Dynamic Risk Measures and PathDependent Second Order PDEs
Abstract
We propose new notions of regular solutions and viscosity solutions for pathdependent second order partial differential equations. Making use of the martingale problem approach to pathdependent diffusion processes, we explicitly construct families of timeconsistent dynamic risk measures on the set of càdlàg paths \(I\!R^n\) valued endowed with the Skorokhod topology. These risk measures are shown to have regularity properties. We prove then that these timeconsistent dynamic risk measures provide viscosity supersolutions and viscosity subsolutions for pathdependent semilinear second order partial differential equations.
Keywords
Pathdependent PDE Risk measures Martingale problemsMSC:
35D40 35R15 35K55 60J60 91B301 Introduction
In contrast with the classical setting, the notion of regular solution for a pathdependent PDE (1) needs to deal with càdlàg paths. Indeed to give a meaning to the partial derivatives \(D_x\phi (u,\omega )\) and \(D^2_x\phi (u,\omega )\) at \((u_0,\omega _0)\), one needs to assume that \(\phi (u_0,\omega )\) is defined for paths \(\omega \) admitting a jump at time \(u_0\). Peng has introduced in [20] a notions of regular and viscosity solution for pathdependent second order PDEs. In [20] a regular or a viscosity solution for a pathdependent PDE is a progressive function \(\phi (t,\omega )\) defined on the space of càdlàg paths endowed with the uniform norm topology and the notion of continuity and partial derivatives are those introduced by Dupire [12]. A comparison theorem is proved in this setting [20]. The motivation comes mainly from the theory of BSDE and examples of regular solutions to pathdependent PDEs can be constructed from BSDEs [18]. The main drawback for this approach based on [12] is that the uniform norm topology on the set of càdlàg paths is not separable, hence it is not a Polish space. Recently Ekren et al. proposed a notion of viscosity solution for pathdependent PDEs in the setting of continuous paths in [13, 14]. This work was motivated by the fact that a continuous function defined on the set of continuous paths does not have a unique extension into a continuous function on the set of càdlàg paths. Therefore it is suitable that the notion of viscosity solution for functions defined only on the set of continuous paths does not require to extend the function to the set of càdlàg paths. The approach developed in [13, 14] is also based on BSDE.
In the present paper we introduce a new notion of regular and viscosity solution for pathdependent second order PDEs (Sect. 2). A solution to (1) is a progressive function \(\phi \) defined on \(I\!R_+ \times \varOmega \) where \(\varOmega \) is the set of càdlàg paths. In contrast with [20] and many works on pathdependent problems, we consider the Skorokhod topology on the set of càdlàg paths. Thus \(\varOmega \) is a Polish space. This property is very important. To define the continuity and regularity properties for a progressive function, we make use of the one to one correspondence between progressive functions on \(I\!R_+ \times \varOmega \) and strictly progressive functions on \(I\!R_+ \times \varOmega \times I\!R^n\) established in [3]. A function \(\phi \) defined on \(I\!R_+ \times \varOmega \) is progressive if \(\phi (s,\omega )=\phi (s,\omega ')\) as soon as \(\omega (u)=\omega '(u)\) for all \(0 \le u \le s\). A function \(\overline{\phi }\) defined on \(I\!R_+ \times \varOmega \times I\!R^n\) is strictly progressive if \(\overline{\phi }(s,\omega ,x)=\overline{\phi }(s,\omega ',x)\) as soon as \( \omega (u)=\omega '(u)\) for all \(0 \le u <s\). The one to one correspondence is given by \(\overline{\phi }(s,\omega ,x)=\phi (s,\omega *_sx)\) where \((\omega *_sx)(u)=\omega (u)\) for all \(0 \le u <s\) and \((\omega *_sx)(u)=x\) for all \( u \ge s\). The continuity and regularity properties that we want for a progressive function \(\phi \) are derived from the usual continuity and regularity properties for \(\overline{\phi }\) via the above one to one correspondence. For example, \(D_x\phi (u,\omega )\) is defined as \(D_x\phi (u,\omega ):=D_x\overline{\phi }(u,\omega ,\omega (u))\) where \(D_x\overline{\phi }\) is the usual partial derivative of \(\overline{\phi }\) with respect to the third variable. Notice that via the above one to one correspondence, the regularity properties for a progressive function \(\phi \) are defined in a very natural way. This is in contrast with the most commonly used regularity definitions first introduced in [12].
The notion of viscosity solution that we introduce in the present paper is motivated by our construction of a solution to semilinear second order pathdependent PDEs based on the martingale problem approach.
Our study for viscosity solutions of pathdependent PDEs allows then to introduce a new definition of viscosity solution for pathdependent functions defined only on the set of continuous paths. As in [13, 14], this does not require to extend the function nor the coefficient functions appearing in the pathdependent PDE to the set of càdlàg paths. However our approach is very different from the one introduced in [13, 14].
These dynamic risk measures are constructed using probability measures solution to a pathdependent martingale problem. This approach is motivated by the Feynman Kac formula and more specifically by the link between solutions of a parabolic second order PDE and probability measures solutions to a martingale problem. The martingale problem has been first introduced and studied by Stroock and Varadhan [10, 11] in the case of continuous diffusion processes. The martingale problem is linked to stochastic differential equations. However the martingale problem formulation is intrinsic and is very well suitable to construct risk measures. In [22] the martingale problem has been extended and studied to the case of jump diffusions. In [3], the study of the martingale problem is extended to the pathdependent case which means that the functions a and b (and also the jump measure) are no more defined on \(I\!R_+ \times I\!R^n\) but on \(I\!R_+ \times \varOmega \). The question of existence and uniqueness of a solution to a pathdependent martingale problem is addressed in [3] in a general setting of diffusions with a pathdependent jump term. In the case where there is no jump term and under Lipschitz conditions on the coefficients, the existence and uniqueness of a solution has been already established in [8] from the stochastic differential equation point of view.
In Sect. 3, we recall some results from [3] on the martingale problem for pathdependent diffusion processes and study the support of a probability measure solution to the pathdependent martingale problem for \({\mathscr {L}}^{a,b}\).
The theory of dynamic risk measures on a filtered probability space has been developped in recent years. In the case of a Brownian filtration, dynamic risk measures coincide with gexpectations introduced by Peng [21]. An important property for dynamic risk measures is time consistency. The time consistency property for dynamic risk measures is the analogue of the Dynamic Programming Principle. For sublinear dynamic risk measures time consistency has been characterized by Delbaen [9]. For general convex dynamic risk measures two different characterizations of time consistency have been given. One by Cheridito et al. [7], the other by BionNadal [5]. This last characterization of time consistency is very useful in order to construct time consistent dynamic risk measures.
Following [5], one can construct a time consistent dynamic risk measure as soon as one has a stable set of equivalent probability measures \({\mathscr {Q}}\) and a penalty defined on \({\mathscr {Q}}\) satisfying some conditions. In Sect. 4, we construct a stable set of probability measures on the set \(\varOmega \) of càdlàg paths. In the whole paper a is a given bounded progressively continuous function defined on \(I\!R_+ \times \varOmega \) such that \(a(s,\omega )\) is invertible for all \((s,\omega )\). For all \(r \ge 0\) and \(\omega \in \varOmega \) the set of probability measures \({\mathscr {Q}}_{r,\omega }\) is a stable set generated by probability measures \(Q^{a,b}_{r,\omega }\) solution to the martingale problem for \({\mathscr {L}}^{a,b}\) starting from \(\omega \) at time r. The functions b are assumed to satisfy some uniform BMO condition. In Sect. 5 we construct penalties on the stable set \({\mathscr {Q}}_{r,\omega }\) from a pathdependent function g. Some growth conditions are assumed on the function g to ensure integrability properties for the penalties. With such a stable set and penalties, we construct in Sect. 6 time consistent convex dynamic risk measures. More precisely for all r and \(\omega \) we construct a time consistent convex dynamic risk measure \(\rho ^{r,\omega }_{s,t}\) on the filtered probability space \((\varOmega ,({\mathscr {B}}_{t}),Q^{a}_{r,\omega })\) where \(Q^{a}_{r,\omega }\) means \(Q^{a,0}_{r,\omega }\) and \(({\mathscr {B}}_{t})\) is the canonical filtration.
We prove also that the upper semicontinuous envelope of R(h) is a viscosity subsolution for (2).
When the above function h is defined only on the set of continuous paths, it is the same for the function R(h). We prove then that R(h) provides a viscosity supersolution and a viscosity subsolution for (2) on the set of continuous paths.
2 Solution of Pathdependent PDEs
In this section we introduce new notions for regular and viscosity solutions for second order pathdependent PDEs on the set of càdlàg paths. In contrast with [20] and all the papers using the notions of continuity and derivative introduced by Dupire [12], we work with the Skorohod topology on the set of càdlàg paths. A solution to a pathdependent PDE (1) is a progressive function \(\phi (t,\omega )\) where t belongs to \(I\!R_+\) and \(\omega \) belongs to the set of càdlàg paths.
2.1 Topology and Regularity Properties
In the whole paper \(\varOmega \) denotes the set of càdlàg paths with the Skorohod topology. The set \(\varOmega \) is then a Polish space (i.e. is metrizable and separable). Polish spaces have nice properties which are very important in the construction of solutions for pathdependent PDEs. Among them are the existence of regular conditional probability distributions, the equivalence between relative compactness and tightness for a set of probability measures, to name a few.
To define the continuity and regularity properties for progressive functions, we use the one to one correspondence between progressive functions on \(I\!R_+ \times \varOmega \) and strictly progressive functions on \(I\!R_+ \times \varOmega \times I\!R^n\) that we have established in [3].
A function \(\phi \) defined on \(I\!R_+ \times \varOmega \) is progressive if \(\phi (s,\omega )=\phi (s,\omega ')\) as soon as \(\omega (u)=\omega '(u)\) for all \(0 \le u \le s\).
A function \(\overline{\phi }\) defined on \(I\!R_+ \times \varOmega \times I\!R^n\) is strictly progressive if \(\overline{\phi }(s,\omega ,x)=\overline{\phi }(s,\omega ',x)\) as soon as \( \omega (u)=\omega '(u)\) for all \(0 \le u <s\).
2.2 Regular Solution
Making use of the one to one corrrespondence between progressive functions on \(I\!R_+ \times \varOmega \) and strictly progressive functions on \(I\!R_+ \times \varOmega \times I\!R^n\), we can then give the following definition for a solution to a general pathdependent PDE.
Definition 1
\((\omega *_ux)(s)=\omega (s) \;\forall s<u\), and \((\omega *_ux)(s)=x\; \forall s \ge u\). The partial derivatives of \(\overline{v}\) are the usual ones, the continuity notion for \(\overline{v}\) is the usual one.
2.3 Viscosity Solutions on the Set of Càdlàg Paths
The following definitions are motivated by the construction of viscosity solutions for pathdependent PDEs that we develop in the following sections. Our construction of solutions is based on the martingale problem approach for pathdependent diffusions. The support of every probability measure \(Q^{a,b}_{r,\omega _0}\) solution to the martingale problem for \({\mathscr {L}}^{a,b}\) starting from \(\omega _0\) at time r is contained in the set of paths which coincide with \(\omega _0\) up to time r. This is a motivation for the following weak notion of continuity and also for the weak notion of local minimizer (or local maximizer) that we introduce in the definition of viscosity solution.
Definition 2
Definition 3
Let v be a progressively measurable function on \((I\!R_+\,\times \,\varOmega ,({\mathscr {B}}_t))\) where \( \varOmega \) is the set of càdlàg paths with the Skorokhod topology and \(({\mathscr {B}}_t)\) the canonical filtration.
 1.v is a viscosity supersolution of (4) if v is lower semicontinuous in viscosity sense, and if for all \((t_0,\omega _0)\in I\!R_+ \times \varOmega \),

