-
2
-
-
0000405904
-
-
10.1103/PhysRevLett.83.4204
-
A. Imamoglu, D. D. Awschalom, G. Burkard, D. P. DiVincenzo, D. Loss, M. Sherwin, and A. Small, Phys. Rev. Lett. 83, 4204 (1999). 10.1103/PhysRevLett.83. 4204
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 4204
-
-
Imamoglu, A.1
Awschalom, D.D.2
Burkard, G.3
Divincenzo, D.P.4
Loss, D.5
Sherwin, M.6
Small, A.7
-
3
-
-
34547405126
-
-
10.1103/PhysRevLett.99.040501
-
S. M. Clark, Kai-Mei C. Fu, T. D. Ladd, and Y. Yamamoto, Phys. Rev. Lett. 99, 040501 (2007). 10.1103/PhysRevLett.99.040501
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 040501
-
-
Clark, S.M.1
Fu, K.C.2
Ladd, T.D.3
Yamamoto, Y.4
-
4
-
-
33646233461
-
-
10.1126/science.1126074
-
M. Atatüre, J. Dreiser, A. Badolato, A. Högele, K. Karrai, and A. Imamoglu, Science 312, 551 (2006). 10.1126/science.1126074
-
(2006)
Science
, vol.312
, pp. 551
-
-
Atatüre, M.1
Dreiser, J.2
Badolato, A.3
Högele, A.4
Karrai, K.5
Imamoglu, A.6
-
5
-
-
34548282525
-
-
10.1103/PhysRevLett.99.097401
-
X. Xu, Y. Wu, Bo Sun, Q. Huang, J. Cheng, D. G. Steel, A. S. Bracker, D. Gammon, C. Emary, and L. J. Sham, Phys. Rev. Lett. 99, 097401 (2007). 10.1103/PhysRevLett.99.097401
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 097401
-
-
Xu, X.1
Wu, Y.2
Sun, B.3
Huang, Q.4
Cheng, J.5
Steel, D.G.6
Bracker, A.S.7
Gammon, D.8
Emary, C.9
Sham, L.J.10
-
6
-
-
38549176662
-
-
10.1038/nature06472
-
B. D. Gerardot, D. Brunner, P. A. Dalgarno, P. Öhberg, S. Seidl, M. Kroner, K. Karrai, N. G. Stoltz, P. M. Petroff, and R. J. Warburton, Nature (London) 451, 441 (2008). 10.1038/nature06472
-
(2008)
Nature (London)
, vol.451
, pp. 441
-
-
Gerardot, B.D.1
Brunner, D.2
Dalgarno, P.A.3
Öhberg, P.4
Seidl, S.5
Kroner, M.6
Karrai, K.7
Stoltz, N.G.8
Petroff, P.M.9
Warburton, R.J.10
-
7
-
-
43749108833
-
-
10.1103/PhysRevLett.100.197401
-
A. J. Ramsay, S. J. Boyle, R. S. Kolodka, J. B. B. Oliveira, J. Skiba-Szymanska, H. Y. Liu, M. Hopkinson, A. M. Fox, and M. S. Skolnick, Phys. Rev. Lett. 100, 197401 (2008). 10.1103/PhysRevLett.100.197401
-
(2008)
Phys. Rev. Lett.
, vol.100
, pp. 197401
-
-
Ramsay, A.J.1
Boyle, S.J.2
Kolodka, R.S.3
Oliveira, J.B.B.4
Skiba-Szymanska, J.5
Liu, H.Y.6
Hopkinson, M.7
Fox, A.M.8
Skolnick, M.S.9
-
8
-
-
56249098912
-
-
10.1038/nature07530
-
D. Press, T. D. Ladd, B. Zhang, and Y. Yamamoto, Nature (London) 456, 218 (2008). 10.1038/nature07530
-
(2008)
Nature (London)
, vol.456
, pp. 218
-
-
Press, D.1
Ladd, T.D.2
Zhang, B.3
Yamamoto, Y.4
-
9
-
-
1642387526
-
-
10.1103/PhysRevB.69.075320
-
Pochung Chen, C. Piermarocchi, L. J. Sham, D. Gammon, and D. G. Steel, Phys. Rev. B 69, 075320 (2004). 10.1103/PhysRevB.69.075320
-
(2004)
Phys. Rev. B
, vol.69
, pp. 075320
-
-
Chen, P.1
Piermarocchi, C.2
Sham, L.J.3
Gammon, D.4
Steel, D.G.5
-
10
-
-
79956002683
-
-
10.1063/1.1483112
-
G. Medeiros-Ribeiro, M. V. B. Pinheiro, V. L. Pimentel, and E. Marega, Appl. Phys. Lett. 80, 4229 (2002). 10.1063/1.1483112
-
(2002)
Appl. Phys. Lett.
