-
3
-
-
0033092791
-
-
M. Oestreich, J. Hübner, D. Hägele, P. J. Klar, W. Heimbrodt, W. W. Rühle, D. E. Ashenford, and B. Lunn, Appl. Phys. Lett. 74, 1251 (1999).
-
(1999)
Appl. Phys. Lett.
, vol.74
, pp. 1251
-
-
Oestreich, M.1
Hübner, J.2
Hägele, D.3
Klar, P.J.4
Heimbrodt, W.5
Rühle, W.W.6
Ashenford, D.E.7
Lunn, B.8
-
4
-
-
0000050851
-
-
D. Hägele, M. Oestreich, W. W. Rühle, N. Nestle, and K. Eberl, Appl. Phys. Lett. 73, 1580 (1998).
-
(1998)
Appl. Phys. Lett.
, vol.73
, pp. 1580
-
-
Hägele, D.1
Oestreich, M.2
Rühle, W.W.3
Nestle, N.4
Eberl, K.5
-
5
-
-
0033576696
-
-
R. Fiederling, M. Keim, G. Reuscher, W. Ossau, G. Schmidt, A. Waag, and L. W. Molenkamp, Nature (London) 402, 787 (1999).
-
(1999)
Nature (London)
, vol.402
, pp. 787
-
-
Fiederling, R.1
Keim, M.2
Reuscher, G.3
Ossau, W.4
Schmidt, G.5
Waag, A.6
Molenkamp, L.W.7
-
7
-
-
0038044789
-
-
J. Rudolph, D. Hägele, H. M. Gibbs, G. Khitrova, and M. Oestreich, Appl. Phys. Lett. 82, 4516 (2003).
-
(2003)
Appl. Phys. Lett.
, vol.82
, pp. 4516
-
-
Rudolph, J.1
Hägele, D.2
Gibbs, H.M.3
Khitrova, G.4
Oestreich, M.5
-
9
-
-
0001220974
-
-
T. C. Damen, L. Vina, J. E. Cunningham, J. Shah, and L. J. Sham, Phys. Rev. Lett. 67, 3432 (1991).
-
(1991)
Phys. Rev. Lett.
, vol.67
, pp. 3432
-
-
Damen, T.C.1
Vina, L.2
Cunningham, J.E.3
Shah, J.4
Sham, L.J.5
-
10
-
-
30344463438
-
-
1 mW excitation power corresponds to a carrier density of about 2.1× 1012 cm-2. This relationship is also used for the simulations.
-
1 mW excitation power corresponds to a carrier density of about 2.1× 1012 cm-2. This relationship is also used for the simulations.
-
-
-
-
11
-
-
0009689805
-
-
E. L. Blansett, M. G. Raymer, G. Khitrova, H. M. Gibbs, D. K. Serkland, A. A. Allerman, and K. M. Geib, Opt. Express 9, 312 (2001).
-
(2001)
Opt. Express
, vol.9
, pp. 312
-
-
Blansett, E.L.1
Raymer, M.G.2
Khitrova, G.3
Gibbs, H.M.4
Serkland, D.K.5
Allerman, A.A.6
Geib, K.M.7
-
13
-
-
0029271279
-
-
P. Michler, A. Lohner, W. W. Rühle, and G. Reiner, Appl. Phys. Lett. 66, 1599 (1995).
-
(1995)
Appl. Phys. Lett.
, vol.66
, pp. 1599
-
-
Michler, P.1
Lohner, A.2
Rühle, W.W.3
Reiner, G.4
-
14
-
-
0004536783
-
-
S. Hallstein, J. Berger, M. Hilpert, H. C. Schneider, W. W. Rühle, F. Jahnke, S. W. Koch, H. M. Gibbs, G. Khitrova, and M. Oestreich, Phys. Rev. B 56, R7076 (1997).
