Angle-resolved photoemission study of the evolution of band structure and charge density wave properties in RTe3 (R=Y, La, Ce, Sm, Gd, Tb, and Dy)

被引:183
作者
Brouet, V. [1 ,2 ,3 ]
Yang, W. L. [2 ,3 ]
Zhou, X. J. [2 ,3 ]
Hussain, Z. [2 ]
Moore, R. G. [3 ,4 ,5 ]
He, R. [3 ,4 ,5 ]
Lu, D. H. [3 ]
Shen, Z. X. [2 ,3 ,4 ,5 ]
Laverock, J. [6 ]
Dugdale, S. B. [6 ]
Ru, N. [4 ,5 ]
Fisher, I. R. [4 ,5 ]
机构
[1] Univ Paris 11, CNRS, Phys Solides Lab, UMR8502, F-91405 Orsay, France
[2] Lawrence Berkeley Natl Lab, Berkeley, CA 94720 USA
[3] Stanford Univ, Stanford Synchrotron Radiat Lab, Stanford, CA 94305 USA
[4] Stanford Univ, Geballe Lab Adv Mat, Stanford, CA 94305 USA
[5] Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
[6] Univ Bristol, HH Wills Phys Lab, Bristol BS8 1TL, Avon, England
来源
PHYSICAL REVIEW B | 2008年 / 77卷 / 23期
基金
英国工程与自然科学研究理事会;
关键词
D O I
10.1103/PhysRevB.77.235104
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We present a detailed angle-resolved photoemission spectroscopy (ARPES) investigation of the RTe(3) family, which sets this system as an ideal "textbook" example for the formation of a nesting driven charge density wave (CDW). This family indeed exhibits the full range of phenomena that can be associated to CDW instabilities, from the opening of large gaps on the best nested parts of Fermi surface (up to 0.4 eV), to the existence of residual metallic pockets. ARPES is the best suited technique to characterize these features, thanks to its unique ability to resolve the electronic structure in k space. An additional advantage of RTe(3) is that the band structure can be very accurately described by a simple two dimensional tight-binding (TB) model, which allows one to understand and easily reproduce many characteristics of the CDW. In this paper, we first establish the main features of the electronic structure by comparing our ARPES measurements with the linear muffin-tin orbital band calculations. We use this to define the validity and limits of the TB model. We then present a complete description of the CDW properties and of their strong evolution as a function of R. Using simple models, we are able to reproduce perfectly the evolution of gaps in k space, the evolution of the CDW wave vector with R, and the shape of the residual metallic pockets. Finally, we give an estimation of the CDW interaction parameters and find that the change in the electronic density of states n(E(F)), due to lattice expansion when different R ions are inserted, has the correct order of magnitude to explain the evolution of the CDW properties.
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页数:16
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