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2 and Its Interfaces, edited by S. T. Pantelides and G. Lucovsky (Material Research Society, Pittsburgh, 1990); The Physics and Technology of Amorphous Silicon Dioxide, edited by C. R. Helms and B. E. Deal (Plenum, New York, 1989).
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2 Interface 2
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Helms, C.R.1
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Plenum, New York
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2 and Its Interfaces, edited by S. T. Pantelides and G. Lucovsky (Material Research Society, Pittsburgh, 1990); The Physics and Technology of Amorphous Silicon Dioxide, edited by C. R. Helms and B. E. Deal (Plenum, New York, 1989).
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Devine, R.A.B.1
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Material Research Society, Pittsburgh
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2 and Its Interfaces, edited by S. T. Pantelides and G. Lucovsky (Material Research Society, Pittsburgh, 1990); The Physics and Technology of Amorphous Silicon Dioxide, edited by C. R. Helms and B. E. Deal (Plenum, New York, 1989).
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Pantelides, S.T.1
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McFeely, F.R.1
Zhang, K.Z.2
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Lee, S.4
Bender, J.E.5
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8
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85033177317
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note
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2/Si interface as well as a summary of the Si-O ring size discussion in Ref. 6.
-
-
-
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11
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85033190190
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note
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Initial state effects refer to structural and compositional features of the material that influence the energy level of the core state prior to interaction with the exciting photon. In general, any change that effects the valence electron distribution will also cause the energy of the core electrons to vary.
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-
-
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12
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85033178694
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note
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Final state effects refer to mechanisms that serve to stabilize (or destabilize) the positively charged core-hole state that is formed upon ejection of the photoelectron from the emitting atom.
-
-
-
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13
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85033180055
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note
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Extrinsic effects are defined as those not related to the specific geometric or electronic structure of the material to be studied, but are instead related to details of the experimental conditions. For example, charging occurs when insulating samples are exposed to an x-ray source.
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-
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14
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33751498968
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P. A. Agaskar, Inorg. Chem. 30, 2707 (1991); P. A. Agaskar and W. G. Klemperer, Inorg. Chim. Acta 229, 355 (1995); C. L. Frye and W. T. Collins, J. Am. Chem. Soc. 92, 5586 (1970); R. Müller, R. Kohne, and S. Sliwinski, J. Prakt. Chem. 9, 71 (1959).
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33748956618
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P. A. Agaskar, Inorg. Chem. 30, 2707 (1991); P. A. Agaskar and W. G. Klemperer, Inorg. Chim. Acta 229, 355 (1995); C. L. Frye and W. T. Collins, J. Am. Chem. Soc. 92, 5586 (1970); R. Müller, R. Kohne, and S. Sliwinski, J. Prakt. Chem. 9, 71 (1959).
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33947294857
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P. A. Agaskar, Inorg. Chem. 30, 2707 (1991); P. A. Agaskar and W. G. Klemperer, Inorg. Chim. Acta 229, 355 (1995); C. L. Frye and W. T. Collins, J. Am. Chem. Soc. 92, 5586 (1970); R. Müller, R. Kohne, and S. Sliwinski, J. Prakt. Chem. 9, 71 (1959).
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Frye, C.L.1
Collins, W.T.2
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33751498968
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P. A. Agaskar, Inorg. Chem. 30, 2707 (1991); P. A. Agaskar and W. G. Klemperer, Inorg. Chim. Acta 229, 355 (1995); C. L. Frye and W. T. Collins, J. Am. Chem. Soc. 92, 5586 (1970); R. Müller, R. Kohne, and S. Sliwinski, J. Prakt. Chem. 9, 71 (1959).
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Müller, R.1
Kohne, R.2
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M. M. Banaszak Holl and F. R. McFeely, Phys. Rev. Lett. 72, 2441 (1993); S. Lee, S. Makan, M. M. Banaszak Holl, and F. R. McFeely, J. Am. Chem. Soc. 116, 11 819 (1994); K. Z. Zang, L. M. Meeuwenberg, M. M. Banaszak Holl, and F. R. McFeely, Jpn. J. Appl. Phys. 36, 1622 (1997).
