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Volumn 7, Issue 3, 2007, Pages 831-836

Far-field imaging of optical second-harmonic generation in single GaN nanowires

Author keywords

[No Author keywords available]

Indexed keywords

MICROSCOPIC IMAGING; NANOPHOTONICS; NANOSCALE MATERIALS; QUASI-STATIC APPROXIMATION;

EID: 34047137561     PISSN: 15306984     EISSN: None     Source Type: Journal    
DOI: 10.1021/nl0624420     Document Type: Article
Times cited : (99)

References (27)
  • 12
    • 34047167671 scopus 로고    scopus 로고
    • We estimate that the ∼100 fs laser pulses broaden to between 200 and 300 fs after passing through a pulse extractor and the objective
    • We estimate that the ∼100 fs laser pulses broaden to between 200 and 300 fs after passing through a pulse extractor and the objective.
  • 18
    • 34047127821 scopus 로고    scopus 로고
    • Because SHG is insensitive to the polarity of the wurtzite c-axis, when referring to the c-axis or other vectors, we mean a direction parallel to the stated vector
    • Because SHG is insensitive to the polarity of the wurtzite c-axis, when referring to the c-axis or other vectors, we mean a direction parallel to the stated vector.
  • 20
    • 34047171689 scopus 로고    scopus 로고
    • Our approximations also neglect a weak depolarization that exists even for the component of P(2ω) parallel to the NW. This depolarization arises because of charge associated with the nonzero divergence of F(2ω) at the boundary of the illuminated A more accurate treatment might assume that the emitting region acts as an emitting ellipsoid, but the aspect ratio of the emitting of ∼9 for excitation and ∼6 for SH emission (based on field, not intensity, profiles) significantly reduces the depolarization along the NW
    • (2ω) at the boundary of the illuminated volume. A more accurate treatment might assume that the emitting region acts as an emitting ellipsoid, but the aspect ratio of the emitting volume of ∼9 for excitation and ∼6 for SH emission (based on field, not intensity, profiles) significantly reduces the depolarization along the NW.
  • 25
    • 34047183930 scopus 로고    scopus 로고
    • We neglect the birefringence of wurtzite GaN and use the ordinary index of refraction n to determine the dielectric constant, n2 at optical frequencies. Because the difference between the ordinary and extraordinary index of refraction is small, negligible error in the depolarization factors is incurred
    • 2 at optical frequencies. Because the difference between the ordinary and extraordinary index of refraction is small, negligible error in the depolarization factors is incurred.
  • 27
    • 34047136291 scopus 로고    scopus 로고
    • We also note that χzxz was neglected in the analysis of the near-field SHG from ZnO NWs in ref 3. For those NWs, which grew along the c-axis, χxzx would have contributed a weak component of P (2ω) perpendicular to the NW that varied with incident polarization
    • (2ω) perpendicular to the NW that varied with incident polarization.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.