, vol.80
, pp. 4229
-
-
Medeiros-Ribeiro, G.1
Pinheiro, M.V.B.2
Pimentel, V.L.3
Marega, E.4
-
11
-
-
84988751828
-
-
10.1103/PhysRevB.65.195315
-
M. Bayer, G. Ortner, O. Stern, A. Kuther, A. A. Gorbunov, A. Forchel, P. Hawrylak, S. Fafard, K. Hinzer, T. L. Reinecke, S. N. Walck, J. P. Reithmaier, F. Klopf, and F. Schäfer, Phys. Rev. B 65, 195315 (2002), and references therein. 10.1103/PhysRevB.65.195315
-
(2002)
Phys. Rev. B
, vol.65
, pp. 195315
-
-
Bayer, M.1
Ortner, G.2
Stern, O.3
Kuther, A.4
Gorbunov, A.A.5
Forchel, A.6
Hawrylak, P.7
Fafard, S.8
Hinzer, K.9
Reinecke, T.L.10
Walck, S.N.11
Reithmaier, J.P.12
Klopf, F.13
Schäfer, F.14
-
12
-
-
13944282517
-
-
10.1103/PhysRevB.70.235337
-
T. Nakaoka, T. Saito, J. Tatebayashi, and Y. Arakawa, Phys. Rev. B 70, 235337 (2004). 10.1103/PhysRevB.70.235337
-
(2004)
Phys. Rev. B
, vol.70
, pp. 235337
-
-
Nakaoka, T.1
Saito, T.2
Tatebayashi, J.3
Arakawa, Y.4
-
13
-
-
20044372613
-
-
10.1103/PhysRevB.71.115334
-
M. Sénès, B. Urbaszek, X. Marie, T. Amand, J. Tribollet, F. Bernardot, C. Testelin, M. Chamarro, and J. M. Gérard, Phys. Rev. B 71, 115334 (2005). 10.1103/PhysRevB.71.115334
-
(2005)
Phys. Rev. B
, vol.71
, pp. 115334
-
-
Sénès, M.1
Urbaszek, B.2
Marie, X.3
Amand, T.4
Tribollet, J.5
Bernardot, F.6
Testelin, C.7
Chamarro, M.8
Gérard, J.M.9
-
14
-
-
14944341560
-
-
10.1103/PhysRevB.70.241305
-
A. V. Koudinov, I. A. Akimov, Y. G. Kusrayev, and F. Henneberger, Phys. Rev. B 70, 241305 (R) (2004). 10.1103/PhysRevB.70.241305
-
(2004)
Phys. Rev. B
, vol.70
, pp. 241305
-
-
Koudinov, A.V.1
Akimov, I.A.2
Kusrayev, Y.G.3
Henneberger, F.4
-
15
-
-
29644442260
-
-
10.1103/PhysRevB.72.161312
-
D. N. Krizhanovskii, A. Ebbens, A. I. Tartakovskii, F. Pulizzi, T. Wright, M. S. Skolnick, and M. Hopkinson, Phys. Rev. B 72, 161312 (R) (2005). 10.1103/PhysRevB.72.161312
-
(2005)
Phys. Rev. B
, vol.72
, pp. 161312
-
-
Krizhanovskii, D.N.1
Ebbens, A.2
Tartakovskii, A.I.3
Pulizzi, F.4
Wright, T.5
Skolnick, M.S.6
Hopkinson, M.7
-
16
-
-
33745778853
-
-
10.1103/PhysRevB.74.041301
-
T. Kiessling, A. V. Platonov, G. V. Astakhov, T. Slobodskyy, S. Mahapatra, W. Ossau, G. Schmidt, K. Brunner, and L. W. Molenkamp, Phys. Rev. B 74, 041301 (R) (2006). 10.1103/PhysRevB.74.041301
-
(2006)
Phys. Rev. B
, vol.74
, pp. 041301
-
-
Kiessling, T.1
Platonov, A.V.2
Astakhov, G.V.3
Slobodskyy, T.4
Mahapatra, S.5
Ossau, W.6
Schmidt, G.7
Brunner, K.8
Molenkamp, L.W.9
-
17
-
-
34547106297
-
-
10.1103/PhysRevB.76.045331
-
Y. Léger, L. Besombes, L. Maingault, and H. Mariette, Phys. Rev. B 76, 045331 (2007). 10.1103/PhysRevB.76.045331
-
(2007)
Phys. Rev. B
, vol.76
, pp. 045331
-
-
Léger, Y.1
Besombes, L.2
Maingault, L.3
Mariette, H.4
-
18
-
-
0042311014
-
-
10.1103/PhysRevLett.90.247403
-
B. Urbaszek, R. J. Warburton, K. Karrai, B. D. Gerardot, P. M. Petroff, and J. M. Garcia, Phys. Rev. Lett. 90, 247403 (2003). 10.1103/PhysRevLett.90. 247403
