-
3
-
-
0000865323
-
-
M. H. Brodsky, R. S. Title, K. Weiser, and G. D. Pettit, Phys. Rev. B 1, 2632 (1970).
-
(1970)
Phys. Rev. B
, vol.1
, pp. 2632
-
-
Brodsky, M.H.1
Title, R.S.2
Weiser, K.3
Pettit, G.D.4
-
4
-
-
3342924374
-
-
0031-9007 10.1103/PhysRevLett.47.1480.
-
G. D. Cody, T. Tiedje, B. Abeles, B. Brooks, and Y. Goldstein, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.47.1480 47, 1480 (1981).
-
(1981)
Phys. Rev. Lett.
, vol.47
, pp. 1480
-
-
Cody, G.D.1
Tiedje, T.2
Abeles, B.3
Brooks, B.4
Goldstein, Y.5
-
5
-
-
1242343449
-
-
0163-1829 10.1103/PhysRevB.39.1953.
-
T. Datta and J. A. Woollam, Phys. Rev. B 0163-1829 10.1103/PhysRevB.39. 1953 39, 1953 (1989).
-
(1989)
Phys. Rev. B
, vol.39
, pp. 1953
-
-
Datta, T.1
Woollam, J.A.2
-
6
-
-
0001088864
-
-
0163-1829 10.1103/PhysRevB.43.2131.
-
D. Dasgupta, F. Demichelis, C. F. Pirri, and A. Tagliaferro, Phys. Rev. B 0163-1829 10.1103/PhysRevB.43.2131 43, 2131 (1991).
-
(1991)
Phys. Rev. B
, vol.43
, pp. 2131
-
-
Dasgupta, D.1
Demichelis, F.2
Pirri, C.F.3
Tagliaferro, A.4
-
7
-
-
0035451225
-
-
0022-3093 10.1016/S0022-3093(01)00728-1.
-
S. K. O'Leary, B. J. Fogal, D. J. Lockwood, J. -M. Baribeau, M. Nol, and J. C. Zwinkels, J. Non-Cryst. Solids 0022-3093 10.1016/S0022-3093(01)00728-1 290, 57 (2001).
-
(2001)
J. Non-Cryst. Solids
, vol.290
, pp. 57
-
-
O'Leary, S.K.1
Fogal, B.J.2
Lockwood, D.J.3
Baribeau, J.-M.4
Nol, M.5
Zwinkels, J.C.6
-
8
-
-
0035914566
-
-
0038-1098 10.1016/S0038-1098(01)00422-7.
-
B. J. Fogal, S. K. O'Leary, D. J. Lockwood, J. -M. Baribeau, M. Nol, and J. C. Zwinkels, Solid State Commun. 0038-1098 10.1016/S0038-1098(01)00422-7 120, 429 (2001).
-
(2001)
Solid State Commun.
, vol.120
, pp. 429
-
-
Fogal, B.J.1
O'Leary, S.K.2
Lockwood, D.J.3
Baribeau, J.-M.4
Nol, M.5
Zwinkels, J.C.6
-
9
-
-
0021558454
-
-
in, edited by J. I. Pankove (Academic, New York), Vol.,.
-
G. D. Cody, in Hydrogenated Amorphous Silicon, Semiconductors and Semimetals, edited by, J. I. Pankove, (Academic, New York, 1984), Vol. 21B, p. 11.
-
(1984)
Hydrogenated Amorphous Silicon, Semiconductors and Semimetals
, vol.21
, pp. 11
-
-
Cody, G.D.1
-
10
-
-
0005702423
-
-
0031-9007 10.1103/PhysRevLett.44.749.
-
R. S. Crandall, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.44.749 44, 749 (1980).
-
(1980)
Phys. Rev. Lett.
, vol.44
, pp. 749
-
-
Crandall, R.S.1
-
16
-
-
0000400936
-
-
0163-1829 10.1103/PhysRevB.31.5187.
-
W. B. Jackson, S. M. Kelso, C. C. Tsai, J. W. Allen, and S. -J. Oh, Phys. Rev. B 0163-1829 10.1103/PhysRevB.31.5187 31, 5187 (1985).
-
(1985)
Phys. Rev. B
, vol.31
, pp. 5187
-
-
Jackson, W.B.1
Kelso, S.M.2
Tsai, C.C.3
Allen, J.W.4
Oh, S.-J.5
-
17
-
-
54049140177
-
-
Collectively, the influence of these individual optical transition matrix elements may be treated in terms of an overall aggregate optical transition matrix element (Ref.).
-
Collectively, the influence of these individual optical transition matrix elements may be treated in terms of an overall aggregate optical transition matrix element (Ref.).
-
-
-
-
18
-
-
0038636106
-
-
0003-6951 10.1063/1.1568148.
-
S. K. O'Leary, Appl. Phys. Lett. 0003-6951 10.1063/1.1568148 82, 2784 (2003).
-
(2003)
Appl. Phys. Lett.
, vol.82
, pp. 2784
-
-
O'Leary, S.K.1
-
19
-
-
0002122113
-
-
0022-3093 10.1016/0022-3093(70)90193-6.
