简单介绍了半导体自旋电子学的研究对象和内容,主要包括磁性半导体、磁性/半导体复合结构、非磁性半导体量子阱和纳米结构中的自旋现象,以及半导体的自旋注入等.综述了半导体自旋电子学目前的研究进展及其在自旋电子器件和量子信息处理中的应用.
参考文献
| [1] | Baibich M N;Broto J M;Fert A .[J].Physical Review Letters,1988,61:2472. |
| [2] | Ohno H;Matrukura F;Ohno Y.[J].JSAP International,2002(05):4. |
| [3] | Furdyna I K;Kossut I.Semiconductor and Semimetals[M].New York:Academic Press,1988 |
| [4] | Munekata H;Ohno H;Von Molnar S et al.[J].Physical Review Letters,1989,63:1849. |
| [5] | De Boeck J;Oersterholt R;Van Esch A et al.[J].Applied Physics Letters,1996,68:2744. |
| [6] | Hu C M;Nitta J;Jensen A .[J].Physical Review B,2001,63:125333. |
| [7] | Schmidit G;Ferrand D;Molenkamp L W et al.[J].Physical Review B,2000,62:4790. |
| [8] | Hammar P R;Johnson M .[J].Physical Review B,2000,61:7207. |
| [9] | Alvarado S F;Renaud Ph .[J].Physical Review Letters,1992,68:1387. |
| [10] | Wolf S A;Awschalom D D;Buhrman R A et al.[J].Science,2001,294(16):1488. |
| [11] | LaBella V P;Bullock D W;Ding Z et al.[J].Science,2001,292:1518. |
| [12] | Zhu H J;Ramsteiner M;Kostial H et al.[J].Physical Review Letters,2001,87:016601. |
| [13] | Monsma D;Lodder J C;Popma Th J A et al.[J].Physical Review Letters,1995,74:5260. |
| [14] | Rippard WH.;Buhrman RA. .Spin-dependent hot electron transport in Co/Cu thin films[J].Physical review letters,2000(5):971-974. |
| [15] | Rashba E I .[J].Physical Review B,2000,62:16267. |
| [16] | Tang H X;Monzon F G;Lifshitz R et al.[J].Physical Review B,2000,61:4437. |
| [17] | Mallnowski A;Britton R S;Grevatt T et al.[J].Physical Review B,2000,62:13034. |
| [18] | Kato Y K;Myers R C;Gossard A C et al.[J].Physical Review Letters,2004,93:176601. |
| [19] | Sasakura H.;Ohshima T.;Muto S. .Quantum gates using spin states of triple quantum dot[J].Physica, E. Low-dimensional systems & nanostructures,2001(1/3):458-462. |
| [20] | Ohno,H;Chiba,D;Matsukura,F;Omiya,T;Abe,E;Dietl,T;Ohno,Y;Ohtani,K .Electric-field control of ferromagnetism.[J].Nature,2000(6815):944-946. |
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