2013
DOI: 10.1016/j.optcom.2013.01.018
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Mechanisms for fabrications and nonlinear optical properties of Pd and Pt nanoparticles by femtosecond laser

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Cited by 27 publications
(21 citation statements)
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“…This phenomenon is also noteworthy for Pt NPs suspensions at varied wavelengths, e.g., at 792 nm of 120 fs, 1064 nm of 50 ps, and 800 nm with femtosecond pules . In regard of narrow interval band structure of Pt NPs as discussed above, Fan and his co‐workers interpreted the underlying mechanism for prominent saturable absorption as interband electron transition by monophoton absorption . Besides, they inferred that the origin of the self‐focusing refraction is through the electronic mechanisms of hot electrons arising from the strong nonlinear absorption .…”
Section: Resultsmentioning
confidence: 69%
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“…This phenomenon is also noteworthy for Pt NPs suspensions at varied wavelengths, e.g., at 792 nm of 120 fs, 1064 nm of 50 ps, and 800 nm with femtosecond pules . In regard of narrow interval band structure of Pt NPs as discussed above, Fan and his co‐workers interpreted the underlying mechanism for prominent saturable absorption as interband electron transition by monophoton absorption . Besides, they inferred that the origin of the self‐focusing refraction is through the electronic mechanisms of hot electrons arising from the strong nonlinear absorption .…”
Section: Resultsmentioning
confidence: 69%
“…It is worth noting that the glass dispersed with Pt NPs behaves stronger with nonlinear absorption (Im χ (3) = −2.23 × 10 −10 esu) comparing with nonlinear refraction (Re χ (3) = 1.23 × 10 −11 esu) in magnitude. This phenomenon is also noteworthy for Pt NPs suspensions at varied wavelengths, e.g., at 792 nm of 120 fs, 1064 nm of 50 ps, and 800 nm with femtosecond pules . In regard of narrow interval band structure of Pt NPs as discussed above, Fan and his co‐workers interpreted the underlying mechanism for prominent saturable absorption as interband electron transition by monophoton absorption .…”
Section: Resultsmentioning
confidence: 88%
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“…Furthermore, we can calculate the real and imaginary parts of the third-order nonlinear susceptibility (χ (3) ) of the film samples by equations (1) and (2) 31 ,where n 0 , c, ε 0 and λ are linear refractive index, speed of light, permittivity of free space and the wavelength of the laser light of the film sample, respectively. The total third-order nonlinear susceptibility χ (3) can be calculated by equation (3).…”
Section: Resultsmentioning
confidence: 99%
“…The calculated β and γ values are applied to deduce the real and imaginary part of the third-order nonlinear susceptibility according to Eqs. (6) and (7) [53].…”
Section: Nonlinear Optical Properties Studiesmentioning
confidence: 99%