v is bounded from below on \(D_{\varepsilon }(t_0,\omega _0)\) for some \(\varepsilon >0\).
 for all strictly progressive function \(\overline{\phi }\in {\mathscr {C}}_b^{1,0,2} (I\!R_+ \times \varOmega \times I\!R^n)\) such that \(v(t_0,\omega _0)=\phi (t_0,\omega _0)\), and \((t_0,\omega _0 )\) is a minimizer of \(v\phi \) on \(D_{\varepsilon }(t_0,\omega _0)\) for some \(\varepsilon >0\),at point \((t_0,\omega _0,\omega _0(t_0))\).$$\begin{aligned} H(u,\omega *_ux,\phi (u,\omega ,x),\partial _u\phi (u,\omega ,x),D_x\phi (u,\omega ,x),D^2_x\phi (u,\omega ,x)\ge 0 \end{aligned}$$(8)

 2.v is a viscosity subsolution of (4) if v is upper semicontinuous in viscosity sense, and for all \((t_0,\omega _0)\),

v is bounded from above on \(D_{\varepsilon }(t_0,\omega _0)\) for some \(\varepsilon >0\)
 for all strictly progressive function \(\overline{\phi }\in {\mathscr {C}}_b^{1,0,2} (I\!R_+ \times \varOmega \times I\!R^n)\) such that \(v(t_0,\omega _0)=\phi (t_0,\omega _0)\), and \((t_0,\omega _0 )\) is a maximizer of \(v\phi \) on \(D_{\varepsilon }(t_0,\omega _0)\) for some \(\varepsilon >0\),at point \((t_0,\omega _0,\omega _0(t_0))\).$$\begin{aligned} H(u,\omega *_ux,\phi (u,\omega ,x),\partial _u\phi (u,\omega ,x),D_x\phi (u,\omega ,x),D^2_x\phi (u,\omega ,x)\le 0 \end{aligned}$$(9)

 3.
v is a viscosity solution if v is both a viscosity supersolution and a viscosity subsolution.
2.4 Viscosity Solution on the Set of Continuous Paths
Recently Ekren et al. [13, 14] introduced a notion of viscosity solution of a pathdependent second order PDE for a function v defined on the set of continuous paths. One motivation for this was to define the notion of viscosity solution without extending the function v to the set of càdlàg paths.
We can notice that within our setting we can also define a notion of viscosity solution for a function v defined only on the set of continuous paths without extending v. We give the following definition which is very different from that of [13, 14] and much simpler.
Definition 4

v is bounded from below on \(\tilde{D}_{\varepsilon }(t_0,\omega _0)\) for some \(\varepsilon >0\),
 for all function strictly progressive \(\overline{\phi }\in {\mathscr {C}}_b^{1,0,2} (I\!R_+ \times \varOmega \times I\!R^n)\) such that \(v(t_0,\omega _0)=\phi (t_0,\omega _0)\), and \((t_0,\omega _0 )\) is a minimizer of \(v\phi \) on \(\tilde{D}_{\varepsilon }(t_0,\omega _0)\) for some \(\varepsilon >0\),at point \((t_0,\omega _0,\omega _0(t_0))\).$$\begin{aligned} H(u,\omega *_ux,\overline{\phi }(u,\omega ,x),\partial _u \overline{\phi }(u,\omega ,x),D_x\overline{\phi }(u,\omega ,x),D^2_x \overline{\phi }(u,\omega ,x)\ge 0 \end{aligned}$$(10)
Here \(\varOmega \) is the set of càdlàg paths with the Skorokhod topology, \(\tilde{D}_{\varepsilon }\) is the intersection of \(D_{\varepsilon }\) with the set of continuous paths, and \(\phi (u,\omega )=\overline{\phi }(u,\omega ,\omega (u))\).
We will now construct time consistent dynamic risk measures making use of probability measures solution to a pathdependent martingale problem. We will then prove that this leads to viscosity solutions to pathdependent PDEs (2).
3 Pathdependent Martingale Problem
Definition 5
In [3] we have studied the more general martingale problem associated with pathdependent diffusions with jumps. We have shown that the good setting to prove that the martingale problem is well posed is to deal with diffusions operators whose coefficients a and b are progressively continuous.
Recall the following result from [3].
Theorem 1
 1.
Let a be a progressively continuous bounded function defined on \(I\!R_+ \times \varOmega \) with values in the set of non negative matrices. Assume that \(a(s,\omega )\) is invertible for all \((s,\omega )\). Let b be a progressively measurable bounded function defined on \(I\!R_+ \times \varOmega \) with values in \(I\!R^n\). For all \((r,\omega _0)\), the martingale problem for \({\mathscr {L}}^{a,ab}\) starting from \(\omega _0\) at time r is well posed i.e. admits a unique solution \(Q^{a,ab}_{r,\omega _0}\) on the set of càdlàg paths.
 2.Assume furthermore that b is progressively continuous bounded. Consider the set of probability measures \({\mathscr {M}}_1(\varOmega )\) equipped with the weak topology. Then the mapis continuous on \(\{(r,\omega ,x) \;\;\omega =\omega *_rx\}\).$$(r,\omega ,x) \in I\!R_+ \times \varOmega \times I\!R^n \rightarrow Q^{a,ab}_{r,\omega *_r x} \in {\mathscr {M}}_1(\varOmega )$$
3.1 The Role of Continuous Paths
In all the following \(Q^{a}_{r,\omega _0}\) means \(Q^{a,0}_{r,\omega _0}\)
We start with a result which proves that the probability measure \(Q^{a,ab}_{r,\omega _0}\) is supported by paths which are continuous after time r.
Proposition 1
Every probability measure \(Q^{a,ab}_{r,\omega _0}\) solution to the martingale problem for \({\mathscr {L}}^{a,ab}\) starting from \(\omega _0\) at time r is supported by paths which are continuous after time r, i.e. continuous on \([r,\infty [\).
Proof
The probability measure \(Q^{a,ab}_{r,\omega _0}\) is equivalent with \(Q^{a}_{r,\omega _0}\). Thus we can assume that \(b=0\).
The function a is progressively continuous. This means that the function \(\overline{a}\) is continuous. Let \(a_n\) be the \(\frac{1}{n}\) delayed function defined as \(\overline{a}_n(u,\omega ,x)=\overline{a}(u\frac{1}{n},\omega ,x)\) for all \(u \ge r+\frac{1}{n}\) and \(\overline{a}_n(u,\omega ,x)=\overline{a}(r,\omega ,x)\) for all \(0 \le u \le r+\frac{1}{n}\). The function \(a_n\) is also progressively continuous. Given n, let \(t^n_k\) be an increasing sequence such that \(t^n_0=r\) and \(t^n_{k+2}t^n_k< \frac{1}{n}\).
On a Polish space for every subsigma algebra of the Borel sigma algebra there exists a regular conditional probability distribution. It follows from [22] and the uniqueness of the solution for \({\mathscr {L}}^{a_{n},0}\) starting from \(\omega \) at time \(t^{n}_{k}\), that for all \(t^{n}_{k}\), \(Q^{a_{n}}_{t^{n}_{k},\omega }(\xi )= E_{Q^{a_{n}}_{r,\omega _{0}}}(\xi {\mathscr {B}}_{t^{n}_{k}})(\omega )\) for \(Q^{a_{n}}_{r,\omega _{0}}\) almost all \(\omega \). Let \(a_{n,\omega }(u,x)=\overline{a}_n(u,\omega ,x)\) Let \(A_k=\{\omega ',\;\omega '_{[t^n_{k},t^n_{k+2}[} \in {\mathscr {C}}([t^n_{k},t^n_{k+2}[)\}\). Given \(\omega \) the function \(a_{n,\omega }\) is not pathdependent. It follows then from [11] that \(Q^{a_{n,\omega }}_{t^n_k,\omega }\) is supported by paths continuous on \([t^n_k,\infty [\). We remark that \(\overline{a}_n(u,\omega ',x)=a_{n,\omega }(u,x)\) for all \(t^n_{k} \le u \le t^n_{k+2}\) and all \(\omega '\) such that \(\omega '(u)=\omega (u)\) for all \(u \le t^n_{k}\). It follows that \(Q^{a_{n}}_{t^{n}_{k},\omega }(A_k)=1\) for all \(\omega \). We deduce by induction that \(Q^{a_{n}}_{r,\omega _{0}}(\{\omega ',\;\omega '_{[r,\infty [} \in {\mathscr {C}}([r,\infty [,I\!R^{n})\}=1\).
The \(a_n\) being uniformly bounded, for given r and \(\omega _0\), the set of probabilty measures \(\{Q^{a_{n}}_{r,\omega _{0}}, n \in I\!\!N^{*}\}\) is weakly relatively compact. There is a subsequence weakly converging to a probability measure Q. From the continuity assumption on a, it follows that Q solves the martingale problem for \({\mathscr {L}}^{a,0}\) starting from \(\omega _0\) at time r. The uniqueness of the solution to this martingale problem implies that \(Q=Q^{a}_{r,\omega _0}\). The set \(\{\omega ',\;\omega '_{[r,\infty [} \in {\mathscr {C}}([r,\infty [,I\!R^n)\}\) is a closed subset of \(\varOmega \). It follows from the Portmanteau Theorem, see e.g. [2] Theorem 2.1, that \(Q^{a}_{r,\omega _0}(\{\omega ',\omega '_{[r,\infty [} \in {\mathscr {C}}([r,\infty [,I\!R^n)\}=1\)
Corollary 1
Remark 1
In the simpler case where the function a is only defined on the set of continuous paths, the continuity hypothesis is just the usual continuity hypothesis for a function defined on \(I\!R_+ \times {\mathscr {C}}([I\!R_+,I\!R^n))\) for the uniform norm topology. The associated martingale problem: probability measure solution to the martingale problem for \({\mathscr {L}}^{a,0}\) starting from \(\omega _0\) at time r can only be stated for initial continuous paths \(\omega _0\) (otherwise the pathdependent function \(a(u,\omega )\) should be defined for paths \(\omega \) which can have jumps before time u).
4 Stable Set of Probability Measures Solution to a Pathdependent Martingale Problem
In all the paper \(\varOmega \) denotes the set of càdlàg paths endowed with the Skorokhod topology. From now on, \(a(s,\omega )\) is a given progressively continuous function on \(I\!R_+ \times \varOmega \) with values in non negative matrices. We assume that a is bounded and that \(a(s,\omega )\) is invertible for all \((s,\omega )\). The explicit construction of dynamic risk measures developed here, making use of probability measures solutions to a martingale problem was first initiated in the unpublished preprint [4] in the Markovian case. We have introduced in [5] a general method to construct time consistent convex dynamic risk measures. This construction makes use of two tools. The first one is a set \({\mathscr {Q}}\) of equivalent probability measures stable by composition and stable by bifurcation (cf. [5] Definition 4.1). The second one consists in penalties \(\alpha _{s,t}(Q)\), \(s\le t\) defined for every probability measure Q in \({\mathscr {Q}}\), satisfying the local condition and the cocycle condition. The corresponding definitions are recalled in the Appendix.
4.1 Multivalued Mapping and Continuous Selector
Definition 6
X denotes the quotient of \(I\!R_+ \times \varOmega \times I\!R^n\) by the equivalence relation \(\sim \): \((t,\omega , x)\sim (t',\omega ',x')\) if \(t=t'\), \(x=x'\) and \(\omega (u)=\omega '(u) \, \forall u<t\). The metric topology on X is induced by the one to one map from X into a subset of \(I\!R_+ \times \varOmega \times I\!R^n\): \((t,\omega , x)\rightarrow (t,\omega *_tx,x)\),
where \(\omega *_tx\) has been defined in Sect. 2.2 Eq. (3).
The following observation is straightforward.
Remark 2
The set X is equipped with the metric topology defined above. Then every progressively continuous map on \(I\!R_+ \times \varOmega \) defines a unique continuous map on X.
Furthermore every map continuous on the subset \(\{(r,\omega ,x),\; \omega =\omega *_rx\}\) of \(I\!R_+ \times \varOmega \times I\!R^n\) defines also a unique continuous map on X.
Recall now the definition of a multivalued mapping from X to Y. We use here the terminology chosen in [9]. Notice that the terminology used in [1] for multivalued mapping is correspondence.
Definition 7
 1.
\(\varLambda \) is convex if \(\forall (t,\omega ,x) \in X\), \(\varLambda (t,\omega ,x)\) is a convex subset of \(I\!R^n\).
 2.
\(\varLambda \) is closed if for all \((t,\omega ,x)\), \(\varLambda (t,\omega ,x)\) is closed.
Recall the following definition of a continuous selector (Definition 16.57 of [1]).
Definition 8
A selector from a multivalued mapping \(\varLambda \) from X into \(I\!R^n\) is a function \(s: X \rightarrow I\!R^n\) such that \(s(t,\omega ,x) \in \varLambda (t,\omega ,x)\) for all \((t,\omega ,x) \in X\). A continuous selector is a selector which is continuous.
Recall the following definition from [1] (Definition 16.2 and Lemma 16.5):
Definition 9

For every closed subset F of \(I\!R^n\), \(\varLambda ^u(F)=\{(t,\omega ,x) \in X : \varLambda (t,\omega ,x) \subset F\}\) is closed

For every open subset V of \(I\!R^n\), \(\varLambda ^l(V)=\{(t,\omega ,x) \in X : \varLambda (t,\omega ,x) \cap V\ne \emptyset \}\) is open
Recall the following Michael Selection Theorem (cf. [1] Theorem 16.61)
Theorem 2
A lower hemicontinuous mapping from a paracompact space into a Banach space with non empty closed convex values admits a continuous selector.
Recall also that every metrizable space is paracompact (Theorem 2.86 of [1]).
4.2 Stable Set of Probability Measures Associated to a Multivalued Mapping
In all the following, \(\varLambda \) is a closed convex lower hemicontinuous multivalued mapping from X into \(I\!R^n\). In the following \((X_t)\) denotes the canonical process on \(\varOmega \) : For all càdlàg path \(\omega \), \(X_t(\omega )=\omega (t)\). \(({\mathscr {B}}_t)\) is the canonical filtration.
Given the progressively continuous matrix valued map a, given \(r \ge 0\), and \(\omega \in \varOmega \), we want to associate to \(\varLambda \) a stable set \({\mathscr {Q}}_{r,\omega }(\varLambda )\) of probability measures on \((\varOmega ,{\mathscr {B}})\) all equivalent with the probability measure \(Q^a_{r,\omega }\) on \({\mathscr {B}}_t\). Furthermore we want to construct a continuous function v on X. Therefore we start with continuous selectors \(\overline{\lambda }\) from \(\varLambda \).
Definition 10
Let a be progressively continuous bounded defined on \(I\!R_+ \times \varOmega \) with values in non negative matrices, such that \(a(t,\omega )\) is invertible for all \((t,\omega )\). Let \(\varLambda \) be a closed convex lower hemicontinuous multivalued mapping from X into \(I\!R^n\).

We define \(L(\varLambda )\) to be the set of continuous bounded selectors from the multivalued mapping \(\varLambda \).
 For given \(r \ge 0\) and \(\omega \in \varOmega \), the set \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\) is the stable set of probability measures generated by the probability measures \( Q_{r,\omega }^{a,a\lambda }, \overline{\lambda }\in L(\varLambda )\) with \(\lambda (t,\omega ')= \overline{\lambda }(t,\omega ',X_t(\omega '))\)$$\begin{aligned} (\frac{dQ^{a, a\lambda }_{r,\omega }}{dQ^{a}_{r,\omega }})_{{\mathscr {B}}_T}= exp[\int _r^T \langle \lambda (t,\omega '),dX_t \rangle \,\frac{1}{2} \int _r^T \langle \lambda (t,\omega '),a(t,\omega ')\lambda (t,\omega ') \rangle dt] \end{aligned}$$
We give now a description of the set \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\).
Definition 11
Remark 3
Every process \(\overline{\mu }\) in \(\tilde{L}(\varLambda )\) is bounded strictly progressive and \({\mathscr {P}} \times {\mathscr {B}}(I\!R^n)\) measurable where \({\mathscr {P}}\) is the predictable sigma algebra. However there is no uniform bound.
Proposition 2
 1.
Let a be as above and \(\overline{\mu }\in \tilde{L}(\varLambda )\). For all \(r \ge 0\) and all \(\omega \in \varOmega \), there is a unique solution to the martingale problem for \({\mathscr {L}}^{a,a\mu }\) starting from \(\omega \) at time r with \(\mu (u,\omega )=\overline{\mu }(u,\omega ,\omega (u))\). Furthermore for all \(r<s\), the map \(\omega ' \rightarrow Q^{a,a\mu }_ {s,\omega '}\) is \({\mathscr {B}}_s\) measurable and is a regular conditional probability distribution of \(Q^{a,a\mu }_ {r,\omega }\) given \({\mathscr {B}}_s\).
 2.
Given \(0 \le r \), the set \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\) is the set of all probability measures \(Q^{a, a\mu }_{r,\omega }\) for some process \(\overline{\mu }\) belonging to \(\tilde{L}(\varLambda )\).
Proof
Let \(\overline{\mu }\in \tilde{L}(\varLambda )\). There is a finite subdivision \(0=s_0< \cdots <s_i<s_{i+1}<\cdots s_k<\infty \) such that \(\overline{\mu }\) is described by Eq. (13). Let r and \(\omega \). We prove first by induction on k that there is a unique solution Q to the martingale problem for \({\mathscr {L}}^{a,a\mu }\) starting from \(\omega \) at time r and that Q belongs to \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\).
For \(k=0\) the result is true by hypothesis.
The end of the proof of the inductive step follows then from Eq. (14), from the \({\mathscr {B}}_{s_k}\) measurability of the map \(\omega ' \rightarrow Q^{a,a \lambda _{{k},j}}_{{s_{k}},\omega '}(\xi )\) and from the definition of \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\).
On the other hand it is easy to verify that the set \(\{ Q^{a,a\mu }_{r,\omega }:\;\overline{\mu }\in \tilde{L}(\varLambda )\}\) is stable. \(\square \)
5 Construction of Penalties
In the preceding section we have constructed for all given \((r,\omega )\) a stable set of probability measures \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\) associated to a multivalued mapping \(\varLambda \). In this section we construct penalties \(\alpha _{st}(Q)\) for all \(r \le s \le t\) and all \(Q \in \tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\) making use of a function g.
Lemma 1
If \(g(t,\omega ,0)=0 \;\forall (t,\omega )\), f takes values in \([0,\infty ]\).
If g takes values in \([0,\infty ]\) and satisfies \(\forall (t,\omega ),\; inf_{y \in \varLambda (t,\omega ,X_t(\omega ))} g(t,\omega ,y)=0\) then for all \((t,\omega )\), \(f(t,\omega ,0)=0\).
Notice that, since \(\varLambda \) is a closed convex multivalued mapping, replacing g by \(\tilde{g}\), one can always assume that for all \((t,\omega )\), \(dom(g(t,\omega ,.)=\{y \in I\!R^d\; g(t,\omega ,y)<\infty \}\) is closed, convex and equal to \(\varLambda (t,\omega ,X_t(\omega ))\). We assume this in all the remainder.
Definition 12
 1.g satisfies the following polynomial growth condition (GC1) if there is \(K>0\), \(m \in I\!\!N^*\) and \(\varepsilon >0\) such that$$\begin{aligned} \forall y \in \varLambda (u,\omega ,X_u(\omega )), \;g(u,\omega ,y) \le K(1+\sup _{s \le u}X_s(\omega ))^m (1+y^{2\varepsilon }) \end{aligned}$$(17)
 2.g satisfies the growth condition (GC2) if there is \(K>0\) such that$$\begin{aligned} \forall y \in \varLambda (u,\omega ,X_u(\omega )), \;g(u,\omega ,y) \le K(1+y^{2}) \end{aligned}$$(18)
Recall the following definition of BMO processes.
Definition 13
Definition 14
We need to verify that the penalties are well defined for all BMO processes and that they satisfy the local property and the cocycle condition. (Definition introduced in [5], Definition 4.3 and recalled in the Appendix).
Proposition 3
Assume that the process \(\mu \) belongs to \(BMO(Q^{a}_{r,\omega })\). Let C such that \(\mu _{BMO(Q^{a}_{r,\omega })} \le C\).

