-
1
-
-
67650049899
-
-
International Technology Roadmap for Semiconductors available at
-
International Technology Roadmap for Semiconductors available at http://www.itrs.net
-
-
-
-
2
-
-
20544447617
-
-
S. E. Thompson, G. Sun, K. Wu, J. Lim, and T. Nishida, Tech. Dig. - Int. Electron Devices Meet. 2004, 221.
-
Tech. Dig. - Int. Electron Devices Meet.
, vol.2004
, pp. 221
-
-
Thompson, S.E.1
Sun, G.2
Wu, K.3
Lim, J.4
Nishida, T.5
-
3
-
-
21644454069
-
-
H. Irie, K. Kita, K. Kyuno, and A. Toriumi, Tech. Dig. - Int. Electron Devices Meet. 2004, 225.
-
Tech. Dig. - Int. Electron Devices Meet.
, vol.2004
, pp. 225
-
-
Irie, H.1
Kita, K.2
Kyuno, K.3
Toriumi, A.4
-
4
-
-
67650053041
-
-
F. Payet, F. Boeuf, C. Ortolland, and T. Skotnicki, Tech. Dig. - Int. Conf. Solid State Devices Mater. 2006, 176.
-
Tech. Dig. - Int. Conf. Solid State Devices Mater.
, vol.2006
, pp. 176
-
-
Payet, F.1
Boeuf, F.2
Ortolland, C.3
Skotnicki, T.4
-
5
-
-
0342853202
-
-
10.1088/0268-1242/12/12/001
-
F. Schaffler, Semicond. Sci. Technol. 12, 1515 (1997). 10.1088/0268-1242/12/12/001
-
(1997)
Semicond. Sci. Technol.
, vol.12
, pp. 1515
-
-
Schaffler, F.1
-
6
-
-
10644250257
-
-
10.1103/PhysRev.136.B864
-
P. Hohenberg and W. Kohn, Phys. Rev. 136, B864 (1964). 10.1103/PhysRev.136.B864
-
(1964)
Phys. Rev.
, vol.136
, pp. 864
-
-
Hohenberg, P.1
Kohn, W.2
-
10
-
-
33750668607
-
-
10.1103/PhysRevB.39.1871
-
C. G. Van de Walle, Phys. Rev. B 39, 1871 (1989). 10.1103/PhysRevB.39. 1871
-
(1989)
Phys. Rev. B
, vol.39
, pp. 1871
-
-
Van De Walle, C.G.1
-
12
-
-
0000469409
-
-
10.1103/PhysRevB.60.5404
-
S.-H. Wei and A. Zunger, Phys. Rev. B 60, 5404 (1999). 10.1103/PhysRevB.60.5404
-
(1999)
Phys. Rev. B
, vol.60
, pp. 5404
-
-
Wei, S.-H.1
Zunger, A.2
-
15
-
-
33751538015
-
-
10.1103/PhysRevB.74.195208
-
D. Rideau, M. Feraille, L. Ciampolini, M. Minondo, C. Tavernier, H. Jaouen, and A. Ghetti, Phys. Rev. B 74, 195208 (2006). 10.1103/PhysRevB.74. 195208
-
(2006)
Phys. Rev. B
, vol.74
, pp. 195208
-
-
Rideau, D.1
Feraille, M.2
Ciampolini, L.3
Minondo, M.4
Tavernier, C.5
Jaouen, H.6
Ghetti, A.7
-
18
-
-
0000126213
-
-
10.1103/PhysRevB.51.17398
-
L.-W. Wang and A. Zunger, Phys. Rev. B 51, 17398 (1995). 10.1103/PhysRevB.51.17398
-
(1995)
Phys. Rev. B
, vol.51
, pp. 17398
-
-
Wang, L.-W.1
Zunger, A.2
-
19
-
-
0001630651
-
-
10.1103/PhysRevB.59.15806
-
L.-W. Wang and A. Zunger, Phys. Rev. B 59, 15806 (1999). 10.1103/PhysRevB.59.15806
-
(1999)
Phys. Rev. B
, vol.59
, pp. 15806
-
-
Wang, L.-W.1
Zunger, A.2
-
20
-
-
2442522754
-
-
10.1103/PhysRev.94.1498
-
J. C. Slater and G. F. Koster, Phys. Rev. 94, 1498 (1954). 10.1103/PhysRev.94.1498
-
(1954)
Phys. Rev.
