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    ๆœ้ฎฎๅˆๆœŸ้›ฒๅฑฑๅœ–์˜ ็•ซ้ขจ

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    ๆœ้ฎฎๅˆๆœŸ้›ฒๅฑฑๅœ–๏ผˆ้‘ๅฑฑ็™ฝ้›ฒๅœ–๏ผ‰๋Š” ์ฃผ๋กœ ๅฎ‹ไปฃ็ฑณๆฐ์˜ ้›ฒๆž—์— ๅทจๅฑฑ์„ ๆŠ˜่กทํ•œ ๅ…ƒไปฃ้ซ˜ๅ…‹ๆญ์˜ ใ€ˆ้›ฒๆฉซ็ง€ๅถบๅœ–ใ€‰์™€ ๊ฐ™์€ ๆฑŸๅ—็ณป้›ฒๅฑฑๅœ–์˜ ์˜ํ–ฅ์„ ์ค‘์‹ฌ์œผ๋กœ์—ฐ๊ตฌ๋˜์–ด ์™”๋‹ค๏ผŽ๊ทธ๋Ÿฌ๋‚˜ ํ•œํŽธ์œผ๋กœ ๅ…ƒๆœซ์— ๊ทธ๋ ค์ง„ ๆ–นๅพž็พฉ์˜ ใ€ˆ้›ฒๅฑฑๅœ–ๅทใ€‰๊ณผ ๊ฐ™์€ ่ฏๅŒ—็ณป์˜ ์ž‘ํ’ˆ๋„ ้›ฒๅฑฑๅœ–๋ผ๊ณ  ๋ถˆ๋ฆฌ๋Š”๋ฐ๏ผŒๆœฌ็จฟ์—์„œ๋Š” ์–‘์‹์— ๊ด€๊ณ„์—†์ด ์ด์ž‘ํ’ˆ๋“ค์ด ้›ฒๅฑฑ์ด๋ผ ๋ถˆ๋ฆฌ๋Š” ์ด์œ ๊ฐ€ ็ฑณๆฐ์˜ ้›ฒๆž—์ด๋ผ๋Š” ๋ชจํ‹ฐํ”„๋ฅผ ๅ…ฑๆœ‰ํ•˜๊ธฐ ๋•Œ๋ฌธ์ด๋ผ ๋ณด์•˜๊ณ  ๆœ้ฎฎๅˆๆœŸ์—๋„ ็ฑณๆฐ์˜ ้›ฒๆž—์„ ๆŠ˜่กทํ•œ ๋‹ค์–‘ํ•œ ็•ซ้ขจ์˜ ้›ฒๅฑฑๅœ–๊ฐ€๊ทธ๋ ค์กŒ๋‹ค๋Š” ๊ฒƒ์— ๋Œ€ํ•ด ่€ƒๅฏŸํ–ˆ๋‹ค๏ผŽๅคงๅ’Œๆ–‡่ฏ้คจ ์†Œ์žฅ ใ€ˆ้›ฒๅฑฑๅœ–ใ€‰ 6์ ์€ ้ซ˜ๅ…‹ๆญ็ณป์˜ ๊ตฌ๋„๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ ํ•˜๋ฉด์„œ๋„้ข็š„์ธ ํ‘œํ˜„์— ์ค‘์ ์„ ๋‘” ้ซ˜ๅ…‹ๆญ์˜ ใ€ˆ้›ฒๆฉซ็ง€ๅถบๅœ–ใ€‰์— ๋น„ํ•ด ็ทš็š„์ธ ๆจ“้–ฃ์ด๋‚˜ๆจนๆžๆณ•์ด ๋”ํ•ด์ ธ ์žˆ๋Š” ์ ์—์„œ ๅ…ƒๆœซ้›ฒๅฑฑๅœ–์˜ ๅฝฑ้Ÿฟ์ด ๋‘๋“œ๋Ÿฌ์ง€๋ฉฐ ๅฑฑๅฎน่กจ็พ์—๋Š” ๅ…ƒๆœซ็››ๆ‡‹์˜ ๊ฐ„๋žตํ™”ํ•œ ๆŠซ้บป็šด๊ณผ ่ƒกๆค’้ปž๏ผŒ๊ทธ๋ฆฌ๊ณ  ๅ…ƒๆœซ์˜ ๅ‰ๆต™ๆดพ็š„์ธ ็•ซ้ขจ ๋“ฑ์„ ๆŠ˜่กทํ•ด์„œ ์žฌํ•ด์„ํ•œ ์ž‘ํ’ˆ์ด๋ผ ๋ณด์•˜๋‹ค๏ผŽๅ—็ฆชๅฏบ ์†Œ์žฅ ๅ‚ณ้ซ˜็„ถๆš‰็ญ†ใ€ˆ ้›ฒๅฑฑๅœ–ใ€‰์™€ใ€ˆ ้›ชๅฑฑๅœ–ใ€‰๋Š” ๊ทธ ๅฑฑๅ‹ข ํ‘œํ˜„์ด ๅ…ƒไบบ็ญ†ใ€ˆ้‘ๅฑฑ็™ฝ้›ฒๅœ–ใ€‰๏ผˆๅฐๅŒ—ๆ•…ๅฎฎๅš็‰ฉ้™ข๏ผ‰์— ๋ณด์ด๋Š” ๅ…ƒๆœซ์˜ ๅ‰ๆต™ๆดพ็š„์ธ ๊ฑฐ์นœ ็ญ†่‡ด์™€์œ ์‚ฌํ•˜๋ฉฐ๏ผŒใ€ˆ้›ฒๅฑฑๅœ–ใ€‰์˜ ๋†’์ด ์†Ÿ์€ ๅทจๅฑฑ๊ณผ ้›ฒๆž—์˜ ์กฐํ•ฉ ๋“ฑ์œผ๋กœ ๋ณผ ๋•Œ ๅ…ƒๆœซ้›ฒๅฑฑๅœ–์˜ ์˜ํ–ฅ์„ ๋ฐ›์€ ๊ฒƒ์œผ๋กœ ๋ณด์ธ๋‹ค๏ผŽ๊ทธ๋ฆฌ๊ณ  ๆœ้ฎฎๅˆๆœŸ์—๋Š” ๊ณ„์ ˆ์˜ ๋ณ€ํ™”๋ฅผ ๋‹ด์€ ๅฑฑๆฐด็•ซ๊ฐ€ ์œ ํ–‰ํ•˜๋Š”๋ฐ๏ผŒํŠนํžˆ 15์„ธ๊ธฐ ํ›„๋ฐ˜์˜ ๆˆๅฎ—ๆœŸ์— ้›ฒๅฑฑๅœ–์™€ ้›ชๅฑฑๅœ–๋ฅผํ•จ๊ป˜ ๊ฐ์ƒํ–ˆ๋‹ค๋Š” ๊ธฐ๋ก์ด ์ž์ฃผ ๋ณด์ด๋Š” ์ ๊ณผ ๋‘ ์ž‘ํ’ˆ์ด ๆœ้ฎฎๅˆๆœŸๅฑฑๆฐด็•ซ์— ํ”ํžˆ ๋ณด์ด๋Š” ๅฐ็จฑๆง‹ๅœ–๋ฅผ ์ทจํ•œ ์ ์—์„œ ๅ‰ๆต™ๆดพๅฑฑๆฐด์˜ ์˜ํ–ฅ์„ ๋ฐ›์€ 15์„ธ๊ธฐ ํ›„๋ฐ˜์˜ ๆœ้ฎฎๅˆๆœŸ์ž‘ํ’ˆ์œผ๋กœ ๋ณด์•˜๋‹ค๏ผŽไนๅทžๅœ‹็ซ‹ๅš็‰ฉ้คจ ์†Œ์žฅใ€ˆ ็€Ÿๆน˜ๅ…ซๆ™ฏๅœ–ใ€‰์˜ ็…™ๅฏบๆšฎ้˜์€ ๆฑŸๅ—ๅฑฑๆฐด๋กœ ๋ถ„๋ฅ˜๋˜๋Š”้ซ˜ๅ…‹ๆญ็ณป์˜ ํ™”ํ’์„ ๊ณ„์Šนํ•˜๊ณ  ์žˆ์œผ๋‚˜ ็ดฐ้ƒจๆๅฏซ์—๋Š” 15์„ธ๊ธฐ ํ›„๋ฐ˜๋ถ€ํ„ฐ ๋ณด์ด๋Š”ๆœ้ฎฎๅˆๆœŸ ํŠน์œ ์˜ ็Ÿญ็ทš้ปž็šด์˜ ๅˆๆœŸ็š„์ธ ํŠน์ง•์ด ๋ณด์ธ๋‹ค๏ผŽ๊ทธ๋ฆฌ๊ณ  ์ด๋Š” ๅ…ซๆ™ฏ ์ค‘์˜ ่ฏๅŒ—ๅฑฑๆฐด์˜ ์˜ํ–ฅ์ด ๋‘๋“œ๋Ÿฌ์ง„ ์ž‘ํ’ˆ์—์„œ๋„ ์‚ฌ์šฉ๋˜๋Š”๋ฐ ์ด๋Ÿฌํ•œ ์ ์—์„œ ็Ÿญ็ทš้ปž็šด์€ ่ฏๅŒ—็ณป๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๆฑŸๅ—็ณปๅฑฑๆฐด์—๋„ ์“ฐ์˜€๋‹ค๋Š” ๊ฒƒ์„ ์•Œ ์ˆ˜ ์žˆ๋‹ค๏ผŽ๋˜ํ•œ์ด ๊ทธ๋ฆผ์€ ็…™ๅฏบๆšฎ้˜์˜ ์ฃผ์š”ํ•œ ๋ชจํ‹ฐํ”„์ธ ๆจ“้–ฃ์ด๋‚˜ ๅƒงไพถ ๋“ฑ์˜ ็ทš็š„์ธ ํ‘œํ˜„์ด๊ฑฐ์˜ ๋ณด์ด์ง€ ์•Š๋Š” ๊ฒƒ์ด ํŠน์ด์ ์ธ๋ฐ๏ผŒ์ด๊ฒƒ์€ ๅ…ƒๆœซ์˜ ้›ฒๅฑฑๅœ–๋ณด๋‹ค๋Š” ๅคๅผ์ธ ้ซ˜ๅ…‹ๆญ์˜ใ€ˆ ้›ฒๆฉซ็ง€ๅถบๅœ–ใ€‰์— ๊ฐ€๊นŒ์šฐ๋ฉฐ๏ผŒ๊ทธ๋ฆฌ๊ณ  ์—ฌ๊ธฐ์— ๆฑŸๅ—ๅฑฑๆฐด์˜ ๅปฃ้—Šํ•œ ๆฐด้ข่กจ็พ์ด ๆŠ˜่กท๋˜์–ด ์žˆ๋Š” ้›ฒๅฑฑๅœ–๋กœ ์ดํ•ด๋œ๋‹ค๏ผŽไนๅทžๅœ‹็ซ‹ๅš็‰ฉ้คจ ์†Œ์žฅใ€ˆ ็€Ÿๆน˜ๅ…ซๆ™ฏๅœ–ใ€‰์˜ ๆดžๅบญ็ง‹ๆœˆ์€ ่ฏๅŒ—็ณป์˜ ๅฑฑๅฎน์— ๆฑŸๅ—็ณป์˜ ๋“œ๋„“์€ ๆฐด้ข๏ผŒ๊ฑฐ๊ธฐ์— ้›ฒๆž—๊ณผ ๅฑ‹่ˆ ๋“ฑ ้›ฒๅฑฑ์˜ ๋ชจํ‹ฐํ”„๋ฅผ ๆŠ˜่กทํ•œ ์ž‘ํ’ˆ์ธ๋ฐๅ…ƒๆœซ ๅผต็พฝ์˜โ€œ ๅ”ๅญ่ฏ้›ฒๅฑฑๆญŒโ€ ๋“ฑ์—์„œ ์ด๋Ÿฌํ•œ ๆŠ˜่กท็•ซ้ขจ์„ ์Š๊ณ  ์žˆ๊ณ ๏ผŒๆ–นๅพž็พฉ์˜ใ€ˆ ้›ฒๅฑฑๅœ–ๅทใ€‰์ด ์ด๋Ÿฌํ•œ ๆŠ˜่กทๆจฃๅผ์„ ๋ณด์ด๋Š” ์ ์—์„œ ๆœ้ฎฎๅˆๆœŸ์—๋„ ์ด๋Ÿฌํ•œ ์ž‘ํ’ˆ์ด ้›ฒๅฑฑๅœ–๋ผ ๋ถˆ๋ ธ์„ ๊ฐ€๋Šฅ์„ฑ์ด ๋†’๋‹ค๋Š” ๊ฒƒ์„ ๋…ผํ–ˆ๋‹ค๏ผŽๅ‚ณ็Ž‰ๆพ—็ญ†ใ€ˆ ้›ฒๅฑฑๅœ–ใ€‰๋Š” ็Ž‰ๆพ—์˜ ์ž‘ํ’ˆ์œผ๋กœ ์ „ํ•˜๋˜ ๊ฒƒ์ด๋‚˜ ่ฟ‘ๅนด์— ๆœ้ฎฎๆ™‚ไปฃ์˜์ž‘ํ’ˆ์œผ๋กœ ์ˆ˜์ •๋˜์—ˆ์œผ๋ฉฐ ๆœฌ็จฟ์—์„œ๋Š” ๅฑฑ็จœ์˜ ้ปžๆ๋‚˜ ๅฑฑ้ข์˜ ็ทšๆ ๋“ฑ์ด ็Ÿญ็ทš้ปž็šด์˜ ์ดˆ๊ธฐ์ ์ธ ํŠน์ง•์ด ๋ณด์—ฌ ์กฐ์„ ์‹œ๋Œ€์˜ 15์„ธ๊ธฐ๋ง๊ฒฝ์˜ ์ž‘ํ’ˆ์ด๋ผ ๋ณด์•˜๋‹ค๏ผŽ์ด์ƒ๊ณผ ๊ฐ™์ด ๆœ้ฎฎๅˆๆœŸ้›ฒๅฑฑๅœ–๋Š” ๋‹ค์–‘ํ•œ ํ™”ํ’์˜ ์ ˆ์ถฉ์ ์ธ ๊ฒฝํ–ฅ์ด ๋ณด์ธ๋‹ค๏ผŽ์ด๋Ÿฌํ•œ ๊ฒฝํ–ฅ์€ ๅ…ƒไปฃๅพฉๅคไธป็พฉ์— ์˜ํ•ด ํƒ„์ƒํ•œ ๆŠ˜่กท็•ซ้ขจ์ธ ้ซ˜ๅ…‹ๆญ็ณป้›ฒๅฑฑ์—์„œ ๋น„๋กฏํ•œ ๊ฒƒ์œผ๋กœ ๊ทธ ๆ€ๆฝฎ๊ฐ€ ๆœ้ฎฎๅˆๆœŸ็•ซๅฃ‡์—๋„ ์˜ํ–ฅ์„ ์ฃผ์–ด ๋‹ค์–‘ํ•˜๊ฒŒ ๆŠ˜่กท๋˜๊ณ  ์žฌํ•ด์„๋œ ๆœ้ฎฎๅˆๆœŸ ํŠน์œ ์˜ ้›ฒๅฑฑๅœ–๊ฐ€ ๊ทธ๋ ค์ง€๊ฒŒ ๋œ ๊ฒƒ์ด๋‹ค

