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<metadata xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/"><dc:title>Positive Markov processes in Laplace duality</dc:title><dc:creator>Foucart,	Clément	(Avtor)
	</dc:creator><dc:creator>Vidmar,	Matija	(Avtor)
	</dc:creator><dc:subject>positive Markov process</dc:subject><dc:subject>duality of semigroups</dc:subject><dc:subject>duality of generators</dc:subject><dc:subject>Laplace transform</dc:subject><dc:subject>complete monotonicity</dc:subject><dc:subject>Laplace symbol</dc:subject><dc:subject>Lévy-Khintchine function</dc:subject><dc:subject>martingale problem</dc:subject><dc:subject>branching process</dc:subject><dc:subject>stochastic population model</dc:subject><dc:description>This article develops a general framework for Laplace duality between positive Markov processes in which the one-dimensional Laplace transform of one process can be represented through that of another. We show that a process admits a Laplace dual if and only if it satisfies a certain complete monotonicity condition. Moreover, we analyse how the conventions adopted for the values of $0 \cdot \infty$ and $\infty \cdot 0$ are reflected in the weak continuity/absorptivity properties of the processes in duality at the boundaries $0$ and $\infty$. A broad class of generators admitting Laplace duals is identified, and we provide sufficient conditions under which the associated martingale problems are well-posed with the solutions being in duality at the level of their semigroups. Laplace duality is shown to furnish a unifying structure for several generalizations of continuous-state branching processes, e.g. those with immigration or evolving in random environments. Along the way, a theorem originally due to Ethier and Kurtz – connecting duality of generators to that of the associated semigroups – is refined, and we provide a concise proof of the Courrège form for the pointwise infinitesimal generator of a positive Markov process whose domain includes the exponential functions. The latter leads naturally to the notion of a Laplace symbol, which is a parsimonious encoding of the infinitesimal dynamics of the process.</dc:description><dc:date>2026</dc:date><dc:date>2026-08-17 14:54:43</dc:date><dc:type>Neznano</dc:type><dc:identifier>31908</dc:identifier><dc:identifier>UDK: 519.2</dc:identifier><dc:identifier>ISSN pri članku: 1083-6489</dc:identifier><dc:identifier>DOI: 10.1214/26-EJP1582</dc:identifier><dc:identifier>COBISS_ID: 287982851</dc:identifier><dc:language>sl</dc:language></metadata>