-
(1997)
Phys. Rev. B
, vol.56
, pp. 7076
-
-
Hallstein, S.1
Berger, J.2
Hilpert, M.3
Schneider, H.C.4
Rühle, W.W.5
Jahnke, F.6
Koch, S.W.7
Gibbs, H.M.8
Khitrova, G.9
Oestreich, M.10
-
19
-
-
0001034666
-
-
R. Terauchi, Y. Ohno, T. Adachi, A. Sato, F. Matsukura, A. Tackeuchi, and H. Ohno, Jpn. J. Appl. Phys., Part 1 38, 2549 (1999).
-
(1999)
Jpn. J. Appl. Phys., Part 1
, vol.38
, pp. 2549
-
-
Terauchi, R.1
Ohno, Y.2
Adachi, T.3
Sato, A.4
Matsukura, F.5
Tackeuchi, A.6
Ohno, H.7
-
20
-
-
30344481492
-
-
Spin relaxation at room temperature is governed by the Dyakonov-Perel mechanism. For this mechanism the spin relaxation time follows τs ∝ E e1 -2, where Ee1 is the electron confinement energy.
-
Spin relaxation at room temperature is governed by the Dyakonov-Perel mechanism. For this mechanism the spin relaxation time follows τs ∝ E e1 -2, where Ee1 is the electron confinement energy.
-
-
-
-
21
-
-
0001624546
-
-
Y. Ohno, R. Terauchi, T. Adachi, F. Matsukura, and H. Ohno, Phys. Rev. Lett. 83, 4196 (1999).
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 4196
-
-
Ohno, Y.1
Terauchi, R.2
Adachi, T.3
Matsukura, F.4
Ohno, H.5
-
22
-
-
19644400946
-
-
S. Döhrmann, D. Hägele, J. Rudolph, M. Bichler, D. Schuh, and M. Oestreich, Phys. Rev. Lett. 93, 147405 (2004).
-
(2004)
Phys. Rev. Lett.
, vol.93
, pp. 147405
-
-
Döhrmann, S.1
Hägele, D.2
Rudolph, J.3
Bichler, M.4
Schuh, D.5
Oestreich, M.6
-
23
-
-
30344487748
-
-
Valence-band mixing and therefore gain characteristics change with crystal orientation. The reduced symmetry in (110) QWs will favor a stable, slightly elliptically polarized laser mode.
-
Valence-band mixing and therefore gain characteristics change with crystal orientation. The reduced symmetry in (110) QWs will favor a stable, slightly elliptically polarized laser mode.
-
-
-
-
24
-
-
0035336093
-
-
T. Adachi, Y. Ohno, F. Matsukura, and H. Ohno, Physica E (Amsterdam) 10, 36 (2001).
-
(2001)
Physica e (Amsterdam)
, vol.10
, pp. 36
-
-
Adachi, T.1
Ohno, Y.2
Matsukura, F.3
Ohno, H.4
-
25
-
-
30344431610
-
-
At the high excitation densities shown in Fig. 3(b), the PL lines of the QW and the GaAs substrate are strongly broadened and overlap spectrally. The values for τs were obtained from single-exponential fits to the degree of polarization starting about 175 ps after laser excitation when the short-lived PL from the substrate has decayed.
-
At the high excitation densities shown in Fig. 3(b), the PL lines of the QW and the GaAs substrate are strongly broadened and overlap spectrally. The values for τs were obtained from single-exponential fits to the degree of polarization starting about 175 ps after laser excitation when the short-lived PL from the substrate has decayed.
-
-
-
-
26
-
-
30344481213
-
-
The electron spin polarization in an electrically pumped VCSEL must be achieved in a spin injector. The spin aligner should be placed directly next to the QWs to avoid loss of spin polarization during transport from the spin injector to the gain medium.
-
The electron spin polarization in an electrically pumped VCSEL must be achieved in a spin injector. The spin aligner should be placed directly next to the QWs to avoid loss of spin polarization during transport from the spin injector to the gain medium.
-
-
-
|