Titlebook: Evolution Processes and the Feynman-Kac Formula; Brian Jefferies Book 1996 Springer Science+Business Media Dordrecht 1996 Feynman-Kac form

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https://doi.org/10.1007/978-3-322-89173-0l operators .., . = ±1, ±2,..., acting on ..((0, ∞); ℂ.). The first order part of .. looks similar to the generator of the direct sum of translations in each component of . ∈ ..((0, ∞); ℂ.). The part of order zero has a 1/.-singularity at . = 0.

冷峻

Evolution Processes, measured by a collection of operator valued set functions that may or may not be .-additive. Typically, the set functions are constructed from a semigroup representing the undisturbed evolution of a system, and a spectral measure by which perturbations are implemented.

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漂白

Integration with respect to Unbounded Set Functions,〈..〉. to be operator valued measures, that is, set functions defined on a .-algebra of sets, .-additive for the strong operator topology. One obstacle that arises is that for . > 0, the set function .. may not be bounded on the algebra generated by basic events before time ..

Extemporize

The Radial Dirac Process,l operators .., . = ±1, ±2,..., acting on ..((0, ∞); ℂ.). The first order part of .. looks similar to the generator of the direct sum of translations in each component of . ∈ ..((0, ∞); ℂ.). The part of order zero has a 1/.-singularity at . = 0.

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Mathematics and Its Applicationshttp://image.papertrans.cn/e/image/317658.jpg

MIRTH

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Entscheidungstheoretische PlanungThe mathematical description of an evolving physical system must formulate two fundamental aspects of physical reasoning—a description of the dynamics of the system and a method for making observations.

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