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 247403
-
-
Urbaszek, B.1
Warburton, R.J.2
Karrai, K.3
Gerardot, B.D.4
Petroff, P.M.5
Garcia, J.M.6
-
19
-
-
35748983902
-
-
10.1038/nphys748
-
M. Ediger, G. Bester, A. Badolato, P. M. Petroff, K. Karrai, A. Zunger, and R. J. Warburton, Nat. Phys. 3, 774 (2007). 10.1038/nphys748
-
(2007)
Nat. Phys.
, vol.3
, pp. 774
-
-
Ediger, M.1
Bester, G.2
Badolato, A.3
Petroff, P.M.4
Karrai, K.5
Zunger, A.6
Warburton, R.J.7
-
20
-
-
0033707357
-
-
10.1103/PhysRevLett.84.5648
-
A. Hartmann, Y. Ducommun, E. Kapon, U. Hohenester, and E. Molinari, Phys. Rev. Lett. 84, 5648 (2000). 10.1103/PhysRevLett.84.5648
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 5648
-
-
Hartmann, A.1
Ducommun, Y.2
Kapon, E.3
Hohenester, U.4
Molinari, E.5
-
21
-
-
3543059738
-
-
10.1038/35016030
-
R. J. Warburton, C. Schäflein, D. Haft, F. Bickel, A. Lorke, K. Karrai, J. M. Garcia, W. Schoenfeld, and P. M. Petroff, Nature (London) 405, 926 (2000). 10.1038/35016030
-
(2000)
Nature (London)
, vol.405
, pp. 926
-
-
Warburton, R.J.1
Schäflein, C.2
Haft, D.3
Bickel, F.4
Lorke, A.5
Karrai, K.6
Garcia, J.M.7
Schoenfeld, W.8
Petroff, P.M.9
-
22
-
-
0035886381
-
-
10.1103/PhysRevB.64.165301
-
D. V. Regelman, E. Dekel, D. Gershoni, E. Ehrenfreund, A. J. Williamson, J. Shumway, A. Zunger, W. V. Schoenfeld, and P. M. Petroff, Phys. Rev. B 64, 165301 (2001). 10.1103/PhysRevB.64.165301
-
(2001)
Phys. Rev. B
, vol.64
, pp. 165301
-
-
Regelman, D.V.1
Dekel, E.2
Gershoni, D.3
Ehrenfreund, E.4
Williamson, A.J.5
Shumway, J.6
Zunger, A.7
Schoenfeld, W.V.8
Petroff, P.M.9
-
23
-
-
28644447369
-
-
10.1103/PhysRevB.71.155325
-
S. Rodt, A. Schliwa, K. Pötschke, F. Guffarth, and D. Bimberg, Phys. Rev. B 71, 155325 (2005). 10.1103/PhysRevB.71.155325
-
(2005)
Phys. Rev. B
, vol.71
, pp. 155325
-
-
Rodt, S.1
Schliwa, A.2
Pötschke, K.3
Guffarth, F.4
Bimberg, D.5
-
24
-
-
33646480189
-
-
10.1103/PhysRevB.73.205321
-
M. H. Baier, A. Malko, E. Pelucchi, D. Y. Oberli, and E. Kapon, Phys. Rev. B 73, 205321 (2006). 10.1103/PhysRevB.73.205321
-
(2006)
Phys. Rev. B
, vol.73
, pp. 205321
-
-
Baier, M.H.1
Malko, A.2
Pelucchi, E.3
Oberli, D.Y.4
Kapon, E.5
-
25
-
-
29744448732
-
-
10.1103/PhysRevB.72.195332
-
A. Malko, D. Y. Oberli, M. H. Baier, E. Pelucchi, F. Michelini, K. F. Karlsson, M.-A. Dupertuis, and E. Kapon, Phys. Rev. B 72, 195332 (2005). 10.1103/PhysRevB.72.195332
-
(2005)
Phys. Rev. B
, vol.72
, pp. 195332
-
-
Malko, A.1
Oberli, D.Y.2
Baier, M.H.3
Pelucchi, E.4
Michelini, F.5
Karlsson, K.F.6
Dupertuis, M.-A.7
Kapon, E.8
-
28
-
-
0000491669
-
-
For an application of the method of invariants, see also: 10.1103/PhysRevB.6.3836
-
For an application of the method of invariants, see also: A. K. Bhattacharjee and S. Rodriguez, Phys. Rev. B 6, 3836 (1972). 10.1103/PhysRevB.6.3836
-
(1972)
Phys. Rev. B
, vol.6
, pp. 3836
-
-
Bhattacharjee, A.K.1
Rodriguez, S.2
-
29
