-
1
-
-
0033248423
-
-
RMPHAT 0034-6861,. 10.1103/RevModPhys.71.231
-
G. P. Brivio and M. I. Trioni, Rev. Mod. Phys. RMPHAT 0034-6861 71, 231 (1999). 10.1103/RevModPhys.71.231
-
(1999)
Rev. Mod. Phys.
, vol.71
, pp. 231
-
-
Brivio, G.P.1
Trioni, M.I.2
-
2
-
-
0034922513
-
-
ARPLAP 0066-426X,. 10.1146/annurev.physchem.52.1.681
-
A. Nitzan, Annu. Rev. Phys. Chem. ARPLAP 0066-426X 52, 681 (2001). 10.1146/annurev.physchem.52.1.681
-
(2001)
Annu. Rev. Phys. Chem.
, vol.52
, pp. 681
-
-
Nitzan, A.1
-
3
-
-
0038442872
-
-
SCIEAS 0036-8075,. 10.1126/science.1081572
-
A. Nitzan and M. A. Ratner, Science SCIEAS 0036-8075 300, 1384 (2003). 10.1126/science.1081572
-
(2003)
Science
, vol.300
, pp. 1384
-
-
Nitzan, A.1
Ratner, M.A.2
-
4
-
-
7544240964
-
-
SSREDI 0167-5729,. 10.1016/j.surfre2004.09.002
-
X. -Y. Zhu, Surf. Sci. Rep. SSREDI 0167-5729 56, 1 (2004). 10.1016/j.surfrep.2004.09.002
-
(2004)
Surf. Sci. Rep.
, vol.56
, pp. 1
-
-
Zhu, X.-Y.1
-
5
-
-
0034291813
-
-
SUMIEK 0749-6036,. 10.1006/spmi.2000.0920
-
S. Datta, Superlattices Microstruct. SUMIEK 0749-6036 28, 253 (2000). 10.1006/spmi.2000.0920
-
(2000)
Superlattices Microstruct.
, vol.28
, pp. 253
-
-
Datta, S.1
-
6
-
-
0000500139
-
-
PRBMDO 0163-1829,. 10.1103/PhysRevB.55.5266
-
A. Umerski, Phys. Rev. B PRBMDO 0163-1829 55, 5266 (1997). 10.1103/PhysRevB.55.5266
-
(1997)
Phys. Rev. B
, vol.55
, pp. 5266
-
-
Umerski, A.1
-
9
-
-
0004419840
-
-
JCPSA6 0021-9606,. 10.1063/1.476841
-
W. Tian, S. Datta, S. Hong, R. Reifenberger, J. I. Henderson, and C. P. Kubiak, J. Chem. Phys. JCPSA6 0021-9606 109, 2874 (1998). 10.1063/1.476841
-
(1998)
J. Chem. Phys.
, vol.109
, pp. 2874
-
-
Tian, W.1
Datta, S.2
Hong, S.3
Reifenberger, R.4
Henderson, J.I.5
Kubiak, C.P.6
-
10
-
-
77956243546
-
-
Throughout this work, "self-consistent" will describe iterative, numerical methods for calculating desirable quantities. Expressions not requiring self-consistent evaluation will be classified as "closed-form" or "analytical" depending on the necessity or obviation, respectively, of numerical techniques (e.g., numerical quadrature) during their evaluation
-
Throughout this work, "self-consistent" will describe iterative, numerical methods for calculating desirable quantities. Expressions not requiring self-consistent evaluation will be classified as "closed-form" or "analytical" depending on the necessity or obviation, respectively, of numerical techniques (e.g., numerical quadrature) during their evaluation.
-
-
-
-
11
-
-
4243656226
-
-
PRVAAH 0096-8250,. 10.1103/PhysRev.178.1123
-
D. M. Newns, Phys. Rev. PRVAAH 0096-8250 178, 1123 (1969). 10.1103/PhysRev.178.1123
-
(1969)
Phys. Rev.
, vol.178
, pp. 1123
-
-
Newns, D.M.1
-
12
-
-
2842617037
-
-
PRVAAH 0096-8250,. 10.1103/PhysRev.124.41
-
P. W. Anderson, Phys. Rev. PRVAAH 0096-8250 124, 41 (1961). 10.1103/PhysRev.124.41
-
(1961)
Phys. Rev.
, vol.124
, pp. 41
-
-
Anderson, P.W.1
-
13
-
-
77956259172
-
-
These subsurface Green functions are easily obtainable using the Haydock recursion method (Refs.), see Secs.
-
These subsurface Green functions are easily obtainable using the Haydock recursion method (Refs.), see Secs..
