Atomic and electronic structure of decagonal Al-Ni-Co alloys and approximant phases

被引:35
作者
Krajcí, M
Hafner, J
Mihalkovic, M
机构
[1] Univ Vienna, Inst Mat Phys, A-1090 Vienna, Austria
[2] Univ Vienna, Ctr Computat Mat Sci, A-1090 Vienna, Austria
[3] Slovak Acad Sci, Inst Phys, SK-84228 Bratislava, Slovakia
来源
PHYSICAL REVIEW B | 2000年 / 62卷 / 01期
关键词
D O I
10.1103/PhysRevB.62.243
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Detailed investigations of the atomic and electronic structures of decagonal AlNiCo alloys have been performed. Several different models for the decagonal structure have been investigated: A model based on a rhombic-hexagon tiling proposed by Henley and models based on a cluster decoration of the Penrose tiling with large rhombus edge. The topology of the structural models has been refined on the basis of the existing x-ray-diffraction data which, however, do;not allow us to specify the chemical decoration uniquely. The chemical order on the decagonal lattice has been optimized via the comparison of the calculated electronic spectra with photoemission and soft-x-ray data and using total-energy calculations. The electronic structure calculations for large periodic approximants with up to 1276 atoms/cell have been performed self-consistently using a real-space tight-binding linear muffin-tin orbital technique. The best a,agreement with the experimental spectra is achieved for a large-rhombus-tiling model with the innermost ring of the pentagonal columnar clusters occupied by Ni atoms only. This configuration also has the lowest total energy. As in decagonal AlCuCo we find a high density of states at the Fermi level, but the chemical ordering is very different: whereas in d-AlCuCo direct Cu-Cu neighbors are suppressed and there is a slight preference for Co-Co homocoordination, in d-AlNiCo a strong Ni-Ni interaction stabilizes the innermost Ni ring, direct Co-Co neighbors are suppressed and there is a strong Co-Al interaction.
引用
收藏
页码:243 / 255
页数:13
相关论文
共 57 条
[1]  
Andersen O.K., 1986, Electronic band structure and its applications, DOI DOI 10.1007/3540180982_1
[2]  
[Anonymous], 1991, PEARSONS HDB CRYSTAL
[3]   ANISOTROPIC OPTICAL CONDUCTIVITY OF DECAGONAL QUASI-CRYSTALS [J].
BASOV, DN ;
TIMUSK, T ;
BARAKAT, F ;
GREEDAN, J ;
GRUSHKO, B .
PHYSICAL REVIEW LETTERS, 1994, 72 (12) :1937-1940
[4]   Electronic distributions and pseudo-gap in quasicrystalline decagonal Al65Cu15Co20 and Al70Co15Ni15 alloys [J].
BelinFerre, E ;
Dankhazi, Z ;
Fournes, V ;
Sadoc, A ;
Berger, C ;
Muller, H ;
Kirchmayr, H .
JOURNAL OF PHYSICS-CONDENSED MATTER, 1996, 8 (34) :6213-6228
[5]   QUASICRYSTAL WITH ONE-DIMENSIONAL TRANSLATIONAL SYMMETRY AND A TENFOLD ROTATION AXIS [J].
BENDERSKY, L .
PHYSICAL REVIEW LETTERS, 1985, 55 (14) :1461-1463
[6]  
BIANCHI AD, 1997, P 6 INT C QUAS TOK 1, P471
[7]   LINEAR-MUFFIN-TIN-ORBITAL (LMTO) SUPERCELL AND LMTO RECURSION CALCULATIONS FOR THE ELECTRONIC-STRUCTURE OF METALLIC GLASSES - CA7AL3 [J].
BOSE, SK ;
JASWAL, SS ;
ANDERSEN, OK ;
HAFNER, J .
PHYSICAL REVIEW B, 1988, 37 (17) :9955-9963
[8]   ENFORCEMENT OF MATCHING RULES BY CHEMICAL ORDERING IN THE DECAGONAL ALCUCO QUASI-CRYSTAL [J].
BURKOV, SE .
PHYSICAL REVIEW B, 1993, 47 (18) :12325-12328
[9]   STRUCTURE MODEL OF THE AL-CU-CO DECAGONAL QUASI-CRYSTAL [J].
BURKOV, SE .
PHYSICAL REVIEW LETTERS, 1991, 67 (05) :614-617
[10]   ELECTRONIC-STRUCTURE AND TRANSPORT IN A MODEL APPROXIMANT OF THE DECAGONAL QUASI-CRYSTAL AL-CU-CO [J].
DELAISSARDIERE, GT ;
FUJIWARA, T .
PHYSICAL REVIEW B, 1994, 50 (14) :9843-9850