-
-
0000587220
-
-
10.1103/PhysRevB.11.1512
-
K. Cho, S. Suga, W. Dreybrodt, and F. Willmann, Phys. Rev. B 11, 1512 (1975). 10.1103/PhysRevB.11.1512
-
(1975)
Phys. Rev. B
, vol.11
, pp. 1512
-
-
Cho, K.1
Suga, S.2
Dreybrodt, W.3
Willmann, F.4
-
30
-
-
72649083748
-
-
Using the method of invariants, the representation of the Zeeman Hamiltonian in the spinor basis states of the irreducible representation, Γ4, is a 2×2 matrix, which is expressed as a linear combination of the Pauli spin matrices with equal coefficients in front of σx and σy since σx and σy transform according to the same irreducible representation Γ3 and a different coefficient in front of σz since σz transforms according to another irreducible representation Γ2 of C3v.
-
Using the method of invariants, the representation of the Zeeman Hamiltonian in the spinor basis states of the irreducible representation, Γ4, is a 2×2 matrix, which is expressed as a linear combination of the Pauli spin matrices with equal coefficients in front of σx and σy since σx and σy transform according to the same irreducible representation Γ3 and a different coefficient in front of σz since σz transforms according to another irreducible representation Γ2 of C3v.
-
-
-
-
31
-
-
72649095185
-
-
If the hole state belong to either one or other one-dimensional representation of C3v, Γ5, or Γ6, a magnetic field applied in the (x,y) plane does not lift the degeneracy of the Kramers degenerate hole states (gxh = gyh =0). A magnetic field applied along the z axis lifts this degeneracy and introduces a linear dependence with Bz (gzh ≠0) in the Zeeman Hamiltonian.
-
If the hole state belong to either one or other one-dimensional representation of C3v, Γ5, or Γ6, a magnetic field applied in the (x,y) plane does not lift the degeneracy of the Kramers degenerate hole states (gxh = gyh =0). A magnetic field applied along the z axis lifts this degeneracy and introduces a linear dependence with Bz (gzh ≠0) in the Zeeman Hamiltonian.
-
-
-
-
32
-
-
4243360713
-
-
10.1103/PhysRevLett.76.3005
-
D. Gammon, E. S. Snow, B. V. Shanabrook, D. S. Katzer, and D. Park, Phys. Rev. Lett. 76, 3005 (1996). 10.1103/PhysRevLett.76.3005
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 3005
-
-
Gammon, D.1
Snow, E.S.2
Shanabrook, B.V.3
Katzer, D.S.4
Park, D.5
-
33
-
-
36949030426
-
-
10.1103/PhysRevB.76.235304
-
E. Poem, J. Shemesh, I. Marderfeld, D. Galushko, N. Akopian, D. Gershoni, B. D. Gerardot, A. Badolato, and P. M. Petroff, Phys. Rev. B 76, 235304 (2007). 10.1103/PhysRevB.76.235304
-
(2007)
Phys. Rev. B
, vol.76
, pp. 235304
-
-
Poem, E.1
Shemesh, J.2
Marderfeld, I.3
Galushko, D.4
Akopian, N.5
Gershoni, D.6
Gerardot, B.D.7
Badolato, A.8
Petroff, P.M.9
-
34
-
-
32644478602
-
-
10.1103/PhysRevLett.96.026804;
-
C. E. Pryor and M. E. Flatté, Phys. Rev. Lett. 96, 026804 (2006) 10.1103/PhysRevLett.96.026804
-
(2006)
Phys. Rev. Lett.