 1.
Assume that g satisfies the growth condition (GC1). Then Eq. (20) defines a random variable in \(L_p(Q^{a}_{r,\omega })\) for all \(1\le p < \infty \), and for given p, the \(L_p(Q^{a}_{r,\omega })\) norms of \(\alpha _{s,t}(Q^{a,a\mu }_{r,\omega })\) are uniformly bounded for \(r \le s \le t \le T\), for all \(\mu \) such that \(\mu _ {BMO(Q^a_{r,\omega })} \le C\). \(\alpha _{s,t}(Q^{a, a\mu }_{r,\omega })\) belongs also to \(L_1(Q^{a,a\mu }_{r,\omega })\) and the \(L_1(Q^{a,a\mu }_{r,\omega })\) norms of \(\alpha _{s,t}(Q^{a,a\mu }_{r,\omega })\) are uniformly bounded for \(\mu _ {BMO(Q^a_{r,\omega })} \le C\) and \(r \le s \le t \le T\).
 2.
Assume that g satisfies (GC2), then the random variables \(\alpha _{s,t}(Q^{a,a\mu }_{r,\omega })\) belong to \(L_{\infty }(Q^{a}_{r,\omega })\) and are uniformly bounded for \(\mu _ {BMO(Q^a_{r,\omega })} \le C\) and \(r \le s \le t \le T\).
 3.
In case g is non negative, Eq. (20) defines a non negative \({\mathscr {B}}^r_s\) random variable.
 1.
 Assume that g satisfies the growth condition (GC1) or (GC2). Then the penalty defined in (20) satisfies the cocycle condition for every \(Q^{a, a\mu }_{r,\omega }\): Let \(r \le s \le t \le u\)$$\begin{aligned} \;\;\alpha _{s,u}(Q^{a, a\mu }_{r,\omega })=\alpha _{s,t}(Q^{a, a\mu }_{r,\omega })+E_{Q^{a,a \mu }_{r,\omega }}(\alpha _{t,u}(Q^{a, a\mu }_{r,\omega }){\mathscr {B}}_{s}) \end{aligned}$$(21)

The penalty defined in (20) is local on \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\)

If \(g(t,\omega ,0)=0\; \forall (t,\omega ) \in I\!R^+ \times \varOmega \), The probability measure \(Q^{a}_{r,\omega }\) has zero penalty.
Proof
 1.Assume that the function g satisfies the growth condition (GC1). Without loss of generality one can assume that \(m \ge 2\). Choose \(p_1>1\) such that \((2\varepsilon )p_1=2\). Let q be the conjugate exponent of \(p_1\). It follows from the conditional Hölder inequality and the equivalence of the BMO norms with respect to \(Q^{a}_{r,\omega }\) and \(Q^{a,a \mu }_{r,\omega }\) thatLet \(p_0\) be such that Eq. (19) is satisfied for \(P=Q^a_{r,\omega }\). Let \(q_0\) be the conjugate exponent of \(p_0\). It follows from conditional Hölder inequality and (19) that$$\begin{aligned} E_{Q^{a,a \mu }_{r,\omega }}( \int \limits _{s}^{t} (1+\sup _{s \le u}X_s(\omega ))^m \mu _u(\omega )^{2\varepsilon }d u{\mathscr {B}}_{s}) \nonumber \\ \le K_1C^{\frac{1}{p_1}}[E_{Q^{a,a\mu }_{r,\omega }} ( \sup _{s \le s' \le u}(1+X_{s'})^{mq}){\mathscr {B}}_s]^{\frac{1}{q}} (ts)^{\frac{1}{q}} \end{aligned}$$(22)for all \(j \ge 1\). The first assertion of 1 of the proposition follows then from the Eqs. (22) and (23) and the inequality \(E_{Q^a_{r,\omega }}(\sup _{s \le u \le t}(1+X_t)^{k}))<\infty \) for all \(k \ge 2\) ( [16], Chap. 2 Sect. 5). The second asssertion of 1. of the proposition follows from Eq. (22) and then from Eq. (23) applied with \({\mathscr {B}}_s\) equal to the trivial sigma algebra.$$\begin{aligned}&E_{Q^{a,a \mu }_{r,\omega }}( \sup _{s' \le u }(1+X_{s'})^{mq}{\mathscr {B}}_s)) \le K_C E_{Q^{a}_{r,\omega }}(\sup _{s \le s' \le t}(1+X_{s'})^{mqq_0}{\mathscr {B}}_s)^{\frac{1}{q_0}}\nonumber \\&\qquad \qquad \qquad \qquad \qquad \le K_C E_{Q^{a}_{r,\omega }}(\sup _{s \le s' \le t}(1+X_{s'})^{mqjq_0}{\mathscr {B}}_s)^{\frac{1}{q_0j}} \end{aligned}$$(23)
 2.Assume that g satisfies the the growth condition (GC2). ThusThe result follows then from the BMO condition.$$\alpha _{st}(Q^{a,a\mu }_{r,\omega }) \le K E_{Q^{a,a\mu }_{r,\omega }}( \int \limits _{s}^{t} (1+\mu _u(\omega )^2) d u{\mathscr {B}}_{s})$$
 3.
The case g non negative is trivial.

The cocycle condition (21) follows easily from the definition (20) and the above integrability.

We prove now that the penalty \(\alpha \) is local on \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\). Let \(\overline{\mu },\overline{\nu }\in \tilde{L}(\varLambda )\). The probability measures \(Q^{a, a\mu }_{r,\omega }\) and \(Q^{a, a\nu }_{r,\omega }\) are equivalent to \(Q^{a}_{r,\omega }\). Let \(r \le s \le t\) and A be \({\mathscr {B}}_{s}\)measurable. Assume that for all X in \(L^{\infty }({\mathscr {B}}_{t}),\; E_{Q^{a, a\mu }_{r,\omega }}(X{\mathscr {B}}_{s})1_A= E_{Q^{a, a\nu }_{r,\omega }}(X{\mathscr {B}}_{s})1_A\). It follows from the equality \(\frac{{\mathscr {E}}(a\mu )_t}{{\mathscr {E}}(a\mu )_s} 1_A=\frac{{\mathscr {E}}(a\nu )_t}{{\mathscr {E}}(a\nu )_s} 1_A\) and the \({\mathscr {P}} \times {\mathscr {B}}(I\!R^n)\) measurability of \(\overline{\mu }\) and \(\overline{\nu }\) that \(1_{]s,t[}1_A\mu =1_{]s,t[}1_A\nu \) \(Q^{a}_{r,\omega }\) a.s. From (20) we get \(\alpha _{s,t}(Q^{a,a \mu }_{r,\omega })1_A=\alpha _{s,t}(Q^{a,a \nu }_{r,\omega })1_A\). Thus the penalty \(\alpha \) is local on \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\).

