-
1
-
-
68249103823
-
-
APPLAB 0003-6951 10.1063/1.3191675
-
X. Lu, Appl. Phys. Lett. APPLAB 0003-6951 10.1063/1.3191675 95, 041903 (2009).
-
(2009)
Appl. Phys. Lett.
, vol.95
, pp. 041903
-
-
Lu, X.1
-
2
-
-
0037425189
-
-
APPLAB 0003-6951 10.1063/1.1565499
-
S. Tixier, Appl. Phys. Lett. APPLAB 0003-6951 10.1063/1.1565499 82, 2245 (2003).
-
(2003)
Appl. Phys. Lett.
, vol.82
, pp. 2245
-
-
Tixier, S.1
-
3
-
-
71749085843
-
-
JAPIAU 0021-8979 10.1063/1.3259434
-
K. M. Yu, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.3259434 106, 103709 (2009).
-
(2009)
J. Appl. Phys.
, vol.106
, pp. 103709
-
-
Yu, K.M.1
-
4
-
-
0035356466
-
-
JAPIAU 0021-8979 10.1063/1.1368156
-
I. Vurgaftman, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.1368156 89, 5815 (2001).
-
(2001)
J. Appl. Phys.
, vol.89
, pp. 5815
-
-
Vurgaftman, I.1
-
5
-
-
49449114171
-
-
1475-7435 10.1504/IJNT.2008.019828
-
T. Tiedje, Int. J. Nanotechnol. 1475-7435 10.1504/IJNT.2008.019828 5, 963 (2006).
-
(2006)
Int. J. Nanotechnol.
, vol.5
, pp. 963
-
-
Tiedje, T.1
-
6
-
-
44049093329
-
x
-
DOI 10.1063/1.2918844
-
X. Lu, Appl. Phys. Lett. APPLAB 0003-6951 10.1063/1.2918844 92, 192110 (2008). (Pubitemid 351713444)
-
(2008)
Applied Physics Letters
, vol.92
, Issue.19
, pp. 192110
-
-
Lu, X.1
Beaton, D.A.2
Lewis, R.B.3
Tiedje, T.4
Whitwick, M.B.5
-
7
-
-
46649113360
-
-
APPLAB 0003-6951 10.1063/1.2953176
-
G. Pettinari, Appl. Phys. Lett. APPLAB 0003-6951 10.1063/1.2953176 92, 262105 (2008).
-
(2008)
Appl. Phys. Lett.
, vol.92
, pp. 262105
-
-
Pettinari, G.1
-
8
-
-
77956317550
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.81.235211
-
G. Pettinari, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.81.235211 81, 235211 (2010).
-
(2010)
Phys. Rev. B
, vol.81
, pp. 235211
-
-
Pettinari, G.1
-
9
-
-
48449101748
-
-
1098-0121 10.1103/PhysRevB.78.035325
-
G. Ciatto, Phys. Rev. B 1098-0121 10.1103/PhysRevB.78.035325 78, 035325 (2008);
-
(2008)
Phys. Rev. B
, vol.78
, pp. 035325
-
-
Ciatto, G.1
-
10
-
-
78649753421
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.82.201304
-
G. Ciatto, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.82.201304 82, 201304 (R) (2010).
-
(2010)
Phys. Rev. B
, vol.82
, pp. 201304
-
-
Ciatto, G.1
-
11
-
-
0037087918
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.65.115203
-
A. Janotti, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.65.115203 65, 115203 (2002).
-
(2002)
Phys. Rev. B
, vol.65
, pp. 115203
-
-
Janotti, A.1
-
13
-
-
40849116339
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.77.085209
-
S. Francoeur, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.77.085209 77, 085209 (2008).
-
(2008)
Phys. Rev. B
, vol.77
, pp. 085209
-
-
Francoeur, S.1
-
14
-
-
58149242336
-
-
JAPIAU 0021-8979 10.1063/1.3041479
-
R. N. Kini, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.3041479 104, 113534 (2008).
-
(2008)
J. Appl. Phys.
, vol.104
, pp. 113534
-
-
Kini, R.N.1
-
15
-
-
0013419130
-
-
APPLAB 0003-6951 10.1063/1.97481
-
J. Wagner, Appl. Phys. Lett. APPLAB 0003-6951 10.1063/1.97481 49, 1080 (1986).
-
(1986)
Appl. Phys. Lett.
