979 resultados para Riemann-Liouville derivatives and integrals of fractional order
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Directory section is not illustrated. Illustrated ads for Presbyterian Hospital and Woman's Medical College, Eclectic Medical Institute, and Densmore Typewriter.
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Bibliography: Fournier's series: p. [411]-418; The conduction of heat: p.[419]-429.
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Paged continuously.
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v. 1 Maine, New Hampshire, Vermont.--v. 2. Massachusetts, Rhode Island, Connecticut.
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Mode of access: Internet.
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"Memorandum of certain 1946-1947 references not incorporated in regular text": p. xvii-xxv.
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Includes index.
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Mode of access: Internet.
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Mode of access: Internet.
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Mode of access: Internet.
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Includes "Letter from Mr. Ruskin" to the compiler (2 p.)
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Thesis (Master's)--University of Washington, 2016-06
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Denote the set of 21 non-isomorphic cubic graphs of order 10 by L. We first determine precisely which L is an element of L occur as the leave of a partial Steiner triple system, thus settling the existence problem for partial Steiner triple systems of order 10 with cubic leaves. Then we settle the embedding problem for partial Steiner triple systems with leaves L is an element of L. This second result is obtained as a corollary of a more general result which gives, for each integer v greater than or equal to 10 and each L is an element of L, necessary and sufficient conditions for the existence of a partial Steiner triple system of order v with leave consisting of the complement of L and v - 10 isolated vertices. (C) 2004 Elsevier B.V. All rights reserved.
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Wigner functions play a central role in the phase space formulation of quantum mechanics. Although closely related to classical Liouville densities, Wigner functions are not positive definite and may take negative values on subregions of phase space. We investigate the accumulation of these negative values by studying bounds on the integral of an arbitrary Wigner function over noncompact subregions of the phase plane with hyperbolic boundaries. We show using symmetry techniques that this problem reduces to computing the bounds on the spectrum associated with an exactly solvable eigenvalue problem and that the bounds differ from those on classical Liouville distributions. In particular, we show that the total "quasiprobability" on such a region can be greater than 1 or less than zero. (C) 2005 American Institute of Physics.