T h e firew ork s disaster in en sch ede P art 1: O verview an d reconstru ction
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Then the change of variables, or area formula holds for f provided removing from counting into the multiplicity function the set where f is not approximately H¨ older continuous1.
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Neumann started investigation of the quantity k T K k 0 (which he called the configuration constant of K) in order to get a proof for the existence of the solution of the
2 To introduce the natural and adapted bases in tangent and cotangent spaces of the subspaces H 1 and H 2 of H it is convenient to use the matrix representation of
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In this case (X t ) t≥0 is in fact a continuous (F t X,∞ ) t≥0 -semimartingale, where the martingale component is a Wiener process and the bounded variation component is an
In this section we consider the submodular flow problem, the independent flow problem and the polymatroidal flow problem, which we call neoflow problems.. We discuss the equivalence
The orthogonality test using S t−1 (Table 14), M ER t−2 (Table 15), P P I t−1 (Table 16), IP I t−2 (Table 17) and all the variables (Table 18) shows that we cannot reject the