-
-
-
-
14
-
-
65649123773
-
-
JPCAFH 1089-5639,. 10.1021/jp811492u
-
M. G. Reuter, T. Hansen, T. Seideman, and M. A. Ratner, J. Phys. Chem. A JPCAFH 1089-5639 113, 4665 (2009). 10.1021/jp811492u
-
(2009)
J. Phys. Chem. A
, vol.113
, pp. 4665
-
-
Reuter, M.G.1
Hansen, T.2
Seideman, T.3
Ratner, M.A.4
-
15
-
-
0037102985
-
-
CMPHC2 0301-0104,. 10.1016/S0301-0104(02)00341-5
-
G. Cuniberti, G. Fagas, and K. Richter, Chem. Phys. CMPHC2 0301-0104 281, 465 (2002). 10.1016/S0301-0104(02)00341-5
-
(2002)
Chem. Phys.
, vol.281
, pp. 465
-
-
Cuniberti, G.1
Fagas, G.2
Richter, K.3
-
16
-
-
33745212790
-
-
SUSCAS 0039-6028,. 10.1016/0039-6028(71)90115-4
-
D. Kalkstein and P. Soven, Surf. Sci. SUSCAS 0039-6028 26, 85 (1971). 10.1016/0039-6028(71)90115-4
-
(1971)
Surf. Sci.
, vol.26
, pp. 85
-
-
Kalkstein, D.1
Soven, P.2
-
17
-
-
0001134378
-
-
SUSCAS 0039-6028,. 10.1016/0039-6028(73)90279-3
-
R. Haydock and M. J. Kelly, Surf. Sci. SUSCAS 0039-6028 38, 139 (1973). 10.1016/0039-6028(73)90279-3
-
(1973)
Surf. Sci.
, vol.38
, pp. 139
-
-
Haydock, R.1
Kelly, M.J.2
-
18
-
-
0000505130
-
-
JCOMEL 0953-8984,. 10.1088/0953-8984/11/39/307
-
A. Losev, S. Vlaev, and T. Mishonov, J. Phys.: Condens. Matter JCOMEL 0953-8984 11, 7501 (1999). 10.1088/0953-8984/11/39/307
-
(1999)
J. Phys.: Condens. Matter
, vol.11
, pp. 7501
-
-
Losev, A.1
Vlaev, S.2
Mishonov, T.3
-
19
-
-
0037453799
-
-
JCOMEL 0953-8984,. 10.1088/0953-8984/15/6/327
-
A. Losev, J. Phys.: Condens. Matter JCOMEL 0953-8984 15, 1007 (2003). 10.1088/0953-8984/15/6/327
-
(2003)
J. Phys.: Condens. Matter
, vol.15
, pp. 1007
-
-
Losev, A.1
-
20
-
-
0001354953
-
-
PRBMDO 0163-1829,. 10.1103/PhysRevB.7.3629
-
T. L. Einstein and J. R. Schrieffer, Phys. Rev. B PRBMDO 0163-1829 7, 3629 (1973). 10.1103/PhysRevB.7.3629
-
(1973)
Phys. Rev. B
, vol.7
, pp. 3629
-
-
Einstein, T.L.1
Schrieffer, J.R.2
-
22
-
-
67649512451
-
-
JPCAFH 1089-5639,. 10.1021/jp900301f
-
A. Landau, A. Nitzan, and L. Kronik, J. Phys. Chem. A JPCAFH 1089-5639 113, 7451 (2009). 10.1021/jp900301f
-
(2009)
J. Phys. Chem. A
, vol.113
, pp. 7451
-
-
Landau, A.1
Nitzan, A.2
Kronik, L.3
-
23
-
-
84987064319
-
-
IJQCB2 0020-7608,. 10.1002/qua.560260516
-
N. Montella, V. Barone, and G. del Re, Int. J. Quantum Chem. IJQCB2 0020-7608 26, 769 (1984). 10.1002/qua.560260516
-
(1984)
Int. J. Quantum Chem.
, vol.26
, pp. 769
-
-
Montella, N.1
Barone, V.2
Del Re, G.3
-
25
-
-
0001091430
-
-
JCPSA6 0021-9606,. 10.1063/1.477116
-
S. N. Yaliraki and M. A. Ratner, J. Chem. Phys. JCPSA6 0021-9606 109, 5036 (1998). 10.1063/1.477116
-
(1998)
J. Chem. Phys.
, vol.109
, pp. 5036
-
-
Yaliraki, S.N.1
Ratner, M.A.2
-
26
-
-
0141676026
-
-
JCPSA6 0021-9606,. 10.1063/1.1597197
-
C. -K. Wang and Y. Luo, J. Chem. Phys. JCPSA6 0021-9606 119, 4923 (2003). 10.1063/1.1597197
-
(2003)
J. Chem. Phys.
, vol.119
, pp. 4923
-
-
Wang, C.-K.1
Luo, Y.2
-
27
-
-
0009148565
-
-
SUSCAS 0039-6028,. 10.1016/0039-6028(85)90813-1
-
H. -J. Brocksch and K. H. Bennemann, Surf. Sci. SUSCAS 0039-6028 161, 321 (1985). 10.1016/0039-6028(85)90813-1
-
(1985)
Surf. Sci.
