{s}\Bigg)}^{\frac{p}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le \widetilde{C}(p,T)\mathbb{E}\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}+\widetilde{C}_{p}\mathbb{E}\Bigg[{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{p}+{\Bigg({\int _{0}^{T}}d|R|_{s}\Bigg)}^{p}\Bigg].\end{array}\]
Finally, letting n to $+\infty $ and using Fatou’s lemma, (34) follows.
Step 2. Since $p\ge 2$, we can apply Itô’s formula with the ${\mathcal{C}}^{2}$ function $|y{|}^{p}$ to $|Y_{t}{|}^{p}$. Note that
where
and
where $\alpha _{p}=\min (\frac{p}{2},p(p-1){3}^{1-p})$.
\[ \frac{\partial \theta }{\partial y_{i}}(y)=py_{i}|y{|}^{p-2},\hspace{2em}\frac{{\partial }^{2}\theta }{\partial y_{i}\partial y_{j}}(y)=p|y{|}^{p-2}\delta _{i,j}+p(p-2)y_{i}y_{j}|y{|}^{p-4},\]
where $\delta _{i,j}$ is the Kronecker delta. Thus, for every $t\in [0,T]$, we have
(41)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle |Y_{t}{|}^{p}& \displaystyle =|\xi {|}^{p}+p{\int _{t}^{T}}Y_{s-}|Y_{s-}{|}^{p-2}dR_{s}+p{\int _{t}^{T}}Y_{s}|Y_{s}{|}^{p-2}f(s,Y_{s},Z_{s},V_{s})ds\\{} & \displaystyle \hspace{1em}-p{\int _{t}^{T}}Y_{s-}|Y_{s-}{|}^{p-2}dM_{s}-p{\int _{t}^{T}}Y_{s}|Y_{s}{|}^{p-2}Z_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-p{\int _{t}^{T}}\hspace{-0.1667em}\int _{U}\big(Y_{s-}|Y_{s-}{|}^{p-2}V_{s}(e)\big)\widehat{\pi }(de,ds)\hspace{0.1667em}-\hspace{0.1667em}\frac{1}{2}{\int _{t}^{T}}\hspace{-0.1667em}\hspace{-0.1667em}\operatorname{Trace}\big({D}^{2}\theta (Y_{s})Z_{s}{Z_{s}^{t}}\big)ds\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\hspace{-0.1667em}\int _{U}\big({\big|Y_{s-}+V_{s}(e)\big|}^{p}-|Y_{s-}{|}^{p}-pY_{s-}|Y_{s-}{|}^{p-2}V_{s}(e)\big)\pi (de,ds)-\mathrm{\aleph }_{t},\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathrm{\aleph }_{t}& \displaystyle =\frac{1}{2}{\int _{t}^{T}}\sum \limits_{1\le i,j\le d}\frac{{\partial }^{2}\theta }{\partial y_{i}\partial y_{j}}(Y_{s})d{\big[{M}^{i},{M}^{j}\big]_{s}^{c}}\\{} & \displaystyle \hspace{1em}+\sum \limits_{t<s\le T}\big(|Y_{s-}+\Delta M_{s}{|}^{p}-|Y_{s-}{|}^{p}-pY_{s-}|Y_{s-}{|}^{p-2}\Delta M_{s}\big).\end{array}\]
Following arguments from [9, Prop. 2], we have that (44)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle -{\int _{t}^{T}}\int _{U}\big({\big|Y_{s-}+V_{s}(e)\big|}^{p}-|Y_{s-}{|}^{p}-pY_{s-}|Y_{s-}{|}^{p-2}V_{s}(e)\big)\pi (de,ds)\\{} & \displaystyle \hspace{1em}\le -p(p-1){3}^{1-p}{\int _{t}^{T}}|Y_{s-}{|}^{p-2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds),\end{array}\]Consequently, in view of estimates (42), (43), and (44), Eq. (41) becomes
But from assumption $(A)$ and the fact that $\mu \le -2{L}^{2}\le 0$ (since $\mu +2{L}^{2}\le 0$) we deduce by using the inequality $ab\le \frac{1}{2\epsilon }{a}^{2}+\frac{\epsilon }{2}{b}^{2}$ that
Choosing $\epsilon =\frac{\alpha _{p}}{p}$, we obtain in view of the last inequality that
Let us set $X=|\xi {|}^{p}+\frac{p{L}^{2}}{\alpha _{p}}{\int _{t}^{T}}|Y_{s}{|}^{p}\hspace{0.1667em}ds+p{\int _{t}^{T}}|Y_{s}{|}^{p-1}|f_{s}|ds+p{\int _{t}^{T}}|Y_{s-}{|}^{p-1}dR_{s}$, $\varUpsilon _{t}={\int _{0}^{t}}Y_{s}|Y_{s}{|}^{p-2}Z_{s}dW_{s}$, $\varTheta _{t}={\int _{0}^{t}}\int _{U}Y_{s-}|Y_{s-}{|}^{p-2}V_{s}(e)\hspace{0.1667em}\widehat{\pi }(de,ds)$, and $\varGamma _{t}={\int _{0}^{t}}Y_{s-}|Y_{s-}{|}^{p-2}dM_{s}$.
(45)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle |Y_{t}{|}^{p}+\alpha _{p}{\int _{t}^{T}}|Y_{s}{|}^{p-2}|Z{|_{s}^{2}}ds+\alpha _{p}{\int _{t}^{T}}\int _{U}|Y_{s}{|}^{p-2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\\{} & \displaystyle \hspace{2em}+\alpha _{p}{\int _{t}^{T}}|Y_{s}{|}^{p-2}d{[M]_{s}^{c}}+\alpha _{p}\sum \limits_{t<s\le T}|Y_{s}{|}^{p-2}|\Delta M_{s}{|}^{2}\\{} & \displaystyle \hspace{1em}\le |\xi {|}^{p}+p{\int _{t}^{T}}Y_{s-}|Y_{s-}{|}^{p-2}dR_{s}+p{\int _{t}^{T}}Y_{s}|Y_{s}{|}^{p-2}f(s,Y_{s},Z_{s},V_{s})ds\\{} & \displaystyle \hspace{2em}-p{\int _{t}^{T}}Y_{s-}|Y_{s-}{|}^{p-2}dM_{s}-p{\int _{t}^{T}}Y_{s}|Y_{s}{|}^{p-2}Z_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t}^{T}}\int _{U}Y_{s-}|Y_{s-}{|}^{p-2}V_{s}(e)\hspace{0.1667em}\widehat{\pi }(de,ds).\end{array}\](46)
\[ Y_{s}f(s,Y_{s},Z_{s},V_{s})\le \frac{{L}^{2}}{\epsilon }|Y_{s}{|}^{2}+|Y_{s}|f_{s}+\frac{\epsilon }{2}|Z_{s}{|}^{2}+\frac{\epsilon }{2}\int _{U}{\big|V_{s}(e)\big|}^{2}\lambda (de).\](47)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle |Y_{t}{|}^{p}+\frac{\alpha _{p}}{2}{\int _{t}^{T}}|Y_{s}{|}^{p-2}|Z{|_{s}^{2}}ds+\alpha _{p}{\int _{t}^{T}}\int _{U}|Y_{s}{|}^{p-2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\\{} & \displaystyle \hspace{2em}+\alpha _{p}{\int _{t}^{T}}|Y_{s}{|}^{p-2}d[M]_{s}\\{} & \displaystyle \hspace{1em}\le |\xi {|}^{p}+\frac{p{L}^{2}}{\alpha _{p}}{\int _{t}^{T}}|Y_{s}{|}^{p}ds+p{\int _{t}^{T}}|Y_{s}{|}^{p-1}f_{s}ds+p{\int _{t}^{T}}|Y_{s-}{|}^{p-1}dR_{s}\\{} & \displaystyle \hspace{2em}+\frac{\alpha _{p}}{2}{\int _{t}^{T}}|Y_{s}{|}^{p-2}\big\| V_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}ds-p{\int _{t}^{T}}Y_{s}|Y_{s}{|}^{p-2}Z_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t}^{T}}\int _{U}Y_{s-}|Y_{s-}{|}^{p-2}V_{s}(e)\hspace{0.1667em}\widehat{\pi }(de,ds)-p{\int _{t}^{T}}Y_{s-}|Y_{s-}{|}^{p-2}dM_{s}.\end{array}\]It follows from the BDG inequality that $\varUpsilon _{t}$, $\varTheta _{t}$, and $\varGamma _{t}$ are uniformly integrable martingales. Indeed, by Young’s inequality we have
and
The claim holds since the last terms of (48), (49), and (50) are finite. This is due to the fact that $Y\in {\mathcal{S}}^{p}$, which implies by the first step of the proof that $Z\in {\mathcal{M}}^{p}$, $V\in {\mathcal{L}}^{p}$, and $M\in {\mathbb{M}}^{p}$. Moreover, we have
Hence, in view of (51), taking the expectation in (47) yields
(48)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathbb{E}\big({[\varUpsilon ]_{T}^{\frac{1}{2}}}\big)& \displaystyle \le \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p-1}{\Bigg({\int _{0}^{T}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{1}{2}}\Bigg]\\{} & \displaystyle \le \frac{p-1}{p}\mathbb{E}\Big(\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\Big)+\frac{1}{p}\mathbb{E}{\Bigg({\int _{0}^{T}}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}},\end{array}\](49)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathbb{E}\big({[\varTheta ]_{T}^{\frac{1}{2}}}\big)& \displaystyle \le \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p-1}{\Bigg({\int _{0}^{T}}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{1}{2}}\Bigg]\\{} & \displaystyle \le \frac{p-1}{p}\mathbb{E}\Big(\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\Big)+\frac{1}{p}\mathbb{E}{\Bigg({\int _{0}^{T}}\big\| V_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}ds\Bigg)}^{\frac{p}{2}},\end{array}\](50)