, vol.94
, pp. 1498
-
-
Slater, J.C.1
Koster, G.F.2
-
22
-
-
41449092126
-
-
10.1103/PhysRevB.77.115316
-
Y. M. Niquet and D. C. Mojica, Phys. Rev. B 77, 115316 (2008). 10.1103/PhysRevB.77.115316
-
(2008)
Phys. Rev. B
, vol.77
, pp. 115316
-
-
Niquet, Y.M.1
Mojica, D.C.2
-
23
-
-
41749098089
-
-
10.1109/TED.2007.902879;
-
G. Klimeck, S. S. Ahmed, Hansang Bae, N. Kharche, S. Clark, B. Haley, Sunhee Lee, M. Naumov, Hoon Ryu, F. Saied, M. Prada, M. Korkusinski, T. B. Boykin, and R. Rahman, IEEE Trans. Electron Devices 54, 2079 (2007) 10.1109/TED.2007.902879
-
(2007)
IEEE Trans. Electron Devices
, vol.54
, pp. 2079
-
-
Klimeck, G.1
Ahmed, S.S.2
Bae, H.3
Kharche, N.4
Clark, S.5
Haley, B.6
Lee, S.7
Naumov, M.8
Ryu, H.9
Saied, F.10
Prada, M.11
Korkusinski, M.12
Boykin, T.B.13
Rahman, R.14
-
24
-
-
41749112698
-
-
10.1109/TED.2007.904877
-
G. Klimeck, S. S. Ahmed, N. Kharche, M. Korkusinski, M. Usman, M. Prada, and T. B. Boykin, IEEE Trans. Electron Devices 54, 2090 (2007). 10.1109/TED.2007.904877
-
(2007)
IEEE Trans. Electron Devices
, vol.54
, pp. 2090
-
-
Klimeck, G.1
Ahmed, S.S.2
Kharche, N.3
Korkusinski, M.4
Usman, M.5
Prada, M.6
Boykin, T.B.7
-
25
-
-
33751181011
-
-
10.1103/PhysRevB.74.205323
-
M. Luisier, A. Schenk, W. Fichtner, and G. Klimeck, Phys. Rev. B 74, 205323 (2006). 10.1103/PhysRevB.74.205323
-
(2006)
Phys. Rev. B
, vol.74
, pp. 205323
-
-
Luisier, M.1
Schenk, A.2
Fichtner, W.3
Klimeck, G.4
-
28
-
-
38849136468
-
-
10.1103/PhysRevB.77.085301
-
A. Lherbier, M. P. Persson, Y. M. Niquet, F. Triozon, and S. Roche, Phys. Rev. B 77, 085301 (2008). 10.1103/PhysRevB.77.085301
-
(2008)
Phys. Rev. B
, vol.77
, pp. 085301
-
-
Lherbier, A.1
Persson, M.P.2
Niquet, Y.M.3
Triozon, F.4
Roche, S.5
-
29
-
-
29744433030
-
-
10.1103/PhysRevB.72.193204
-
A. S. Martins, T. B. Boykin, G. Klimeck, and B. Koiller, Phys. Rev. B 72, 193204 (2005). 10.1103/PhysRevB.72.193204
-
(2005)
Phys. Rev. B
, vol.72
, pp. 193204
-
-
Martins, A.S.1
Boykin, T.B.2
Klimeck, G.3
Koiller, B.4
-
30
-
-
42149086504
-
-
10.1063/1.2901182
-
M. Diarra, C. Delerue, Y. M. Niquet, and G. Allan, J. Appl. Phys. 103, 073703 (2008). 10.1063/1.2901182
-
(2008)
