In this paper, the XPS study of SnO2 thin films deposited by the L-CVD technique are presented. The influence of exposition of the as-deposited samples to oxygen O2 and hydrogen H2 on their stoichiometry was determined. Moreover, on the basis of detailed shape analysis of the Sn3d5/2 and O1s XPS peaks, the chemical shift of binding energy corresponding to the change of sample stoichiometry was separated from a shift of the binding energy corresponding to the change of interface Fermi level position EF-Ev in the band gap, using a new procedure of deconvolution of the core level XPS peaks. The shift of the Sn3d5/2 peak by approximately 0.5 eV towards the lower binding energy after highest H2 exposure was interpreted as a true chemical shift due to an increase of Sn2+ component, whereas the shift of Sn3d5/2 peak and O1s peak after highest O2 exposure by approximately 0.5 eV towards the lower binding energy was interpreted as a result of the shift of the interface Fermi level position in the band gap towards the top of valence band at the surface, which corresponds to a deep accumulation layer typical for SnO2 thin films. © 2001 Elsevier Science B.V.

XPS study of the L-CVD deposited SnO2 thin films exposed to oxygen and hydrogen

Larciprete;
2001

Abstract

In this paper, the XPS study of SnO2 thin films deposited by the L-CVD technique are presented. The influence of exposition of the as-deposited samples to oxygen O2 and hydrogen H2 on their stoichiometry was determined. Moreover, on the basis of detailed shape analysis of the Sn3d5/2 and O1s XPS peaks, the chemical shift of binding energy corresponding to the change of sample stoichiometry was separated from a shift of the binding energy corresponding to the change of interface Fermi level position EF-Ev in the band gap, using a new procedure of deconvolution of the core level XPS peaks. The shift of the Sn3d5/2 peak by approximately 0.5 eV towards the lower binding energy after highest H2 exposure was interpreted as a true chemical shift due to an increase of Sn2+ component, whereas the shift of Sn3d5/2 peak and O1s peak after highest O2 exposure by approximately 0.5 eV towards the lower binding energy was interpreted as a result of the shift of the interface Fermi level position in the band gap towards the top of valence band at the surface, which corresponds to a deep accumulation layer typical for SnO2 thin films. © 2001 Elsevier Science B.V.
2001
Inglese
391
2
198
203
http://www.scopus.com/inward/record.url?eid=2-s2.0-0035898890&partnerID=40&md5=adc06783580a73114fe94d38921c135e
Binding energy
Chemical vapor deposition
Energy gap
Fermi level
Gas adsorption
Hydrogen
Oxygen
Semiconducting tin compounds
Stoichiometry
Thin films
X ray photoelectron spectroscopy
Chemical shift
Semiconducting films
cited By (since 1996)59; Conference of org.apache.xalan.xsltc.dom.DOMAdapter@6ec3d533 ; Conference Date: org.apache.xalan.xsltc.dom.DOMAdapter@7ae24014 Through org.apache.xalan.xsltc.dom.DOMAdapter@1bdd2013; Conference Code:58286
10
info:eu-repo/semantics/article
262
Szuber, ; Ja, ; Czempik, ; Ga, ; Larciprete, Rosanna; Rb, ; Koziej, ; Da, ; Adamowicz, ; Ba,
01 Contributo su Rivista::01.01 Articolo in rivista
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/243762
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