This paper shows that in copper oxide based compounds where Cu ions are in a square planar geometry with four coordination oxygen ions, i.e. CuO and Nd2CuO4, the Cu2p 3 2 (3d)10L) X-ray photoelectron core lines are narrower than in similar compounds with Cu ions in a pyramidal or octahedral geometry with five or six neighboring oxygens, i.e. Bi2Sr2CaCu2O8 and La2CuO4. To explain this difference two different charge transfer mechanisms from the oxygen p orbitals to the Cu3d orbitals are proposed. For square planar geometry (CuO4) only the px,y → dxjavax.xml.bind.JAXBElement@337bf26c - yjavax.xml.bind.JAXBElement@4aae6dcb charge transfer is allowed, whereas for octahedral or pyramidal geometry the additional pz → dzjavax.xml.bind.JAXBElement@48ef4e23 transition could take place. These two different final state configurations will produce different ionization potentials for the Cu2p 3 2 core levels. © 1992.

The fine structure of the Cu2p 3 2 X-ray photoelectron spectra of copper oxide based compounds / Parmigiani, F.; Depero, L. E.; Minerva, T.; Torrance, J. B.. - In: JOURNAL OF ELECTRON SPECTROSCOPY AND RELATED PHENOMENA. - ISSN 0368-2048. - 58:4(1992), pp. 315-323. [10.1016/0368-2048(92)85017-2]

The fine structure of the Cu2p 3 2 X-ray photoelectron spectra of copper oxide based compounds

Parmigiani F.;Minerva T.;
1992

Abstract

This paper shows that in copper oxide based compounds where Cu ions are in a square planar geometry with four coordination oxygen ions, i.e. CuO and Nd2CuO4, the Cu2p 3 2 (3d)10L) X-ray photoelectron core lines are narrower than in similar compounds with Cu ions in a pyramidal or octahedral geometry with five or six neighboring oxygens, i.e. Bi2Sr2CaCu2O8 and La2CuO4. To explain this difference two different charge transfer mechanisms from the oxygen p orbitals to the Cu3d orbitals are proposed. For square planar geometry (CuO4) only the px,y → dxjavax.xml.bind.JAXBElement@337bf26c - yjavax.xml.bind.JAXBElement@4aae6dcb charge transfer is allowed, whereas for octahedral or pyramidal geometry the additional pz → dzjavax.xml.bind.JAXBElement@48ef4e23 transition could take place. These two different final state configurations will produce different ionization potentials for the Cu2p 3 2 core levels. © 1992.
1992
58
4
315
323
The fine structure of the Cu2p 3 2 X-ray photoelectron spectra of copper oxide based compounds / Parmigiani, F.; Depero, L. E.; Minerva, T.; Torrance, J. B.. - In: JOURNAL OF ELECTRON SPECTROSCOPY AND RELATED PHENOMENA. - ISSN 0368-2048. - 58:4(1992), pp. 315-323. [10.1016/0368-2048(92)85017-2]
Parmigiani, F.; Depero, L. E.; Minerva, T.; Torrance, J. B.
File in questo prodotto:
File Dimensione Formato  
1-s2.0-0368204892850172-main.pdf

Accesso riservato

Tipologia: Versione pubblicata dall'editore
Dimensione 665.31 kB
Formato Adobe PDF
665.31 kB Adobe PDF   Visualizza/Apri   Richiedi una copia
Pubblicazioni consigliate

Licenza Creative Commons
I metadati presenti in IRIS UNIMORE sono rilasciati con licenza Creative Commons CC0 1.0 Universal, mentre i file delle pubblicazioni sono rilasciati con licenza Attribuzione 4.0 Internazionale (CC BY 4.0), salvo diversa indicazione.
In caso di violazione di copyright, contattare Supporto Iris

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11380/1274964
Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 41
  • ???jsp.display-item.citation.isi??? 43
social impact