General rightsIt is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulationsIf you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: http://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. A detailed and systematic angle-resolved photoemission spectroscopy investigation of the doping dependence of the normal-state Fermi surface ͑FS͒ of modulation-free ͑Pb,Bi͒-2212 is presented. The FS does not change in topology away from hole like at any stage. The FS area does not follow the usual curve describing T c vs x for the hole-doped cuprates, but is downshifted in doping by ca. 0.05 holes per Cu site, indicating the consequences of a significant bilayer splitting of the FS across the whole doping range. The strong k dependence of the FS width is shown to be doping independent. The relative strength of the shadow FS has a doping dependence mirroring that of T c .
The clearly resolved bilayer splitting in ARPES spectra of the underdoped Pb-Bi2212 compound rises the question of how the bonding and antibonding sheets of the Fermi surface are gapped in the superconducting state. Here we compare the superconducting gaps for both split components and show that within the experimental uncertainties they are identical. By tuning the relative intensity of the bonding and antibonding bands using different excitation conditions we determine the precise k-dependence of the leading edge gap. Significant deviations from the simple cos(kx)-cos(ky) gap function for the studied doping level are detected. PACS numbers: 74.25.Jb, 74.72.Hs, 71.18.+y One of the crucial steps in the evolution of our understanding of superconductors has been the discovery of the energy gap between the ground state and the quasiparticle excitations of the system. Photoemission is one of those experimental techiques which provided direct evidence for the existence of such a gap in the high-temperature superconducting cuprates 1,2,3 . Subsequent ARPES investigations 4,5,6 clearly demonstrated the anisotropic character of the gap which now is considered as a hallmark of the high temperature superconductors. Detailed studies of the symmetry properties of the gap suggested a purely d -wave character 7 in case of the optimally 8 and overdoped 9 samples, as well as noticeable deviations from the simplest d-wave scenario upon underdoping 9 .More recently, ARPES has made another step forward -technical improvements of the method allowed to resolve additional features in the momentum and energy distributions of the photoelectrons which were not resolved before. Among the new achievments is the recent observation of the bilayer splitting (BS) in over-and underdoped Bi 2 Sr 2 CaCu 2 O 8+δ and (Pb,Bi) 2 Sr 2 CaCu 2 O 8+δ bilayer compounds 10,11,12 . The presence of the BS implies that some of the conclusions based on the earlier ARPES data should be revised. As a result of such a revisit it was already established that, for example, the famous broadening of the ARPES features in momentum 12 and energy 13 could be at least partially accounted for by the bilayer splitting. Very recent investigations, in which differentiation between bonding and antibonding components is essential, imply that the more active part of the Brillouin zone in a sense of a coupling to other degrees of freedom is the antinodal region of the Fermi surface rather than the (π,0)-point itself 14,15 . At the same time detection of the BS not only provides answers but also results in further new questions. One of such natural and straightforward questions in the light of these findings is 'how does the superconducting gap be-have on both Fermi surface sheets?' Could it be that the superconductivity in Bi2212 is a sheet-dependent one as, for instance, is the case in 2H-NbSe 2 16 or MgB 2 17 ? Does the strong correlation between the so-called range parameter (related to the hopping integral t' ) and T cmax , found recently 18 for nearly all hole-doped one-...
The joys and pitfalls of Fermi surface mapping in Bi2Sr2CaCu2O8+d using angle resolved photoemission Borisenko, S.V.; Golden, M.S.; Legner, S.; Pichler, T.; Dürr, C.; Knupfer, M.; Fink, J.; Yang, G.; Abell, S. General rightsIt is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulationsIf you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: http://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. We have carried out experimental and theoretical studies of the unoccupied electronic structure of Sr 2 CuO 3 , which can be regarded as the best realization of a one-dimensional model system containing cuprate chains. In the polarization-dependent x-ray absorption spectra, the contributions to the upper Hubbard band from states originating from the two inequivalent oxygen sites are energetically well separated. Theoretical analysis of the measured hole distribution within cluster calculations reveals a markedly enhanced effective nearest-neighbor intersite Coulomb interaction, V pd ϳ2 to 3 eV, or sizable contributions from next-nearest-neighbor interactions, provided a finite on-site energy difference of the two inequivalent oxygen sites ⌬ pp is taken into account. Including next-nearest-neighbor interactions, reasonable agreement can be achieved with recent electron energy-loss spectroscopy data from the same compound. The 2p oxygen orbital analysis of the unoccupied electronic structure of the single-chain cuprate Sr 2 CuO 3 reveals strong similarities with that of the double chain compound SrCuO 2 .
We have investigated the lowest binding-energy electronic structure of the model cuprate Sr 2 CuO 2 Cl 2 using angle-resolved photoemission spectroscopy. Our data from about 80 cleavages of Sr 2 CuO 2 Cl 2 single crystals give a comprehensive, self-consistent picture of the nature of the first electron-removal state in this model undoped CuO 2-plane cuprate. First, we show a strong dependence on the polarization of the excitation light which is understandable in the context of the matrix element governing the photoemission process, which gives a state with the symmetry of a Zhang-Rice singlet. Secondly, the strong, oscillatory dependence of the intensity of the Zhang-Rice singlet on the exciting photon energy is shown to be consistent with interference effects connected with the periodicity of the crystal structure in the crystallographic c direction. Thirdly, we measured the dispersion of the first electron-removal states along ⌫→(,) and ⌫→(,0), the latter being controversial in the literature, and have shown that the data are best fitted using an extended tJ model, and extract the relevant model parameters. An analysis of the spectral weight of the first ionization states for different excitation energies within the approach used by Leung et al. ͓Phys. Rev. B 56, 6320 ͑1997͔͒ results in a strongly photon-energy dependent ratio between the coherent and incoherent spectral weight. The possible reasons for this observation and its physical implications are discussed.
The strong dependence of the momentum distribution of the photoelectrons on experimental conditions raises the question as to whether angle-resolved photoemission spectroscopy (ARPES) is able to provide an accurate reflection of the Fermi surface in Bi-based cuprate superconductors. In this paper we experimentally prove that the main contribution to the intensity variation comes from matrix elements effects and develop an approach to overcome this problem. We introduce a concept of 'self-normalization' which makes the spectra essentially independent of both the matrix elements and particular experimental parameters. On the basis of this concept we suggest a simple and precise method of Fermi surface determination in quasi-2D systems. 74.25.Jb, 74.72.Hs, 71.18.+y
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