The last point follows easily from the definition of the penalty. \(\square \)
6 Time Consistent Dynamic Risk Measures Associated to Pathdependent Martingale Problems
We change the sign in the classical definition of risk measures in order to avoid the minus sign which appears in the time consistency property for usual dynamic risk measures. In fact \(\rho _{st}(X)\) are “usual” dynamic risk measures.
6.1 Normalized TimeConsistent Convex Dynamic Risk Measures
Proposition 4
For given \(0 \le r \le t\) and Y in \(L^{\infty }(\varOmega ^r,{\mathscr {B}}^r_{t},Q^{a}_{r,y})\), the process \((\rho ^{r,\omega }_{s,t}(Y))_{r \le s \le t}\) admits a càdlàg version.
Proof
The proof of the regularity of paths which was given in [6] Theorem 3 for normalized convex dynamic risk measures time consistent for stopping times can be extended to normalized convex dynamic risk measures time consistent for deterministic times. \(\square \)
We have the following extension of the dynamic risk measure to random variables essentially bounded from below:
Corollary 2
The definition of \(\rho ^{r,\omega }_{s,t}(Y)\) can be extended to random variables Y \(({\mathscr {B}}_t)\)measurable which are only essentially bounded from below.
\(\rho ^{r,\omega }_{s,t}(Y)=\lim _{n \rightarrow \infty } \rho ^{r,\omega }_{s,t}(Y\wedge n)\). For every Y essentially bounded from below, the process \((\rho ^{r,\omega }_{s,t}(Y))\) is optional.
Proof
Let Y be \({\mathscr {B}}_t\)measurable and \(Q^a_{r,\omega }\)essentially bounded from below, Y is the increasing limit of \(Y_n=Y \wedge n\) as n tends to \(\infty \). Define \(\rho ^{r,\omega }_{s,t}(Y)\) as the increasing limit of \(\rho ^{r,\omega }_{s,t}(Y_n)\). As we already know that for given s and t, \(\rho ^{r,\omega }_{s,t}(Y) \) defined on bounded random variables by formula (24) is continuous from below, the extended definition coincides with the previous one on \(Q^{a}_{r,\omega }\)essentially bounded random variables.
From Proposition 4 for every n one can choose a càdlàg version of the process \(\rho ^{r,\omega }_{s,t}(Y_n)\). Thus the map \((s,\omega ) \rightarrow \rho ^{r,\omega }_{s,t}(Y)= \lim \rho ^{r,\omega }_{s,t}(Y_n)\) is measurable for the optional sigma algebra. \(\square \)
6.2 General TimeConsistent Convex Dynamic Risk Measures
In this section the function g (and thus the penalty) is not assumed to be non negative.
Definition 15
In the following, \(p_0\) is chosen such that the reverse Hölder inequality (19) is satisfied for \(a \phi \).
Theorem 3
Let \((r,\omega )\). Assume that the multivalued set \(\varLambda \) is \(BMO(Q^{a}_{r,\omega })\). Let \(\tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\) be the stable set of probability measures defined in Definition 10.

Assume that g satisfies the growth condition (GC1). The above Eq. (25) defines a dynamic risk measure \((\rho ^{r,\omega }_{s,t})\) on \(L_{p}(Q^{a}_{r,\omega },({\mathscr {B}}_t))\) for all \(q_0\le p <\infty \), (where \(q_0\) is the conjugate exponent of \(p_0\) chosen as above). These dynamic risk measures are time consistent for stopping times taking a finite number of values.

Assume that g satisfies the growth condition (GC2). The above Eq. (25) defines a dynamic risk measure \((\rho ^{r,\omega }_{s,t})\) on \(L_{\infty }(Q^{a}_{r,\omega },({\mathscr {B}}_t))\) , and also on every \(L_{p}(Q^{a}_{r,\omega },({\mathscr {B}}_t))\) for \(q_0 \le p < \infty \). These dynamic risk measures are time consistent for stopping times taking a finite number of values.
Proof
There is a constant \(C>0\) such that for all \(Q^{a, a\mu }_{r,\omega }\in \tilde{\mathscr {Q}}_{r,\omega }(\varLambda )\), \(a\mu _{BMO(Q^{a}_{r,\omega })} \le C\). It follows from the reverse Hölder inequality (19), that for all non negative measurable Y, \(E_{Q^{a,a\mu }_{r,\omega }}(Y{\mathscr {B}}_s) \le K_C (E_{Q^{a}_{r,\omega }}(Y^{q_0}{\mathscr {B}}_s)^{\frac{1}{q_0}}\). Thus \(Y \rightarrow E_{Q^{a,a\mu }_{r,\omega }}(Y{\mathscr {B}}_s) \) defines a linear continuous map on \(L_p(Q^{a}_{r,\omega })\) with values \(L_p(Q^{a}_{r,\omega })\) for all \(q_0 \le p \le \infty \), and that for given p, the norms of these linear maps are uniformly bounded for \({\varLambda }\) valued.
From Proposition 3, it follows then that Eq. (25) defines a dynamic risk measure \((\rho ^{r,\omega }_{s,t})\) on \(L_{p}(Q^{a}_{r,\omega },({\mathscr {B}}_t))\) for all \(q_0 \le p < \infty \) in case (GC1). Under assumption (GC2), equation (25) defines a dynamic risk measure \((\rho ^{r,\omega }_{s,t})\) on \(L_{p}(Q^{a}_{r,\omega },({\mathscr {B}}_t))\) for all \(L_p\), \(q_0 \le p \le \infty \).
The time consistency for stopping times taking a finite number of values follows from the stability property of the set of probability measures as well as the cocycle and local property of the penalties (cf. [5] in \(L_{\infty }\) case). The proof is the same in \(L_p\) case.
7 Strong Feller Property
7.1 Feller Property for Continuous Parameters
We assume that the progressively measurable function g is a Caratheodory function on \(I\!R_+ \times \varOmega \times I\!R^n\), that is for all u, \((\omega ,x) \rightarrow g(u,\omega ,x)\) is continuous. The support of \(Q^{a,\mu }_{r,\omega }\) is contained in the paths \(\omega '\) continuous on \([r,\infty [\) (Proposition 1) and which coincide with \(\omega \) on [0, r]. It follows that for every function \(\lambda \) progressively continuous bounded, and all \(u > r\), the function \(\omega ' \rightarrow g(u,\omega ',\lambda (u,\omega '))\) is continuous on the support of \(Q^{a,a\lambda }_{r,\omega }\). We prove then the following Feller property for the penalty.
Proposition 5
Let a be progressively continuous bounded such that \(a(s,\omega )\) is invertible for all \((s,\omega )\). Let \(\lambda \) be progressively continuous bounded. Assume that g is a real valued Caratheodory function satisfying the growth condition (GC1) or (GC2).
 1.There is a strictly progressive real valued map L(g) on \([0,t] \times \varOmega \times I\!R^n\) continuous on \(\{(s,\omega ,x),\; \omega =\omega *_sx\}\) such that$$\begin{aligned} E_{Q^{a,a\lambda }_{s,\omega *_s x}}\int _s^t g(u, \omega ',\lambda (u,\omega ') du )=L(g)(s,\omega ,x) \;\;\;\forall s \le t\;\; \omega \; \text {and} \; x \end{aligned}$$(26)
 2.For all \(0 \le r \le s \le t\), and \(\omega \in \varOmega \), there is a \(Q^{a, \lambda }_{r,\omega }\)null set N such that for all \(\omega _1 \in N^c\),$$\begin{aligned} E_{Q^{ a, a\lambda }_{r,\omega }}(\int _s^t g(u, \omega ',\lambda (u,\omega ')) du {\mathscr {B}}_s)(\omega _1)=L(g)(s,\omega _1,X_s(\omega _1)) \end{aligned}$$(27)
Proof
We only need to prove 1.
Step 1: Assume that the function g is bounded. Then \(\int _s^t g(u, \omega ',\lambda (u,\omega ')) du\) is a continuous bounded function of \(\omega '\) on the support of \(Q^{a,a\lambda }_{s,\omega }\). The map \(\lambda \) being progressively continuous bounded, the continuity property for L(g) follows easily from Theorem 1.
Step 2: general case. Notice that \(\lambda \) is bounded.
Thus under assumption (GC2), \(g(u,\omega ',\lambda (u,\omega ')\) is uniformly bounded and the continuity property of L(g) follows from step 1.
We introduce now a class of \({\mathscr {B}}_t\) measurable functions on \(\varOmega \) satisfying a continuity condition derived from the progressive continuity condition that we have introduced for progressive functions and from the continuity property proved in Theorem 1.
Definition 16

\(h(\omega )=\tilde{h} (\omega *_t X_t(\omega ),X_t(\omega ))\)

\(\tilde{h} (\omega ,x)=\tilde{h} (\omega ',x) \; \text {if}\; \omega (u)=\omega '(u) \;\;\forall u<t\)
Corollary 3
7.2 Feller Property for the Dynamic Risk Measure
Proposition 6
Proof
The proof is done in two steps. The first step is the construction of \(\varPhi _{\mu }(h)\) given \(\mu \). The second step is the construction of \(\nu _s\) given \(\mu \) and s. \(\mu \) belongs to \(\tilde{L}(\varLambda )\). From Definition 11, let \(0=s_0< \cdot \cdot <s_i<s_{i+1} \cdot \cdot <s_k<s_{k+1}=\infty \) be a finite partition such that Eq. (13) is satisfied.
 First step: construction of \(\varPhi _{\mu }(h)\). We construct \(\varPhi _{\mu }(h)\) recursively on \([s_i,s_{i+1}[\). Let \( s_n\) be such that \(s_n<t \le s_{n+1}\). From Corollary 3, for all \(j \in I_n\) there is a strictly progressive map \(L^{a,\lambda _{n,j}}(h)\) continuous on \(\{(u,\omega ,x),\; \omega =\omega *_ux,\; u \le t\}\) satisfying Eq. (29). LetLet \(h_n(\omega )= \varPhi _{\mu }(h)(s_n,\omega ,X_{s_n}(\omega ))\). The function \(h_n\) belongs to \({\mathscr {C}}_{s_n}\) and \(\tilde{h}_n(\omega ,x)= \varPhi _{\mu }(h)(s_n,\omega ,x)\). Then we can proceed on \([s_{n1},s_{n}[\) with \(h_n\). We construct recursively the strictly progressive map \(\varPhi _{\mu }(h)\) continuous on \(\{(u,\omega ,x),\; \omega =\omega *_ux,\; u \le t\}\). Notice that for all \(s \in [s_{i},s_{i+1}]\), there are \({\mathscr {B}}_{s}\) measurable sets \((C_{s,j})_{j \in I_i}\), such that$$\begin{aligned} \varPhi _{\mu }(h)(s,\omega ,x)=\sup _{j \in I_{n}}L^{a,\lambda _{n,j}}(h)(s,\omega ,x)\;\; \forall s \in [s_{n},t[ \end{aligned}$$(33)$$\begin{aligned} \varPhi _{\mu }(h)(s,\omega ,x)=\sum _{j \in I_{i}}1_{C_{s,j}}(\omega )L^{a,\lambda _{i,j}}(h_{i+1})(s,\omega ,x) \end{aligned}$$(34)

