-
2
-
-
33749626663
-
-
10.1016/j.pmatsci.2006.02.002
-
P. H. Mayrhofer, C. Mitterer, L. Hultman, and H. Clemens, Prog. Mater. Sci. 51, 1032 (2006). 10.1016/j.pmatsci.2006.02.002
-
(2006)
Prog. Mater. Sci.
, vol.51
, pp. 1032
-
-
Mayrhofer, P.H.1
Mitterer, C.2
Hultman, L.3
Clemens, H.4
-
4
-
-
0002173308
-
-
10.1016/S0042-207X(00)00143-3
-
L. Hultman, Vacuum 57, 1 (2000). 10.1016/S0042-207X(00)00143-3
-
(2000)
Vacuum
, vol.57
, pp. 1
-
-
Hultman, L.1
-
8
-
-
34548846377
-
-
10.1103/PhysRevLett.99.125503
-
L. Tsetseris, N. Kalfagiannis, S. Logothetidis, and S. T. Pantelides, Phys. Rev. Lett. 99, 125503 (2007). 10.1103/PhysRevLett.99.125503
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 125503
-
-
Tsetseris, L.1
Kalfagiannis, N.2
Logothetidis, S.3
Pantelides, S.T.4
-
10
-
-
56649089767
-
-
10.1016/j.tsf.2008.06.006
-
P. Lazar, B. Rashkova, J. Redinger, R. Podloucky, C. Mitterer, C. Scheu, and G. Dehm, Thin Solid Films 517, 1177 (2008). 10.1016/j.tsf.2008.06.006
-
(2008)
Thin Solid Films
, vol.517
, pp. 1177
-
-
Lazar, P.1
Rashkova, B.2
Redinger, J.3
Podloucky, R.4
Mitterer, C.5
Scheu, C.6
Dehm, G.7
-
11
-
-
34247558037
-
-
10.1103/PhysRevB.75.155437
-
L. Hultman, J. Bareño, A. Flink, H. Söderberg, K. Larsson, V. Petrova, M. Odén, J. E. Greene, and I. Petrov, Phys. Rev. B 75, 155437 (2007). 10.1103/PhysRevB.75.155437
-
(2007)
Phys. Rev. B
, vol.75
, pp. 155437
-
-
Hultman, L.1
Bareño, J.2
Flink, A.3
Söderberg, H.4
Larsson, K.5
Petrova, V.6
Odén, M.7
Greene, J.E.8
Petrov, I.9
-
12
-
-
1642376015
-
-
10.1126/science.1093617
-
C. L. Jia and K. Urban, Science 303, 2001 (2004). 10.1126/science.1093617
-
(2004)
Science
, vol.303
, pp. 2001
-
-
Jia, C.L.1
Urban, K.2
-
13
-
-
63049114269
-
-
10.1038/nmat2380
-
D. Muller, Nature Mater. 8, 263 (2009). 10.1038/nmat2380
-
(2009)
Nature Mater.
, vol.8
, pp. 263
-
-
Muller, D.1
-
14
-
-
36049042572
-
-
10.1016/j.tsf.2007.06.104
-
K. Kutschej, B. Rashkova, J. Shen, D. Edwards, C. Mitterer, and G. Dehm, Thin Solid Films 516, 369 (2007). 10.1016/j.tsf.2007.06.104
-
(2007)
Thin Solid Films
, vol.516
, pp. 369
-
-
Kutschej, K.1
Rashkova, B.2
Shen, J.3
Edwards, D.4
Mitterer, C.5
Dehm, G.6
-
16
-
-
0011236321
-
-
10.1103/PhysRevB.59.1758
-
G. Kresse and D. Joubert, Phys. Rev. B 59, 1758 (1999). 10.1103/PhysRevB.59.1758
-
(1999)
Phys. Rev. B
, vol.59
, pp. 1758
-
-
Kresse, G.1
Joubert, D.2
-
17
-
-
23244460838
-
-
10.1103/PhysRevB.46.6671
-
J. P. Perdew, J. A. Chevary, S. H. Vosko, K. A. Jackson, M. R. Pederson, D. J. Singh, and C. Fiolhais, Phys. Rev. B 46, 6671 (1992). 10.1103/PhysRevB.46. 6671
-
(1992)
Phys. Rev. B
, vol.46
, pp. 6671
-
-
Perdew, J.P.1
Chevary, J.A.2
Vosko, S.H.3
Jackson, K.A.4
Pederson, M.R.5
Singh, D.J.6
Fiolhais, C.7
-
20
-
-
77957350257
-
-
The mean value obtained by averaging over the whole image area is used as a reference. The corresponding spacing difference ( δi ) for each interplanar spacing ( di ) is then obtained by subtracting the mean value ( dmean ), i.e., δi = di - dmean
-
The mean value obtained by averaging over the whole image area is used as a reference. The corresponding spacing difference (δ i) for each interplanar spacing (d i) is then obtained by subtracting the mean value (d m e a n), i.e., δ i = d i - d m e a n.
-
-
-
-
21
-
-
77957370397
-
-
As V L2,3 (509 eV) and OK (532 eV) edges are very close, the quantification for V and N was carried out by using the bulk VN and MgO as standards, and a special procedure was used to calculate the net O integrated intensity. The determination of the L3 / L2 ratio is as follows: (i) firstly, the background is removed and (ii) secondly, the VL edges are fit with a double step continuum model. Finally, after the continuum subtraction, the WL intensities I ( L3 ) and I ( L2 ) are obtained by integration of the peaks under certain energy windows
-
As V L 2, 3 (509 eV) and O K (532 eV) edges are very close, the quantification for V and N was carried out by using the bulk VN and MgO as standards, and a special procedure was used to calculate the net O integrated intensity. The determination of the L 3 / L 2 ratio is as follows: (i) firstly, the background is removed and (ii) secondly, the V L edges are fit with a double step continuum model. Finally, after the continuum subtraction, the WL intensities I (L 3) and I (L 2) are obtained by integration of the peaks under certain energy windows.
-
-
-
-
22
-
-
37149014721
-
-
10.3139/146.101568
-
B. Rashkova, P. Lazar, J. Redinger, R. Podloucky, G. Kothleitner, S. Sturm, K. Kutschej, C. Mitterer, C. Scheu, and G. Dehm, Int. J. Mater. Res. 98, 11 (2007). 10.3139/146.101568
-
(2007)
Int. J. Mater. Res.
, vol.98
, pp. 11
-
-
Rashkova, B.1
Lazar, P.2
Redinger, J.3
Podloucky, R.4
Kothleitner, G.5
Sturm, S.6
Kutschej, K.7
Mitterer, C.8
Scheu, C.9
Dehm, G.10
-
23
-
-
0035159968
-
-
10.1046/j.1365-2818.2001.00946.x
-
F. Hofer, P. Warbichler, A. Scott, R. Brydson, I. Galesi, and B. Kolbesen, J. Microsc. 204, 166 (2001). 10.1046/j.1365-2818.2001.00946.x
-
(2001)
J. Microsc.
, vol.204
, pp. 166
-
-
Hofer, F.1
Warbichler, P.2
Scott, A.3
Brydson, R.4
Galesi, I.5
Kolbesen, B.6
-
24
-
-
0036662389
-
-
10.1023/A:1016099704259
-
M. Wieske, D. S. Su, F. Beckmann, and R. Schlögl, Catal. Lett. 81, 43 (2002). 10.1023/A:1016099704259
-
(2002)
Catal. Lett.
, vol.81
, pp. 43
-
-
Wieske, M.1
Su, D.S.2
Beckmann, F.3
Schlögl, R.4
|