\[ \mathbb{E}\big({[\varGamma ]_{T}^{\frac{1}{2}}}\big)\le \mathbb{E}\Big[\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p-1}{[M]_{T}^{\frac{1}{2}}}\Big]\le \frac{p-1}{p}\mathbb{E}\Big(\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\Big)+\frac{1}{p}\mathbb{E}{[M]_{T}^{\frac{p}{2}}}.\](51)
\[ \mathbb{E}{\int _{t}^{T}}\int _{U}|Y_{s}{|}^{p-2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)=\mathbb{E}{\int _{t}^{T}}|Y_{s}{|}^{p-2}\big\| V_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}ds.\](52)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \frac{\alpha _{p}}{2}\mathbb{E}{\int _{t}^{T}}|Y_{s}{|}^{p-2}|Z{|_{s}^{2}}ds+\frac{\alpha _{p}}{2}\mathbb{E}{\int _{t}^{T}}|Y_{s}{|}^{p-2}\big\| V_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}ds\\{} & \displaystyle \hspace{2em}+\alpha _{p}\mathbb{E}{\int _{t}^{T}}|Y_{s}{|}^{p-2}d[M]_{s}\\{} & \displaystyle \hspace{1em}\le \mathbb{E}[X].\end{array}\]Furthermore, coming back to (47), we deduce in view of (52) that
The BDG inequality implies that
and
Thus, combining estimates (54)–(56) with (52), we deduce that
But, applying Young’s inequality, we get
This, combined with (34), ends the proof. □
(53)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathbb{E}\underset{s\in [t,T]}{\sup }|Y_{s}{|}^{p}& \displaystyle \le 2\mathbb{E}X+p\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }\Bigg|{\int _{s}^{T}}\int _{U}Y_{{u}^{-}}|Y_{{u}^{-}}{|}^{p-2}V_{u}(e)\widehat{\pi }(de,du)\Bigg|\Bigg)\\{} & \displaystyle \hspace{1em}+p\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }\Bigg|{\int _{s}^{T}}Y_{u}|Y_{u}{|}^{p-2}Z_{u}dW_{u}\Bigg|\Bigg)\\{} & \displaystyle \hspace{1em}+p\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }\Bigg|{\int _{s}^{T}}Y_{{u}^{-}}|Y_{{u}^{-}}{|}^{p-2}dM_{u}\Bigg|\Bigg).\end{array}\](54)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle p\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }\Bigg|{\int _{s}^{T}}Y_{u}|Y_{u}{|}^{p-2}Z_{u}dW_{u}\Bigg|\Bigg)\\{} & \displaystyle \hspace{1em}\le d_{p}\mathbb{E}\Bigg[{\Bigg({\int _{t}^{T}}\hspace{0.1667em}|Y_{s}{|}^{2p-2}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{1}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\underset{s\in [t,T]}{\sup }|Y_{s}{|}^{p}+4{d_{p}^{2}}\mathbb{E}\Bigg({\int _{t}^{T}}\hspace{0.1667em}|Y_{s}{|}^{p-2}|Z_{s}{|}^{2}du\Bigg),\end{array}\](55)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle p\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }\Bigg|{\int _{s}^{T}}\int _{U}Y_{{u}^{-}}|Y_{{u}^{-}}{|}^{p-2}V_{u}(e)\widehat{\pi }(de,du)\Bigg|\Bigg)\\{} & \displaystyle \hspace{1em}\le d_{p}\mathbb{E}{\Bigg({\int _{t}^{T}}\int _{U}|Y_{u}{|}^{2p-2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\Bigg)}^{\frac{1}{2}}\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\underset{s\in [t,T]}{\sup }|Y_{s}{|}^{p}+4{d_{p}^{2}}\mathbb{E}\Bigg({\int _{t}^{T}}\hspace{0.1667em}|Y_{u}{|}^{p-2}\big\| V(e)_{u}{\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}du\Bigg),\end{array}\](56)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle p\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }\Bigg|{\int _{s}^{T}}Y_{{u}^{-}}|Y_{{u}^{-}}{|}^{p-2}dM_{u}\Bigg|\Bigg)\\{} & \displaystyle \hspace{1em}\le d_{p}\mathbb{E}{\big(|Y_{s}{|}^{2p-2}d[M]_{s}\big)}^{\frac{1}{2}}\\{} & \displaystyle \hspace{1em}\le \frac{1}{4}\mathbb{E}\underset{s\in [t,T]}{\sup }|Y_{s}{|}^{p}+4{d_{p}^{2}}\mathbb{E}\Bigg({\int _{t}^{T}}\hspace{0.1667em}|Y_{s}{|}^{p-2}d[M]_{s}\Bigg).\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}\displaystyle pC_{p}\mathbb{E}{\int _{t}^{T}}\hspace{0.1667em}|Y_{s}{|}^{p-1}|f_{s}|ds& \displaystyle \le pC_{p}\mathbb{E}\Bigg(\underset{s\in [t,T]}{\sup }|Y_{t}{|}^{p-1}{\int _{t}^{T}}f_{s}ds\Bigg)\\{} & \displaystyle \le \frac{1}{6}\mathbb{E}\underset{s\in [t,T]}{\sup }|Y_{t}{|}^{p}+{d^{\prime }_{p}}\mathbb{E}{\Bigg({\int _{t}^{T}}f_{s}ds\Bigg)}^{p},\end{array}\]
and
\[ pC_{p}\mathbb{E}{\int _{t}^{T}}\hspace{0.1667em}|Y_{s-}{|}^{p-1}dR_{s}\le \frac{1}{6}E\underset{s\in [t,T]}{\sup }|Y_{t}{|}^{p}+{d^{\prime\prime }_{p}}\mathbb{E}{\Bigg({\int _{t}^{T}}d|R|_{s}\Bigg)}^{p}.\]
Consequently, rearranging (57) in view of the two last estimates implies
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathbb{E}\underset{s\in [t,T]}{\sup }|Y_{s}{|}^{p}& \displaystyle \le {C^{\prime }_{p}}\mathbb{E}\Bigg[|\xi {|}^{p}+{\Bigg({\int _{t}^{T}}f_{s}ds\Bigg)}^{p}+{\Bigg({\int _{t}^{T}}d|R|_{s}\Bigg)}^{p}\Bigg]\\{} & \displaystyle \hspace{1em}+{C^{\prime\prime }_{p}}{\int _{t}^{T}}\mathbb{E}\underset{u\in [s,T]}{\sup }|Y_{u}{|}^{p}ds,\hspace{8.53581pt}t\in [0,T].\end{array}\]
Finally, using Gronwall’s lemma, we deduce that
(58)
\[ \mathbb{E}\underset{t\in [0,T]}{\sup }|Y_{t}{|}^{p}\le {C^{\prime }_{p}}{e}^{{C^{\prime\prime }_{p}}T}\mathbb{E}\Bigg[|\xi {|}^{p}+{\Bigg({\int _{0}^{T}}f_{s}ds\Bigg)}^{p}+{\Bigg({\int _{0}^{T}}d|R|_{s}\Bigg)}^{p}\Bigg].\]Lemma 5.
Let $(\xi ,f,R)$ and $({\xi ^{\prime }},{f^{\prime }},{R^{\prime }})$ be two sets of data, each satisfying assumptions $(H1)$–$(H6)$. Let $(Y,Z,V,M)$ and $({Y^{\prime }},{Z^{\prime }},{V^{\prime }},{M^{\prime }})$ denote respectively an ${\mathbb{L}}^{p}$-solution of GRBSDE (1) with data $(\xi ,f,R)$ and $({\xi ^{\prime }},{f^{\prime }},{R^{\prime }})$. Define
\[ (\bar{Y},\bar{Z},\bar{V},\bar{M},\bar{\xi },\bar{f},\bar{R})=\big(Y-{Y^{\prime }},Z-{Z^{\prime }},V-{V^{\prime }},M-{M^{\prime }},\xi -{\xi ^{\prime }},f-{f^{\prime }},R-{R^{\prime }}\big).\]
Then there exists a constant $C>0$, depending on p and T, such that, for every $a\ge \mu +2{L}^{2}$,
(59)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }{e}^{apt}|\bar{Y}_{t}{|}^{p}+{\Bigg({\int _{0}^{T}}{e}^{2at}|\bar{Z}_{t}{|}^{2}dt\Bigg)}^{\frac{p}{2}}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{T}}\int _{U}{e}^{2at}|\bar{V}_{t}{|}^{2}\lambda (de)dt\Bigg)}^{\frac{p}{2}}+{e}^{apT}{[\bar{M}]_{T}^{\frac{p}{2}}}\Bigg]\\{} & \displaystyle \hspace{1em}\le \hspace{0.1667em}C\mathbb{E}\Bigg[{e}^{apT}|\bar{\xi }{|}^{p}+{\Bigg({\int _{0}^{T}}{e}^{at}\big|\bar{f}\big(s,{Y^{\prime }_{t}},{Z^{\prime }_{t}},{V^{\prime }_{t}}\big)\big|dt\Bigg)}^{p}+{\Bigg({\int _{0}^{T}}{e}^{at}d|\bar{R}|_{t}\Bigg)}^{p}\Bigg].\end{array}\]Proof.
