2005
DOI: 10.1002/pssa.200461220
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Modification of cubic susceptibility tensor in birefringent porous silicon

Abstract: PACS 42.65. Ky, 78.20.Fm, 78.67.Bf Polarization-sensitive third-harmonic generation in birefringent (110) porous silicon layers reveals a modification in the cubic susceptibility tensor of silicon caused by strongly anisotropic pores. The ratio 095 939 1566 (7) phys. stat. sol. (a) 202, No. 8 (2005) / www.pss-a.com 1677

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Cited by 13 publications
(4 citation statements)
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References 13 publications
(7 reference statements)
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“…Moreover, the electrostatic model (2) cannot explain the rise of the effective cubic susceptibility in por-Si in comparison with c-Si. Thus, the observed effect seems to be similar to the one found for THG in birefringent mesoporous Si [7]: both χ (3) (ω; ω, −ω, ω) and χ (3) (3ω; ω, ω, ω) cubic susceptibilities for por-Si significantly exceed ones for c-Si and, although the electrostatic effective-medium approximation successfully de-scribes birefringence of mesoporous Si, the nonlinearoptical anisotropy agrees to the predictions based on the effective-medium model only qualitatively. The possible explanation can be connected with the light-localization effects caused by interference of the waves reflected and scattered at the silicon nanoparticles and pores [6,7].…”
Section: Resultssupporting
confidence: 84%
See 1 more Smart Citation
“…Moreover, the electrostatic model (2) cannot explain the rise of the effective cubic susceptibility in por-Si in comparison with c-Si. Thus, the observed effect seems to be similar to the one found for THG in birefringent mesoporous Si [7]: both χ (3) (ω; ω, −ω, ω) and χ (3) (3ω; ω, ω, ω) cubic susceptibilities for por-Si significantly exceed ones for c-Si and, although the electrostatic effective-medium approximation successfully de-scribes birefringence of mesoporous Si, the nonlinearoptical anisotropy agrees to the predictions based on the effective-medium model only qualitatively. The possible explanation can be connected with the light-localization effects caused by interference of the waves reflected and scattered at the silicon nanoparticles and pores [6,7].…”
Section: Resultssupporting
confidence: 84%
“…Microporous Si with the pores of less than 2 nm in diameter exhibits bright visible photoluminescence caused by a quantum-size effect [3]. It was also reported the in- creased efficiency of cubic nonlinear-optical interaction in por-Si detected in microporous Si by z-scan technique [4,5], and in mesoporous Si by the third-harmonic generation (THG) [6,7]. Note that in the latter material typical pore sizes range from 2 to 100 nm.…”
Section: Introductionmentioning
confidence: 93%
“…(6)). In the experiment the fundamental wavelength ranging from 1.1 to 1.5 m (out of the phase-matching region, see below) TH signal polarized along 110 axis was registered in transition geometry with pumping polarized along [001] and 110 64. Experimentally obtained ratio of the TH signals allowed finding the 3 eff component ratio r = 3333 (the phase mismatch was taken into account).…”
mentioning
confidence: 99%
“…A similar anisotropy has been studied earlier in detail for the initial PS films. 22,23 To verify the above findings, we used a Cr:forsterite laser generating 50-fs pulses at a center wavelength of 1250 nm ͑Ref. 24͒ to measure the third-harmonic ͑TH͒ signal generated in OPS structures.…”
mentioning
confidence: 94%