J. Appl. Phys.
, vol.103
, pp. 073703
-
-
Diarra, M.1
Delerue, C.2
Niquet, Y.M.3
Allan, G.4
-
32
-
-
0001059737
-
-
10.1103/PhysRevB.57.6493
-
J.-M. Jancu, R. Scholz, F. Beltram, and F. Bassani, Phys. Rev. B 57, 6493 (1998). 10.1103/PhysRevB.57.6493
-
(1998)
Phys. Rev. B
, vol.57
, pp. 6493
-
-
Jancu, J.-M.1
Scholz, R.2
Beltram, F.3
Bassani, F.4
-
38
-
-
0042999324
-
-
10.1103/PhysRevB.66.125207
-
T. B. Boykin, G. Klimeck, R. C. Bowen, and F. Oyafuso, Phys. Rev. B 66, 125207 (2002). 10.1103/PhysRevB.66.125207
-
(2002)
Phys. Rev. B
, vol.66
, pp. 125207
-
-
Boykin, T.B.1
Klimeck, G.2
Bowen, R.C.3
Oyafuso, F.4
-
40
-
-
34648823370
-
-
10.1103/PhysRevB.76.115202
-
J.-M. Jancu and P. Voisin, Phys. Rev. B 76, 115202 (2007). 10.1103/PhysRevB.76.115202
-
(2007)
Phys. Rev. B
, vol.76
, pp. 115202
-
-
Jancu, J.-M.1
Voisin, P.2
-
41
-
-
67650035884
-
-
This implies the choice of a particular energy reference. See Refs..
-
This implies the choice of a particular energy reference. See Refs..
-
-
-
-
42
-
-
0003999408
-
-
edited by V. Vitek and D. Srolovitz (Plenum Press, New York
-
D. Chadi, in Atomistic Simulation of Materials Beyond Pair Potentials, edited by, V. Vitek, and, D. Srolovitz, (Plenum Press, New York, 1989).
-
(1989)
Atomistic Simulation of Materials beyond Pair Potentials
-
-
Chadi, D.1
-
44
-
-
0001443163
-
-
αp should also include a contribution αp′ from the onsite potential V1 in Eq. 6, whose depth increases, in a first approximation, proportional to the tensile hydrostatic strain on the atom. The absolute valence-band deformation potential av cannot, indeed, be reproduced without this central correction, as shown in semiempirical pseudopotential theory [see, e.g., discussion of 10.1103/PhysRevB.59.15270
-
αp should also include a contribution αp′ from the onsite potential V1 in Eq. 6, whose depth increases, in a first approximation, proportional to the tensile hydrostatic strain on the atom. The absolute valence-band deformation potential av cannot, indeed, be reproduced without this central correction, as shown in semiempirical pseudopotential theory [see, e.g., discussion of T. Mattila, L.-W. Wang, and A. Zunger, Phys. Rev. B 59, 15270 (1999)]; αp′ is expected to be negative at variance with the nearest-neighbor contributions defined in paragraph IIA. 10.1103/PhysRevB.59. 15270
-
(1999)
Phys. Rev. B
, vol.59
, pp. 15270
-
-
Mattila, T.1
Wang, L.-W.2
Zunger, A.3
-
45
-
-
0037171091
-
-
10.1088/0953-8984/14/11/302
-
J.-M. Soler, E. Artacho, J. D. Gale, A. García, J. Junquera, P. Ordejón, and D. Sánchez-Portal, J. Phys.: Condens. Matter 14, 2745 (2002). 10.1088/0953-8984/14/11/302
-
(2002)
J. Phys.: Condens. Matter
, vol.14
, pp. 2745
-
-
Soler, J.-M.1
Artacho, E.2
Gale, J.D.3
García, A.4
Junquera, J.5
Ordejón, P.6
Sánchez-Portal, D.7
-
46
-
-
0001604458
-
-
Since β (d) and γ (d) tend to zero when d→0 or d→ (whatever the orbitals), they have at least one extremum in between. This has been confirmed using, for example, SIESTA orbitals and the screened pseudopotential for Si from 10.1063/1.466486
-
Since β (d) and γ (d) tend to zero when d→0 or d→ (whatever the orbitals), they have at least one extremum in between. This has been confirmed using, for example, SIESTA orbitals and the screened pseudopotential for Si from L.-W. Wang and A. Zunger, J. Chem. Phys. 100, 2394 (1994). The sign of the first-order β (1) and γ (1) is therefore expected to be dependent on the parametrization, especially in an orthogonal approximation where the orbitals have long-range oscillations. 10.1063/1.466486
-
(1994)
