Ab initio electronic structure calculation for single-component molecular conductor Au(tmdt)2 (tmdt = trimethylenetetrathiafulvalenedithiolate)

被引:37
作者
Ishibashi, S
Tanaka, H
Kohyama, M
Tokumoto, M
Kobayashi, A
Kobayashi, H
Terakura, K
机构
[1] Natl Inst Adv Ind Sci & Technol, Res Inst Computat Sci, Tsukuba, Ibaraki 3058568, Japan
[2] AIST, Nantechnol Res Inst, Tsukuba, Ibaraki 3058568, Japan
[3] AIST, Res Inst Ubiquitous Energy Devices, Ikeda, Osaka 5638577, Japan
[4] Univ Tokyo, Grad Sch Sci, Res Ctr Spectrochem, Bunkyo Ku, Tokyo 1130033, Japan
[5] Inst Mol Sci, Okazaki, Aichi 4448585, Japan
[6] Hokkaido Univ, Sapporo, Hokkaido 0010021, Japan
[7] JST, CREST, Kawaguchi, Saitama 3320012, Japan
关键词
single-component molecular conductor; Au(tmdt)(2); ab initio calculation; electronic structure; Fermi surface;
D O I
10.1143/JPSJ.74.843
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We have investigated the electronic structure of Au(tmdt)(2) (tmdt = trimethylenetetrathiafulvalenedithiolate), which is a single-component conductor showing a magnetic phase transition around 100K, by ab initio plane-wave pseudopotential calculations. A single band crosses the Fermi level. This band and the next band below are a result of the strong hybridization between the two neighboring molecular levels near the Fermi level (SOMO and HOMO-1) and the system is more properly described as quarter-filled rather than half-filled in the strong correlation regime. The Fermi surface has corrugated-sheet-like parts nearly parallel to each other. Intraband generalized susceptibility suggests the presence of a nesting vector a*/2 (a* is one of the reciprocal lattice vectors). Spin-polarized calculation on the doubled unit cell along the a axis (a is a lattice vector) results in an antiferromagnetic order. The nesting is not perfect and Fermi-surface pockets remain in the magnetic phase. The implications of the present calculations with regard to experimental results are discussed.
引用
收藏
页码:843 / 846
页数:4
相关论文
共 16 条
[1]   GROUND-STATE OF THE ELECTRON-GAS BY A STOCHASTIC METHOD [J].
CEPERLEY, DM ;
ALDER, BJ .
PHYSICAL REVIEW LETTERS, 1980, 45 (07) :566-569
[2]  
Frisch M. J., 2016, J AM CHEM SOC, DOI DOI 10.1021/JA205566W
[3]   NORM-CONSERVING PSEUDOPOTENTIALS [J].
HAMANN, DR ;
SCHLUTER, M ;
CHIANG, C .
PHYSICAL REVIEW LETTERS, 1979, 43 (20) :1494-1497
[4]   EFFICACIOUS FORM FOR MODEL PSEUDOPOTENTIALS [J].
KLEINMAN, L ;
BYLANDER, DM .
PHYSICAL REVIEW LETTERS, 1982, 48 (20) :1425-1428
[5]  
Kobayashi A, 2001, J MATER CHEM, V11, P2078, DOI 10.1039/b102865k
[6]   NON-LINEAR IONIC PSEUDOPOTENTIALS IN SPIN-DENSITY-FUNCTIONAL CALCULATIONS [J].
LOUIE, SG ;
FROYEN, S ;
COHEN, ML .
PHYSICAL REVIEW B, 1982, 26 (04) :1738-1742
[7]  
MIYAGAWA K, UNPUB ICSM 2004, P71
[8]  
Perdew JP, 1997, PHYS REV LETT, V78, P1396, DOI 10.1103/PhysRevLett.77.3865
[9]   SELF-INTERACTION CORRECTION TO DENSITY-FUNCTIONAL APPROXIMATIONS FOR MANY-ELECTRON SYSTEMS [J].
PERDEW, JP ;
ZUNGER, A .
PHYSICAL REVIEW B, 1981, 23 (10) :5048-5079
[10]   GENERALIZED MAGNETIC-SUSCEPTIBILITIES IN METALS - APPLICATION OF ANALYTIC TETRAHEDRON LINEAR ENERGY METHOD TO SC [J].
RATH, J ;
FREEMAN, AJ .
PHYSICAL REVIEW B, 1975, 11 (06) :2109-2117