By an already used change-of-variable argument we may assume that $a=0$. Obviously, $(\bar{Y},\bar{Z},\bar{V},\bar{M})$ solves the following GBSDE in ${\varXi }^{p}$:
It follows from $(H3)$, $(H5)$, and $(H6)$ that
which means that assumption $(A)$ is satisfied for the generator of GBSDE (60), with $f_{t}\equiv |\bar{f}(t,{y^{\prime }},{z^{\prime }},{v^{\prime }})|$. Thus, by Lemma 4 the desired estimate follows, which ends the proof of Lemma 5. □
(60)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \bar{Y}_{t}& \displaystyle =\bar{\xi }+{\int _{t}^{T}}\big(f(s,Y_{s},Z_{s},V_{s})-{f^{\prime }}\big(s,{Y^{\prime }_{s}},{Z^{\prime }_{s}},{V^{\prime }_{s}}\big)\big)ds+{\int _{t}^{T}}d\bar{R}_{s}-{\int _{t}^{T}}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}\bar{V}_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}d\bar{M}_{s},\hspace{8.53581pt}t\in [0,T].\end{array}\](61)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \widehat{\operatorname{sgn}}(\bar{y})\big(f(t,y,z,v)-{f^{\prime }}\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\big)\\{} & \displaystyle \hspace{1em}=\widehat{\operatorname{sgn}}(\bar{y})\big(f(t,y,z,v)-f\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\big)+\widehat{\operatorname{sgn}}(\bar{y})\bar{f}\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\\{} & \displaystyle \hspace{1em}=\widehat{\operatorname{sgn}}(\bar{y})\big[f(t,y,z,v)-f\big(t,{y^{\prime }},z,v\big)+f\big(t,{y^{\prime }},z,v\big)-f\big(t,{y^{\prime }},{z^{\prime }},v\big)\\{} & \displaystyle \hspace{2em}+f\big(t,{y^{\prime }},{z^{\prime }},v\big)-f\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\big]+\widehat{\operatorname{sgn}}(\bar{y})\bar{f}\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\\{} & \displaystyle \hspace{1em}\le \big|\bar{f}\big(t,{y^{\prime }},{z^{\prime }},{v^{\prime }}\big)\big|+\mu |y|+L|z|+L\| v\| _{{\mathcal{L}_{\lambda }^{2}}},\end{array}\]Now we are able to give the main result of this subsection, the existence and uniqueness of an ${L}^{p}$-solution of GBSDE (1) in the case $p\ge 2$.
Theorem 2.
Let $p\ge 2$ and assume that $(H1)$–$(H6)$ hold. Then, there exists a unique ${\mathbb{L}}^{p}$-solution $(Y,Z,V,M)$ for the GBSDE (1).
Proof.
Uniqueness follows immediately from Lemma 5. Now we deal with the existence. Set $T_{n}(x)=\frac{xn}{|x|\vee n}$ for $n\in {\mathbb{N}}^{\ast }$ and define $\xi _{n}$, $f_{n}$, and ${R}^{n}$ as follows:
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \xi _{n}& \displaystyle =T_{n}(\xi ),\hspace{2em}f_{n}(t,y,z,v)=f(t,y,z,v)-f(t,0,0,0)+T_{n}\big(f(t,0,0,0)\big),\\{} \displaystyle {R_{t}^{n}}& \displaystyle ={\int _{0}^{t}}\mathbb{1}_{\{|R|_{s}\le n\}}dR_{s}.\end{array}\]
Let $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ be a solution of GBSDE (1) associated with $(\xi _{n},f_{n}+dR_{n})$. Hence, by Theorem 1, for every $n\in \mathbb{N}$, there exists a unique solution to $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})\in {\varXi }^{2}$ of GBSDE (1) associated with $({\xi }^{n},f_{n}+d{R}^{n})$, but in fact also in ${\varXi }^{p}$, $p\ge 2$, according to Lemma 4. Our goal now is to show that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence in ${\varXi }^{p}$. For $m\ge n$, applying Lemma 5 yields
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\in [0,T]}{\sup }{\big|{Y_{t}^{m}}-{Y_{t}^{n}}\big|}^{2}+{\Bigg({\int _{0}^{T}}{\big|{Z_{t}^{m}}-{Z_{t}^{n}}\big|}^{2}dt\Bigg)}^{\frac{p}{2}}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{T}}\int _{U}{\big|{V_{t}^{m}}(e)-{V_{t}^{n}}(e)\big|}^{2}\lambda (de)dt\Bigg)}^{\frac{p}{2}}+{\big[{M}^{m}-{M}^{n}\big]_{T}^{\frac{p}{2}}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg[|\xi _{m}-\xi _{n}{|}^{p}+{\Bigg({\int _{0}^{T}}\big|T_{m}\big(f(t,0,0,0)\big)-T_{n}\big(f(t,0,0,0)\big)\big|dt\Bigg)}^{p}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{T}}d\big|{R}^{m}-{R}^{n}\big|_{s}\Bigg)}^{p}\Bigg].\end{array}\]
Therefore, letting n and m to infinity, we conclude that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence in ${\varXi }^{p}$ and its limit $(Y,Z,V,M)\in {\varXi }^{p}$ is a solution of GBSDE (1) associated with $(\xi ,f+dR)$, which ends the proof. □4 Comparison theorem
In this section, we assume that $k=1$ and aim at showing a comparison theorem for GBSDE. Our result, in particular, extends to the case of generalized BSDEs in a general filtration the comparison theorem given in [9, Prop. 4]. We follow the argument of [16]. In particular, we consider the Doléans–Dade exponential local martingale. Let α, β be predictable processes integrable w.r.t. $dt$ and $dW_{t}$, respectively. Let γ be a predictable process defined on $[0,T]\times \varOmega \times \mathbb{R}$ integrable w.r.t. $\widehat{\pi }(de,ds)$. For any $0\le t\le s\le T$, let E be the solution of
Of course, $\varGamma _{t,s}=\exp ({\int _{t}^{s}}\alpha _{r}dr)E_{t,s}$, and
\[ dE_{t,s}=E_{t,s-}\bigg[\beta _{s}dW_{s}+\int _{U}\gamma _{s}(e)\widehat{\pi }(de,ds)\bigg],\hspace{1em}E_{t,t}=1,\]
and let Γ be the solution of
(62)
\[ d\varGamma _{t,s}=\varGamma _{t,s-}\bigg[\alpha _{s}ds+\beta _{s}dW_{s}+\int _{U}\gamma _{s}(e)\widehat{\pi }(de,ds)\bigg],\hspace{1em}\varGamma _{t,t}=1.\]
\[ E_{t,s}=\exp \Bigg({\int _{t}^{s}}\beta _{r}dW_{r}-\frac{1}{2}{\int _{t}^{s}}{\beta _{r}^{2}}dr\Bigg)\prod \limits_{t<r\le s}\big(1+\gamma _{r}(\Delta X_{r})\big){e}^{-\gamma _{r}(\Delta X_{r})},\]
with $X_{t}={\int _{0}^{t}}\int _{U}u\pi (du,ds)$.Note that, classically, if $\gamma _{t}(e)\ge -1,\hspace{2.5pt}d\mathbb{P}\otimes ds\otimes d\lambda (e)$-a.s., then $\varGamma _{t,.}\ge 0$ a.s. (see [16, Prop. 3.1]).
We make the following monotonicity assumption on f w.r.t. v
-
$(H{6^{\prime }})$ For each $(y,z,v,{v^{\prime }})\in \mathbb{R}\times {\mathbb{R}}^{d}\times {({\mathcal{L}_{\lambda }^{2}})}^{2}$, there exists a predictable process $\kappa ={\kappa }^{y,z,v,{v^{\prime }}}:\varOmega \times [0,T]\times U\to \mathbb{R}$ satisfying:\[ f(t,y,z,v)-f\big(t,y,z,{v^{\prime }}\big)\le \int _{U}\big(v(e)-{v^{\prime }}(e)\big){\kappa _{t}^{y,z,v,{v^{\prime }}}}(e)\lambda (de),\]$\mathbb{P}\otimes \mathit{Leb}\otimes \lambda $-a.e.
We begin by showing that a linear GBSDE with jumps can be written as a conditional expectation via an exponential semimartingale. This result will be used to prove the comparison theorem.
Lemma 6.
Assume that $|\beta |$ is bounded and α is bounded from above. Suppose also that, $d\mathbb{P}\otimes dt\otimes \lambda (de)$-a.s.,
and
Let $(f_{t})_{0\le t\le T}$ be a real-valued progressively measurable process, and let $(Y,Z,V,M)$ be the solution of the linear GBSDE
Then, $\mathbb{E}\sup _{s\in [t,T]}|\varGamma _{t,s}{|}^{p}<+\infty $, and if
then the solution $(Y,Z,V,M)$ belongs to ${\varXi }^{p}$.