J. Chem. Phys.
, vol.100
, pp. 2394
-
-
Wang, L.-W.1
Zunger, A.2
-
47
-
-
0037449295
-
-
10.1063/1.1529312
-
J.-M. Jancu, F. Bassani, F. Della Sala, and R. Scholz, Appl. Phys. Lett. 81, 4838 (2002). 10.1063/1.1529312
-
(2002)
Appl. Phys. Lett.
, vol.81
, pp. 4838
-
-
Jancu, J.-M.1
Bassani, F.2
Della Sala, F.3
Scholz, R.4
-
48
-
-
29144453140
-
-
10.1103/PhysRev.145.637
-
P. N. Keating, Phys. Rev. 145, 637 (1966). 10.1103/PhysRev.145.637
-
(1966)
Phys. Rev.
, vol.145
, pp. 637
-
-
Keating, P.N.1
-
50
-
-
0001337022
-
-
10.1103/PhysRev.128.2614
-
L. Kleinman, Phys. Rev. 128, 2614 (1962). 10.1103/PhysRev.128.2614
-
(1962)
Phys. Rev.
, vol.128
, pp. 2614
-
-
Kleinman, L.1
-
51
-
-
67650049898
-
-
The ABINIT code is a common project of the Université Catholique de Louvain, Corning Incorporated, the Ecole Polytechnique of Palaiseau, and other contributors (see
-
The ABINIT code is a common project of the Université Catholique de Louvain, Corning Incorporated, the Ecole Polytechnique of Palaiseau, and other contributors (see http://www.abinit.org).
-
-
-
-
52
-
-
0036827661
-
-
10.1016/S0927-0256(02)00325-7
-
X. Gonze, J.-M. Beuken, R. Caracas, F. Detraux, M. Fuchs, G.-M. Rignanese, L. Sindic, M. Verstraete, G. Zerah, F. Jollet, M. Torrent, A. Roy, M. Mikami, Ph. Ghosez, J.-Y. Raty, and D. C. Allan, Comput. Mater. Sci. 25, 478 (2002). 10.1016/S0927-0256(02)00325-7
-
(2002)
Comput. Mater. Sci.
, vol.25
, pp. 478
-
-
Gonze, X.1
Beuken, J.-M.2
Caracas, R.3
Detraux, F.4
Fuchs, M.5
Rignanese, G.-M.6
Sindic, L.7
Verstraete, M.8
Zerah, G.9
Jollet, F.10
Torrent, M.11
Roy, A.12
Mikami, M.13
Ghosez, Ph.14
Raty, J.-Y.15
Allan, D.C.16
-
53
-
-
20144367100
-
-
10.1524/zkri.220.5.558.65066
-
X. Gonze, G.-M. Rignanese, M. Verstraete, J.-M. Beuken, Y. Pouillon, R. Caracas, F. Jollet, M. Torrent, G. Zerah, M. Mikami, Ph. Ghosez, M. Veithen, J.-Y. Raty, V. Olevano, F. Bruneval, L. Reining, R. Godby, G. Onida, D. R. Hamann, and D. C. Allan, Z. Kristallogr. 220, 558 (2005). 10.1524/zkri.220.5. 558.65066
-
(2005)