Second step: Given \(s \in [r,t]\), construction of the process \(\nu _s\).
There is a unique k such that \(s \in ]s_k, s_{k+1}]\). For \(i>k\) for all \(u \in ]s_i,s_{i+1}]\), defineAnd for \(u \in ]s,s_{k+1}]\), define$$\begin{aligned} \nu _s(u,\omega )=\sum _{j \in I_{i}}1_{C_{s_i,j}}(\omega )\lambda _{i,j}(u,\omega )\;\ \end{aligned}$$(35)and \(\nu _s(u,\omega )=\mu (u,\omega )\) for all \(0 \le u \le s\). It follows from the construction of \(\nu _s\) that the process \(\nu _s\) belongs to \(\tilde{L}(\varLambda )\). It follows also recursively that for all \(i>k\) and \(\omega \in \varOmega \),$$\begin{aligned} \nu _s(u,\omega )=\sum _{j \in I_{k}}1_{C_{s,j}}(\omega )\lambda _{k,j}(u,\omega )\;\ \end{aligned}$$(36)and for all \(\omega \in \varOmega \),$$\begin{aligned} E_{Q^{a, a\nu _s}_{s_i,\omega }}(h)\alpha _{s_i,t}(Q^{a, a\nu _s}_{s_i,\omega })= \varPhi _{\mu }(h)(s_i,\omega ,X_{s_i}(\omega )) \end{aligned}$$(37)By construction the following inequality is satisfied:$$\begin{aligned} E_{Q^{a, a\nu _s}_{s,\omega }}(h)\alpha _{s,t}(Q^{a, a\nu _s}_{s,\omega })= \varPhi _{\mu }(h)(s,\omega ,X_s(\omega )) \end{aligned}$$(38)It follows then from Proposition 2 that$$\begin{aligned} E_{Q^{a, a\mu }_{s,\omega }}(h)\alpha _{s,t}(Q^{a, a\mu }_{s,\omega })\le \varPhi _{\mu }(h)(s,\omega ,X_s(\omega )) \end{aligned}$$(39)and$$ E_{Q^{a, a\mu }_{r,\omega _0}}(h{\mathscr {B}}_s) \alpha _{s,t}(Q^{a, a\mu }_{r,\omega _0}) \le E_{Q^{a, a\nu _s}_{r,\omega _0}}(h{\mathscr {B}}_s) \alpha _{s,t}(Q^{a, a\nu _s}_{r,\omega _0})\;\;Q^{a}_{r,\omega _0}\;a.s. $$$$\begin{aligned}{}[E_{Q^{a, a\nu _s}_{r,\omega _0}}(h{\mathscr {B}}_s) \alpha _{s,t}(Q^{a, a\nu _s}_{r,\omega _0})](\omega ')= \varPhi _{\mu }(h)(s,\omega ',\omega '(s))\;\;Q^{a}_{r,\omega _0}\;a.s. \end{aligned}$$
Theorem 4
Proof
For all \(\mu \in \tilde{L}(\varLambda )\), let \(\varPhi _{\mu }(h)\) be the strictly progressive map, continuous on \(\{(u,\omega ,x),\,\omega =\omega *_ux,\,u \le t\}\) constructed in Proposition 6. Let \(\overline{R}(h)=\sup _{\mu \in \tilde{L}(\varLambda )}\varPhi _{\mu }(h)\). The function \(\overline{R}(h)\) is then lower semi continuous on \(\{(u,\omega ,x),\; \omega =\omega *_ux,\; u \le t\}\). Let \(R(h)(u,\omega )=\overline{R}(h)(u,\omega ,X_u(\omega ))\). Equations (40) and (41) follow easily from Proposition 6.
8 Existence of Viscosity Solutions for Pathdependent PDEs
8.1 Existence of Viscosity Supersolutions
Theorem 5
Fix \((t_0,\omega _0)\). Assume that the mutivalued set \(\varLambda \) is \(BMO(Q^{a}_{t_0,\omega _0})\) (Definition 15). Assume that the function g satisfies the preceding hypothesis (g is a Caratheodory function and satisfies the growth condition (GC1) or (GC2)). Assume furthermore that g is upper semicontinuous on \(\{(s,\omega ,y),(s,\omega ) \in X,\; y \in \varLambda (s,\omega ,\omega (s)\}\). For all r and \(\omega \), let \((\rho ^{r,\omega }_{s,t})\) be the dynamic risk measure given by Eq. (24) where the penalty satisfies Eq. (20).
Let \(h \in {\mathscr {C}}_t\). The function R(h) is progressive and \(\overline{R}(h)\) is lower semi continuous on \(\{(u,\omega ,x),\; \omega =\omega *_ux,\; u \le t\}\) (Theorem 4). R(h) is a viscosity supersolution of the pathdependent second order partial differential equation (43) at each point \((t_0,\omega _0)\) such that \(f(t_0,\omega _0, a(t_0,\omega _0)z)\) is finite for all z.
Proof
Let \(x_0=\omega _0(t_0)\). From Theorem 4, the function R(h) is progressive and \(\overline{R}(h)\) is lower semi continuous on \(\{(u,\omega ,x),\; \omega =\omega *_ux,\; u \le t\}\). We prove first that R(h) is bounded from below on some \(D_{\varepsilon }(t_0,\omega _0)\). \(R(h)(u,\omega ) \ge E_{Q^a_{u,\omega }}(h)\alpha _{ut}(Q^a_{u,\omega })\). For all given \(k \ge 2\), \(E_{Q^a_{u,\omega }}(\sup _{s \le u \le t}(1+X_t)^{k}))\) is uniformly bounded for \((u,\omega ) \in D_{\varepsilon } (t_{0},\omega _{0})\). The result follows then from either the (GC1) condition or the (GC2).
Let \(\phi \) progressive, \(\overline{\phi }\) in \({\mathscr {C}}_b^{1,0,2} (I\!R_+ \times \varOmega \times I\!R^n)\) such that \(\phi (t_0,\omega _0)=R(h)(t_0,\omega _0)\) and \((t_0,\omega _0)\) is a local minimizer of \(R(h) \phi \) on \(D_{\eta }(t_0,\omega _0)\) for some \(\eta >0\).