(64)
\[ \big|\gamma _{t}(e)\big|\le \vartheta (e),\hspace{2.5pt}\hspace{2.5pt}\textit{where}\hspace{2.5pt}\vartheta \in {\mathcal{L}_{\lambda }^{2}}.\](65)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle Y_{t}& \displaystyle =\xi +{\int _{t}^{T}}\bigg[f_{s}+\alpha _{s}Y_{s}+\beta _{s}Z_{s}+\int _{U}\gamma _{s}(u)V_{s}(e)\lambda (de)\bigg]ds+{\int _{t}^{T}}dR_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{T}}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)-{\int _{t}^{T}}Z_{s}dW_{s}-{\int _{t}^{T}}dM_{s}.\end{array}\](66)
\[ \mathbb{E}\Bigg[|\xi {|}^{p}+{\Bigg({\int _{0}^{T}}|f_{s}|ds\Bigg)}^{p}+|R{|_{T}^{p}}\Bigg]<+\infty ,\]Proof.
We first show that $\mathbb{E}\sup _{s\in [t,T]}|\varGamma _{t,s}{|}^{p}<+\infty $. Indeed, by (63), as mentioned previously, it follows that $\varGamma _{t,.}\ge 0$. Combining this with (64), using the fact that $|\beta |$ is bounded and α is bounded from above, and applying [16, Prop. A.1] yield that Γ is p-integrable, that is, $\mathbb{E}|\varGamma _{t,T}{|}^{p}<+\infty $. Hence, using Doob’s inequality, we have that
as desired.
Next, let us show that $(Y,Z,V,M)$ belongs to ${\varXi }^{p}$. Clearly, thanks to the assumptions made on α, β, and γ and the fact $(H{6^{\prime }})$ implies $(H6)$, we can easily see that the generator of the linear GBSDE (65) satisfies assumptions $(H3)$, $(H5)$, and $(H6)$. Thus, in view of this and (66), applying Lemma (4) yields the claim.
It remains to show that $(Y_{t})$ satisfies (67). Indeed, by the Itô product formula we obtain
In view of the boundedness assumptions made on the coefficients β and γ, combined with estimate (68) and the fact that $(Y,Z,V,M)\in {\varXi }^{p}$, it follows that the local martingale N is a uniformly integrable martingale. Therefore, taking the conditional expectation w.r.t. $\mathcal{F}_{t}$ in (69), we obtain
as desired. This ends the proof. □
\[\begin{array}{r@{\hskip0pt}l}\displaystyle d(Y_{s}\varGamma _{t,s})& \displaystyle =\varGamma _{t,s-}dY_{s}+Y_{s-}d\varGamma _{t,s}+d[\varGamma _{t,.},Y]_{s}\\{} & \displaystyle =\varGamma _{t,s-}\bigg(-f_{s}-\alpha _{s}Y_{s}-\beta _{s}Z_{s}-\int _{U}\gamma _{s}(u)V_{s}(u)\lambda (de)\bigg)ds-\varGamma _{t,s-}dR_{s}\\{} & \displaystyle \hspace{1em}+\varGamma _{t,s-}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)+\varGamma _{t,s-}Z_{s}dW_{s}+\varGamma _{t,s-}dM_{s}\\{} & \displaystyle \hspace{1em}+Y_{s-}\varGamma _{t,s-}\bigg(\alpha _{s}ds+\beta _{s}dW_{s}+\int _{U}\gamma _{s}(u)\widehat{\pi }(de,ds)\bigg)\\{} & \displaystyle \hspace{1em}+\varGamma _{t,s-}\beta _{s}Z_{s}ds+\varGamma _{t,s-}\int _{U}V_{s}(e)\gamma _{s}(u)\pi (de,ds)\\{} & \displaystyle =-\varGamma _{t,s}f_{s}ds-\varGamma _{t,s-}dR_{s}+dN_{s},\end{array}\]
with
\[\begin{array}{r@{\hskip0pt}l}\displaystyle dN_{s}& \displaystyle =\varGamma _{t,s-}\int _{U}\big(V_{s}(e)+Y_{s-}\gamma _{s}(e)+V_{s}(e)\gamma _{s}(e)\big)\widehat{\pi }(de,ds)\\{} & \displaystyle \hspace{1em}+\varGamma _{t,s-}(Z_{s}+Y_{s}\beta _{s})dW_{s}+\varGamma _{t,s-}dM_{s}.\end{array}\]
Integrating between t and T yields
(69)
\[ \xi \varGamma _{t,T}-Y_{t}=-{\int _{t}^{T}}\varGamma _{t,s}f_{s}ds-{\int _{t}^{T}}\varGamma _{t,s-}dR_{s}+{\int _{t}^{T}}dN_{s}\hspace{1em}\text{a.s.}\]Proposition 1.
We consider two sets of data $(\xi _{1},f_{1}+dR_{1})$ and $(\xi _{2},f_{2}+dR_{2})$ such that $\xi _{1}$, $\xi _{2}$, $R_{1}$, and $R_{2}$ satisfy $(H1)$. Moreover, we assume that $f_{1}$ and $f_{2}$ satisfy, respectively, $(H1)$–$(H6)$ and $(H1)$–$(H5)$, $(H{6^{\prime }})$. Let $({Y}^{1},{Z}^{1},{V}^{1},{M}^{1})$ and $({Y}^{2},{Z}^{2},{V}^{2},{M}^{2})$ be respectively solutions of GBSDEs (1) associated with $(\xi _{1},f_{1}+dR_{1})$ and $(\xi _{2},f_{2}+dR_{2})$ in some space ${\varXi }^{p}$ with $p\ge 2$. If ${\xi }^{1}\le {\xi }^{2}$, $f_{1}(t,{Y_{t}^{1}},{Z_{t}^{1}},{V_{t}^{1}})\le f_{2}(t,{Y_{t}^{1}},{Z_{t}^{1}},{V_{t}^{1}})$, and for a.e. t, $d{R}^{1}\le d{R}^{2}$, then a.s. ${Y_{t}^{1}}\le {Y_{t}^{2}}$ for any $t\in [0,T]$.
Proof.
Put
since $f_{2}$ satisfies $(H{6^{\prime }})$. Moreover, since $f_{2}$ is Lipschitz continuous w.r.t. z, $|\beta |$ is bounded by L, whereas, by Assumption $(H3)$, α is bounded from above. Moreover, the process ${\kappa _{s}^{{Y_{s}^{2}},{Z_{s}^{2}},{V_{s}^{1}},{V_{s}^{2}}}}$ is controlled by $\vartheta \in {\mathcal{L}_{\lambda }^{2}}$. Note that, since $-1\le {\kappa _{t}^{y,z,\psi ,\phi }}(e)$, it follows that $\varGamma _{t,.}\ge 0$ a.s. Furthermore, in view of the above, we have from Lemma 6 that $\varGamma _{t,.}\in {\mathcal{S}}^{p}$.
\[ \overline{Y}={Y}^{2}-{Y}^{1},\hspace{1em}\overline{Z}={Z}^{2}-{Z}^{1},\hspace{1em}\overline{V}={V}^{2}-{V}^{1},\hspace{1em}\overline{M}={M}^{2}-{M}^{1},\hspace{1em}\overline{R}={R}^{2}-{R}^{1}.\]
Then $(\overline{Y},\overline{Z},\overline{V},\overline{M})$ satisfies
\[ \overline{Y}_{t}=\overline{\xi }+{\int _{t}^{T}}h_{s}ds+{\int _{t}^{T}}d\overline{R}_{s}-{\int _{t}^{T}}\int _{U}\overline{\psi }_{s}(u)\widehat{\pi }(de,ds)-{\int _{t}^{T}}\overline{Z}_{s}dW_{s}-{\int _{t}^{T}}d\overline{M}_{s},\]
where
\[ h_{s}=f_{2}\big({Y_{s}^{2}},{Z_{s}^{2}},{\psi _{s}^{2}}\big)-f_{1}\big({Y_{s}^{1}},{Z_{s}^{1}},{\psi _{s}^{1}}\big).\]
Now we define
\[\begin{array}{r@{\hskip0pt}l}\displaystyle f_{s}& \displaystyle =f_{2}\big({Y_{s}^{1}},{Z_{s}^{1}},{\psi _{s}^{1}}\big)-f_{1}\big({Y_{s}^{1}},{Z_{s}^{1}},{\psi _{s}^{1}}\big),\\{} \displaystyle \alpha _{s}& \displaystyle =\frac{f_{2}({Y_{s}^{2}},{Z_{s}^{1}},{\psi _{s}^{1}})-f_{2}({Y_{s}^{1}},{Z_{s}^{1}},{\psi _{s}^{1}})}{\overline{Y}_{s}}\mathbb{1}_{\overline{Y}_{s}\ne 0},\\{} \displaystyle \beta _{s}& \displaystyle =\frac{f_{2}({Y_{s}^{2}},{Z_{s}^{2}},{\psi _{s}^{1}})-f_{2}({Y_{s}^{2}},{Z_{s}^{1}},{\psi _{s}^{1}})}{\overline{Z}_{s}}\mathbb{1}_{\overline{Z}_{s}\ne 0}.\end{array}\]
Then
(70)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle h_{s}& \displaystyle =f_{s}+\alpha _{s}\overline{Y}_{s}+\beta _{s}\overline{Z}_{s}+f_{2}\big({Y_{s}^{2}},{Z_{s}^{2}},{V_{s}^{2}}\big)-f_{2}\big({Y_{s}^{2}},{Z_{s}^{2}},{V_{s}^{1}}\big)\\{} & \displaystyle \ge f_{s}+\alpha _{s}\overline{Y}_{s}+\beta _{s}\overline{Z}_{s}+\int _{U}{\kappa _{s}^{{Y_{s}^{2}},{Z_{s}^{2}},{V_{s}^{1}},{V_{s}^{2}}}}\overline{V}_{s}(u)\lambda (de),\end{array}\]Now applying Itô’s formula to $\bar{Y}_{s}\varGamma _{t,s}$ for $s\in [t,T]$ and then using inequality (70) together with the non negativity of Γ, we can derive, by doing the same computations as in the proof of Lemma 6, that
where N is a local martingale. Next, applying Lemma 5 yields that $(\bar{Y},\bar{Z},\bar{V},\bar{M})$ belongs to ${\varXi }^{p}$. Since $\varGamma _{t,.}\in {\mathcal{S}}^{p}$, this, combined with the boundedness of β and ${\kappa _{t}^{y,z,\psi ,\phi }}(e)$, implies that N is in fact a martingale.
