Coexistence of localized and delocalized states in Bi-2212 Y/Ca. An investigation of the infrared and optical absorption

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Authors

  • C. H. Rüscher
  • M. Götte
  • B. Schmidt
  • C. Quitmann
  • G. Güntherodt

Research Organisations

External Research Organisations

  • RWTH Aachen University
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Details

Original languageEnglish
Pages (from-to)30-42
Number of pages13
JournalPhysica C: Superconductivity and its Applications
Volume204
Issue number1-2
Publication statusPublished - 20 Dec 1992

Abstract

We have studied the absorption of the system Bi-2212 Y/Ca (Bi2Sr2Ca1-xYxCu2O 8+δ with 0 ≤x≤0.9) in the spectra l range 600 to 20 000 cm-1. We observe systematical changes of the spectra as a function of Y-content. The temperature dependence of the NIR absorption of the samples possessing superconductivity (x < 0.5) shows a change at Tc, indicating its coupling to superconducti vity. We decompose the absorption spectra into at most three different contributions and observe that each changes as a function of Y content. First, a structureless contribution, modelled by α ∼ (h{stroke}ω-Ed)1.5 /h{stroke}ω, is attributed to transitions between delocalized and non-occupied localized states with excitation energy Ed(x). Second, a prominent peak at 13 500 cm-1 (≈ 1.7 eV) for all insulating samples, indicating the charge transfer gap and finally a near infrared (NIR) peak in the range from 1500 cm-1 to 7000 cm-1. The shape of the NIR peak suggests that the absorption is caused by photon assisted hopping of small polarons in disordered systems. We propose a schematic density of states including localized and delocalized states which is in accordance with absorption properties and the obtained fit parameters. In particular the Fermi energy cuts the bandedge of delocalized states at x∼ 0.5 as a result of hole doping (decreasing Y content). This can explain the metal (superconductor) / insulator transition in accordance with electrical transport properties and indicates the coexistence of delocalized and localized states at the Fermi energy for x<0.5.

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Coexistence of localized and delocalized states in Bi-2212 Y/Ca. An investigation of the infrared and optical absorption. / Rüscher, C. H.; Götte, M.; Schmidt, B. et al.
In: Physica C: Superconductivity and its Applications, Vol. 204, No. 1-2, 20.12.1992, p. 30-42.

Research output: Contribution to journalArticleResearchpeer review

Rüscher CH, Götte M, Schmidt B, Quitmann C, Güntherodt G. Coexistence of localized and delocalized states in Bi-2212 Y/Ca. An investigation of the infrared and optical absorption. Physica C: Superconductivity and its Applications. 1992 Dec 20;204(1-2):30-42. doi: 10.1016/0921-4534(92)90569-X
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abstract = "We have studied the absorption of the system Bi-2212 Y/Ca (Bi2Sr2Ca1-xYxCu2O 8+δ with 0 ≤x≤0.9) in the spectra l range 600 to 20 000 cm-1. We observe systematical changes of the spectra as a function of Y-content. The temperature dependence of the NIR absorption of the samples possessing superconductivity (x < 0.5) shows a change at Tc, indicating its coupling to superconducti vity. We decompose the absorption spectra into at most three different contributions and observe that each changes as a function of Y content. First, a structureless contribution, modelled by α ∼ (h{stroke}ω-Ed)1.5 /h{stroke}ω, is attributed to transitions between delocalized and non-occupied localized states with excitation energy Ed(x). Second, a prominent peak at 13 500 cm-1 (≈ 1.7 eV) for all insulating samples, indicating the charge transfer gap and finally a near infrared (NIR) peak in the range from 1500 cm-1 to 7000 cm-1. The shape of the NIR peak suggests that the absorption is caused by photon assisted hopping of small polarons in disordered systems. We propose a schematic density of states including localized and delocalized states which is in accordance with absorption properties and the obtained fit parameters. In particular the Fermi energy cuts the bandedge of delocalized states at x∼ 0.5 as a result of hole doping (decreasing Y content). This can explain the metal (superconductor) / insulator transition in accordance with electrical transport properties and indicates the coexistence of delocalized and localized states at the Fermi energy for x<0.5.",
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T1 - Coexistence of localized and delocalized states in Bi-2212 Y/Ca. An investigation of the infrared and optical absorption

AU - Rüscher, C. H.

AU - Götte, M.

AU - Schmidt, B.

AU - Quitmann, C.

AU - Güntherodt, G.

PY - 1992/12/20

Y1 - 1992/12/20

N2 - We have studied the absorption of the system Bi-2212 Y/Ca (Bi2Sr2Ca1-xYxCu2O 8+δ with 0 ≤x≤0.9) in the spectra l range 600 to 20 000 cm-1. We observe systematical changes of the spectra as a function of Y-content. The temperature dependence of the NIR absorption of the samples possessing superconductivity (x < 0.5) shows a change at Tc, indicating its coupling to superconducti vity. We decompose the absorption spectra into at most three different contributions and observe that each changes as a function of Y content. First, a structureless contribution, modelled by α ∼ (h{stroke}ω-Ed)1.5 /h{stroke}ω, is attributed to transitions between delocalized and non-occupied localized states with excitation energy Ed(x). Second, a prominent peak at 13 500 cm-1 (≈ 1.7 eV) for all insulating samples, indicating the charge transfer gap and finally a near infrared (NIR) peak in the range from 1500 cm-1 to 7000 cm-1. The shape of the NIR peak suggests that the absorption is caused by photon assisted hopping of small polarons in disordered systems. We propose a schematic density of states including localized and delocalized states which is in accordance with absorption properties and the obtained fit parameters. In particular the Fermi energy cuts the bandedge of delocalized states at x∼ 0.5 as a result of hole doping (decreasing Y content). This can explain the metal (superconductor) / insulator transition in accordance with electrical transport properties and indicates the coexistence of delocalized and localized states at the Fermi energy for x<0.5.

AB - We have studied the absorption of the system Bi-2212 Y/Ca (Bi2Sr2Ca1-xYxCu2O 8+δ with 0 ≤x≤0.9) in the spectra l range 600 to 20 000 cm-1. We observe systematical changes of the spectra as a function of Y-content. The temperature dependence of the NIR absorption of the samples possessing superconductivity (x < 0.5) shows a change at Tc, indicating its coupling to superconducti vity. We decompose the absorption spectra into at most three different contributions and observe that each changes as a function of Y content. First, a structureless contribution, modelled by α ∼ (h{stroke}ω-Ed)1.5 /h{stroke}ω, is attributed to transitions between delocalized and non-occupied localized states with excitation energy Ed(x). Second, a prominent peak at 13 500 cm-1 (≈ 1.7 eV) for all insulating samples, indicating the charge transfer gap and finally a near infrared (NIR) peak in the range from 1500 cm-1 to 7000 cm-1. The shape of the NIR peak suggests that the absorption is caused by photon assisted hopping of small polarons in disordered systems. We propose a schematic density of states including localized and delocalized states which is in accordance with absorption properties and the obtained fit parameters. In particular the Fermi energy cuts the bandedge of delocalized states at x∼ 0.5 as a result of hole doping (decreasing Y content). This can explain the metal (superconductor) / insulator transition in accordance with electrical transport properties and indicates the coexistence of delocalized and localized states at the Fermi energy for x<0.5.

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