, vol.96
, pp. 026804
-
-
Pryor, C.E.1
Flatté, M.E.2
-
35
-
-
35548952715
-
-
10.1103/PhysRevLett.99.179901
-
C. E. Pryor and M. E. Flatté, Phys. Rev. Lett. 99, 179901 (E) (2007). 10.1103/PhysRevLett.99.179901
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 179901
-
-
Pryor, C.E.1
Flatté, M.E.2
-
37
-
-
41349083946
-
-
10.1016/j.physe.2007.08.047
-
M. Byszewski, B. Chalupar, K. F. Karlsson, D. Y. Oberli, E. Pelucchi, A. Rudra, and E. Kapon, Physica E (Amsterdam) 40, 1873 (2008). 10.1016/j.physe. 2007.08.047
-
(2008)
Physica e (Amsterdam)
, vol.40
, pp. 1873
-
-
Byszewski, M.1
Chalupar, B.2
Karlsson, K.F.3
Oberli, D.Y.4
Pelucchi, E.5
Rudra, A.6
Kapon, E.7
-
38
-
-
33845408971
-
-
10.1103/PhysRevB.74.245306;
-
P.-F. Braun, B. Urbaszek, T. Amand, X. Marie, O. Krebs, B. Eble, A. Lemaitre, and P. Voisin, Phys. Rev. B 74, 245306 (2006) 10.1103/PhysRevB.74. 245306
-
(2006)
Phys. Rev. B
, vol.74
, pp. 245306
-
-
Braun, P.-F.1
Urbaszek, B.2
Amand, T.3
Marie, X.4
Krebs, O.5
Eble, B.6
Lemaitre, A.7
Voisin, P.8
-
39
-
-
33846337528
-
-
10.1103/PhysRevB.75.035409
-
P. Maletinsky, C. W. Lai, A. Badolato, and A. Imamoglu, Phys. Rev. B 75, 035409 (2007). 10.1103/PhysRevB.75.035409
-
(2007)
Phys. Rev. B
, vol.75
, pp. 035409
-
-
Maletinsky, P.1
Lai, C.W.2
Badolato, A.3
Imamoglu, A.4
-
40
-
-
0013004941
-
-
10.1103/PhysRevB.66.153316
-
J. J. Finley, D. J. Mowbray, M. S. Skolnick, A. D. Ashmore, C. Baker, A. F. G. Monte, and M. Hopkinson, Phys. Rev. B 66, 153316 (2002). 10.1103/PhysRevB.66.153316
-
(2002)
Phys. Rev. B
, vol.66
, pp. 153316
-
-
Finley, J.J.1
Mowbray, D.J.2
Skolnick, M.S.3
Ashmore, A.D.4
Baker, C.5
Monte, A.F.G.6
Hopkinson, M.7
-
41
-
-
0042914898
-
-
10.1002/pssb.200303041
-
C. Schulhauser, A. Högele, R. J. Warburton, A. O. Govorov, W. Schoenfeld, J. M. Garcia, P. M. Petroff, and K. Karrai, Phys. Status Solidi B 238, 293 (2003). 10.1002/pssb.200303041
-
(2003)
Phys. Status Solidi B
, vol.238
, pp. 293
-
-
Schulhauser, C.1
Högele, A.2
Warburton, R.J.3
Govorov, A.O.4
Schoenfeld, W.5
Garcia, J.M.6
Petroff, P.M.7
Karrai, K.8
-
42
-
-
72649098955
-
-
The spinor basis for the degenerate hole states belonging to Γ5 and Γ6 has the explicit form given by { 1 2 (| 3 2, 3 2 □ - | 3 2, - 3 2 □), 1 2 (| 3 2, 3 2 □ + | 3 2, - 3 2 □) }.
-
The spinor basis for the degenerate hole states belonging to Γ5 and Γ6 has the explicit form given by { 1 2 (| 3 2, 3 2 □ - | 3 2, - 3 2 □), 1 2 (| 3 2, 3 2 □ + | 3 2, - 3 2 □) }.