Z. Kristallogr.
, vol.220
, pp. 558
-
-
Gonze, X.1
Rignanese, G.-M.2
Verstraete, M.3
Beuken, J.-M.4
Pouillon, Y.5
Caracas, R.6
Jollet, F.7
Torrent, M.8
Zerah, G.9
Mikami, M.10
Ghosez, Ph.11
Veithen, M.12
Raty, J.-Y.13
Olevano, V.14
Bruneval, F.15
Reining, L.16
Godby, R.17
Onida, G.18
Hamann, D.R.19
Allan, D.C.20
more..
-
55
-
-
36149016819
-
-
10.1103/PhysRev.139.A796
-
L. Hedin, Phys. Rev. 139, A796 (1965). 10.1103/PhysRev.139.A796
-
(1965)
Phys. Rev.
, vol.139
, pp. 796
-
-
Hedin, L.1
-
57
-
-
67650043758
-
-
A detailed description of the present GW results can be found in Ref.. In particular, as mentioned in Ref., LDA- G0 W0 results do not match perfectly the experimental data, and a supplementary rigid "scissor" shift of 0.09 eV for Si and 0.104 eV for Ge has been added to the GW results to obtain the final reference set of bands.
-
A detailed description of the present GW results can be found in Ref.. In particular, as mentioned in Ref., LDA- G0 W0 results do not match perfectly the experimental data, and a supplementary rigid "scissor" shift of 0.09 eV for Si and 0.104 eV for Ge has been added to the GW results to obtain the final reference set of bands.
-
-
-
-
58
-
-
0042312251
-
-
The same GW correction as in the bulk unstrained materials is used in strained Si and Ge. This choice is motivated by 10.1103/PhysRevB.39.7840
-
The same GW correction as in the bulk unstrained materials is used in strained Si and Ge. This choice is motivated by X. Zhu, S. Fahy, and S. G. Louie, Phys. Rev. B 39, 7840 (1989) who reported that there is no quantitative differences between the LDA and GW band-gap pressure dependencies in Si. 10.1103/PhysRevB.39.7840
-
(1989)
Phys. Rev. B
, vol.39
, pp. 7840
-
-
Zhu, X.1
Fahy, S.2
Louie, S.G.3
-
60
-
-
0000732463
-
-
10.1137/0916069
-
R. H. Byrd, P. Lu, J. Nocedal, and C. Zhu, SIAM J. Sci. Comput. (USA) 16, 1190 (1995). 10.1137/0916069
-
(1995)
SIAM J. Sci. Comput. (USA)
, vol.16
, pp. 1190
-
-
Byrd, R.H.1
Lu, P.2
Nocedal, J.3
Zhu, C.4
-
61
-
-
67650038184
-
-
We actually fit the tight-binding parameters on the differences between the strained and unstrained band structures in order to achieve a good description of the deformation potentials, free from the errors on the unstrained band structure.
-
We actually fit the tight-binding parameters on the differences between the strained and unstrained band structures in order to achieve a good description of the deformation potentials, free from the errors on the unstrained band structure.
-
-
-
-
62
-
-
67650055461
-
-
We have, in particular, attempted to optimize simultaneously the onsite energies, nearest-neighbor interactions, β (0) 's and γ (0) 's on the unstrained band structure, and on one [001] and one [111] biaxial strain that do not change the nearest-neighbor bond lengths (to be independent of the Harrison parameters, α 's, β (1) 's and γ (1) 's). We did not evidence any real improvement in the description nor any change in the signs of the β (0) 's.
