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Volumn 81, Issue 19, 2010, Pages

Stark effect of confined shallow levels in phosphorus-doped silicon nanocrystals

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EID: 77955596717     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.195302     Document Type: Article
Times cited : (8)

References (31)
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    • Theoretical calculation considering NC with cubic shape can also be found in literature, see, e.g., 10.1063/1.1994946;
    • Theoretical calculation considering NC with cubic shape can also be found in literature, see, e.g., D. Ahn, J. Appl. Phys. 98, 033709 (2005) 10.1063/1.1994946
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    • Strictly speaking this is proved to be valid for NC with radii up to 3 nm, that is, the larger size considered in Ref.. However, we can reasonably assume also for NCs of larger size that the configuration with P located in the central region of the NC is energetically favored with respect to the one with P close to the NC surface
    • Strictly speaking this is proved to be valid for NC with radii up to 3 nm, that is, the larger size considered in Ref.. However, we can reasonably assume also for NCs of larger size that the configuration with P located in the central region of the NC is energetically favored with respect to the one with P close to the NC surface.
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    • An excellent introduction to envelope-function techniques can be found, e.g., Oxford University Press, Oxford, 10.1093/acprof:oso/9780198507802.001.0001
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    • Actually, Vb corresponds to a saddle point of the potential energy: it is the maximum of the potential from P to the surface well along the field direction (see Fig. ) and it is the lower value of the energy of the barrier delimiting the impurity well.
    • Actually, V b corresponds to a saddle point of the potential energy: it is the maximum of the potential from P to the surface well along the field direction (see Fig.) and it is the lower value of the energy of the barrier delimiting the impurity well.


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