-
-
-
-
43
-
-
72649087935
-
-
If the hole state belong to either one or other one-dimensional representation of C3v, Γ5, or Γ6, the neutral exciton states belong to Γ3 (since Γ4 □ Γ5 = Γ3 and Γ4 □ Γ6 = Γ3) and, thus, are split into two doubly degenerate states, which means that δ= δ□ =0 in the expression of the exchange Hamiltonian.
-
If the hole state belong to either one or other one-dimensional representation of C3v, Γ5, or Γ6, the neutral exciton states belong to Γ3 (since Γ4 □ Γ5 = Γ3 and Γ4 □ Γ6 = Γ3) and, thus, are split into two doubly degenerate states, which means that δ= δ□ =0 in the expression of the exchange Hamiltonian.
-
-
-
-
45
-
-
0031272024
-
-
10.1002/1521-396X(199711)164:1<487::AID-PSSA487>3.0.CO;2-1
-
E. L. Ivchenko, Phys. Status Solidi A 164, 487 (1997). 10.1002/1521-396X(199711)164:1<487::AID-PSSA487>3.0.CO;2-1
-
(1997)
Phys. Status Solidi A
, vol.164
, pp. 487
-
-
Ivchenko, E.L.1
-
47
-
-
24544460485
-
-
10.1103/PhysRevB.35.1242
-
C. Mailhiot and D. L. Smith, Phys. Rev. B 35, 1242 (1987). 10.1103/PhysRevB.35.1242
-
(1987)
Phys. Rev. B
, vol.35
, pp. 1242
-
-
Mailhiot, C.1
Smith, D.L.2
-
48
-
-
72649083513
-
-
This picture is expected to be valid in a perturbative limit and cannot be employed to evaluate the g factors in heterostructures from the effective g factors of the bulk materials.
-
This picture is expected to be valid in a perturbative limit and cannot be employed to evaluate the g factors in heterostructures from the effective g factors of the bulk materials.
-
-
-
-
49
-
-
33748694526
-
-
10.1103/PhysRevB.74.115309
-
P. Pfeffer and W. Zawadzki, Phys. Rev. B 74, 115309 (2006). 10.1103/PhysRevB.74.115309
-
(2006)
Phys. Rev. B
, vol.74
, pp. 115309
-
-
Pfeffer, P.1
Zawadzki, W.2
-
50
-
-
33846521322
-
-
10.1103/PhysRevB.75.033316
-
W. Sheng and A. Babinski, Phys. Rev. B 75, 033316 (2007). 10.1103/PhysRevB.75.033316
-
(2007)
Phys. Rev. B
, vol.75
, pp. 033316
-
-
Sheng, W.1
Babinski, A.2
-
51
-
-
33845944842
-
-
10.1063/1.2402241
-
K. F. Karlsson, V. Troncale, D. Y. Oberli, A. Malko, E. Pelucchi, A. Rudra, and E. Kapon, Appl. Phys. Lett. 89, 251113 (2006). 10.1063/1.2402241
-
(2006)
Appl. Phys. Lett.
, vol.89
, pp. 251113
-
-
Karlsson, K.F.1
Troncale, V.2
Oberli, D.Y.3
Malko, A.4
Pelucchi, E.5
Rudra, A.6
Kapon, E.7
-
52
-
-
0037104390
-
-
10.1103/PhysRevB.66.081310
-
J. G. Tischler, A. S. Bracker, D. Gammon, and D. Park, Phys. Rev. B 66, 081310 (R) (2002). 10.1103/PhysRevB.66.081310
-
(2002)
Phys. Rev. B
, vol.66
, pp. 081310
-
-
Tischler, J.G.1
Bracker, A.S.2
Gammon, D.3
Park, D.4
-
53
-
-
67649500907
-
-
10.1103/PhysRevB.76.033301
-
I. Toft and R. T. Phillips, Phys. Rev. B 76, 033301 (2007). 10.1103/PhysRevB.76.033301
-
(2007)
Phys. Rev. B
, vol.76
, pp. 033301
-
-
Toft, I.1
Phillips, R.T.2
-
54
-
-
72649084131
-
-
In the general case, one can easily show that the linear polarization axes (x and y) are rotated by an angle θ for an arbitrary rotation of the magnetic field around the z axis by minus θ starting from the x axis.
-
In the general case, one can easily show that the linear polarization axes (x and y) are rotated by an angle θ for an arbitrary rotation of the magnetic field around the z axis by minus θ starting from the x axis.
