Optimal stopping of BSDEs with constrained jumps and related double obstacle PDEs

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We consider partial differential equations (PDEs) characterized by an upper barrier that depends on the solution itself and a fixed lower barrier, while accommodating a non-local driver. First, we show a Feynman–Kac representation for the PDE when the driver is local. Specifically, we relate the non-linear Snell envelope, arising from an optimal stopping problem—where the underlying process is the first component in the solution to a stopped backward stochastic differential equation (BSDE) with jumps and a constraint on the jumps process—to a viscosity solution for the PDE. Leveraging this Feynman–Kac representation, we subsequently prove existence and uniqueness of viscosity solutions in the non-local setting by employing a contraction argument. This approach also introduces a novel form of non-linear Snell envelope and expands the probabilistic representation theory for PDEs.

Highlights

  • We consider partial differential equations (PDEs) of the type min{v(t, x) − h(t, x), max{v(t, x) − Mv(t, x), −vt(t, x) − Lv(t, x)−f (t, x, v(t, ·), σ⊤(t, x)∇xv(t, x))}} = 0, ∀(t, x) ∈ [0, T ) × Rd v(T, x) = ψ(x), (1.1)where for each (t, x, z) ∈ [0, T ] × Rd × Rd, the map g → f (t, x, g, z) : C(Rd → R) → R is a functional, Mv(t, x) := infe∈E{v(t, x + γ(t, x, e)) + χ(t, x, e)} and d ∂1L := aj(t, x) ∂xj + 2 d ⊤ ∂2(σσ (t, x))i,j ∂xi∂xj j=1 i,j=1 (1.2)is the infinitesimal generator related to the stochastic differential equation (SDE) s s

  • An alternative Feynman-Kac representation for solutions to standard quasi-variational inequality (QVI) was proposed in [13], where the solution to a QVI is related to the minimal solution of a backward stochastic differential equation (BSDE) with constrained jumps

  • Their result implies that the deterministic function v defined through the relation v(t, x) := Ytt,x,T, with Y t,x,T as in (1.4), is the unique viscosity solution to the PDE obtained by setting h ≡ −∞ in (1.1)

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We consider partial differential equations (PDEs) of the type min{v(t, x) − h(t, x), max{v(t, x) − Mv(t, x), −vt(t, x) − Lv(t, x). An alternative Feynman-Kac representation for solutions to standard QVIs was proposed in [13] (see [5]), where the solution to a QVI is related to the minimal solution of a BSDE with constrained jumps Their result implies that (when f is local) the deterministic function v defined through the relation v(t, x) := Ytt,x,T , with Y t,x,T as in (1.4), is the unique viscosity solution to the PDE obtained by setting h ≡ −∞ in (1.1). [18] further extended the scope of control randomization to zero-sum games by (within a non-markovian framework) relating the solution to the above optimal stopping problem (1.3)-(1.5) to the upper and lower value functions in a stochastic differential game between an impulse controller and a stopper. Since our setting is fundamentally different and for the sake of completeness, a uniqueness proof through viscosity comparison is included as an appendix

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Viscosity solutionsExpand/Collapse icon
Reflected BSDEs with jumps and obstacle problemsExpand/Collapse icon
Preliminary estimatesExpand/Collapse icon
The local settingExpand/Collapse icon
The general settingExpand/Collapse icon
A Uniqueness of viscosity solutions in the local frameworkExpand/Collapse icon
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