Use and limitations of electron flood gun control of surface potential during XPS: two non‐homogeneous sample types

The ability of charge compensation methods to control surface potential is examined for two types of non‐homogenous samples: a small conducting dot on an insulating substrate and an insulating thin film on a conductive substrate. Results demonstrate that two newer types of charge compensation systems have improved performance in relation to some previous flood gun systems, while reaffirming the concept that a primary objective of charge compensation is to find conditions for which the surface potential of the specimen is as uniform as possible. However, experiments involving both flood gun use and specimen grounding demonstrate that peak broadening and shifting can occur when two (or more) potentials are present in the region of analysis. Finally, the ability of interface charge to shift specimen potentials and measured binding energies demonstrates fundamental limitations to the absolute accuracy of binding energy measurements, but also remind us that charging phenomena can be used to obtain important information about the sample. Copyright © 2002 John Wiley & Sons, Ltd.

[1]  M. Engelhard,et al.  Practical Aspects of Charging Phenomena in XPS as demonstrated in Oxidized-Al Films on Al and Al Alloys , 2002 .

[2]  S. Chambers,et al.  Role of oxide ionicity in electronic screening at oxide/metal interfaces , 2001 .

[3]  J. Cazaux About the charge compensation of insulating samples in XPS , 2000 .

[4]  VAMAS TWA2 Project A2: evaluation of static charge stabilization and determination methods in XPS on non‐conducting samples. Report on an inter‐laboratory comparison , 2000 .

[5]  Ilanit Doron-Mor,et al.  Controlled surface charging as a depth-profiling probe for mesoscopic layers , 2000, Nature.

[6]  M. Engelhard,et al.  Influence of Mg on the corrosion of Al , 2000 .

[7]  J. Cazaux,et al.  Mechanisms of charging in electron spectroscopy , 1999 .

[8]  J. Metson Charge compensation and binding energy referencing in XPS analysis , 1999 .

[9]  L. Tjeng,et al.  REDUCTION OF COULOMB AND CHARGE-TRANSFER ENERGIES IN OXIDE FILMS ON METALS , 1999 .

[10]  M. Kelly,et al.  Surface charge neutralization of insulating samples in x-ray photoemission spectroscopy , 1998 .

[11]  P. Rouxhet,et al.  Surface charging of insulating samples in X-ray photoelectron spectroscopy , 1998 .

[12]  J. Fulghum,et al.  Differential charging in XPS. Part III. A comparison of charging in thin polymer overlayers on conducting and non‐conducting substrates , 1997 .

[13]  T. Madey,et al.  Growth and oxidation of ultra-thin Al films on the Re (0001) surface , 1996 .

[14]  J. Fulghum,et al.  Differential Charging in XPS. Part II: Sample Mounting and X‐ray Flux Effects on Heterogeneous Samples , 1996 .

[15]  P. C. Rieke,et al.  Electron beam effects on (CH2)17 self‐assembled monolayer SiO2/Si specimens , 1994 .

[16]  D. Ramaker,et al.  X‐ray photoelectron spectroscopy study on the electrical double layer at an Al2O3–Al interface , 1992 .

[17]  T. Barr Studies in differential charging , 1989 .

[18]  J. Castle,et al.  Biased referencing experiments for the XPS analysis of non-conducting materials , 1986 .

[19]  J. Castle,et al.  The use of an electron flood gun when adopting monochromatic AgLα radiation for the XPS analysis of insulators , 1986 .

[20]  W. Landis,et al.  X‐ray photoelectron spectroscopy applied to gold‐decorated mineral standards of biological interest , 1984 .

[21]  P. Swift Adventitious carbon—the panacea for energy referencing? , 1982 .

[22]  M. Kelly,et al.  Binding-energy reference in X-ray photoelectron spectroscopy of insulators , 1980 .

[23]  N. J. Binkowski,et al.  X-ray photoelectron spectroscopy of silica in theory and experiment , 1976 .