-
We have, in particular, attempted to optimize simultaneously the onsite energies, nearest-neighbor interactions, β (0) 's and γ (0) 's on the unstrained band structure, and on one [001] and one [111] biaxial strain that do not change the nearest-neighbor bond lengths (to be independent of the Harrison parameters, α 's, β (1) 's and γ (1) 's). We did not evidence any real improvement in the description nor any change in the signs of the β (0) 's.
-
-
-
-
63
-
-
0003554309
-
-
edited by O. Madelung, M. Schulz, and H. Weiss, Landolt-Börnstein, New series, Group III, Vol. Springer-Verlag, New-York
-
Physics of Group IV elements and III-V Compounds, edited by, O. Madelung, M. Schulz, and, H. Weiss, Landolt-Börnstein, New series, Group III, Vol. 17, Pt. A (Springer-Verlag, New-York, 1982).
-
(1982)
Physics of Group IV Elements and
, vol.17
-
-
-
64
-
-
0038713703
-
-
10.1088/0022-3719/14/21/011
-
R. G. Humphreys, J. Phys. C 14, 2935 (1981). 10.1088/0022-3719/14/21/011
-
(1981)
J. Phys. C
, vol.14
, pp. 2935
-
-
Humphreys, R.G.1
-
65
-
-
33751056555
-
-
10.1103/PhysRevB.4.3460
-
P. Lawaetz, Phys. Rev. B 4, 3460 (1971). 10.1103/PhysRevB.4.3460
-
(1971)
Phys. Rev. B
, vol.4
, pp. 3460
-
-
Lawaetz, P.1
-
71
-
-
0000291038
-
-
10.1103/PhysRevB.39.1235
-
G. P. Schwartz, M. S. Hybertsen, J. Bevk, R. G. Nuzzo, J. P. Mannaerts, and G. J. Gualtieri, Phys. Rev. B 39, 1235 (1989). 10.1103/PhysRevB.39.1235
-
(1989)
Phys. Rev. B
, vol.39
, pp. 1235
-
-
Schwartz, G.P.1
Hybertsen, M.S.2
Bevk, J.3
Nuzzo, R.G.4
Mannaerts, J.P.5
Gualtieri, G.J.6
-
73
-
-
67650012700
-
-
To plot Figs. 4 5, we used a constant ε / ε ratio and the ab initio internal strain parameter ζ fitted to a second-order polynomial: ε / ε =-0.7708 for Si [001], ε / ε =-0.4392 for Si [111] (ζ=0.5213-1.1156 ε +3.1868 ε2), ε / ε =-0.51 for Si [110] (ζ=0.5254-2.9765 ε +3.4661 ε2), ε / ε =-0.7518 for Ge [001], ε / ε =-0.3717 for Ge [111] (ζ=0.4813-0.9972 ε +0.6567 ε2), and ε / ε =-0.4504 for Ge [110] (ζ=0.4783-2.8113 ε +4.1082 ε2).
-
To plot Figs. 4 5, we used a constant ε / ε ratio and the ab initio internal strain parameter ζ fitted to a second-order polynomial: ε / ε =-0.7708 for Si [001], ε / ε =-0.4392 for Si [111] (ζ=0.5213-1.1156 ε +3.1868 ε2), ε / ε =-0.51 for Si [110] (ζ=0.5254-2.9765 ε +3.4661 ε2), ε / ε =-0.7518 for Ge [001], ε / ε =-0.3717 for Ge [111] (ζ=0.4813-0.9972 ε +0.6567 ε2), and ε / ε =-0.4504 for Ge [110] (ζ=0.4783-2.8113 ε +4.1082 ε2).
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-
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-
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-
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-
-
Since ab initio calculations performed at different strains do not give the band structure on an absolute common energy scale, we choose to align the ab initio and TB highest valence bands on Figs. 4 5. Therefore, only the other bands are indicative of the quality of the TB model.
