Titlebook: Low-Dimensional Molecular Metals; Naoki Toyota,Jens Müller,Michael Lang Book 2007 Springer-Verlag Berlin Heidelberg 2007 Electronic correl

金盤是高原

micronized

Introduction: Historical Remarks, molecular substances [1]. Almost all of these substances were found, however, to be non-magnetic except for an effect which was later called molecular dia- magnetism. In 1927, shortly after quantum mechanics had been established, W. Heitler and F. London [2] had a monumental success in applying thi

strain

Basic Concepts,delocal- ization throughout the crystal. For the charge-transfer salts described in this monograph, free charge carriers (i) are created by combining a donor molecule D, such as TMTSF, BEDT-TTF (hereafter ET) or their derivatives, with an electron acceptor X. Here D should be an . molecule with a su

單調(diào)性

Structural Aspects,hich support the transport of charges through the crystal. In relatively simple metallic compounds like sodium or potassium, the constituent atoms each provide an outer-shell .-electron, which, in turn, becomes the conduction electron,and can be considered as a gas of nearly free carriers. . are des

Occupation

Normal-State Properties,a- terials. As an input for such tight-binding band-structure calculations, the molecular orbitals are usually calculated within the extended-Hückel approxi- mation which uses some empirical molecular parameters [169, 170, 82, 79, 81]. As has been discussed in more detail in [86], the extended-Hücke

從容

Magnetic-Field Effects,cts on the conduction electrons and their dynamics [76, 77, 492, 493]. This is possible because the electron’s charge and spin can interact with the magnetic field via the Lorentz force-induced orbital motion and the Zeeman interaction, respectively. Such studies, often called . (or .), have greatly

盲信者

油膏

Phenomena of Interacting ,- and ,-Electrons, localized .- or .-electrons interacting with conduction electrons. Here we describe the phenomena of interacting π- and .-electrons in (DCNQI).Cu with mixed-valent Cu ions and in quasi-2D (BETS). FeX. (X=Cl,Br)with localized .-spins.

HOWL

Epilogue,eir fascinating properties. Over the years, this field has been subject to tremendous changes triggered by outstanding discoveries and driven by the joint efforts from chemistry and physics to create new classes of conducting materials and to understand their exotic properties.

NATAL

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