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McFeely, F.R.2
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19
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M. M. Banaszak Holl and F. R. McFeely, Phys. Rev. Lett. 72, 2441 (1993); S. Lee, S. Makan, M. M. Banaszak Holl, and F. R. McFeely, J. Am. Chem. Soc. 116, 11 819 (1994); K. Z. Zang, L. M. Meeuwenberg, M. M. Banaszak Holl, and F. R. McFeely, Jpn. J. Appl. Phys. 36, 1622 (1997).
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0011748705
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M. M. Banaszak Holl and F. R. McFeely, Phys. Rev. Lett. 72, 2441 (1993); S. Lee, S. Makan, M. M. Banaszak Holl, and F. R. McFeely, J. Am. Chem. Soc. 116, 11 819 (1994); K. Z. Zang, L. M. Meeuwenberg, M. M. Banaszak Holl, and F. R. McFeely, Jpn. J. Appl. Phys. 36, 1622 (1997).
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Zang, K.Z.1
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21
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0000355943
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S. Lee, M. M. Banaszak Holl, W. H. Hung, and F. R. McFeely, Appl. Phys. Lett. 68, 1081 (1996).
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3343006353
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F. J. Himpsel, F. R. McFeely, A. Taleb-Ibrahimi, J. A. Yarmoff, and G. Hollinger, Phys. Rev. B 38, 6084 (1988).
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Himpsel, F.J.1
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Yarmoff, J.A.4
Hollinger, G.5
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23
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85033178054
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note
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1/2 component of the Si 2p core level has not been removed.
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-
-
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24
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85033185260
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note
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The use of this ratio avoids the introduction of error caused by slight differences in sample alignment which can lead to a variation in absolute intensity from spectrum to spectrum.
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-
-
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25
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85033189045
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-
note
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The reported value is the average of four runs. The standard deviation is given in parentheses.
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26
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85033177601
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-
note
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Equation (5) explicitly assumes that significant islanding does not occur. We explored the effect of such islanding by adding the possibility of a third incomplete layer to the calculation. This resulted in a maximum 10% error in the calculated ratio.
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27
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3743134709
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T. P. E. Auf der Hyde, H.-B. Bürgi, H. Bürgi, and K. W. Törnroos, Chimia 45, 138 (1991).
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Auf Der Hyde, T.P.E.1
Bürgi, H.-B.2
Bürgi, H.3
Törnroos, K.W.4
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28
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85033162260
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Run 3 corresponds to the data in Fig. 7 and run 2 corresponds to the 170 eV data in Fig. 5
-
Run 3 corresponds to the data in Fig. 7 and run 2 corresponds to the 170 eV data in Fig. 5.
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-
-
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29
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85033173161
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See Fig. 6, page 6659 of Ref. 2
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See Fig. 6, page 6659 of Ref. 2.
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30
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0018467123
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S. Iwata and A. Ishizaka, J. Jpn. Inst. Metals 43, 380 (1979); S. Iwata and A. Ishizaka, J. Jpn. Inst. Metals 43, 388 (1979); A. Ishizaka, S. Iwata, and Y. Kamigaki, Surf. Sci. 84, 355 (1979); A. Ishizaka and S. Iwata, Appl. Phys. Lett. 36, 71 (1980).
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85033182756
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See Sec. III, 2, c, page 6673 of Ref. 2
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See Sec. III, 2, c, page 6673 of Ref. 2.
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-
-
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35
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85033166157
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note
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The FWHM of the spectral features in panel C do increase as a function of photon energy, but this is wholly a consequence of the monochromator/ analyzer resolution function.
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36
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0003828439
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Wiley, New York
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The broadening of photoemission features as a sample charges is attributed to the inhomogeneous nature of the resulting charge distribution. Practical Surface Analysis, 2nd ed., edited by D. Briggs and M. P. Seah (Wiley, New York, 1990).
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