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One-dimensional electronic structure effects of single-layer cuprates Bi-2201 and Bi(Pb)-2201

Abstract

The single-layer high-T{sub c} superconductor (BiPb){sub 2}Sr{sub 2-x}La{sub x}CuO{sub 6+{delta}} represents an excellent possibility to study the almost undisturbed CuO{sub 2}-plane, the substantial element of the cuprate superconductors. For this material, a new splitting of the spectral weight at E{sub F} has been observed along the Cu-O bond ({pi}, 0) direction of the Brillouin zone. It will be shown by high-resolution angle-resolved photoemission spectroscopy that similar to the strong polarization dependence the split excitations reveal a distinct 90 deg. asymmetry and exist only below a certain temperature which is probably the transition temperature of the pseudo-gap phase T{sup *}. These observations are additional hints on the one-dimensionality of the electronic structure of the two-dimensional CuO{sub 2}-plane.
Publication Date:
Aug 01, 2004
Product Type:
Journal Article
Resource Relation:
Journal Name: Physica. C, Superconductivity; Journal Volume: 408-410; Journal Issue: 3-4; Conference: 7. M2SRIO: International conference on materials and mechanisms of superconductivity and high temperature superconductors, Rio de Janeiro (Brazil), 25-30 May 2003; Other Information: DOI: 10.1016/j.physc.2004.03.129; PII: S0921453404005350; Copyright (c) 2004 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved; Country of input: International Atomic Energy Agency (IAEA); PBD: Aug 2004
Subject:
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; ASYMMETRY; BRILLOUIN ZONES; COPPER OXIDES; CUPRATES; ELECTRONIC STRUCTURE; EMISSION SPECTROSCOPY; EXCITATION; HIGH-TC SUPERCONDUCTORS; LANTHANUM COMPOUNDS; LAYERS; LEAD COMPOUNDS; ONE-DIMENSIONAL CALCULATIONS; PHOTOEMISSION; POLARIZATION; RESOLUTION; STRONTIUM COMPOUNDS; TRANSITION TEMPERATURE
OSTI ID:
20618362
Country of Origin:
Netherlands
Language:
English
Other Identifying Numbers:
Journal ID: ISSN 0921-4534; PHYCE6; TRN: NL05S0559061860
Submitting Site:
NLN
Size:
page(s) 780-782
Announcement Date:
Aug 21, 2005

Citation Formats

Manzke, Recardo, Dudy, Lenart, Krapf, Alica, Janowitz, Christoph, and Hoechst, Hartmut. One-dimensional electronic structure effects of single-layer cuprates Bi-2201 and Bi(Pb)-2201. Netherlands: N. p., 2004. Web. doi:10.1016/j.physc.2004.03.129.
Manzke, Recardo, Dudy, Lenart, Krapf, Alica, Janowitz, Christoph, & Hoechst, Hartmut. One-dimensional electronic structure effects of single-layer cuprates Bi-2201 and Bi(Pb)-2201. Netherlands. https://doi.org/10.1016/j.physc.2004.03.129
Manzke, Recardo, Dudy, Lenart, Krapf, Alica, Janowitz, Christoph, and Hoechst, Hartmut. 2004. "One-dimensional electronic structure effects of single-layer cuprates Bi-2201 and Bi(Pb)-2201." Netherlands. https://doi.org/10.1016/j.physc.2004.03.129.
@misc{etde_20618362,
title = {One-dimensional electronic structure effects of single-layer cuprates Bi-2201 and Bi(Pb)-2201}
author = {Manzke, Recardo, Dudy, Lenart, Krapf, Alica, Janowitz, Christoph, and Hoechst, Hartmut}
abstractNote = {The single-layer high-T{sub c} superconductor (BiPb){sub 2}Sr{sub 2-x}La{sub x}CuO{sub 6+{delta}} represents an excellent possibility to study the almost undisturbed CuO{sub 2}-plane, the substantial element of the cuprate superconductors. For this material, a new splitting of the spectral weight at E{sub F} has been observed along the Cu-O bond ({pi}, 0) direction of the Brillouin zone. It will be shown by high-resolution angle-resolved photoemission spectroscopy that similar to the strong polarization dependence the split excitations reveal a distinct 90 deg. asymmetry and exist only below a certain temperature which is probably the transition temperature of the pseudo-gap phase T{sup *}. These observations are additional hints on the one-dimensionality of the electronic structure of the two-dimensional CuO{sub 2}-plane.}
doi = {10.1016/j.physc.2004.03.129}
journal = []
issue = {3-4}
volume = {408-410}
journal type = {AC}
place = {Netherlands}
year = {2004}
month = {Aug}
}