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Titlebook: Network Optimization; Panos M. Pardalos,Donald W. Hearn,William W. Hager Conference proceedings 1997 Springer-Verlag Berlin Heidelberg 199

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Rainer E. Burkard,Eranda Çela,Tibor Dudáse the magnesium isotopes, which exhibit a swift transition into the island of inversion with 29Mg lying outside and 31Mg lying inside. In addition, 29Mg lies one neutron outside N=16, so is also able to give in978-3-031-19121-3978-3-031-19119-0Series ISSN 2190-5053 Series E-ISSN 2190-5061
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D. Burton,W. R. Pulleyblank,Ph. L. Tointe the magnesium isotopes, which exhibit a swift transition into the island of inversion with 29Mg lying outside and 31Mg lying inside. In addition, 29Mg lies one neutron outside N=16, so is also able to give in978-3-031-19121-3978-3-031-19119-0Series ISSN 2190-5053 Series E-ISSN 2190-5061
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Panos M. Pardalos,Donald W. Hearn,William W. Hager
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E. Alviti,E. G. Johnson,R. B. Kulkarni,J. L. Nazareth,J. C. Stone have quickly becomea very active field. In the first part of this review, we have summarized the last developmentson the theoretical understanding of the SCM behavior. In these systems, the key analysis of the magneticproperties is the comparison between static susceptibility and dynamic data that
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Cynthia Barnhart,Christopher A. Hane,Pamela H. Vancebine in a unique fashion the magnetic properties of embeddedSMMs with the conductive, optical and mechanical characteristics of a polymeric host. In theframework of the molecular approach to electronics, successful attempts to organize SMMs into bidimensionalarrays on surfaces and to address them in
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Pia Bergendorff,Donald W. Hearn,Motakuri V. Ramanaity in bioimaging. We show that the CNDs are single dipole emitters similar to organic dyes. Thereafter, we present the first experimental method for determining the geometry of the two transition dipoles and their three-dimensional orientations . for each individual emitter. This directly gives us
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David Bernstein,Steven A. Gabrielity in bioimaging. We show that the CNDs are single dipole emitters similar to organic dyes. Thereafter, we present the first experimental method for determining the geometry of the two transition dipoles and their three-dimensional orientations . for each individual emitter. This directly gives us
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