-
-
-
-
55
-
-
33144478781
-
-
10.1103/PhysRevB.73.033306
-
R. M. Stevenson, R. J. Young, P. See, D. G. Gevaux, K. Cooper, P. Atkinson, I. Farrer, D. A. Ritchie, and A. J. Shields, Phys. Rev. B 73, 033306 (2006). 10.1103/PhysRevB.73.033306
-
(2006)
Phys. Rev. B
, vol.73
, pp. 033306
-
-
Stevenson, R.M.1
Young, R.J.2
See, P.3
Gevaux, D.G.4
Cooper, K.5
Atkinson, P.6
Farrer, I.7
Ritchie, D.A.8
Shields, A.J.9
-
56
-
-
37649027864
-
-
10.1103/PhysRevB.70.201308
-
J. J. Finley, M. Sabathil, P. Vogl, G. Abstreiter, R. Oulton, A. I. Tartakovskii, D. J. Mowbray, M. S. Skolnick, S. L. Liew, A. G. Cullis, and M. Hopkinson, Phys. Rev. B 70, 201308 (R) (2004). 10.1103/PhysRevB.70.201308
-
(2004)
Phys. Rev. B
, vol.70
, pp. 201308
-
-
Finley, J.J.1
Sabathil, M.2
Vogl, P.3
Abstreiter, G.4
Oulton, R.5
Tartakovskii, A.I.6
Mowbray, D.J.7
Skolnick, M.S.8
Liew, S.L.9
Cullis, A.G.10
Hopkinson, M.11
-
59
-
-
4344694975
-
-
10.1103/PhysRevB.68.073309
-
G. Bester and A. Zunger, Phys. Rev. B 68, 073309 (2003). 10.1103/PhysRevB.68.073309
-
(2003)
Phys. Rev. B
, vol.68
, pp. 073309
-
-
Bester, G.1
Zunger, A.2
-
60
-
-
28744441564
-
-
10.1103/PhysRevB.71.205301
-
T. Nakaoka, T. Saito, J. Tatebayashi, S. Hirose, T. Usuki, N. Yokoyama, and Y. Arakawa, Phys. Rev. B 71, 205301 (2005). 10.1103/PhysRevB.71.205301
-
(2005)
Phys. Rev. B
, vol.71
, pp. 205301
-
-
Nakaoka, T.1
Saito, T.2
Tatebayashi, J.3
Hirose, S.4
Usuki, T.5
Yokoyama, N.6
Arakawa, Y.7
-
61
-
-
0000516743
-
-
10.1103/PhysRevLett.84.2513
-
O. Benson, C. Santori, M. Pelton, and Y. Yamamoto, Phys. Rev. Lett. 84, 2513 (2000). 10.1103/PhysRevLett.84.2513
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 2513
-
-
Benson, O.1
Santori, C.2
Pelton, M.3
Yamamoto, Y.4
-
62
-
-
33645697299
-
-
10.1103/PhysRevLett.96.130501
-
N. Akopian, N. H. Lindner, E. Poem, Y. Berlatzky, J. Avron, D. Gershoni, B. D. Gerardot, and P. M. Petroff, Phys. Rev. Lett. 96, 130501 (2006). 10.1103/PhysRevLett.96.130501
-
(2006)
Phys. Rev. Lett.
, vol.96
, pp. 130501
-
-
Akopian, N.1
Lindner, N.H.2
Poem, E.3
Berlatzky, Y.4
Avron, J.5
Gershoni, D.6
Gerardot, B.D.7
Petroff, P.M.8
-
63
-
-
30544444958
-
-
10.1038/nature04446
-
R. M. Stevenson, R. J. Young, P. Atkinson, K. Cooper, D. A. Ritchie, and A. J. Shields, Nature (London) 439, 179 (2006). 10.1038/nature04446
-
(2006)
Nature (London)
, vol.439
, pp. 179
-
-
Stevenson, R.M.1
Young, R.J.2
Atkinson, P.3
Cooper, K.4
Ritchie, D.A.5
Shields, A.J.6
-
64
-
-
68649109382
-
-
10.1103/PhysRevLett.103.063601
-
R. Singh and G. Bester, Phys. Rev. Lett. 103, 063601 (2009). 10.1103/PhysRevLett.103.063601
-
(2009)
Phys. Rev. Lett.
, vol.103
, pp. 063601
-
-
Singh, R.1
Bester, G.2
|