107,449 research outputs found

    Idempotent structures in optimization

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    Consider the set A = R āˆŖ {+āˆž} with the binary operations o1 = max and o2 = + and denote by An the set of vectors v = (v1,...,vn) with entries in A. Let the generalised sum u o1 v of two vectors denote the vector with entries uj o1 vj , and the product a o2 v of an element a āˆˆ A and a vector v āˆˆ An denote the vector with the entries a o2 vj . With these operations, the set An provides the simplest example of an idempotent semimodule. The study of idempotent semimodules and their morphisms is the subject of idempotent linear algebra, which has been developing for about 40 years already as a useful tool in a number of problems of discrete optimisation. Idempotent analysis studies infinite dimensional idempotent semimodules and is aimed at the applications to the optimisations problems with general (not necessarily finite) state spaces. We review here the main facts of idempotent analysis and its major areas of applications in optimisation theory, namely in multicriteria optimisation, in turnpike theory and mathematical economics, in the theory of generalised solutions of the Hamilton-Jacobi Bellman (HJB) equation, in the theory of games and controlled Marcov processes, in financial mathematics

    Note: Axiomatic Derivation of the Doppler Factor and Related Relativistic Laws

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    The formula for the relativistic Doppler effect is investigated in the context of two compelling invariance axioms. The axioms are expressed in terms of an abstract operation generalizing the relativistic addition of velocities. We prove the following results. (1) If the standard representation for the operation is not assumed a priori, then each of the two axioms is consistent with both the relativistic Doppler effect formula and the Lorentz-Fitzgerald Contraction. (2) If the standard representation for the operation is assumed, then the two axioms are equivalent to each other and to the relativistic Doppler effect formula. Thus, the axioms are inconsistent with the Lorentz-FitzGerald Contraction in this case. (3) If the Lorentz-FitzGerald Contraction is assumed, then the two axioms are equivalent to each other and to a different mathematical representation for the operation which applies in the case of perpendicular motions. The relativistic Doppler effect is derived up to one positive exponent parameter (replacing the square root). We prove these facts under regularity and other reasonable background conditions.Comment: 12 page

    Approximation of Rough Functions

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    For given pāˆˆ[1,āˆž]p\in\lbrack1,\infty] and gāˆˆLp(R)g\in L^{p}\mathbb{(R)}, we establish the existence and uniqueness of solutions fāˆˆLp(R)f\in L^{p}(\mathbb{R)}, to the equation f(x)āˆ’af(bx)=g(x), f(x)-af(bx)=g(x), where aāˆˆRa\in\mathbb{R}, bāˆˆRāˆ–{0}b\in\mathbb{R} \setminus \{0\}, and āˆ£aāˆ£ā‰ āˆ£bāˆ£1/p\left\vert a\right\vert \neq\left\vert b\right\vert ^{1/p}. Solutions include well-known nowhere differentiable functions such as those of Bolzano, Weierstrass, Hardy, and many others. Connections and consequences in the theory of fractal interpolation, approximation theory, and Fourier analysis are established.Comment: 16 pages, 3 figure
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