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We estimate that the ∼100 fs laser pulses broaden to between 200 and 300 fs after passing through a pulse extractor and the objective
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We estimate that the ∼100 fs laser pulses broaden to between 200 and 300 fs after passing through a pulse extractor and the objective.
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34047127821
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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
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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.
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19
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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
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(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.
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22
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0141522822
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Sanford, N. A.; Robins, L. H.; Davydov, A. V.; Shapiro, A.; Tsvetkov, D. V.; Dmitriev, A. V.; Keller, S.; Mishra, U. K.; DenBaars, S. P. J. Appl. Phys. 2003, 94, 2980.
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Mishra, U.K.8
DenBaars, S.P.9
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Jimbo, T.8
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34047183930
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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
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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.
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34047136291
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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
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(2ω) perpendicular to the NW that varied with incident polarization.
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