Step 1: Continuity properties
By hypothesis \(f(t_0,\omega _0, a(t_0,\omega _0)D_x\overline{\phi }(t_0,\omega _0,x_0))< \infty \). Thus for all \(\varepsilon >0\), there is \(\lambda _0 \in \varLambda (t_0,\omega _0)\) such thatThe multivalued set \(\varLambda \) is assumed to be lower hemicontinuous. It follows that for all \(K>0\), \(\varLambda _K\) is also lower hemicontinuous, where \(\varLambda _K(u,\omega ,x)=\{z \in \varLambda (u,\omega ,x),\, z < K\}\). Choose \(K>\lambda _0\). From Theorem 2, there is thus a continuous bounded selector \(\overline{\lambda }(u,\omega ,x)\) of \(\varLambda _K\) defined on X such that \(\overline{\lambda }(t_0,\omega _0,x_0)=\lambda _0\).$$\begin{aligned} D_x\overline{\phi }(t_0,\omega _0,x_0)^t a (t_0,\omega _0)\lambda _0 g(t_0,\omega _0,\lambda _0)> f(t_0,\omega _0, a(t_0,\omega _0) D_x\overline{\phi }(t_0,\omega _0,x_0))  \varepsilon \end{aligned}$$(44)From the upper semicontinuity condition satisfied by g, and the continuity of the map \(\overline{\lambda }\), it follows that for all \(\varepsilon >0\), there is \(\eta _1>0\), such that for \(t_0 \le u \le t \le t_0+\eta _1\), \( d(\omega ,\omega _0) <\eta _1\) and \(\omega (t)x_0<\eta _1\),From the continuity of the function \(\overline{\lambda }\), the hypothesis \(\overline{\phi }\in {\mathscr {C}}_b^{1,0,2}\) and the progressive continuity of a, there is \(\eta _2\) such that for \(t_0 \le u \le t \le t_0+\,\eta _2\), \(xx_0<\eta _2\) and \( d(\omega *_ux,\omega _0) <\eta _2\),$$\begin{aligned} g(t,\omega ,\overline{\lambda }(t,\omega ,\omega (t)))g(t_0,\omega _0,\lambda _0)< \varepsilon \end{aligned}$$(45)The maps a and \(\lambda \) are bounded. It follows from [22] that there is \(0<\alpha < inf(\eta ,\eta _1,\eta _2)\) such that$$\begin{aligned}&\qquad \qquad \qquad \partial _u \overline{\phi }(u, \omega ,x)+ \frac{1}{2}Trace(D^2_x\overline{\phi }\overline{a}(u,\omega ,x))+(D_x \overline{\phi }^t \overline{a} \overline{\lambda })(u,\omega ,x)\nonumber \\&\partial _u \overline{\phi }(t_0,\omega _0 , x_0)+ \frac{1}{2}Trace(D_x^2 \overline{\phi }\overline{a})(t_0,\omega _0,x_0))+D_x \overline{\phi }^t \overline{a}(t_0,\omega _0,x_0)\lambda _0 \le \varepsilon \end{aligned}$$(46)Let \(C =\{\omega ,\;\omega (u)=\omega _0(u)\; \forall 0 \le u \le t_0,\;\; \sup _{t_0 \le u \le t_0+\alpha } \omega (u)\omega _0(t_0) < inf(\eta ,\eta _1,\eta _2)\}\)$$\begin{aligned} Q^{a, a\lambda }_{t_0,\omega _0}(A)<\varepsilon \;\; with \;\;A=\{\omega \;\; \sup _{t_0 \le u \le t_0+ \alpha }\omega (u)\omega _0(t_0) \ge inf(\eta ,\eta _1,\eta _2)\;\} \end{aligned}$$(47) 
Step 2: Time consistency
For all \(0<\beta <\alpha \), let \(\delta \) be the stopping time \(\delta =\beta 1_C\). The stopping time \(\delta \) takes only 2 different values. By definition of the probability measure \(Q^{a, a\lambda }_{t_0,\omega _0}\), it follows from (47) that \(Q^{a, a\lambda }_{t_0,\omega _0}(C)>(1\varepsilon )\).
The dynamic risk measure \((\rho ^{t_0,\omega _0}_{u,v})_{0 \le u \le v}\), is time consistent for stopping times taking a finite number of values, thusFrom Theorem 4, the lower semi continuous function \(\overline{R}(h)\) satisfies: \((\rho ^{t_0,\omega _0}_{t_0 +\delta ,t}(h)(\omega )=\overline{R}(h)(t_0+\delta ,\omega , X_{t_0+\delta }(\omega ))\) \(Q^{a}_{t_0,\omega _0}\) a.s., and \(\rho ^{t_0,\omega _0}_{t_0,t}(h)=R(h)(t_0,\omega _0)\). Let \(\overline{\lambda }\) be the continuous function defined in step 1. By hypothesis \(R(h) \ge \phi \) on \(D_{\eta }(t_0,\omega _0)\). For all \(\omega \in C\) and \(u \le \beta \), \((u,\omega *_u \omega (u)) \in D_{\eta }(t_0,\omega _0)\). Since the functions R(h) and \(\phi \) are progressive it follows that \(R(h) \ge \phi \) on \([t_0,t_0 +\,\beta ] \times C\). It follows then from the equality \(\phi (t_0,\omega _0)=R(h)(t_0,\omega _0)\) and from the definition of \(\rho ^{t_0,\omega _0}_{t_0,t_0 +\delta }\) that$$\begin{aligned} \rho ^{t_0,\omega _0}_{t_0,t}(h)=\rho ^{t_0,\omega _0}_{t_0,t_0+\delta }(\rho ^{t_0,\omega _0}_{t_0 +\delta ,t}(h)) \end{aligned}$$(48)$$\begin{aligned} \phi (t_0,\omega _0)\ge E_{Q^{a,a \lambda }_{t_0,\omega _0}}[\overline{\phi }(t_0+\delta ,\omega ,X_{t_0+\delta }(\omega ))\int _{t_0}^{t_0+\delta } g(u, \omega ,\lambda (u,\omega ,X_u(\omega )))du] \end{aligned}$$(49) 
Step 3: Martingale problem
The probability measure \(Q^{a,a\lambda }_{t_0,\omega _0}\) is solution to the martingale problem for \({\mathscr {L}}^{a,a\lambda }\) starting from \(\omega _0\) at time \(t_0\). The function \(\overline{\phi }\) is strictly progressive and belongs to \({\mathscr {C}}_b^{1,0,2} (I\!R_+ \times \varOmega \times I\!R^n)\). It follows from the martingale property proved in [3] that$$\begin{aligned}&0 \ge E_{Q^{a, a\lambda }_{t_0,\omega _0}}[\int _{t_0}^{t_0+\delta }(\partial _u \overline{\phi }(u, \omega ,X_u(\omega ))+ \frac{1}{2}Trace((D^2_x\overline{\phi }\overline{a})(u,\omega ,X_u(\omega ))))du ] \nonumber \\&\qquad + E_{Q^{a,a\lambda }_{t_0,\omega _0}}[ \int _{t_0}^{t_0+\delta }(D_x\overline{\phi }^t \overline{a} \overline{\lambda })(u, \omega ,X_u(\omega ))g(u, \omega ,\overline{\lambda }(u,\omega ,X_u(\omega )))du] \end{aligned}$$(50) 
Step 4: Conclusion
Divide (50) by \(\beta \) and let \(\beta \) tend to 0. It follows from the definitions of C and \(\delta \) and the Eqs. (44)–(46) proved in step 1 and \(Q^{a,a\lambda }_{t_0,\omega _0}(C)>1\varepsilon \) thatThis gives the result. \(\square \)$$ \partial _u \overline{\phi }(t_0,\omega _0,x_0)\,\,{\mathscr {L}} \overline{\phi }(t_0,\omega _0,x_0)\,\,f(t_0, \omega _0,\sigma ^t(t_0,\omega _0)D_x\overline{\phi }(t_0,\omega _0,x_0)) \ge 2\varepsilon (1\varepsilon ) $$
8.2 Existence of Viscosity Subsolutions
In this section we will assume that the set \(\varLambda \) has some uniform BMO property.
Definition 17
Of course the above condition is satisfied if \( \sup _{\omega }\int _0 ^\infty \varphi (s,\omega )^2 ds<\infty \).
The name “uniform BMO” property is justifed by the following result.
Lemma 2
Assume that the multivalued mapping \(\varLambda \) is uniformly BMO with respect to a. Then for all \((r,\omega )\) and all process \(\mu \) \(\varLambda \) valued such that \(\overline{\mu }\) is \({\mathscr {P}} \times {\mathscr {B}}(I\!R^n)\) measurable, \(\mu \) belongs to \(BMO(Q^{a}_{r,\omega })\) and \(\mu _{BMO(Q^{a}_{r,\omega })} \le C\)
Proof
Theorem 6
Let \((t_0,\omega _0)\) be given. Assume that the mutivalued set \(\varLambda \) is uniformly BMO with respect to a. Assume that the function g is a Caratheodory function satisfying the growth condition (GC1) or (GC2) and that the Fenchel transform f of g is progressively continuous.
Let \(h \in {\mathscr {C}}_t\). The map \(R(h)^*\) is progressive, \(\overline{R(h)^*}\) is upper semicontinuous in viscosity sense. \(R(h)^*\) is a viscosity subsolution of the pathdependent second order partial differential equation (43).
Proof
Let \(x_0=\omega _0(t_0)\). The progressivity of \(R(h)^*\) follows from the equality \(D_{\eta }(s,\omega )=D_{\eta }(s,\omega *_s\omega (s))\). The upper semicontinuity property follows from the definition of \(R(h)^*\). We prove first that R(h) is bounded on some \(D_{\varepsilon }(t_0,\omega _0)\). \(R(h)(u,\omega )= \sup _{\mu } (E_{Q^{a,a\mu }_{u,\omega }}(h)\alpha _{u,t}(Q^{a,a\mu }_{u,\omega }))\). For given \(k \ge 2\), \(E_{Q^a_{u,\omega }}(\sup _{s \le u \le t}(1+X_t)^{k}))\) is uniformly bounded for \((u,\omega ) \in D_{\varepsilon }\). The result follows then from either the (GC1) condition or the (GC2), and from the uniform BMO hypothesis with similar arguments as in the proof of Proposition 3.
Let \(\phi \) progressive, \(\overline{\phi }\in {\mathscr {C}}_b^{1,0,2} (I\!R_+ \times \varOmega \times I\!R^n)\) such that \(\phi (t_0,\omega _0)=R(h)^*(t_0,\omega _0)\) and such that \((t_0,\omega _0)\) is a maximizer of \(R(h)^* \phi \) on \(D_{\eta }(t_0,\omega _0)\).
 Step 1: Making use of the progressive continuity property of a, f and of the regularity of \(\overline{\phi }\), for all \(n \in I\!\!N^*\), there is \(\eta _n>0\), \(t_0+\eta _n<t\) such that for \(t_0 \le u \le t_0+\eta _n\), \(d(\omega _o,\omega )< \eta _n\) and \(x_0\omega (u)<\eta _n\),$$\begin{aligned} f(u,\omega , (\overline{a} D_x\overline{\phi })(u,\omega ,\omega (u))) \le f (t_0,\omega _0, (\overline{a} D_x\overline{\phi })(t_0,\omega _0,x_0))+ \frac{1}{n} \end{aligned}$$(53)Without loss of generality one can assume \(\eta _n<\eta \). The matrix valued process a being bounded, it follows from [22] that there is \(h_n\) such that for all \(t_0 \le s \le t_0+\eta \) and \(\omega \in D_{\eta }(t_0,\omega _0)\),$$\begin{aligned}&\partial _u \overline{\phi }(u, \omega ,\omega (u))+ \frac{1}{2}Trace(D^2_x \overline{\phi }\overline{a})(u,\omega ,\omega (u)))\nonumber \\&\qquad \partial _u \overline{\phi }(t_0, \omega _0,x_0)+ \frac{1}{2}Trace(D^2_x \overline{\phi }\overline{a})(t_0,\omega _0,x_0)) \le \frac{1}{n} \end{aligned}$$(54)Without loss of generality one can assume that \(h_n <\frac{\eta _n}{2}\). For all \(n>0\) choose \((t_n,\omega _n) \in D_{\frac{\eta _n}{2}}(t_0,\omega _0)\) such that \( \lim _{n \rightarrow \infty } R(h)(t_n,\omega _n)=R(h)^*(t_0,\omega _0) \) and$$\begin{aligned} Q^{a}_{s,\omega }(\{\omega ',\;\sup _{s \le u \le s+h_n} \omega '(u)\omega (s)>\frac{\eta _n}{2}\})<\varepsilon \end{aligned}$$(55)Let \(C_n=\{\omega ',\; \sup _{t_n \le u \le t_n+h_n}\omega '(u)\omega _n(t_n) \le \frac{\eta _n}{2},\; \omega '(v)=\omega _n(v),\; \forall v \le t_n\}\). It follows from Eq. (55) that \(Q^a_{t_n,\omega _n}(C_n)>1\varepsilon \) for all n. From Lemma 2 there is a constant \(C'>0\) such that \( a\mu _{BMO(Q^{a}_{t_n,\omega _n})} \le C'\) for all \(\mu \in \tilde{L}(\varLambda )\) and all n. From [15] it follows that there is \(p_0\) such that the reverse Hölder inequality (19) is satisfied for all \({\mathscr {E}}(a\mu )\) and thus that for all \(\mu \in \tilde{L}(\varLambda )\), and all n, \(Q^{a,a\mu }_{t_n,\omega _n}(C_n^c) \le K_C (\varepsilon )^{\frac{1}{q_0}}\) where \(q_0\) is the conjugate exponent of \(p_0\). The constants \(q_0\) and \(K_c\) depend neither on \(\mu \) nor on n. Thus \(\varepsilon \) can be chosen such that \(Q^{a,a\mu }_{t_n,\omega _n}(C_n)> \frac{1}{2}\) for all n and all \(\mu \in \tilde{L}(\varLambda )\). Let \(\delta _n\) be the stopping time taking only two values \(h_n\) and 0 defined by \(\delta _n=h_n1_{C_n}\).$$\begin{aligned} \phi (t_n,\omega _n) \le R(h)(t_n,\omega _n) +\frac{h_n}{n} \end{aligned}$$(56)

