Abstract:This paper provides a general framework for pricing options with a constant barrier under spectrally one-sided exponential LÃ evy model, and uses it to implement of Carr's approximation for the value of the American put under this model. Simple analytic approximations for the exercise boundary and option value are obtained.
“…Moreover with the advent of these new fluctuation identities and a better understanding of the analytical properties of the function W (q) came the possibility of revisiting and solving a number of classical and modern problems from applied probability, but now with the underlying source of randomness being a general spectrally negative Lévy processes. For example, in the theory of optimal stopping Avram et al (2002Avram et al ( , 2004; Alili and Kyprianou (2005) and Kyprianou (2006), in the theory of optimal control Avram et al (2007) and Loeffen (2007), in the theory of queuing and storage models Dube et al (2004) and Bekker et al (2008), in the theory of branching processes Bingham (1976) and Lambert (2007) Kyprianou and Surya (2007) and in the theory of fragmentation Krell (2007).…”
Section: Spectrally Negative Lévy Processes and Scale Functionsmentioning
We give a review of the state of the art with regard to the theory of scale functions for spectrally negative Lévy processes. From this we introduce a general method for generating new families of scale functions. Using this method we introduce a new family of scale functions belonging to the Gaussian Tempered Stable Convolution (GTSC) class. We give particular emphasis to special cases as well as cross-referencing their analytical behaviour against known general considerations.
Spectrally negative Lévy processes and scale functionsLet X = {X t : t ≥ 0} be a Lévy process defined on a filtered probability space (Ω, F, F, P), where {F t : t ≥ 0} is the filtration generated by X satisfying the usual conditions. For x ∈ R denote by P x the law of X when it is started at x and write simply P 0 = P. Accordingly we shall write E x and E for the associated expectation operators. In this paper we shall assume throughout that X is spectrally negative meaning here that it has no positive jumps and that it is not the negative of a subordinator. It is well known that the latter allows us to talk about the Laplace exponent ψ(θ) := log E[e θX1 ] for (θ) ≥ 0 where in particular we have the Lévy-Khintchine representationwhere a ∈ R, σ ≥ 0 is the Gaussian coefficient and Π is a measure concentrated on (−∞, 0) satisfying (−∞,0) (1∧x 2 )Π(dx) < ∞. The, so-called, Lévy triple (a, σ, Π) completely characterises the process X. For later reference we also introduce the function Φ : [0, ∞) → [0, ∞) as the right inverse of ψ on (0, ∞) so that for all q ≥ 0 Φ(q) = sup{θ ≥ 0 : ψ(θ) = q}.(2)
“…Moreover with the advent of these new fluctuation identities and a better understanding of the analytical properties of the function W (q) came the possibility of revisiting and solving a number of classical and modern problems from applied probability, but now with the underlying source of randomness being a general spectrally negative Lévy processes. For example, in the theory of optimal stopping Avram et al (2002Avram et al ( , 2004; Alili and Kyprianou (2005) and Kyprianou (2006), in the theory of optimal control Avram et al (2007) and Loeffen (2007), in the theory of queuing and storage models Dube et al (2004) and Bekker et al (2008), in the theory of branching processes Bingham (1976) and Lambert (2007) Kyprianou and Surya (2007) and in the theory of fragmentation Krell (2007).…”
Section: Spectrally Negative Lévy Processes and Scale Functionsmentioning
We give a review of the state of the art with regard to the theory of scale functions for spectrally negative Lévy processes. From this we introduce a general method for generating new families of scale functions. Using this method we introduce a new family of scale functions belonging to the Gaussian Tempered Stable Convolution (GTSC) class. We give particular emphasis to special cases as well as cross-referencing their analytical behaviour against known general considerations.
Spectrally negative Lévy processes and scale functionsLet X = {X t : t ≥ 0} be a Lévy process defined on a filtered probability space (Ω, F, F, P), where {F t : t ≥ 0} is the filtration generated by X satisfying the usual conditions. For x ∈ R denote by P x the law of X when it is started at x and write simply P 0 = P. Accordingly we shall write E x and E for the associated expectation operators. In this paper we shall assume throughout that X is spectrally negative meaning here that it has no positive jumps and that it is not the negative of a subordinator. It is well known that the latter allows us to talk about the Laplace exponent ψ(θ) := log E[e θX1 ] for (θ) ≥ 0 where in particular we have the Lévy-Khintchine representationwhere a ∈ R, σ ≥ 0 is the Gaussian coefficient and Π is a measure concentrated on (−∞, 0) satisfying (−∞,0) (1∧x 2 )Π(dx) < ∞. The, so-called, Lévy triple (a, σ, Π) completely characterises the process X. For later reference we also introduce the function Φ : [0, ∞) → [0, ∞) as the right inverse of ψ on (0, ∞) so that for all q ≥ 0 Φ(q) = sup{θ ≥ 0 : ψ(θ) = q}.(2)
“…Boyarchenko and Levendorskiǐ (2002b, Chapter 6) generalized this method for wide classes of Lévy processes, and in Levendorskiǐ (2004), an efficient pricing procedure for the put under exponential jump-diffusion processes was suggested. A different generalization of Carr's randomization method for spectrally negative Lévy processes was used in Avram et al (2002).…”
Abstract. This paper studies stopping problems of the form V = inf 0≤τ ≤T E[U ( max 0≤s≤T Zs Zτ )] for strictly concave or convex utility functions U in a family of increasing functions satisfying certain conditions, where Z is a geometric Brownian motion and T is the time of the nth jump of a Poisson process independent of Z. We obtain some properties of V and offer solutions for the optimal strategies to follow. This provides us with a technique to build numerical approximations of stopping boundaries for the fixed terminal time optimal stopping problem presented in
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