, vol.49
, pp. 1080
-
-
Wagner, J.1
-
16
-
-
0000808299
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.53.12829
-
R. A. Lewis, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.53.12829 53, 12829 (1996).
-
(1996)
Phys. Rev. B
, vol.53
, pp. 12829
-
-
Lewis, R.A.1
-
17
-
-
4244134599
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.2.456
-
P. Fisher and H. Y. Fan, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.2.456 2, 456 (1959);
-
(1959)
Phys. Rev. Lett.
, vol.2
, pp. 456
-
-
Fisher, P.1
Fan, H.Y.2
-
18
-
-
0001692281
-
-
JPSOAW 0022-3719 10.1088/0022-3719/11/2/024
-
R. F. Kirkman, J. Phys. C JPSOAW 0022-3719 10.1088/0022-3719/11/2/024 11, 419 (1978).
-
(1978)
J. Phys. C
, vol.11
, pp. 419
-
-
Kirkman, R.F.1
-
19
-
-
79961102208
-
-
5/2(1Γ7-), respectively (the atomic notation with the subscript giving the total angular momentum is also indicated).
-
5 / 2 (1 Γ 7 -), respectively (the atomic notation with the subscript giving the total angular momentum is also indicated).
-
-
-
-
20
-
-
1242287379
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.67.235204
-
R. A. Lewis, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.67.235204 67, 235204 (2003).
-
(2003)
Phys. Rev. B
, vol.67
, pp. 235204
-
-
Lewis, R.A.1
-
21
-
-
33750713774
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.25.1660
-
N. O. Lipari and A. Baldereschi, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.25.1660 25, 1660 (1970).
-
(1970)
Phys. Rev. Lett.
, vol.25
, pp. 1660
-
-
Lipari, N.O.1
Baldereschi, A.2
-
22
-
-
0009333222
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.12.630
-
P. J. Lin-Chung and B. W. Henvis, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.12.630 12, 630 (1975).
-
(1975)
Phys. Rev. B
, vol.12
, pp. 630
-
-
Lin-Chung, P.J.1
Henvis, B.W.2
-
23
-
-
33845285351
-
-
x on GaAs, the shallow acceptor binding energy increases with respect to the stress-free case due to the removal of the valence band degeneracy: The valence band edge, indeed, acquires a greater heavy-hole character [see e.g., JAPIAU 0021-8979 10.1063/1.366311
-
x on GaAs, the shallow acceptor binding energy increases with respect to the stress-free case due to the removal of the valence band degeneracy: The valence band edge, indeed, acquires a greater heavy-hole character [see e.g., K. S. Kim, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.366311 82, 5103 (1997) and references therein]. The value of acceptor binding energy (∼25 meV) we obtain in our samples is therefore greater than that in a stress-free layer. This increases the true energy difference between the binding energy of the acceptor state we observe and that of the most common substitutional acceptors in GaAs.
-
(1997)
J. Appl. Phys.
, vol.82
, pp. 5103
-
-
Kim, K.S.1
-
24
-
-
0000584811
-
-
JCOMEL 0953-8984 10.1088/0953-8984/3/35/009
-
R. Atzmüller, J. Phys. Condens. Matter JCOMEL 0953-8984 10.1088/0953-8984/3/35/009 3, 6775 (1991).
-
(1991)
J. Phys. Condens. Matter
, vol.3
, pp. 6775
-
-
Atzmüller, R.1
-
25
-
-
0000491669
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.6.3836
-
A. K. Bhattacharjee and S. Rodriguez, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.6.3836 6, 3836 (1972).
-
(1972)
Phys. Rev. B
, vol.6
, pp. 3836
-
-
Bhattacharjee, A.K.1
Rodriguez, S.2
-
27
-
-
79961120124
-
-
-1 (at T ∼4 K). However, phonon-phonon interaction makes the region of zero transmittance broader
-
- 1 (at T ∼4 K). However, phonon-phonon interaction makes the region of zero transmittance broader [
-
-
-
-
28
-
-
25144440423
-
Photon absorption in the Restrahlen band of thin films of GaN and AlN: Two phonon effects
-
DOI 10.1063/1.2034648, 043517
-
J. Yang, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.2034648 98, 043517 (2005)]. (Pubitemid 41344983)
-
(2005)
Journal of Applied Physics
, vol.98
, Issue.4
, pp. 1-5
-
-
Yang, J.1
Brown, G.J.2
Dutta, M.3
Stroscio, M.A.4
-
29
-
-
79961113218
-
-
1 for B> ∼15 T is accounted for by the variation of the Coulomb interaction with field and by nonparabolicity effects in the valence band.
