journal article·2014-08-03

e/aclassification of Hume–Rothery Rhombic Triacontahedron-type approximants based on all-electron density functional theory calculations

U. Mizutani, M. Inukai, H. Sato, E.S. Zijlstra, Q. Lin

Philosophical Magazine· Volume 94· Issue 22
Publisher page

Abstract

There are three key electronic parameters in elucidating the physics behind the Hume–Rothery electron concentration rule: the square of the Fermi diameter (2kF)2, the square of the critical reciprocal lattice vector and the electron concentration parameter or the number of itinerant electrons per atom e/a. We have reliably determined these three parameters for 10 Rhombic Triacontahedron-type 2/1–2/1–2/1 (N = 680) and 1/1–1/1–1/1 (N = 160–162) approximants by making full use of the full-potential linearized augmented plane wave-Fourier band calculations based on all-electron density-functional theory. We revealed that the 2/1–2/1–2/1 approximants Al13Mg27Zn45 and Na27Au27Ga31 belong to two different sub-groups classified in terms of equal to 126 and 109 and could explain why they take different e/a values of 2.13 and 1.76, respectively. Among eight 1/1–1/1–1/1 approximants Al3Mg4Zn3, Al9Mg8Ag3, Al21Li13Cu6, Ga21Li13Cu6, Na26Au24Ga30, Na26Au37Ge18, Na26Au37Sn18 and Na26Cd40Pb6, the first two, the second two and the last four compounds were classified into three sub-groups with = 50, 46 and 42; and were claimed to obey the e/a = 2.30, 2.10–2.15 and 1.70–1.80 rules, respectively.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Quasicrystal Structures and Properties · X-ray Diffraction in Crystallography · Boron and Carbon Nanomaterials Research

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (22)

Show source-provided references
1. 10.1201/b1032410.1201/b10324 ↗
2. 10.1143/JJAP.27.L158710.1143/JJAP.27.L1587 ↗
3. 10.2320/matertrans1989.31.9810.2320/matertrans1989.31.98 ↗
4. 10.2320/matertrans1989.32.42110.2320/matertrans1989.32.421 ↗
5. 10.1080/14786435.2011.60435710.1080/14786435.2011.604357 ↗
6. 10.1080/14786435.2012.65771110.1080/14786435.2012.657711 ↗
7. 10.1039/c2cs35161g10.1039/c2cs35161g ↗
8. 10.1080/14786435.2013.79385510.1080/14786435.2013.793855 ↗
9. 10.1080/14786435.2013.80527610.1080/14786435.2013.805276 ↗
10. Mizutani U.
11. Mizutani U.
12. 10.1021/ic300866q10.1021/ic300866q ↗
13. 10.1002/anie.20120707610.1002/anie.201207076 ↗
14. 10.1103/PhysRevB.52.930010.1103/PhysRevB.52.9300 ↗
15. 10.1016/S0925-8388(02)00159-710.1016/S0925-8388(02)00159-7 ↗
16. 10.1073/pnas.060595410310.1073/pnas.0605954103 ↗
17. 10.1016/S0921-5093(00)01077-710.1016/S0921-5093(00)01077-7 ↗
18. 10.1016/0022-4596(91)90142-510.1016/0022-4596(91)90142-5 ↗
19. 10.1021/ic970588j10.1021/ic970588j ↗
20. Blaha P.
21. 10.1016/j.jnoncrysol.2003.11.06510.1016/j.jnoncrysol.2003.11.065 ↗
22. Tsai A.-P. · 201