“…Meanwhile, nonlinear optical studies of empty-cage C 60 and C 70 have shown that these materials possess both large third order susceptibilities (3) (Ϫ 4 ; 1 , 2 , 3 ) 6-8 ͑ϳ10 Ϫ11 esu compared to a nonresonant value of 5ϫ10 Ϫ10 esu for a polydiacetylene polymer, 9 for example͒ and strong optical limiting behavior. [10][11][12] We report here the first nonlinear optical measurements of an endohedral metallofullerene and find a dramatic enhancement in the third-order nonlinear optical response. Degenerate four-wave mixing ͑DFWM͒ experiments on solutions of the endohedral metallofullerene Er 2 @C 82 ͑Fig.…”
Copyright by the AIP Publishing. Heflin, JR; Marciu, D; Figura, C; et al., "Enhanced nonlinear optical response of an endohedral metallofullerene through metal-to-cage charge transfer," Appl. Phys. Lett. 72, 2788Lett. 72, (1998; http:// dx
“…Meanwhile, nonlinear optical studies of empty-cage C 60 and C 70 have shown that these materials possess both large third order susceptibilities (3) (Ϫ 4 ; 1 , 2 , 3 ) 6-8 ͑ϳ10 Ϫ11 esu compared to a nonresonant value of 5ϫ10 Ϫ10 esu for a polydiacetylene polymer, 9 for example͒ and strong optical limiting behavior. [10][11][12] We report here the first nonlinear optical measurements of an endohedral metallofullerene and find a dramatic enhancement in the third-order nonlinear optical response. Degenerate four-wave mixing ͑DFWM͒ experiments on solutions of the endohedral metallofullerene Er 2 @C 82 ͑Fig.…”
Copyright by the AIP Publishing. Heflin, JR; Marciu, D; Figura, C; et al., "Enhanced nonlinear optical response of an endohedral metallofullerene through metal-to-cage charge transfer," Appl. Phys. Lett. 72, 2788Lett. 72, (1998; http:// dx
“…For studying the T\ -* T n spectrum, the intersystem crossing (discussed above) is used to populate the Ti level. The T\ -* T n absorption has been reported to be stronger than the S o -• S n absorption, and this could provide a mechanism 178 to account for the observed nonlinear absorption leading to "optical limiting" of transmitted, transient, visible light in both C 6 o and C 70 (7 ns pulses at 532 nm) (see Sec. XV).…”
A review of the structure and properties of fullerenes is presented. Emphasis is given to their behavior as molecular solids. The structure and property modifications produced by alkali-metal doping are summarized, including modification to the electronic structure, lattice modes, transport, and optical properties. Particular emphasis is given to the alkali-metal-doped fullerenes because of their importance as superconductors. A review of the structure and properties of fullerene-based graphene tubules is also given, including a model for their one-dimensional electronic band structure. Potential applications for fullerene-based materials are suggested.
“…Materials with third-order optical nonlinearities have been investigated widely for their applications in opto-electronic and all-optical devices such as eye and sensor protection, optical phase conjugation, high-speed all optical switches, optical bistability, optical limiting devices, optical modulators and so on [47][48][49] . Organic materials exhibiting strong nonlinear optical properties have attracted considerable interest in recent years because of their possible applications in nonlinear optical devices [50][51] .…”
Solvent-free synthesis of isobenzofuran-1(3H)-ones have been described via reaction of phthalaldehydic acid (2-carboxybenzaldehyde) with methylaryl or cyclic ketones using sulfuric acid immobilized on silica (H 2 SO 4 -SiO 2 ) in excellent yields (70-88%). The catalyst can be recovered by simple filtration and reused. Also, some of these compounds has been studied the third-order nonlinear optical properties by laser Gaussian z-scan techniques.
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