-
1 for B > ∼15 T is accounted for by the variation of the Coulomb interaction with field and by nonparabolicity effects in the valence band.
-
-
-
-
30
-
-
33747130393
-
Giant spin-orbit bowing in GaAs1-xBix
-
DOI 10.1103/PhysRevLett.97.067205
-
B. Fluegel, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.97. 067205 97, 067205 (2006). (Pubitemid 44223142)
-
(2006)
Physical Review Letters
, vol.97
, Issue.6
, pp. 067205
-
-
Fluegel, B.1
Francoeur, S.2
Mascarenhas, A.3
Tixier, S.4
Young, E.C.5
Tiedje, T.6
-
31
-
-
0000083130
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.48.7910
-
J.-P. Cheng, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.48.7910 48, 7910 (1993).
-
(1993)
Phys. Rev. B
, vol.48
, pp. 7910
-
-
Cheng, J.-P.1
-
32
-
-
79961104794
-
-
+ transition for energies above the GaAs reststrahlen band is due to magnetopolaron effects; see Ref. 28.
-
+ transition for energies above the GaAs reststrahlen band is due to magnetopolaron effects; see Ref. 28.
-
-
-
-
33
-
-
0005904038
-
-
SSCOA4 0038-1098 10.1016/0038-1098(69)90543-2
-
G. E. Stillman, Solid State Commun. SSCOA4 0038-1098 10.1016/0038- 1098(69)90543-2 7, 921 (1969).
-
(1969)
Solid State Commun.
, vol.7
, pp. 921
-
-
Stillman, G.E.1
-
34
-
-
0029251507
-
-
SSCOA4 0038-1098 10.1016/0038-1098(94)00799-3
-
H. Kobori, Solid State Commun. SSCOA4 0038-1098 10.1016/0038-1098(94) 00799-3 93, 363 (1995).
-
(1995)
Solid State Commun.
, vol.93
, pp. 363
-
-
Kobori, H.1
-
35
-
-
0032631350
-
-
MSBTEK 0921-5107 10.1016/S0921-5107(99)00057-4
-
Y. Iye, Mater. Sci. Eng. B MSBTEK 0921-5107 10.1016/S0921-5107(99)00057-4 63, 88 (1999).
-
(1999)
Mater. Sci. Eng. B
, vol.63
, pp. 88
-
-
Iye, Y.1
-
36
-
-
0042244787
-
-
1098-0121 10.1103/PhysRevB.48.4437
-
M. Kunzer, Phys. Rev. B 1098-0121 10.1103/PhysRevB.48.4437 48, 4437 (1993).
-
(1993)
Phys. Rev. B
, vol.48
, pp. 4437
-
-
Kunzer, M.1
-
37
-
-
78649747600
-
-
PLRBAQ 1098-0121 10.1103/PhysRevB.82.193204
-
H.-X. Deng, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.82.193204 82, 193204 (2010).
-
(2010)
Phys. Rev. B
, vol.82
, pp. 193204
-
-
Deng, H.-X.1
-
38
-
-
0040449905
-
-
Neutral double acceptors [e.g., Be0, Zn0, and Hg0 in Ge] have spectra similar to those of single acceptors [see e.g., PLRBAQ 1098-0121 10.1103/PhysRevB.28.6953
-
Neutral double acceptors [e.g., Be 0, Zn 0, and Hg 0 in Ge] have spectra similar to those of single acceptors [see e.g., J. W. Cross, Phys. Rev. B PLRBAQ 1098-0121 10.1103/PhysRevB.28.6953 28, 6953 (1983) and references therein].
-
(1983)
Phys. Rev. B
, vol.28
, pp. 6953
-
-
Cross, J.W.1
|