(71)
\[ -d(\bar{Y}_{s}\varGamma _{t,s})\ge \varGamma _{t,s}f_{s}ds+\varGamma _{t,s-}d\bar{R}_{s}-dN_{s},\]Therefore, integrating between t and T in (71) and then taking the conditional expectation w.r.t. $\mathcal{F}_{t}$, we deduce
\[ \overline{Y}_{t}\ge \mathbb{E}\Bigg[\varGamma _{t,T}\overline{\xi }+{\int _{t}^{T}}\varGamma _{t,s}f_{s}ds+{\int _{t}^{T}}\varGamma _{t,s-}d\overline{R}_{s}\Big|\mathcal{F}_{t}\Bigg],\hspace{1em}t\in [0,T],\hspace{2.5pt}\text{a.s.}\]
To conclude, recall that $\varGamma _{t,s}\ge 0$ a.s. and, by assumptions, $\overline{\xi }\ge 0$, $f_{s}\ge 0$, and ${\int _{t}^{T}}d\overline{R}_{s}\ge 0$. Consequently, it follows that, for all $t\in [0,T]$, $\overline{Y}_{t}\ge 0$ a.s. Since ${Y}^{1}$ and ${Y}^{2}$ are càdlàg processes, we obtain that ${Y_{t}^{1}}\le {Y_{t}^{2}}$ a.s., and the conclusion follows. □Notice that assumptions $(H1)$–$(H6)$ made on $f_{1}$ are imposed only to ensure the existence of a solution $({Y}^{1},{Z}^{1},{V}^{1},{M}^{1})$. The following corollary, which follows immediately from Proposition 1, gives again a uniqueness result for GBSDE (1) in ${\varXi }^{p}$ in dimension 1.
Corollary 1.
Let $p\ge 2$ and assume $(H1)$–$(H5)$ and $(H{6^{\prime }})$. Then there exists at most one solution $(Y,Z,V,M)$ to GBSDE (1) in ${\varXi }^{p}$.
5 Generalized BSDEs with random terminal time
In this section, we study the issue of existence and uniqueness of ${\mathbb{L}}^{p}(p\ge 2)$-solutions of GBSDEs with random terminal time. We follow the approach in [14, Section 4]. Let τ be an $\mathcal{F}$-stopping time, not necessarily bounded. Assumptions considered in the case of GBSDE with constant time (precisely, $(H2)$, $(H3)$, $(H5)$, and $(H6)$) still hold except for $(H4)$ and $(H1)$, for which we give the analogues for $p\ge 2$:
-
$(H{4^{\prime }})$ $\forall r>0$, $\forall n\in \mathbb{N}$, the mapping $t\in [0,T]\to \sup _{|y|\le r}|f(t,y,0,0)-f(t,0,0,0)|$ belongs to ${\mathbb{L}}^{1}(\varOmega \times (0,n))$.
-
$(H{1^{\prime }})$ For some $\rho \in \mathbb{R}$ such that $\rho >\nu :=\mu +\frac{2p{L}^{2}}{\alpha _{p}}$, where $\alpha _{p}=\min (\frac{p}{2},p(p-1){3}^{1-p})$,
Finally, we will need the following additional assumption on ξ and f:
$(H7)$ ξ is $\mathcal{F}_{\tau }$-measurable, and $\mathbb{E}[{({\int _{0}^{\tau }}{e}^{\rho \tau }|f(t,\xi _{t},\eta _{t},\gamma _{t})|ds)}^{p}]<+\infty $, where $\xi _{t}=\mathbb{E}(\xi |\mathcal{F}_{t})$ and $(\eta ,\gamma ,N)$ are given by the martingale representation
\[ \xi =\mathbb{E}(\xi )+{\int _{0}^{+\infty }}\eta _{s}dW_{s}+{\int _{0}^{+\infty }}\int _{U}\gamma _{s}(e)\widehat{\pi }(de,ds)+N_{\tau },\]
with N orthogonal to W and $\widetilde{\pi }$. Moreover, the following holds:
Next, let us make precise the notion of a solution of GBSDE with random terminal time.
Definition 2.
We say that a quadruple $(Y,Z,V,M)\in \mathcal{S}\times \mathcal{H}(0,T)\times \mathcal{P}\times \mathbb{M}_{\mathit{loc}}$ with values in ${\mathbb{R}}^{k}\times {\mathbb{R}}^{k\times d}\times {\mathbb{R}}^{k}\times {\mathbb{R}}^{k}$ is a solution of GBSDE (1) with random terminal time τ and data $(\xi ,f+dR)$ if
Furthermore, a solution is said to be ${\mathbb{L}}^{p}$ if we have
-
• on $\{t\ge \tau \}$, $Y_{t}=\xi $ and $Z_{t}=V_{t}=M_{t}=0$, $\mathbb{P}$-a.s.,
-
• $t\to f(t,Y_{t},Z_{t},V_{t})\mathbb{1}_{\{t\le \tau \}}\in {L}^{1}(0,+\infty )$, $Z\in {\mathbb{L}_{\mathit{loc}}^{2}}(W)$, $V\in G_{\mathit{loc}}(\pi )$, and
-
• $\mathbb{P}$-a.s., for all $t\in [0,T]$,
(73)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle Y_{t\wedge \tau }& \displaystyle =Y_{T\wedge \tau }+{\int _{t\wedge \tau }^{T\wedge \tau }}f(s,Y_{s},Z_{s},V_{s})ds+{\int _{t\wedge \tau }^{T\wedge \tau }}dR_{s}-{\int _{t\wedge \tau }^{T\wedge \tau }}Z_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}V_{s}(e)\widehat{\pi }(de,ds)-{\int _{t\wedge \tau }^{T\wedge \tau }}dM_{s}.\end{array}\]
(74)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{e}^{p\rho (t\wedge \tau )}|Y_{t\wedge \tau }{|}^{p}+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p}ds+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p-2}|Z_{s}{|}^{2}ds\\{} & \displaystyle \hspace{2em}+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p-2}\| V_{s}{\| _{{L_{\lambda }^{2}}}^{2}}ds+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p-2}d[M]_{s}\Bigg]\\{} & \displaystyle \hspace{1em}<+\infty .\end{array}\]Proof.
Assume that there exist two solutions $(Y,Z,V,M)$ and $({Y^{\prime }},{Z^{\prime }},{V^{\prime }},{M^{\prime }})$ of GBSDE (73) that satisfy estimate (74). Set $(\bar{Y},\bar{Z},\bar{V},\bar{M})=(Y-{Y^{\prime }},Z-{Z^{\prime }},V-{V^{\prime }},M-{M^{\prime }})$.
Applying Itô’s formula, as in step 2 of Proposition 4, to ${e}^{p\rho s}|\bar{Y}_{s}{|}^{p}$ over the interval $[t\wedge \tau ,T\wedge \tau ]$, we obtain an analogue of (41)
where
The following estimates, which are analogues of (43) and (44), hold:
and
where $\alpha _{p}=\min (\frac{p}{2},p(p-1){3}^{1-p})$.
