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Coupling to a phononic mode in Bi2xPbxSr2CaCu2O8+δ: Angle-resolved photoemission

Beate Ziegler, Beate Müller, Alica Krapf, Helmut Dwelk, Christoph Janowitz, and Recardo Manzke
Phys. Rev. B 77, 054520 – Published 29 February 2008

Abstract

The kink in the dispersion and the drop in the width observed by angle-resolved photoemission in the nodal direction of the Brillouin zone of Bi2xPbxSr2CaCu2O8+δ [(Pb)Bi2212] has attracted broad interest. Surprisingly, optimally lead-doped (Pb)Bi2212 with TC>89K and the shadow band have not been investigated so far, although the origin of the kink and the drop is still under strong debate. In this context a resonant magnetic-mode scenario and an electron-phonon coupling scenario have been discussed controversially. Here we analyze the relevant differences between both scenarios and conclude that the kink and the drop are caused by a coupling of the electronic system to a phononic mode at least in the nodal direction. It is found that besides the dispersion and the drop in the width, also the peak height as a previously employed criterion can be used to define the energy scale of the interaction, giving a previously unknown means for a precise and consistent determination of the kink energy.

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  • Received 8 January 2007

DOI:https://doi.org/10.1103/PhysRevB.77.054520

©2008 American Physical Society

Authors & Affiliations

Beate Ziegler, Beate Müller, Alica Krapf, Helmut Dwelk, Christoph Janowitz, and Recardo Manzke

  • Humboldt-Universität zu Berlin, Institut für Physik, Newtonstrasse 15, 12489 Berlin, Germany

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Vol. 77, Iss. 5 — 1 February 2008

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Images

  • Figure 1
    Figure 1
    (Color online) Momentum distribution curves (MDCs) of optimally doped (Pb)Bi2212 (sample 1) taken at 20 K with a photon energy of 22 eV. (a) MDC at 20 meV binding energy containing the main band and shadow band. (b) Measured direction of the Brillouin zone. (c) MDC’s of main band and (d) shadow band.Reuse & Permissions
  • Figure 2
    Figure 2
    (Color online) Dispersion of the main (red squares) and the shadow band (blue circles) of optimally doped (Pb)Bi2212 (sample 1).Reuse & Permissions
  • Figure 3
    Figure 3
    (Color online) Intensity at peak maximum of the main band (a) and of the shadow band (b) of optimally doped (Pb)Bi2212 (sample 1). The black dashed lines are guides to the eye.Reuse & Permissions
  • Figure 4
    Figure 4
    (Color online) (a) Area under the momentum distribution curves of optimally doped (Pb)Bi2212 (sample 1) showing a minimum between ω30meV and ω60meV. (b) Dispersion of the main band of optimally doped (Pb)Bi2212 (sample 1). The black lines are guides to the eye.Reuse & Permissions
  • Figure 5
    Figure 5
    (Color online) FWHM of optimally doped (Pb)Bi2212 (sample 1) of the main band (a) and of the shadow band (b). The black dashed lines are guides to the eye.Reuse & Permissions
  • Figure 6
    Figure 6
    (Color online) (a) Dispersion, (b) peak height, and (c) FWHM of the main band of optimally doped (Pb)Bi2201 (sample 4). Red squares: data. Black dashed line: guide to the eye.Reuse & Permissions
  • Figure 7
    Figure 7
    (Color online) Intensity at peak maximum for different temperatures of slightly overdoped (Pb)Bi2212 (sample 3).Reuse & Permissions
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