-
3
-
-
0000586534
-
-
10.1038/380141a0
-
Y. Moritomo, A. Asamitsu, H. Kuwahara, and Y. Tokura, Nature (London) 380, 141 (1996). 10.1038/380141a0
-
(1996)
Nature (London)
, vol.380
, pp. 141
-
-
Moritomo, Y.1
Asamitsu, A.2
Kuwahara, H.3
Tokura, Y.4
-
5
-
-
0027115880
-
-
10.1038/358136a0
-
R. Cohen, Nature (London) 358, 136 (1992). 10.1038/358136a0
-
(1992)
Nature (London)
, vol.358
, pp. 136
-
-
Cohen, R.1
-
6
-
-
33746493822
-
-
10.1107/S0108768195003752
-
Y. A. Abramov, V. G. Tsirelson, V. E. Zavodnik, S. A. Ivanov, and I. D. Brown, Acta Crystallogr., Sect. B: Struct. Sci. 51, 942 (1995). 10.1107/S0108768195003752
-
(1995)
Acta Crystallogr., Sect. B: Struct. Sci.
, vol.51
, pp. 942
-
-
Abramov, Y.A.1
Tsirelson, V.G.2
Zavodnik, V.E.3
Ivanov, S.A.4
Brown, I.D.5
-
7
-
-
0034451531
-
-
10.1103/PhysRevB.62.13942
-
N. Sai and D. Vanderbilt, Phys. Rev. B 62, 13942 (2000). 10.1103/PhysRevB.62.13942
-
(2000)
Phys. Rev. B
, vol.62
, pp. 13942
-
-
Sai, N.1
Vanderbilt, D.2
-
8
-
-
38949178378
-
-
10.1088/0953-8984/20/8/085204
-
R. Blinc, V. V. Laguta, B. Zalar, M. Itoh, and H. Krakauer, J. Phys.: Condens. Matter 20, 085204 (2008). 10.1088/0953-8984/20/8/085204
-
(2008)
J. Phys.: Condens. Matter
, vol.20
, pp. 085204
-
-
Blinc, R.1
Laguta, V.V.2
Zalar, B.3
Itoh, M.4
Krakauer, H.5
-
10
-
-
70350634648
-
-
http://www.FPLO.de
-
-
-
-
11
-
-
33645898818
-
-
10.1103/PhysRevB.45.13244
-
J. P. Perdew and Y. Wang, Phys. Rev. B 45, 13244 (1992). 10.1103/PhysRevB.45.13244
-
(1992)
Phys. Rev. B
, vol.45
, pp. 13244
-
-
Perdew, J.P.1
Wang, Y.2
-
12
-
-
70350634649
-
-
We also calculated the EFG for the low-symmetry phases of BTO and STO. Whereas the calculational results for BTO agree well with the experiment, the discrepancy for STO remains unchanged and of unclear reason.
-
We also calculated the EFG for the low-symmetry phases of BTO and STO. Whereas the calculational results for BTO agree well with the experiment, the discrepancy for STO remains unchanged and of unclear reason.
-
-
-
-
14
-
-
36049054436
-
-
10.1103/PhysRev.181.987
-
L. F. Mattheiss, Phys. Rev. 181, 987 (1969). 10.1103/PhysRev.181.987
-
(1969)
Phys. Rev.
, vol.181
, pp. 987
-
-
Mattheiss, L.F.1
-
15
-
-
0000878218
-
-
10.1103/PhysRevB.6.4718
-
L. F. Mattheiss, Phys. Rev. B 6, 4718 (1972). 10.1103/PhysRevB.6.4718
-
(1972)
Phys. Rev. B
, vol.6
, pp. 4718
-
-
Mattheiss, L.F.1
-
16
-
-
0011065899
-
-
10.1103/PhysRevB.2.3918
-
L. F. Mattheiss, Phys. Rev. B 2, 3918 (1970). 10.1103/PhysRevB.2.3918
-
(1970)
Phys. Rev. B
, vol.2
, pp. 3918
-
-
Mattheiss, L.F.1
-
17
-
-
0000096252
-
-
10.1103/PhysRevLett.29.1383
-
T. Wolfram, Phys. Rev. Lett. 29, 1383 (1972). 10.1103/PhysRevLett.29.1383
-
(1972)
Phys. Rev. Lett.
, vol.29
, pp. 1383
-
-
Wolfram, T.1
-
21
-
-
70350661363
-
-
The parameters Vπ and Vσ are from the WE (p-d) model and Vpdπ = Vπ and Vpdσ are from the Harrison (s-p-d) model, see Appendix 0, Sec. 3.
-
The parameters Vπ and Vσ are from the WE (p-d) model and Vpdπ = Vπ and Vpdσ are from the Harrison (s-p-d) model, see Appendix 0, Sec. 3.
-
-
-
-
23
-
-
70350628092
-
-
ε denotes the energy of the atomic level and E, as used before, denotes the energy-level corrected by the crystal field: Δσ = Ed - Ep = εd - εp + δCF,σ, cf. Eq. 26. Note, that δCF,m is different for m=π and m=σ, since εd is the atomic energy level and thus does not depend on m. This is the main reason, that, δCF,σ > δCF,π. Furthermore, δCF,σ has strong dependence on a.
-
ε denotes the energy of the atomic level and E, as used before, denotes the energy-level corrected by the crystal field: Δσ = Ed - Ep = εd - εp + δCF,σ, cf. Eq. 26. Note, that δCF,m is different for m=π and m=σ, since εd is the atomic energy level and thus does not depend on m. This is the main reason, that, δCF,σ > δCF,π. Furthermore, δCF,σ has strong dependence on a.
-
-
-
-
25
-
-
36149009235
-
-
10.1103/PhysRev.78.748
-
J. C. Slater, Phys. Rev. 78, 748 (1950). 10.1103/PhysRev.78.748
-
(1950)
Phys. Rev.
, vol.78
, pp. 748
-
-
Slater, J.C.1
-
26
-
-
70350636334
-
-
The origin of the discrepancy with respect to the sign might be due to a different definition of the EFG in the applied codes.
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The origin of the discrepancy with respect to the sign might be due to a different definition of the EFG in the applied codes.
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-
-
-
27
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70350625919
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Note, that we use another sign in the definition of nEw compared to Ref Eqs. 30 31.
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Note, that we use another sign in the definition of nEw compared to Ref Eqs. 30 31.
-
-
-
-
28
-
-
70350640123
-
-
Ph.D. thesis, TU Dresden
-
K. Koch, Ph.D. thesis, TU Dresden, 2009.
-
(2009)
-
-
Koch, K.1
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