(75)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {e}^{p\rho (t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}\\{} & \displaystyle \hspace{1em}={e}^{p\rho (T\wedge \tau )}|\bar{Y}_{T\wedge \tau }{|}^{p}\\{} & \displaystyle \hspace{2em}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\big[\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\big(f(s,Y_{s},Z_{s},V_{s})-f\big(s,{Y^{\prime }_{s}},{Z^{\prime }_{s}},{V^{\prime }_{s}}\big)\big)-\rho |\bar{Y}_{s}{|}^{p}\big]ds\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}d\bar{M}_{s}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}{e}^{p\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}\bar{V}_{s}(e)\widehat{\pi }(de,ds)\\{} & \displaystyle \hspace{2em}-\frac{1}{2}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\operatorname{Trace}\big({D}^{2}\theta (\bar{Y}_{s})\bar{Z}_{s}{\bar{Z}_{s}^{t}}\big)ds\\{} & \displaystyle \hspace{2em}-{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}{e}^{p\rho s}\big({\big|\bar{Y}_{s-}+\bar{Y}_{s}(e)\big|}^{p}\\{} & \displaystyle \hspace{2em}-|\bar{Y}_{s-}{|}^{p}-p\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}\bar{Y}_{s}(e)\big)\pi (de,ds)-\mathrm{\aleph }_{t},\end{array}\](76)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathrm{\aleph }_{t}& \displaystyle =\frac{1}{2}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\sum \limits_{1\le i,j\le d}\frac{{\partial }^{2}\theta }{\partial y_{i}\partial y_{j}}(Y_{s})d{\big[{\bar{M}}^{i},{\bar{M}}^{j}\big]_{s}^{c}}\\{} & \displaystyle \hspace{1em}+\sum \limits_{t\wedge \tau <s\le T\wedge \tau }{e}^{p\rho s}\big(|\bar{Y}_{s-}+\Delta \bar{M}_{s}{|}^{p}-|\bar{Y}_{s-}{|}^{p}-pY_{s-}|\bar{Y}_{s-}{|}^{p-2}\Delta \bar{M}_{s}\big).\end{array}\](77)
\[ \mathrm{\aleph }_{t}\ge \alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s-}|d[\bar{M}]_{s},\](78)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle -{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}{e}^{p\rho s}\big({\big|\bar{Y}_{s-}+\bar{V}_{s}(e)\big|}^{p}-|\bar{Y}_{s-}{|}^{p}-p\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}\bar{Y}_{s}(e)\big)\pi (de,ds)\\{} & \displaystyle \hspace{1em}\le -p(p-1){3}^{1-p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s-}{|}^{p-2}{\big|\bar{Y}_{s}(e)\big|}^{2}\pi (de,ds),\end{array}\]Therefore, rearranging (75), in view of (42), (77), and (78) yields
But from the assumptions on f (using (46) with $\epsilon =\frac{\alpha _{p}}{p}$) and Young’s inequality we have that
Furthermore, observe that by the integrability conditions on the solution all the local martingales appearing in (79) are uniformly integrable. Moreover, the following holds:
Thus, taking the expectation in (79), we obtain, in view of the above, that
Note that the same result holds with ρ replaced by ${\rho ^{\prime }}$, with $\mu +\frac{{p}^{2}{L}^{2}}{{\alpha _{p}^{2}}}<{\rho ^{\prime }}<\rho $. Therefore, we have, for any $0\le t\le T$,
Consequently, letting $T\to +\infty $, we deduce in view of estimate (74) that $\bar{Y}_{t}=0$.
(79)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {e}^{p\rho (t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s}{|}^{p-2}|\bar{Z}_{s}{|}^{2}ds\\{} & \displaystyle \hspace{2em}+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\int _{U}|\bar{Y}_{s}{|}^{p-2}{\big|\bar{V}_{s}(e)\big|}^{2}\pi (de,ds)+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s-}|d[\bar{M}]_{s}\\{} & \displaystyle \hspace{1em}\le {e}^{p\rho (T\wedge \tau )}|\bar{Y}_{T\wedge \tau }{|}^{p}\\{} & \displaystyle \hspace{2em}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}\big[\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\big(f(s,Y_{s},Z_{s},V_{s})-f\big(s,{Y^{\prime }_{s}},{Z^{\prime }_{s}},{V^{\prime }_{s}}\big)\big)-\rho |\bar{Y}_{s}{|}^{p}\big]ds\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}d\bar{M}_{s}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}{e}^{\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}\bar{V}_{s}(e)\hspace{0.1667em}\widehat{\pi }(de,ds).\end{array}\](80)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\big(f(s,Y_{s},Z_{s},V_{s})-f\big(s,{Y^{\prime }_{s}},{Z^{\prime }_{s}},{V^{\prime }_{s}}\big)\big)-\rho |\bar{Y}_{s}{|}^{p}\\{} & \displaystyle \hspace{1em}\le \bigg(\mu +\frac{2p{L}^{2}}{\alpha _{p}}-\rho \bigg)|\bar{Y}_{s}{|}^{p}+\frac{\alpha _{p}}{p}|\bar{Y}_{s}{|}^{p-2}|\bar{Z}_{s}{|}^{2}+\frac{\alpha _{p}}{p}|\bar{Y}_{s}{|}^{p-2}\| \bar{V}_{s}{\| _{{\mathbb{L}_{\lambda }^{2}}}^{2}}\\{} & \displaystyle \hspace{1em}\le \frac{\alpha _{p}}{p}|\bar{Y}_{s}{|}^{p-2}|\bar{Z}_{s}{|}^{2}+\frac{\alpha _{p}}{p}|\bar{Y}_{s}{|}^{p-2}\| \bar{V}_{s}{\| _{{\mathbb{L}_{\lambda }^{2}}}^{2}}.\end{array}\](81)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\int _{U}|Y_{s}{|}^{p-2}{\big|V_{s}(e)\big|}^{2}\pi (de,ds)\\{} & \displaystyle \hspace{1em}=\mathbb{E}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\int _{U}|Y_{s}{|}^{p-2}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds.\end{array}\](82)
\[ \mathbb{E}{e}^{p\rho (t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}\le \mathbb{E}{e}^{p\rho (T\wedge \tau )}|\bar{Y}_{T\wedge \tau }{|}^{p}.\](83)
\[ \mathbb{E}{e}^{p{\rho ^{\prime }}(t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}\le {e}^{p({\rho ^{\prime }}-\rho )T}\mathbb{E}{e}^{p\rho (T\wedge \tau )}|\bar{Y}_{T\wedge \tau }{|}^{p}.\]Since $(Y,Z,V,M)$ and $({Y^{\prime }},{Z^{\prime }},{V^{\prime }},{M^{\prime }})$ satisfy GBSDE (73) with $Y={Y^{\prime }}$, then by the uniqueness of the Doob–Meyer decomposition of semimartingales it follows that $(Z,V,M)=({Z^{\prime }},{V^{\prime }},{M^{\prime }})$, whence the uniqueness of the solution of (73). □
Proposition 3.
Assume that $(H{1^{\prime }})$, $(H2)$, $(H3)$, $(H{4^{\prime }})$, $(H5)$, $(H6)$, and $(H7)$ are in force. Then, GBSDE (1) has a solution satisfying
Moreover,
for some constant $C>0$ depending only on p, L, and μ.
(84)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{t\ge 0}{\sup }{e}^{p\rho (t\wedge \tau )}|Y_{t\wedge \tau }{|}^{p}+{e}^{p\rho (t\wedge \tau )}|Y_{t\wedge \tau }{|}^{p}+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p}ds\\{} & \displaystyle \hspace{2em}+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p-2}|Z_{s}{|}^{2}ds+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s}{|}^{p-2}\| V_{s}{\| _{{L_{\lambda }^{2}}}^{2}}ds\\{} & \displaystyle \hspace{2em}+{\int _{0}^{T\wedge \tau }}{e}^{p\rho s}|Y_{s-}{|}^{p-2}d[M]_{s}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg[{e}^{p\rho \tau }|\xi {|}^{p}+{\Bigg({\int _{0}^{\tau }}{e}^{\rho \tau }\big|f(s,0,0,0)\big|ds\Bigg)}^{p}+{\Bigg({\int _{0}^{\tau }}{e}^{\rho \tau }d|R|_{s}\Bigg)}^{p}\Bigg].\end{array}\](85)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{\Bigg({\int _{0}^{\tau }}{e}^{2\rho s}|Z_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{\tau }}\int _{U}{e}^{2\rho s}{\big|V_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{\tau }}{e}^{2\rho s}d[M]_{s}\Bigg)}^{\frac{p}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}\Bigg[{e}^{p\rho \tau }|\xi {|}^{p}+{\Bigg({\int _{0}^{\tau }}{e}^{\rho \tau }\big|f(s,0,0,0)\big|ds\Bigg)}^{p}+{\Bigg({\int _{0}^{\tau }}{e}^{\rho \tau }d|R|_{s}\Bigg)}^{p}\Bigg],\end{array}\]Proof.
We follow the line of the argument of [14, Thm. 4.1]. For each $n\in \mathbb{N}$, we construct a solution $\{({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})\}$ as follows. By Theorem 2, on the interval $[0,n]$,
and for $t\ge n$, we have by assumption $(H7)$ that ${Y_{t}^{n}}=\xi _{t}$, ${Z_{t}^{n}}=\eta _{t}$, ${V_{t}^{n}}(e)=\gamma _{t}(e)$, ${M_{t}^{n}}=N_{t}$.
(86)
\[\begin{array}{r@{\hskip0pt}l}\displaystyle {Y_{t}^{n}}& \displaystyle =\mathbb{E}(\xi \mid \mathcal{F}_{n})+{\int _{t}^{n}}\mathbb{1}_{[0,\tau ]}(s)f\big(s,{Y_{s}^{n}},{Z_{s}^{n}},{V_{s}^{n}}\big)ds+{\int _{t}^{n}}\mathbb{1}_{[0,\tau ]}(s)dR_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t}^{n}}{Z_{s}^{n}}dW_{s}-{\int _{t}^{n}}\int _{U}{V_{s}^{n}}(e)\widehat{\pi }(de,ds)-{\int _{t}^{n}}d{M_{s}^{n}},\end{array}\]
Step 1. We first show that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ satisfies estimate (84). Applying Itô’s formula to ${e}^{p\rho s}|{Y_{s}^{n}}{|}^{p}$ over the interval $[t\wedge \tau ,T\wedge \tau ]$ for $0\le t\le T\le n$ and combining with (42), (77), and (78) yield
Note that all the local martingales in the last inequality are true martingales. Thus, taking the expectation in (87), we get in view of (81) that
where
But by Young’s inequality we have
and
Consequently, combining (89) with (90) and (91) and letting $T\to +\infty $, we deduce that
Finally, going back to (88), we conclude in view of (90), (91), and (92) that estimate (84) holds for $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$.
