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Zhu and He [(2018). A new closed-form formula for pricing European options under a skew Brownian motion. The European Journal of Finance 24(12): 1063–1074] provided an innovative closed-form solution by replacing the standard Brownian motion in the Black–Scholes framework using a particular skew Brownian motion. Their formula involves numerically integrating the product of the Guassian density and corresponding distribution function. Being different from their pricing formula, we derive a much simpler formula that only involves the Gaussian distribution function and Owen's $T$ function.
Simulated tempering is a popular method of allowing Markov chain Monte Carlo algorithms to move between modes of a multimodal target density
$\pi$
. Tawn, Moores and Roberts (2021) introduces the Annealed Leap-Point Sampler (ALPS) to allow for rapid movement between modes. In this paper we prove that, under appropriate assumptions, a suitably scaled version of the ALPS algorithm converges weakly to skew Brownian motion. Our results show that, under appropriate assumptions, the ALPS algorithm mixes in time
$O(d [\log d]^2)$
or O(d), depending on which version is used.
where \hbox{$\bar{b}$}b̅ is a smooth real function except at point0 where \hbox{$\bar{b}(0+)\neq \bar{b}(0-)$}b̅(0 + ) ≠b̅(0 −). The main idea is to sample an exact skeleton ofX using analgorithm deduced from the convergence of the solutions of the skew perturbed equation(2)
towards X solution of (1) as β ≠0 tends to 0. In this note, we show that this convergence induces the convergenceof exact simulation algorithms proposed by the authors in [Pierre Étoré and MiguelMartinez. Monte Carlo Methods Appl. 19 (2013) 41–71] for thesolutions of (2) towards a limit algorithm.Thanks to stability properties of the rejection procedures involved as β tends to 0, we prove that this limit algorithm is anexact simulation algorithm for the solution of the limit equation (1). Numerical examples are shown to illustratethe performance of this exact simulation algorithm.
Nearly fifty years after the introduction of skew Brownian motion by Itô and McKean (1963), the first passage time distribution remains unknown. In this paper we first generalize results of Pitman and Yor (2011) and Csáki and Hu (2004) to derive formulae for the distribution of ranked excursion heights of skew Brownian motion, and then use these results to derive the first passage time distribution.
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