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Volumn 72, Issue 4, 2005, Pages

Auger recombination of excitons in semimagnetic quantum dot structure in a magnetic field

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EID: 33749233446     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.72.045302     Document Type: Article
Times cited : (43)

References (16)
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    • W. Heimbrodt and P. J. Klar, in Magnetic nanostructures, edited by, H. S. Nalwa,, (American Scientific Publishers, California 2002), pp. 1-58.
    • (2002) Magnetic Nanostructures , pp. 1-58
    • Heimbrodt, W.1    Klar, P.J.2
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    • JAPIAU 0021-8979 10.1063/1.341700
    • J. K. Furdyna, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.341700 64, R29 (1988).
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    • Furdyna, J.K.1
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    • 14644422362 scopus 로고    scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.69.085321
    • Nguen Que Huong and J. L. Birman, Phys. Rev. B PRBMDO 0163-1829 10.1103/PhysRevB.69.085321 69, 085321 (2004).
    • (2004) Phys. Rev. B , vol.69 , pp. 085321
    • Que Huong, N.1    Birman, J.L.2
  • 16
    • 84856131962 scopus 로고    scopus 로고
    • Besides the mixing of 3dt2 and 4p states of an isolated Mn ion, the crystal field mixes 3dt2 and valence band states. This mixing is responsible for the giant Zeeman effect in DMS and the parameter of the mixing can be found from the value of the hole exchange constant β. The effect of the mixing can be comparable with that of the 3d-4p Mn ion mixing and increases effectiveness of the Auger recombination of bright excitons.
    • Besides the mixing of 3dt2 and 4p states of an isolated Mn ion, the crystal field mixes 3dt2 and valence band states. This mixing is responsible for the giant Zeeman effect in DMS and the parameter of the mixing can be found from the value of the hole exchange constant β. The effect of the mixing can be comparable with that of the 3d-4p Mn ion mixing and increases effectiveness of the Auger recombination of bright excitons.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.