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {e}^{p\rho (t\wedge \tau )}{\big|{Y_{t\wedge \tau }^{n}}\big|}^{p}+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}{\big|{Y_{s}^{n}}\big|}^{p-2}{\big|{Z_{s}^{n}}\big|}^{2}ds\\{} & \displaystyle \hspace{2em}+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\int _{U}{\big|{Y_{s}^{n}}\big|}^{p-2}{\big|{V_{s}^{n}}(e)\big|}^{2}\pi (de,ds)+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}\big|{Y_{s-}^{n}}\big|d\big[{M}^{n}\big]_{s}\\{} & \displaystyle \hspace{1em}\le {e}^{p\rho (T\wedge \tau )}{\big|{Y_{T\wedge \tau }^{n}}\big|}^{p}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}\big[{Y_{s}^{n}}{\big|{Y_{s}^{n}}\big|}^{p-2}f\big(s,{Y_{s}^{n}},{Z_{s}^{n}},{V_{s}^{n}}\big)-\rho {\big|{Y_{s}^{n}}\big|}^{p}\big]ds\\{} & \displaystyle \hspace{2em}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}{Y_{s}^{n}}{\big|{Y_{s}^{n}}\big|}^{p-2}dR_{s}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}{Y_{s-}^{n}}{\big|{Y_{s-}^{n}}\big|}^{p-2}d{M_{s}^{n}}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}{Y_{s}^{n}}{\big|{Y_{s}^{n}}\big|}^{p-2}{Z_{s}^{n}}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}{e}^{\rho s}{Y_{s-}^{n}}{\big|{Y_{s-}^{n}}\big|}^{p-2}{V_{s}^{n}}(e)\hspace{0.1667em}\widehat{\pi }(de,ds).\end{array}\]
But, from the assumptions on f combined with Young’s inequality we get, for a small enough constant $\delta >0$,
\[\begin{array}{r@{\hskip0pt}l}\displaystyle y|y{|}^{p-2}f(t,y,z,v)& \displaystyle \le \bigg(\mu +\frac{2p{L}^{2}}{\alpha _{p}-p\delta }\bigg)|y{|}^{p}+|y{|}^{p-1}\big|f(t,0,0,0)\big|\\{} & \displaystyle \hspace{1em}+\bigg(\frac{\alpha _{p}}{p}-\delta \bigg)|y{|}^{p-2}|z{|}^{2}+\bigg(\frac{\alpha _{p}}{p}-\delta \bigg)|y{|}^{p-2}\| v\| _{{\mathbb{L}_{\lambda }^{2}}}.\end{array}\]
Then, choosing δ such that $\mu +\frac{2p{L}^{2}}{\alpha _{p}-p\delta }<\rho $, we deduce from the above that
(87)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {e}^{p\alpha (t\wedge \tau )}{\big|{Y_{t\wedge \tau }^{n}}\big|}^{p}+p\bar{\rho }{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\alpha s}{\big|{Y_{s}^{n}}\big|}^{p}ds+p\delta {\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\alpha s}{\big|{Y_{s}^{n}}\big|}^{p-2}{\big|{Z_{s}^{n}}\big|}^{2}ds\\{} & \displaystyle \hspace{2em}+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\alpha s}{\big|{Y_{s}^{n}}\big|}^{p-2}{\big|{V_{s}^{n}}(e)\big|}^{2}\pi (de,ds)+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\alpha s}{\big|{Y_{s}^{n}}\big|}^{p-2}d\big[{M}^{n}\big]_{s}\\{} & \displaystyle \hspace{2em}-p\bigg(\frac{\alpha _{p}}{p}-\delta \bigg){\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\alpha s}{\big|{Y_{s}^{n}}\big|}^{p-2}\big\| {V_{s}^{n}}{\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}ds\\{} & \displaystyle \hspace{1em}\le {e}^{p\alpha (T\wedge \tau )}{\big|{Y_{T\wedge \tau }^{n}}\big|}^{p}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\alpha s}{\big|{Y_{s}^{n}}\big|}^{p-1}\big|f(s,0,0,0)\big|ds\\{} & \displaystyle \hspace{2em}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}{\big|{Y_{s}^{n}}\big|}^{p-1}d|R|_{s}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}{Y_{s-}^{n}}{\big|{Y_{s-}^{n}}\big|}^{p-2}d{M_{s}^{n}}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}{Y_{s}^{n}}{\big|{Y_{s}^{n}}\big|}^{p-2}{Z_{s}^{n}}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{T\wedge \tau }}\int _{U}{e}^{\rho s}{Y_{s-}^{n}}{\big|{Y_{s-}^{n}}\big|}^{p-2}{V_{s}^{n}}(e)\hspace{0.1667em}\widehat{\pi }(de,ds).\end{array}\](88)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{e}^{p\rho (t\wedge \tau )}{\big|{Y_{t\wedge \tau }^{n}}\big|}^{p}+p\delta {\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}{\big|{Y_{s}^{n}}\big|}^{p}ds+p\delta {\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}{\big|{Y_{s}^{n}}\big|}^{p-2}{\big|{Z_{s}^{n}}\big|}^{2}ds\\{} & \displaystyle \hspace{2em}+p\delta {\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}{\big|{Y_{s}^{n}}\big|}^{p-2}\big\| {V_{s}^{n}}\big\| _{{\mathcal{L}_{\lambda }^{2}}}ds+\alpha _{p}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}{\big|{Y_{s}^{n}}\big|}^{p-2}d\big[{M}^{n}\big]_{s}\Bigg]\\{} & \displaystyle \hspace{1em}\le \mathbb{E}[X],\end{array}\]
\[\begin{array}{r@{\hskip0pt}l}\displaystyle X& \displaystyle ={e}^{p\rho (T\wedge \tau )}{\big|{Y_{T\wedge \tau }^{n}}\big|}^{p}+p{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{p\rho s}{\big|{Y_{s}^{n}}\big|}^{p-1}\big|f(s,0,0,0)\big|ds\\{} & \displaystyle \hspace{1em}+p{\int _{t\wedge \tau }^{T\wedge \tau }}\hspace{0.1667em}{e}^{p\rho s}{\big|{Y_{s-}^{n}}\big|}^{p-1}d|R|_{s}.\end{array}\]
Next, as in the proof of Lemma 4, including a $\sup _{s\in [t,T]}$ in (87) and applying the BDG inequality, we get in view of (88) that
(89)
\[ \mathbb{E}\Big[\underset{s\in [t,T]}{\sup }{e}^{p\rho (s\wedge \tau )}{\big|{Y_{s\wedge \tau }^{n}}\big|}^{p}\Big]\le C_{p}\mathbb{E}[X].\](90)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle p\mathbb{E}{\int _{t\wedge \tau }^{T\wedge \tau }}\hspace{0.1667em}{e}^{p\rho s}|Y_{s}{|}^{p-1}\big|f(s,0,0,0)\big|ds\\{} & \displaystyle \hspace{1em}\le p\mathbb{E}\Bigg(\underset{s\in [t\wedge \tau ,T\wedge \tau ]}{\sup }{e}^{(p-1)\rho s}|Y_{t}{|}^{p-1}{\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}\big|f(s,0,0,0)\big|ds\Bigg)\\{} & \displaystyle \hspace{1em}\le \frac{1}{6}\mathbb{E}\Big(\underset{s\in [t\wedge \tau ,T\wedge \tau ]}{\sup }{e}^{p\rho s}|Y_{t}{|}^{p}\Big)+{d^{\prime }_{p}}\mathbb{E}{\Bigg({\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}\big|f(s,0,0,0)\big|ds\Bigg)}^{p},\end{array}\](91)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle p\mathbb{E}{\int _{t\wedge \tau }^{T\wedge \tau }}\hspace{0.1667em}{e}^{p\rho s}|Y_{s-}{|}^{p-1}d|R|_{s}\\{} & \displaystyle \hspace{1em}\le \frac{1}{6}E\big(\underset{s\in [t\wedge \tau ,T\wedge \tau ]}{\sup }{e}^{p\rho s}|Y_{t}{|}^{p}\big)+{d^{\prime\prime }_{p}}\mathbb{E}{\Bigg({\int _{t\wedge \tau }^{T\wedge \tau }}{e}^{\rho s}d|R|_{s}\Bigg)}^{p}.\end{array}\](92)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Big[\underset{t\ge 0}{\sup }{e}^{p\rho (t\wedge \tau )}{\big|{Y_{t\wedge \tau }^{n}}\big|}^{p}\Big]\\{} & \displaystyle \hspace{1em}\le {C^{\prime\prime }_{p}}\mathbb{E}\Bigg[{e}^{p\rho \tau }|\xi {|}^{p}+{\Bigg({\int _{0}^{\tau }}{e}^{\rho s}\big|f(s,0,0,0)\big|ds\Bigg)}^{p}+{\Bigg({\int _{0}^{\tau }}{e}^{\rho s}d|R|_{s}\Bigg)}^{p}\Bigg].\end{array}\]
Step 2. Let us show that $({Y}^{n},{Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence. For $m>n$, define
\[ \bar{Y}_{t}={Y_{t}^{m}}-{Y_{t}^{n}},\hspace{1em}\bar{Z}_{t}={Z_{t}^{m}}-{Z_{t}^{n}},\hspace{1em}\bar{V}_{t}={V_{t}^{m}}-{V_{t}^{n}},\hspace{1em}\bar{M}_{t}={M_{t}^{m}}-{M_{t}^{n}}.\]
For $n\le t\le m$, we have
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \bar{Y}_{t}& \displaystyle ={\int _{t\wedge \tau }^{m\wedge \tau }}f\big(s,{Y_{s}^{m}},{Z_{s}^{m}},{V_{s}^{m}}\big)ds-{\int _{t\wedge \tau }^{m\wedge \tau }}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t\wedge \tau }^{m\wedge \tau }}\int _{U}\bar{V}_{s}(e)\widehat{\pi }(du,ds)-\bar{M}_{m\wedge \tau }+\bar{M}_{t\wedge \tau }.\end{array}\]
