Universal high energy anomaly in the angle-resolved photoemission spectra of high temperature superconductors: Possible evidence of spinon and holon branches

被引:177
作者
Graf, J. [1 ]
Gweon, G. -H.
McElroy, K.
Zhou, S. Y.
Jozwiak, C.
Rotenberg, E.
Bill, A.
Sasagawa, T.
Eisaki, H.
Uchida, S.
Takagi, H.
Lee, D. -H.
Lanzara, A.
机构
[1] Lawrence Berkeley Lab, Div Mat Sci, Berkeley, CA 94720 USA
[2] Swiss Fed Inst Technol, CH-1015 Lausanne, Switzerland
[3] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[4] Univ Calif Santa Cruz, Dept Phys, Santa Cruz, CA 95064 USA
[5] Lawrence Berkeley Lab, Adv Light Source, Berkeley, CA 94720 USA
[6] Univ Tokyo, Dept Adv Mat Sci, Kashiwa, Chiba 2778561, Japan
[7] AIST, Tsukuba, Ibaraki 3058568, Japan
[8] Univ Tokyo, Dept Phys, Bunkyo Ku, Tokyo 1138656, Japan
[9] RIKEN, Inst Phys & Chem Res, Wako, Saitama 3510198, Japan
关键词
D O I
10.1103/PhysRevLett.98.067004
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
A universal high energy anomaly in the single particle spectral function is reported in three different families of high temperature superconductors by using angle-resolved photoemission spectroscopy. As we follow the dispersing peak of the spectral function from the Fermi energy to the valence band complex, we find dispersion anomalies marked by two distinctive high energy scales, E-1 approximate to 0.38 eV and E-2 approximate to 0.8 eV. E-1 marks the energy above which the dispersion splits into two branches. One is a continuation of the near parabolic dispersion, albeit with reduced spectral weight, and reaches the bottom of the band at the Gamma point at approximate to 0.5 eV. The other is given by a peak in the momentum space, nearly independent of energy between E-1 and E-2. Above E-2, a bandlike dispersion reemerges. We conjecture that these two energies mark the disintegration of the low-energy quasiparticles into a spinon and holon branch in the high T-c cuprates.
引用
收藏
页数:4
相关论文
共 21 条
[1]   Importance of matrix elements in the ARPES spectra of BISCO [J].
Bansil, A ;
Lindroos, M .
PHYSICAL REVIEW LETTERS, 1999, 83 (24) :5154-5157
[2]  
Bansil A., COMMUNICATION
[3]   The non-Fermi liquid behavior and diagonal lattice stripes in cuprate superconductors [J].
Bianconi, A ;
Saini, NL ;
Lanzara, A ;
Avila, J ;
Asensio, MC ;
Tajima, S ;
Gu, GD ;
Koshizuka, N .
PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 1999, 317 :304-311
[4]  
Campuzano J C., 2004, The physics of superconductors, V2
[5]   Angle-resolved photoemission studies of the cuprate superconductors [J].
Damascelli, A ;
Hussain, Z ;
Shen, ZX .
REVIEWS OF MODERN PHYSICS, 2003, 75 (02) :473-541
[6]  
Denlinger J. D., COMMUNICATION
[7]   Spectroscopic evidence for a pseudogap in the normal state of underdoped high-T-c superconductors [J].
Ding, H ;
Yokoya, T ;
Campuzano, JC ;
Takahashi, T ;
Randeria, M ;
Norman, MR ;
Mochiku, T ;
Kadowaki, K ;
Giapintzakis, J .
NATURE, 1996, 382 (6586) :51-54
[8]  
GRACIA D, COMMUNICATION
[9]  
GRAF J, UNPUB
[10]   Direct observation of complete Fermi surface, imperfect nesting, and gap anisotropy in the high-temperature incommensurate charge-density-wave compound SmTe3 [J].
Gweon, GH ;
Denlinger, JD ;
Clack, JA ;
Allen, JW ;
Olson, CG ;
DiMasi, E ;
Aronson, MC ;
Foran, B ;
Lee, S .
PHYSICAL REVIEW LETTERS, 1998, 81 (04) :886-889