-
N. K. Hindley, J. Non-Cryst. Solids 0022-3093 10.1016/0022-3093(70)90193- 6 5, 17 (1970).
-
(1970)
J. Non-Cryst. Solids
, vol.5
, pp. 17
-
-
Hindley, N.K.1
-
20
-
-
54049129453
-
-
The occupancy of the electronic states plays a role in determining the optical absorption (Ref.), but this is not expected to be significant except for very high temperatures.
-
The occupancy of the electronic states plays a role in determining the optical absorption (Ref.), but this is not expected to be significant except for very high temperatures.
-
-
-
-
22
-
-
54049125924
-
-
In Eq., we implicitly assume that Nv (E) is negligible for energies above the Fermi energy and that Nc (E) is negligible for energies below the Fermi energy.
-
In Eq., we implicitly assume that Nv (E) is negligible for energies above the Fermi energy and that Nc (E) is negligible for energies below the Fermi energy.
-
-
-
-
24
-
-
0019570849
-
-
0038-1098 10.1016/0038-1098(81)90258-1.
-
W. -C. Chen, B. J. Feldman, J. Bajaj, F. -M. Tong, and G. K. Wong, Solid State Commun. 0038-1098 10.1016/0038-1098(81)90258-1 38, 357 (1981).
-
(1981)
Solid State Commun.
, vol.38
, pp. 357
-
-
Chen, W.-C.1
Feldman, B.J.2
Bajaj, J.3
Tong, F.-M.4
Wong, G.K.5
-
25
-
-
0020276392
-
-
0038-1098 10.1016/0038-1098(82)90890-0.
-
D. Redfield, Solid State Commun. 0038-1098 10.1016/0038-1098(82)90890-0 44, 1347 (1982).
-
(1982)
Solid State Commun.
, vol.44
, pp. 1347
-
-
Redfield, D.1
-
27
-
-
0000466016
-
-
0003-6951 10.1063/1.120963.
-
L. Jiao, I. Chen, R. W. Collins, C. R. Wronski, and N. Hata, Appl. Phys. Lett. 0003-6951 10.1063/1.120963 72, 1057 (1998).
-
(1998)
Appl. Phys. Lett.
, vol.72
, pp. 1057
-
-
Jiao, L.1
Chen, I.2
Collins, R.W.3
Wronski, C.R.4
Hata, N.5
-
28
-
-
18744390012
-
-
0021-8979 10.1063/1.1504174.
-
S. K. O'Leary and S. M. Malik, J. Appl. Phys. 0021-8979 10.1063/1.1504174 92, 4276 (2002).
-
(2002)
J. Appl. Phys.
, vol.92
, pp. 4276
-
-
O'Leary, S.K.1
Malik, S.M.2
-
29
-
-
3142775728
-
-
0957-4522 10.1023/B:JMSE.0000031593.62734.3a.
-
S. K. O'Leary, J. Mater. Sci.: Mater. Electron. 0957-4522 10.1023/B:JMSE.0000031593.62734.3a 15, 401 (2004).
-
(2004)
J. Mater. Sci.: Mater. Electron.
, vol.15
, pp. 401
-
-
O'Leary, S.K.1
-
30
-
-
7044270759
-
-
0021-8979 10.1063/1.1778478.
-
S. K. O'Leary, J. Appl. Phys. 0021-8979 10.1063/1.1778478 96, 3680 (2004).
-
(2004)
J. Appl. Phys.
, vol.96
, pp. 3680
-
-
O'Leary, S.K.1
-
31
-
-
54049122403
-
-
Many of these analyses, while not explicitly said to be JDOS analyses, implicitly are.
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Many of these analyses, while not explicitly said to be JDOS analyses, implicitly are.
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-
-
-
33
-
-
54049094190
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Please note that while Eqs. of the present analysis bear a strong resemblance with Eqs. (4)-(7) of O'Leary (Ref.), there is, in fact, a critical distinction. In the work of O'Leary (Ref.), instead of Evμ and Ecμ defining the limits of the integrations, E vT and E cT define the limits. The two formalisms are identical only for the special case for which Evμ is set to E vT and Ecμ is set to E cT.
-
Please note that while Eqs. of the present analysis bear a strong resemblance with Eqs. (4)-(7) of O'Leary (Ref.), there is, in fact, a critical distinction. In the work of O'Leary (Ref.), instead of Evμ and Ecμ defining the limits of the integrations, E vT and E cT define the limits. The two formalisms are identical only for the special case for which Evμ is set to E vT and Ecμ is set to E cT.
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-
-
-
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-
-
In a recent paper, Mok and O'Leary (Ref.) employ this selection of PECVD a -Si:H DOS modeling parameters.
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In a recent paper, Mok and O'Leary (Ref.) employ this selection of PECVD a -Si:H DOS modeling parameters.
-
-
-
-
35
-
-
37249046607
-
-
0021-8979 10.1063/1.2817822.
-
T. M. Mok and S. K. O'Leary, J. Appl. Phys. 0021-8979 10.1063/1.2817822 102, 113525 (2007).
-
(2007)
J. Appl. Phys.
, vol.102
, pp. 113525
-
-
Mok, T.M.1
O'Leary, S.K.2
-
36
-
-
0024047563
-
-
0950-0839 10.1080/09500838808214730.
-
M. Abkowitz, Philos. Mag. Lett. 0950-0839 10.1080/09500838808214730 58, 53 (1988).
-
(1988)
Philos. Mag. Lett.
, vol.58
, pp. 53
-
-
Abkowitz, M.1
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