2015
DOI: 10.1063/1.4906852
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Nanosecond and ultrafast optical power limiting in luminescent Fe2O3 hexagonal nanomorphotype

Abstract: Efficient ultrafast optical limiting using single walled carbon nanotubes functionalized noncovalently with free base and metalloporphyrins Nonlinear optical absorption and optical power limiting properties of Fe 2 O 3 hexagonal nanomorphotype are investigated using open aperture Z-scan technique with the 5 ns and 100 fs laser pulses, at 532 nm and 800 nm excitation domains. At relatively low pulse energies (below 5 lJ), sample shows saturable absorption (SA), but on going to the higher energies an interesting… Show more

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Cited by 50 publications
(18 citation statements)
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“…Optical transitions are forbidden in bulk Fe 2 O 3 due to localized d‐d transitions . Appearance of PL bands in hematite nanoparticles might be due to quantum confinement effect; particle size influences photoluminescence phenomenon significantly . Broad emission band centered at around 564 nm (2.2 eV) corresponds to band edge transition .…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Optical transitions are forbidden in bulk Fe 2 O 3 due to localized d‐d transitions . Appearance of PL bands in hematite nanoparticles might be due to quantum confinement effect; particle size influences photoluminescence phenomenon significantly . Broad emission band centered at around 564 nm (2.2 eV) corresponds to band edge transition .…”
Section: Resultsmentioning
confidence: 99%
“…These defects form donor states below conduction band in forbidden energy level . Nonradiative peaks at 656 nm (1.89 eV), 682 nm (1.82 eV), and 753 nm (1.65 eV) appeared from the transitions of trapped electrons in different defect states of oxygen vacancies on the surface of nanostructured α‐Fe 2 O 3 …”
Section: Resultsmentioning
confidence: 99%
“…They suggested that these peaks are due to the band-edge emission of the α–Fe 2 O 3 nanoparticles [59]. Recently, the PL emission peaks at 532, 567, 646, and 697 nm observed by Thomas et al [60]. These peaks related to different optical band edges due to quantum confinement effect.…”
Section: Resultsmentioning
confidence: 99%
“…The fitting values of nonlinear absorption coefficient β at 500, 700 and 900 nm were found to be (7.49 ± 0.23) × 10 −3 , (1.68 ± 0.078) × 10 −3 and (0.81 ± 0.03) × 10 −3 cm/GW for BPQDs, respectively. The obtained nonlinear absorption coefficients of these BPQDs are higher than those of other optical-limiting materials such as CdSe QDs with average size of around 2 nm ((1.1 ± 0.15) × 10 −3 cm/GW) [ 49 ], CdO nanoflakes (0.69 × 10 −3 cm/GW) [ 50 ] and Fe 2 O 3 hexagonal nanostructures (0.82 × 10 −3 cm/GW) [ 51 ], obtained by using the similar femtosecond laser pulses. These results indicated that BPQDs can act as good broadband optical-limiting materials in the visible range.…”
Section: Resultsmentioning
confidence: 99%