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Volumn 85, Issue 24, 2012, Pages

Understanding the role of Si doping on surface charge and optical properties: Photoluminescence study of intrinsic and Si-doped InN nanowires

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EID: 84863326381     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.85.245313     Document Type: Article
Times cited : (30)

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    • However, the PL peak energy maintains more or less the same value, ∼0.674 eV. For details, see Ref. 46.
    • However, the PL peak energy maintains more or less the same value, ∼ 0.674 eV. For details, see Ref. 46.
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    • -3. For a Si cell temperature difference of ∼100C, in general, the Si-doping concentration will vary by another factor of ∼10.
    • - 3. For a Si cell temperature difference of ∼ 100C, in general, the Si-doping concentration will vary by another factor of ∼ 10.
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    • As discussed in Sec. , due to the enhanced n-type characteristics, similar approaches (as those for undoped InN nanowires) did not find evidence of excitons.
    • As discussed in Sec., due to the enhanced n -type characteristics, similar approaches (as those for undoped InN nanowires) did not find evidence of excitons.
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    • F is pinned to the conduction band in the near-surface region.
    • F is pinned to the conduction band in the near-surface region.
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    • F at the near-surface region will be pinned to a higher energy.
    • F at the near-surface region will be pinned to a higher energy.
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    • See Ref. 46; the flat band situation cannot explain the presence of high electron density in the near-surface region and low electron density in the bulk region.
    • See Ref. 46; the flat band situation cannot explain the presence of high electron density in the near-surface region and low electron density in the bulk region.
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    • The low-energy peak EPLL is not observable at low temperatures. This is because (1) EPLL shifts to higher energy at low temperatures and it merges with EPLH [see Fig. ], and (2) the intensity of EPLH increases much faster than that of EPLL with decreasing temperature such that EPLH overshadows EPLL at low temperatures [see Fig. ]. The reason for this can be ascribed to the evolution of the emission region to the near-surface as discussed in the main text, as well as the reduced nonradiative recombination rate in the near-surface region at low temperatures.
    • The low-energy peak E PL L is not observable at low temperatures. This is because (1) E PL L shifts to higher energy at low temperatures and it merges with E PL H [see Fig.], and (2) the intensity of E PL H increases much faster than that of E PL L with decreasing temperature such that E PL H overshadows E PL L at low temperatures [see Fig.]. The reason for this can be ascribed to the evolution of the emission region to the near-surface as discussed in the main text, as well as the reduced nonradiative recombination rate in the near-surface region at low temperatures.


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