Consequently, again for $n\le t\le m$,
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {e}^{p\rho (t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}+\alpha _{p}{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s}{|}^{p-2}|\bar{Z}_{s}{|}^{2}ds\\{} & \displaystyle \hspace{2em}+\alpha _{p}{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}\int _{U}|\bar{Y}_{s}{|}^{p-2}{\big|\bar{V}_{s}(e)\big|}^{2}\pi (de,ds)+\alpha _{p}{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s-}|d[\bar{M}]_{s}\\{} & \displaystyle \hspace{1em}\le p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\big[\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}f\big(s,{Y_{s}^{m}},{Z_{s}^{m}},{V_{s}^{m}}\big)-\rho |\bar{Y}_{s}{|}^{p}\big]ds\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\bar{Z}_{s}dW_{s}-p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}d\bar{M}_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{m\wedge \tau }}\int _{U}{e}^{\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}\bar{V}_{s}(e)\hspace{0.1667em}\widehat{\pi }(de,ds)\\{} & \displaystyle \hspace{1em}\le p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\big[\mu |\bar{Y}_{s}{|}^{p}+L|\bar{Y}_{s}{|}^{p-1}|\bar{Z}_{s}|+L|\bar{Y}_{s}{|}^{p-1}\big\| \bar{V}_{s}(e)\big\| _{{\mathcal{L}_{\lambda }^{2}}}-\rho |\bar{Y}_{s}{|}^{p}\big]ds\\{} & \displaystyle \hspace{2em}+p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}f(s,\xi _{s},\eta _{s},\gamma _{s})ds-p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\bar{Y}_{s}|\bar{Y}_{s}{|}^{p-2}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}d\bar{M}_{s}\\{} & \displaystyle \hspace{2em}-p{\int _{t\wedge \tau }^{m\wedge \tau }}\int _{U}{e}^{\rho s}\bar{Y}_{s-}|\bar{Y}_{s-}{|}^{p-2}\bar{V}_{s}(e)\hspace{0.1667em}\widehat{\pi }(de,ds).\end{array}\]
We deduce by already used arguments that
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[\underset{n\le t\le m}{\sup }{e}^{p\rho (t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}+{\int _{n\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s}{|}^{p}ds+{\int _{n\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s}{|}^{p-2}|\bar{Z}_{s}{|}^{2}ds\\{} & \displaystyle \hspace{2em}+{\int _{n\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}\int _{U}|\bar{Y}_{s}{|}^{p-2}\big\| \bar{V}_{s}(e){\big\| _{{\mathcal{L}_{\lambda }^{2}}}^{2}}ds+{\int _{n\wedge \tau }^{m\wedge \tau }}{e}^{p\rho s}|\bar{Y}_{s-}|d[\bar{M}]_{s}\Bigg]\\{} & \displaystyle \hspace{1em}\le C\mathbb{E}{\Bigg({\int _{n\wedge \tau }^{\tau }}{e}^{\rho s}\big|f(s,\xi _{s},\eta _{s},\gamma _{s})\big|ds\Bigg)}^{p},\end{array}\]
and the last term tends to zero as $n\to \infty $.Next, for $t\le n$,
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \bar{Y}_{t}& \displaystyle =\bar{Y}_{n}+{\int _{t\wedge \tau }^{n\wedge \tau }}\big(f\big(s,{Y_{s}^{m}},{Z_{s}^{m}},{V_{s}^{m}}\big)-f\big(s,{Y_{s}^{n}},{Z_{s}^{n}},{V_{s}^{n}}\big)\big)ds-{\int _{t\wedge \tau }^{n\wedge \tau }}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{1em}-{\int _{t\wedge \tau }^{n\wedge \tau }}\int _{U}\widehat{V}_{s}(e)\widehat{\pi }(de,ds)-\bar{M}_{n\wedge \tau }+\bar{M}_{t\wedge \tau }.\end{array}\]
Arguing as in Proposition 2, we get
\[\begin{array}{r@{\hskip0pt}l}\displaystyle \mathbb{E}{e}^{p\rho (t\wedge \tau )}|\bar{Y}_{t\wedge \tau }{|}^{p}\mathbb{E}{\int _{0}^{\tau }}{e}^{p\rho s}|\bar{Y}_{s}{|}^{p}ds& \displaystyle \le \mathbb{E}{e}^{p\rho (n\wedge \tau )}|\bar{Y}_{n}{|}^{p}\\{} & \displaystyle \le C\mathbb{E}{\Bigg({\int _{n\wedge \tau }^{\tau }}{e}^{\rho s}\big|f(s,\xi _{s},\eta _{s},\gamma _{s})\big|ds\Bigg)}^{p},\end{array}\]
and letting $n\to \infty $, the convergence of the sequence ${Y}^{n}$ follows.Next, it remains to show the convergence of the martingale part $({Z}^{n},{V}^{n},{M}^{n})$. We follow the proof of Lemma 4. We apply Itô’s formula to ${e}^{2\rho s}|\bar{Y}_{s}{|}^{2}$ for $n\le t\le m$:
Next, arguing similarly for the case $t\le n$, we get
Consequently, letting $n\to \infty $, we deduce from the above that, in both cases, the sequence $({Z}^{n},{V}^{n},{M}^{n})$ is a Cauchy sequence for the norm
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle {\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}|\bar{Z}_{s}{|}^{2}ds+{\int _{t\wedge \tau }^{m\wedge \tau }}\int _{U}{e}^{2\rho s}{\big|\bar{V}_{s}(e)\big|}^{2}\pi (de,ds)+{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}d[\bar{M}]_{s}\\{} & \displaystyle \hspace{1em}=2{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}\big[\bar{Y}_{s}\big(f\big(s,{Y_{s}^{m}},{Z_{s}^{m}},{V_{s}^{m}}\big)-f(s,\xi _{s},\eta _{s},\gamma _{s})\big)-\rho |\bar{Y}_{s}{|}^{2}\big]ds\\{} & \displaystyle \hspace{2em}+2{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}\bar{Y}_{s}f(s,\xi _{s},\eta _{s},\gamma _{s})ds-2{\int _{0}^{\tau _{n}}}{e}^{2\rho s}\bar{Y}_{s}\bar{Z}_{s}dW_{s}\\{} & \displaystyle \hspace{2em}-2{\int _{t\wedge \tau }^{m\wedge \tau }}\int _{U}{e}^{2\rho s}\bar{Y}_{s-}\bar{V}_{s}(e)\widehat{\pi }(de,ds)-2{\int _{t\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}\bar{Y}_{s-}d\bar{M}_{s}.\end{array}\]
Mimicking the same argumentation used to obtain (34) (assumptions on f and BDG and Young inequalities) leads to
(93)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{\Bigg({\int _{n\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}|\bar{Z}_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{n\wedge \tau }^{m\wedge \tau }}\int _{U}{e}^{2\rho s}{\big|\bar{V}_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{n\wedge \tau }^{m\wedge \tau }}{e}^{2\rho s}d[\bar{M}]_{s}\Bigg)}^{\frac{p}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C(p,T)\Bigg[\mathbb{E}\underset{t\ge n}{\sup }{e}^{p\rho s}|\bar{Y}_{t}{|}^{p}+\mathbb{E}{\Bigg({\int _{n\wedge \tau }^{\tau }}{e}^{\rho s}\big|f(s,\xi _{s},\eta _{s},\gamma _{s})\big|ds\Bigg)}^{p}\Bigg].\end{array}\](94)
\[\begin{array}{r@{\hskip0pt}l}& \displaystyle \mathbb{E}\Bigg[{\Bigg({\int _{0}^{n\wedge \tau }}{e}^{2\rho s}|\bar{Z}_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+{\Bigg({\int _{0}^{n\wedge \tau }}\int _{U}{e}^{2\rho s}{\big|\bar{V}_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}\\{} & \displaystyle \hspace{2em}+{\Bigg({\int _{0}^{n\wedge \tau }}{e}^{2\rho s}d[\bar{M}]_{s}\Bigg)}^{\frac{p}{2}}\Bigg]\\{} & \displaystyle \hspace{1em}\le C(p,T)\big[\mathbb{E}\underset{t\ge n}{\sup }{e}^{p\rho n\wedge \tau }|\bar{Y}_{n\wedge \tau }{|}^{p}\big].\end{array}\]
\[ \mathbb{E}{\Bigg({\int _{0}^{\tau }}{e}^{2\rho s}|\bar{Z}_{s}{|}^{2}ds\Bigg)}^{\frac{p}{2}}+\mathbb{E}{\Bigg({\int _{0}^{\tau }}\int _{U}{e}^{2\rho s}{\big|\bar{V}_{s}(e)\big|}^{2}\lambda (de)ds\Bigg)}^{\frac{p}{2}}+\mathbb{E}{\Bigg({\int _{0}^{\tau }}{e}^{2\rho s}d[\bar{M}]_{s}\Bigg)}^{\frac{p}{2}},\]
and thus it converges to $(Z,V,M)$. Finally, the limit $(Y,Z,V,M)$ is a solution of GBSDE (73) that satisfies estimates (84) and (85). □