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Volumn 71, Issue 3, 2005, Pages

Selective dynamic nuclear spin polarization in a spin-blocked double dot

Author keywords

[No Author keywords available]

Indexed keywords

ARSENIC; INDIUM;

EID: 15444380537     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.71.033307     Document Type: Article
Times cited : (24)

References (24)
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    • (2001) Phys. Rev. B , vol.64 , pp. 125316
    • Khaetskii, A.V.1    Nazarov, Yu.V.2
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    • A. V. Khaetskii and Yu. V. Nazarov, Phys. Rev. B 64, 125316 (2001); J. Schliemann, A. V. Khaetskii, and D. Loss, ibid. 66, 245303 (2002); R. de Sousa and S. Das Sarma, ibid. 67, 033301 (2003); 68, 115322 (2003).
    • (2002) Phys. Rev. B , vol.66 , pp. 245303
    • Schliemann, J.1    Khaetskii, A.V.2    Loss, D.3
  • 6
    • 0037437978 scopus 로고    scopus 로고
    • A. V. Khaetskii and Yu. V. Nazarov, Phys. Rev. B 64, 125316 (2001); J. Schliemann, A. V. Khaetskii, and D. Loss, ibid. 66, 245303 (2002); R. de Sousa and S. Das Sarma, ibid. 67, 033301 (2003); 68, 115322 (2003).
    • (2003) Phys. Rev. B , vol.67 , pp. 033301
    • De Sousa, R.1    Das Sarma, S.2
  • 7
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    • A. V. Khaetskii and Yu. V. Nazarov, Phys. Rev. B 64, 125316 (2001); J. Schliemann, A. V. Khaetskii, and D. Loss, ibid. 66, 245303 (2002); R. de Sousa and S. Das Sarma, ibid. 67, 033301 (2003); 68, 115322 (2003).
    • (2003) Phys. Rev. B , vol.68 , pp. 115322
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    • Inoshita, T.1    Tarucha, S.2
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    • W. E. Carlos, S. G. Bishop, and D. J. Treacy, Phys. Rev. B 43, 12 512 (1991); Appl. Phys. Lett. 49, 528 (1986).
    • (1986) Appl. Phys. Lett. , vol.49 , pp. 528
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    • note
    • The crystal structure of pure GaAs is zinc-blende with cubic symmetry. No noticeable field gradient is expected due to this symmetry.
  • 19
    • 0000264198 scopus 로고
    • Amsterdam
    • J. V. Kranendonk, Physica (Amsterdam) 20, 781 (1954).
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  • 20
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    • Abragam, A.1
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    • (1996) Principles of Magnetic Resonance
    • Slichter, C.P.1
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    • note
    • We have assumed that the electron g-factor is negative and the triplet is the ground state at zero magnetic field. One could equivalently discuss the other triplet state |1,1〉=|↑〉|↑〉 if the singlet is the ground state when there is no magnetic field (Ref. 7).


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