Electrons of alkali metals in regular nanospaces of zeolites

• Published in: Advances in physics: X Vol. 2; no. 2; pp. 254 - 280
• Main Authors: Nakano, Takehito, Nozue, Yasuo
• Format: Journal Article
• Language: English
• Published: Abingdon Taylor & Francis 04.03.2017; Taylor & Francis Ltd; Taylor & Francis Group
• Subjects: 71.30.+h metal-insulator transitions and other electronic transitions; 71.38.-k polarons and electron-phonon interactions; 73.22.-f Electronic structure of nanoscale materials and related systems; 75.75.-c magnetic properties of nanostructures; Alkali metals; Antiferromagnetism; Cages; Electron phonon interactions; Electron states; Electron transfer; Ferrimagnetism; Ferromagnetism; Free electrons; insulator-to-metal transition; Jellium; Metal clusters; Metals; Nano clusters; Polarons; Properties (attributes); Quantum wells; S N diagrams; spin-orbit interaction; Spin-orbit interactions; Zeolites
• ISSN: 2374-6149; 2374-6149
• DOI: 10.1080/23746149.2017.1280415

The s-electrons of alkali metals loaded into regular nanospaces (nanocages) of zeolite crystals display novel electronic properties, such as a ferrimagnetism, a ferromagnetism, an antiferromagnetism, an insulator-to-metal transition, etc., depending on the kind of alkali metals, their loading density, and the structure type of zeolite frameworks. These properties are entirely different from those in bulk alkali metals of free-electrons. Alkali-metal clusters are stabilized in cages of zeolites, and new quantum states of s-electrons, such as 1s, 1p, and 1d states in the spherical quantum-well model, are formed. An electron correlation, a polaron effect, and an orbital degeneracy in the quantum states of s-electrons play critical roles in taking on the novel electronic properties. Electronic properties can be overviewed systematically by a coarse-grained model of localized s-electron states in cages based on the tight-binding approximation, followed by the t-U-S-n diagram of the correlated polaron system given by the so-called Holstein-Hubbard Hamiltonian: an electron transfer energy through windows of cages (t), a Coulomb repulsion energy between two s-electrons in the same cage (U), a short-range electron-phonon interaction energy due to the cation displacements (S), and an average number of s-electrons per cage (n). Beyond the jellium background model of alkali-metal clusters, a huge spin-orbit interaction has been observed in the 1p degenerate orbitals of clusters, similarly to the Rashba mechanism.