Titlebook: π-Electron Magnetism; From Molecules to Ma Jaume Veciana,D. Arčon,C. Rovira Book 2001 Springer-Verlag Berlin Heidelberg 2001 Inorganic Chem

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An Organic Radical Crystal Showing Spontaneous Ferromagnetic Order,thways outside the brain and spinal cord. Functionally, the brain is organized in two main sections: the cerebral cortex and the subcortical areas; the latter includes the basal ganglia, hippocampus, internal capsule, brainstem, and cerebellum. The spinal cord extends from the foramen magnum to the

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Metal-Aminoxyl-Based Molecular Magnets, investigations and procedures performed in the field.IncludNuclear medicine has become an ever-changing and expanding diagnostic and therapeutic medical profession. The day-to-day innovations seen in the field are, in great part, due to the integration of many scientific bases with complex technolo

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Magnetic Properties of Thiazyl Radicals,elevant to nuclear medicine. In the first part, the atomic theory (in brief), electron configuration, electron binding energy, atomic emissions, nuclear structure and nuclear forces are described. In the second part, radioactivity is described in detail which is an important topic in nuclear physics

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Magnetism in Fullerene Derivatives,ook on transport in semiconductors.Only textbook with perturWhen the ?rst edition ofBasic Semiconductor Physics was published in 2001, there were already many books, review papers and scienti?c journals de- ing with various aspects of semiconductor physics. Since many of them were dealing with speci

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Molecular Compounds Showing a Spin Ladder Behaviour,d Cardona in this field.Includes supplementary material: More than 50 years have passed since the invention of the transistor in De­ cember 1947. The study of semiconductors was initiated in the 1930s but we had to wait for 30 years (till the 1960s) to understand the physics of semi­ conductors. Whe

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Back Matteras been reached. It has been seen that simple tensile or compressive yielding can be avoided when the introduction of a safety factor imposes a maximum allowable elastic stress limit for a material. In practice stress states are often biaxial or triaxial, e.g. a plate with forces distributed over it

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