-
Since ab initio calculations performed at different strains do not give the band structure on an absolute common energy scale, we choose to align the ab initio and TB highest valence bands on Figs. 4 5. Therefore, only the other bands are indicative of the quality of the TB model.
-
-
-
-
75
-
-
39549085834
-
-
10.1109/TED.2007.902880
-
E. Ungersboeck, S. Dhar, G. Karlowatz, V. Sverdlov, H. Kosina, and S. Selberherr, IEEE Trans. Electron Devices 54, 2183 (2007). 10.1109/TED.2007. 902880
-
(2007)
IEEE Trans. Electron Devices
, vol.54
, pp. 2183
-
-
Ungersboeck, E.1
Dhar, S.2
Karlowatz, G.3
Sverdlov, V.4
Kosina, H.5
Selberherr, S.6
-
77
-
-
0001157567
-
-
10.1103/PhysRevB.40.5683
-
J. Weber and M. I. Alonso, Phys. Rev. B 40, 5683 (1989). 10.1103/PhysRevB.40.5683
-
(1989)
Phys. Rev. B
, vol.40
, pp. 5683
-
-
Weber, J.1
Alonso, M.I.2
-
79
-
-
0001619112
-
-
10.1063/1.351262
-
D. J. Robbins, L. T. Canham, S. J. Barnett, A. D. Pitt, and P. Calcott, J. Appl. Phys. 71, 1407 (1992). 10.1063/1.351262
-
(1992)
J. Appl. Phys.
, vol.71
, pp. 1407
-
-
Robbins, D.J.1
Canham, L.T.2
Barnett, S.J.3
Pitt, A.D.4
Calcott, P.5
-
80
-
-
0001888922
-
-
10.1063/1.96271
-
D. V. Lang, R. People, J. C. Bean, and A. M. Sergent, Appl. Phys. Lett. 47, 1333 (1985). 10.1063/1.96271
-
(1985)
Appl. Phys. Lett.
, vol.47
, pp. 1333
-
-
Lang, D.V.1
People, R.2
Bean, J.C.3
Sergent, A.M.4
-
81
-
-
0009454687
-
-
10.1063/1.107199
-
J. Spitzer, K. Thonke, R. Sauer, H. Kibbel, H. J. Herzog, and E. Kasper, Appl. Phys. Lett. 60, 1729 (1992). 10.1063/1.107199
-
(1992)
Appl. Phys. Lett.
, vol.60
, pp. 1729
-
-
Spitzer, J.1
Thonke, K.2
Sauer, R.3
Kibbel, H.4
Herzog, H.J.5
Kasper, E.6
-
82
-
-
0028764144
-
-
10.1063/1.113079
-
C. W. Liu, J. C. Sturm, Y. R. J. Lacroix, M. L. W. Thewalt, and D. D. Perovic, Appl. Phys. Lett. 65, 76 (1994). 10.1063/1.113079
-
(1994)
Appl. Phys. Lett.
, vol.65
, pp. 76
-
-
Liu, C.W.1
Sturm, J.C.2
Lacroix, Y.R.J.3
Thewalt, M.L.W.4
Perovic, D.D.5
-
83
-
-
0031996993
-
-
10.1109/16.658686
-
S. Takagi, J. L. Hoyt, K. Rim, J. J. Wesler, and J. F. Gibbons, IEEE Trans. Electron Devices 45, 494 (1998). 10.1109/16.658686
-
(1998)
IEEE Trans. Electron Devices
, vol.45
, pp. 494
-
-
Takagi, S.1
Hoyt, J.L.2
Rim, K.3
Wesler, J.J.4
Gibbons, J.F.5
-
86
-
-
67650032059
-
-
These twofold and threefold degenerate basis functions will be appropriate linear combinations of the d orbitals for other orientations of the crystal with respect to the x, y, and z axes.
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These twofold and threefold degenerate basis functions will be appropriate linear combinations of the d orbitals for other orientations of the crystal with respect to the x, y, and z axes.
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