Step 2: Time consistency
Making use of the time consistency of the risk measure \((\rho ^{t_n,\omega _n}_{u,v})\), and of the following equations deduced from Theorem 4,$$ R(h)(t_n,\omega _n)=\rho ^{t_n,\omega _n}_{t_n,t}(h) $$it follows that$$ \rho ^{t_n,\omega _n}_{t_n+\delta _n,t}(h)=R(h)(t_n+\delta _n,.)\;\; Q^a_{t_n,\omega _n}\;a.s. $$It follows from the definition of the risk measure \((\rho ^{t_n,\omega _n}_{t_n,t_n+\delta _n})\), that for all n there is a process \(\mu _n\) in \(\tilde{L}(\varLambda )\) such that$$ R(h)(t_n,\omega _n)=\rho ^{t_n,\omega _n}_{t_n,t_n+\delta _n}(R(h)(t_n+\delta _n,.)) $$For all \(\omega ' \in C_n\), \((t_n+h_n,\omega '*_{t_n+h_n}\omega '(t_n+h_n)) \in D_{\eta }(t_0,\omega _0)\). The functions R(h) and \(\phi \) are progressive and satisfy \( R(h) \le R(h)^* \le \phi \) on \(D_{\eta }(t_0,\omega _0)\). It follows that$$\begin{aligned} R(h)(t_n,\omega _n) \le E_{Q^{a, a\mu _n}_{t_n,\omega _n}}(R(h)(t_n+\delta _n,.))\alpha _{t_n,t_n+\delta _n}(Q^{a, a\mu _n}_{t_n,\omega _n})+\frac{h_n}{n} \end{aligned}$$(57)From Eqs. (56)–(58), it follows that$$\begin{aligned} R(h)(t_n+\delta _n, \omega ') \le \phi (t_n+\delta _n,\omega ')\;\;\forall \omega ' \in C_n \end{aligned}$$(58)$$\begin{aligned} \phi (t_n,\omega _n) \le E_{Q^{a, a\mu _n}_{t_n,\omega _n}}[\phi (t_n+\delta _n,.)\,\int _{t_n}^{t_n+\delta _n}g (u,\omega ',\mu _n(u,\omega '))du]\,+\,2\frac{h_n}{n} \end{aligned}$$(59) 
Step 3: Martingale problem
Given \((t_n,\omega _n)\), the probability measure \(Q^{a, a\mu _n}_{t_n,\omega _n}\) is solution to the martingale problem \({\mathscr {L}}^{a,a\mu _n}\) starting from \(\omega _n\) at time \(t_n\). The strictly progressive function \(\overline{\phi }\) belongs to \({\mathscr {C}}_b^{1,0,2}\). It follows from [3] and from Eq. (59) thatBy definition of f it follows that$$\begin{aligned}&0 \le E_{Q^{a, a\mu _n}_{t_n,\omega _n}}[\int _{t_n}^{t_n+\delta _n}(\partial _u \overline{\phi }(u, \omega ',(\omega '(u)))+ \frac{1}{2}Trace(D^2_x \overline{\phi }\overline{a})(u,\omega ',\omega '(u)) )du ]\nonumber \\&+ E_{Q^{a, a\mu _n}_{t_n,\omega _n}}[ \int _{t_n}^{t_n+\delta _n}(D_x\overline{\phi }^t(u, \omega ',\omega '(u)) a(u,\omega ') \mu _n(u,\omega ')g(u, \omega ',\mu _n(u,\omega ')))du]+2\frac{h_n}{n} \end{aligned}$$(60)$$\begin{aligned}&0 \le E_{Q^{a,a \mu _n}_{t_n,\omega _n}}[\int _{t_n}^{t_n+\delta _n}(\partial _u \overline{\phi }(u, \omega ',\omega '(u)))+ \frac{1}{2}Trace((D^2_x\overline{\phi }\overline{a})(u,\omega ',\omega '(u))) du ] \nonumber \\&\qquad + E_{Q^{a, a\mu _n}_{t_n,\omega _n}}[ \int _{t_n}^{t_n+\delta _n} f(u, \omega ',(\overline{a} D_x \overline{\phi })(u,\omega ',\omega '(u)))du]+2\frac{h_n}{n} \end{aligned}$$(61) 
Step 4: Conclusion
Divide equation (61) by \(h_n\) and let n tend to \(\infty \). The result follows from step 1, the inequality \(Q^{a, a\mu _n}_{t_n,\omega _n}(C_n) \ge \frac{1}{2}\) for all n and \(\delta _n=h_n 1_{C_n}\). \(\square \)
8.3 Existence of Viscosity Solutions on the Set of Continuous Paths
On the set of continuous paths \({\mathscr {C}}(I\!R_+ \times I\!R^n)\) we consider the uniform norm topology. In this section we assume that the function a is only defined on \(I\!R_+ \times {\mathscr {C}}(I\!R_+ \times I\!R^n)\) and that it is continuous. For every continuous function h on the space of continuous paths \({\mathscr {C}}(I\!R_+ \times I\!R^n)\) such that \(h(\omega )=h(\omega ')\) if \(\omega (u)=\omega '(u)\) for all \(u \le t\), the corresponding function R(h) is constructed as above. In this case the function R(h) is defined only on the set of continuous paths (more precisely on \([0,t] \times {\mathscr {C}}(I\!R_+ \times I\!R^n)\)). We make use of the definition of viscosity solution on the set of continuous paths introduced in Sect. 2.4 (Definition 4). To prove that R(h) is a viscosity supersolution, to define \(R(h)^*\) and prove that it is a viscosity subsolution, we do not need to extend the functions a nor R(h). Indeed as the support of the probability measure \(Q^{a}_{r,\omega }\) is contained in the set of continuous paths, we just need to use the restrictions of the function \(\overline{\phi }\) and of its partial derivatives to the set \(I\!R_+ \times {\mathscr {C}}(I\!R_+ \times I\!R^n) \times I\!R^n\). The proofs given for Theorems 5 and 6 can be easily adapted to prove the analog result in the setting of continuous paths.
Thus the setting of continuous paths can be considered as a “particular case” of the setting of càdlàg paths.
9 Conclusion and Perspectives

In contrast with other papers, we consider on the set \(\varOmega \) of càdlàg paths the Skorokhod topology. \(\varOmega \) is thus a Polish space. This property is fundamental for the construction of solutions for pathdependent PDE that we give in the present paper.

The notions of partial derivative for progressive functions that we introduce are defined in a very natural way by considering a progressive function of two variables as a function of three variables.
In addition we introduce also a notion of viscosity solution on the set of continuous paths.
Making use of the martingale problem approach to pathdependent diffusion processes, we then construct time consistent dynamic risk measures \(\rho ^{r,\omega }_{st}\). The stable set of probability measures used for the construction of \(\rho ^{r,\omega }_{st}\) is a set generated by probability measures solution to the pathdependent martingale problem for \({\mathscr {L}}^{a,a\mu }\) starting form \(\omega \) at time r. The pathdependent progressively continuous bounded function a is given and takes values in the set of invertible non negative matrices. The pathdependent functions \(\mu \) are progressively continuous and vary accordingly to a multivalued mapping \(\varLambda \). This construction is done in a very general setting. In particular the coefficients \(\mu \) are not uniformly bounded. We just assume that they satisfy some uniform BMO condition. To construct the penalties, we make use of a pathdependent function g satisfying some polynomial growth condition with respect to the path and some \(L_2\) condition with respect to the process \(\mu \) related to the BMO condition. In contrast with the usual setting of BSDE, in all this construction no Lipschitz hypothesis are assumed. Notice however that the Lipschitz setting can also be studied within our approach: instead of starting with progressively continuous maps a and \(\mu \), one could start from a subfamily of maps which, for example, satisfy some uniform continuity condition (as K Lipschitz maps).
We show that these risk measures provide explicit solutions for semilinear pathdependent PDEs (2). First, we prove that the risk measures \(\rho ^{r,\omega }_{st}\) satisfy the following Feller property. For every function h \({\mathscr {B}}_t\) measurable having some continuity property, there is a progressively lower semicontinuous function R(h) such that \(\rho ^{r,\omega }_{rt}(h(X_t))=R(h)(r,\omega )\) and \(R(h)(t,\omega )=h(t,\omega )\). Next, the function R(h) is proved to be a viscosity supersolution for a semilinear pathdependent PDE (2), where the function f itself is associated to g by duality on the multivalued mapping \(\varLambda \). We prove also that the upper semi continuous envelope of R(h) is a viscosity subsolution for the pathdependent semi linear second order PDE (2).
Here we have proved the progressive lower semi continuity for R(h). To prove the progressive continuity property, additional hypothesis should be added, e.g. Lipschitz conditions. Another way of proving the continuity is to apply a comparison Theorem. The study of comparison theorems and of continuity properties in this setting, as well as the study of solutions to fully non linear pathdependent PDE will be the subject of future work.
Notes
Acknowledgments
This work was partly done while at the Center for Advanced Studies at the Norwegian Academy of Science and Letters (CAS, Oslo). It is a pleasure to thank Giulia Di Nunno and Fred Espen Benth for the invitation to contribute to the CAS program in Stochastics in Environmental and Financial Economics (SEFE), and to give a talk at the inaugural SEFE conference.
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