, vol.161
, pp. 321
-
-
Brocksch, H.-J.1
Bennemann, K.H.2
-
29
-
-
0000781318
-
-
PRBMDO 0163-1829,. 10.1103/PhysRevB.54.17954
-
K. Nakada, M. Fujita, G. Dresselhaus, and M. S. Dresselhaus, Phys. Rev. B PRBMDO 0163-1829 54, 17954 (1996). 10.1103/PhysRevB.54.17954
-
(1996)
Phys. Rev. B
, vol.54
, pp. 17954
-
-
Nakada, K.1
Fujita, M.2
Dresselhaus, G.3
Dresselhaus, M.S.4
-
30
-
-
0034899566
-
-
PRBMDO 0163-1829,. 10.1103/PhysRevB.63.245401
-
W. T. Geng, M. Kim, and A. J. Freeman, Phys. Rev. B PRBMDO 0163-1829 63, 245401 (2001). 10.1103/PhysRevB.63.245401
-
(2001)
Phys. Rev. B
, vol.63
, pp. 245401
-
-
Geng, W.T.1
Kim, M.2
Freeman, A.J.3
-
31
-
-
42749103486
-
-
PRBMDO 0163-1829,. 10.1103/PhysRevB.70.205416
-
Y. Xue and M. A. Ratner, Phys. Rev. B PRBMDO 0163-1829 70, 205416 (2004). 10.1103/PhysRevB.70.205416
-
(2004)
Phys. Rev. B
, vol.70
, pp. 205416
-
-
Xue, Y.1
Ratner, M.A.2
-
32
-
-
36849016335
-
-
PRBMDO 0163-1829,. 10.1103/PhysRevB.76.233401
-
O. Hod, J. E. Peralta, and G. E. Scuseria, Phys. Rev. B PRBMDO 0163-1829 76, 233401 (2007). 10.1103/PhysRevB.76.233401
-
(2007)
Phys. Rev. B
, vol.76
, pp. 233401
-
-
Hod, O.1
Peralta, J.E.2
Scuseria, G.E.3
-
33
-
-
33645993207
-
-
JCPSA6 0021-9606,. 10.1063/1.468314
-
V. Mujica, M. Kemp, and M. A. Ratner, J. Chem. Phys. JCPSA6 0021-9606 101, 6849 (1994). 10.1063/1.468314
-
(1994)
J. Chem. Phys.
, vol.101
, pp. 6849
-
-
Mujica, V.1
Kemp, M.2
Ratner, M.A.3
-
35
-
-
0001343569
-
-
JPSOAW 0022-3719,. 10.1088/0022-3719/5/20/004
-
R. Haydock, V. Heine, and M. J. Kelly, J. Phys. C JPSOAW 0022-3719 5, 2845 (1972). 10.1088/0022-3719/5/20/004
-
(1972)
J. Phys. C
, vol.5
, pp. 2845
-
-
Haydock, R.1
Heine, V.2
Kelly, M.J.3
-
37
-
-
77956252160
-
-
The use of Eq. in the derivation of Eq. is only correct when the augmented Hamiltonian is Hermitian [Eq. is only valid for Hermitian Hamiltonians]. If the augmented Hamiltonian is not Hermitian, as caused by an infinite system size in this work, Eq. can be obtained from the resolvent, G (E) = [EI-H] -1, instead of the retarded Green function. In this case, solutions to Eq. are no longer guaranteed to be unique; however, we can choose the solution that satisfies the properties of the retarded Green function (Ref.)
-
The use of Eq. in the derivation of Eq. is only correct when the augmented Hamiltonian is Hermitian [Eq. is only valid for Hermitian Hamiltonians]. If the augmented Hamiltonian is not Hermitian, as caused by an infinite system size in this work, Eq. can be obtained from the resolvent, G (E) = [EI-H] -1, instead of the retarded Green function. In this case, solutions to Eq. are no longer guaranteed to be unique; however, we can choose the solution that satisfies the properties of the retarded Green function (Ref.).
-
-
-
-
38
-
-
77956260366
-
-
in Eq. is three times the canonical standard deviation in the Gaussian distribution. 99% of the density is localized within (E-ε) ±σ
-
σ in Eq. is three times the canonical standard deviation in the Gaussian distribution. 99% of the density is localized within (E-ε) ±σ.
-
-
-
|