-
3
-
-
79958242516
-
-
note
-
2) was 4.1 eV.
-
-
-
-
4
-
-
3343006353
-
-
prb PRBMDO 0163-1829
-
F. J. Himpsel, F. R. McFeely, A. Taleb-Ibrahimi, and J. A. Yarmoff, Phys. Rev. B 38, 6084 (1988). prb PRBMDO 0163-1829
-
(1988)
Phys. Rev. B
, vol.38
, pp. 6084
-
-
Himpsel, F.J.1
McFeely, F.R.2
Taleb-Ibrahimi, A.3
Yarmoff, J.A.4
-
5
-
-
0000268239
-
-
apl APPLAB 0003-6951
-
Z. H. Lu, S. P. Tay, R. Cao, and P. Pianetta, Appl. Phys. Lett. 67, 2836 (1995). apl APPLAB 0003-6951
-
(1995)
Appl. Phys. Lett.
, vol.67
, pp. 2836
-
-
Lu, Z.H.1
Tay, S.P.2
Cao, R.3
Pianetta, P.4
-
6
-
-
0035894205
-
-
jaJAPIAU 0021-8979
-
A. Herrera-Gomez, F. S. Aguirre-Tostado, Y. Sun, P. Pianetta, Z. Yu, D. Marshall, R. Droopad, and W. E. Spicer, J. Appl. Phys. 90, 6070 (2001). jap JAPIAU 0021-8979
-
(2001)
J. Appl. Phys.
, vol.90
, pp. 6070
-
-
Herrera-Gomez, A.1
Aguirre-Tostado, F.S.2
Sun, Y.3
Pianetta, P.4
Yu, Z.5
Marshall, D.6
Droopad, R.7
Spicer, W.E.8
-
7
-
-
0031548650
-
-
asu ASUSEE 0169-4332
-
G. Lucovsky, A. Banerjee, H. Niimi, K. Koh, B. Hinds, C. Meyer, G. Lupke, and H. Kurz, Appl. Surf. Sci. 117/118, 202 (1997). asu ASUSEE 0169-4332
-
(1997)
Appl. Surf. Sci.
, vol.117-118
, pp. 202
-
-
Lucovsky, G.1
Banerjee, A.2
Niimi, H.3
Koh, K.4
Hinds, B.5
Meyer, C.6
Lupke, G.7
Kurz, H.8
-
8
-
-
79958206730
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-
A copy of AAnalyzer can be obtained at
-
A copy of AAnalyzer can be obtained at http://arcos.qro.cinvestav.mx/ ∼aanalyzer/
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-
-
-
9
-
-
0032615232
-
-
jaJAPIAU 0021-8979
-
L. G. Gosset, J. J. Ganem, H. J. von Bardeleben, S. Rigo, I. Trimaille, J. L. Cantin, T. Akermark, and I. C. Vickridge, J. Appl. Phys. 85, 3661 (1999). jap JAPIAU 0021-8979
-
(1999)
J. Appl. Phys.
, vol.85
, pp. 3661
-
-
Gosset, L.G.1
Ganem, J.J.2
Von Bardeleben, H.J.3
Rigo, S.4
Trimaille, I.5
Cantin, J.L.6
Akermark, T.7
Vickridge, I.C.8
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11
-
-
79958194991
-
-
note
-
2 films), the use of relative sensibility factors yields to large uncertainties.
-
-
-
-
12
-
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0000944801
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-
jaJAPIAU 0021-8979
-
J. P. Chang, M. L. Green, V. M. Donnelly, R. L. Opila, J. Eng, J. Sapjeta, P. J. Silverman, and B. Weir, J. Appl. Phys. 87, 4449 (2000). jap JAPIAU 0021-8979
-
(2000)
J. Appl. Phys.
, vol.87
, pp. 4449
-
-
Chang, J.P.1
Green, M.L.2
Donnelly, V.M.3
Opila, R.L.4
Eng, J.5
Sapjeta, J.6
Silverman, P.J.7
Weir, B.8
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13
-
-
0003037887
-
-
as discussed by Cumpson, a Laplace transform is only of very limited use in this connection, whether it is done with a maximum entropy method or with any other regularization method. It also shows that, without a regularization method, it is impossible to perform the Laplace back transform because the problem is numerically unstable. jer JESRAW 0368-2048
-
P. Cumpson, J. Electron Spectrosc. Relat. Phenom. 73, 25 (1995); as discussed by Cumpson, a Laplace transform is only of very limited use in this connection, whether it is done with a maximum entropy method or with any other regularization method. It also shows that, without a regularization method, it is impossible to perform the Laplace back transform because the problem is numerically unstable. jer JESRAW 0368-2048
-
(1995)
J. Electron Spectrosc. Relat. Phenom.
, vol.73
, pp. 25
-
-
Cumpson, P.1
-
14
-
-
33745682743
-
-
phr PHRVAO 0031-899X
-
W. E. Spicer, Phys. Rev. 112, 114 (1958). phr PHRVAO 0031-899X
-
(1958)
Phys. Rev.
, vol.112
, pp. 114
-
-
Spicer, W.E.1
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18
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79958198185
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-
note
-
L should be regarded as an upper limit of the actual film thickness, and those reported in Table II as the lower limit of the actual density.
-
-
-
-
19
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79958225220
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If the analysis were done without accounting for depth profile effects, the amount of N and O would be subestimated due to their smaller escape depth
-
If the analysis were done without accounting for depth profile effects, the amount of N and O would be subestimated due to their smaller escape depth.
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-
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