Direct evidence of band modification and suppression of superstructure in TiSe2 upon Fe intercalation:: An angle-resolved photoemission study

被引:42
作者
Cui, XY
Negishi, H
Titova, SG
Shimada, K [1 ]
Ohnishi, A
Higashiguchi, M
Miura, Y
Hino, S
Jahir, AM
Titov, A
Bidadi, H
Negishi, S
Namatame, H
Taniguchi, M
Sasaki, M
机构
[1] Hiroshima Univ, Hiroshima Synchrotron Radiat Ctr, Higashihiroshima 7390046, Japan
[2] Hiroshima Univ, Grad Sch Sci, Higashihiroshima 7398526, Japan
[3] Hiroshima Univ, Grad Sch Adv Sci Matter, Higashihiroshima 7398530, Japan
[4] RAS, Urals Div, Inst Met, Ekaterinburg, Russia
[5] Yamagata Univ, Fac Sci, Dept Phys, Yamagata 9908560, Japan
[6] RAS, Urals Div, Inst Met Phys, Ekaterinburg 620219, Russia
[7] Tabriz Univ, Fac Sci, Dept Phys, Tabriz 51664, Iran
关键词
D O I
10.1103/PhysRevB.73.085111
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We present electrical resistivity (rho) measurements for the intercalation compound FexTiSe2 (0 <= x < 0.16) over the temperature range from 4.2 to 300 K, and angle-resolved photoemission spectra for x=0, 0.05, and 0.14 at 50 and 250 K (or 280 K). At 250 K, TiSe2 is a semimetal having hole pockets centered at the Gamma point and electron pockets around the L points of the Brillouin zone. Upon intercalation, Fe-derived flat bands appear just below the Fermi energy, and the Se 4p derived bands forming hole pockets at the Gamma point are lowered. At 50 K, band folding due to 2ax2ax2c superlattice is observed clearly near the L point for the host and x=0.05, while it vanishes for x=0.14, consistent with the rho-T data. The critical concentration for the suppression of the superstructure (0.05 < x(c)<= 0.075) can be explained reasonably well by the percolation threshold of a two-dimensional-trianglar lattice consisting of seven Ti atoms, which is estimated to 1/14 (=0.0714).
引用
收藏
页数:6
相关论文
共 30 条
[1]   STRUCTURAL STUDY OF MXTISE2 COMPOUNDS (M=FE,CO,NI) [J].
ARNAUD, Y ;
CHEVRETON, M ;
AHOUANDJINOU, A ;
DANOT, M ;
ROUXEL, J .
JOURNAL OF SOLID STATE CHEMISTRY, 1976, 18 (01) :9-15
[2]  
BARANOV NV, 2001, J PHYS CONDENS MATT, V16, P9243
[3]   Pseudogapped Fermi surfaces of 1T-TaS2 and 1T-TaSe2:: A charge density wave effect -: art. no. 125117 [J].
Bovet, M ;
Popovic, D ;
Clerc, F ;
Koitzsch, C ;
Probst, U ;
Bucher, E ;
Berger, H ;
Naumovic, D ;
Aebi, P .
PHYSICAL REVIEW B, 2004, 69 (12)
[4]   ELECTRONIC PROPERTIES AND SUPERLATTICE FORMATION IN SEMIMETAL TISE2 [J].
DISALVO, FJ ;
MONCTON, DE ;
WASZCZAK, JV .
PHYSICAL REVIEW B, 1976, 14 (10) :4321-4328
[5]   TRANSPORT PROPERTIES AND PHASE-TRANSITION IN TI1-XMXSE2 (M = TA OR V) [J].
DISALVO, FJ ;
WASZCZAK, JV .
PHYSICAL REVIEW B, 1978, 17 (10) :3801-3807
[6]   Bulk and surface electronic structure of 1T-TiS2 and 1T-TiSe2 [J].
Fang, CM ;
deGroot, RA ;
Haas, C .
PHYSICAL REVIEW B, 1997, 56 (08) :4455-4463
[7]   X-ray studies of phonon softening in TiSe2 [J].
Holt, M ;
Zschack, P ;
Hong, H ;
Chou, MY ;
Chiang, TC .
PHYSICAL REVIEW LETTERS, 2001, 86 (17) :3799-3802
[8]  
Hufner S., 2003, Advanced Texts in Physics, DOI [10.1007/978-3-662-09280-4, DOI 10.1007/978-3-662-09280-4]
[9]   STRUCTURAL DISTORTION IN TISE2 AND RELATED MATERIALS - POSSIBLE JAHN-TELLER EFFECT [J].
HUGHES, HP .
JOURNAL OF PHYSICS C-SOLID STATE PHYSICS, 1977, 10 (11) :L319-L323
[10]   THE ELECTRONIC AND MAGNETIC-PROPERTIES OF THE 3D TRANSITION-METAL INTERCALATES OF TIS2 [J].
INOUE, M ;
HUGHES, HP ;
YOFFE, AD .
ADVANCES IN PHYSICS, 1989, 38 (05) :565-604