    ๆœ้ฎฎๅˆๆœŸ้›ฒๅฑฑๅ›ณใฎๅ›ณๆง˜

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    Moving to the diversification of the Gabonese economy

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    Factors Affecting the Exfoliation of Graphite Intercalation Compounds for Graphene Synthesis

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    We investigate the mechanism of the intercalation-aided exfoliation of graphite using van der Waals force-corrected density functional theory (DFT) calculations. From a comparative study on various intercalation systems, we find that, depending on the intercalant species, the exfoliation energies vary significantly, not only due to the size of intercalants but also due to interactions with the host graphite. While it is generally perceived that an expanded interlayer distance with intercalants weakens the binding between graphene layers, as the van der Waals forces decrease, the calculations reveal that the intercalation of electronegative or electropositive intercalants (e.g., Li, K, F, Cl, and Br) result in a 1.5-5-fold higher exfoliation energy than pristine graphite due to additional binding forces from charge transfer between intercalants and graphene layers. Furthermore, we demonstrate that this additional binding force could be manipulated with cointercalation or neutral intercalants, which hints at effective exfoliation strategies with graphite intercalation compounds. This theoretical study broadens our understanding of the mechanism underlying graphite exfoliation and will facilitate development of more effective exfoliation strategies for other related layered materials

    Extremely large, non-oxidized graphene flakes based on spontaneous solvent insertion into graphite intercalation compounds

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    Demand for an effective strategy for exfoliating layered materials into flakes without perturbing their intrinsic structure is growing. Herein, we introduce an effective fabrication method of large-sized non-oxidized graphene flakes (NOGFs) as a representative example of a general strategy using spontaneous insertion of exfoliating medium into a layered material. We fabricated a ternary graphite intercalation compound (t-GIC) with stoichiometry of KC24(THF)(2), and analyzed its morphology and electronic structure through experimental and computational approach. Interactions between the t-GIC and aprotic organic solvents with different polarities were investigated, where a unique swelling behavior was observed with dimethyl sulfoxide (DMSO). Based on the analysis of the phenomena, we demonstrate facile exfoliation of the t-GIC in polyvinyl pyrrolidone (PVP)-DMSO solution for fabrication of highly crystalline and large-sized NOGFs. The lateral size of the NOGFs ranges over 30 mu m, while the 98% having thickness below 10 layers. The NOGF film exhibits supreme electrical conductivity of 3.36 x 10(5) S/m, which is, to our best knowledge, the highest value for a thin conductive film made of graphene flakes. (C) 2018 Elsevier Ltd. All rights reserved.

    Blue Graphene Quantum Dots with High Color Purity by Controlling Subdomain Formation for Light-Emitting Devices

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    As an alternative to Cd-free quantum dots (QDs), graphene quantum dots (GQDs) have potential because of their various advantages, such as color tunability, nontoxicity, cost effectiveness, and photostability. However, realization of a useful blue emission from GQDs requires a narrower full width at half-maximum (FWHM) and color purity in Commission Internationale de l'Eclairage (CIE) coordinates for display applications. These emission characteristics are strongly dependent on precise control of the sp(2) C subdomain, considered as the band-gap origin of GQDs. Here, we report a preparation for blue GQDs with improved color purity obtained from KC24 graphite intercalation compounds. The as-synthesized KC24-GQD exhibits high color purity with a photoluminescence FWHM of 70 nm and CIE coordinates of (0.159, 0.082), which can be attributed to the controlled oxidation of graphene by intercalated K ions with an arrangement of KC24 surrounding seven sp(2) C hexagons favorable for the formation of uniform subdomains. Furthermore, intrinsic emission-dominant fluorescence and phosphorescence from a powdered KC24-GQD-dispersed boron oxynitride matrix, as well as from solution-based KC24-GQD, prove its applicability to various light-emitting devices.

    Molecular-level hybridization of single-walled carbon nanotubes and a copper complex with counterbalanced electrostatic interactions

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    Abstract Hybridization and wet processibility are highly desired development strategies for next-generation nanomaterials. In particular, the hybridization of carbon nanotubes (CNTs) and transition metals has been investigated for decades owing to the numerous advantages, such as high mechanical and electrical properties. However, manufacturing nano-hybridized CNTs/transition metals is complicated, and no studies have been reported on the dispersion and hybridization of transition metals with single-walled CNTs (SWCNTs) without any harsh or destructive methods due to the strong van der Waals forces. Herein, we demonstrate a one-step dispersion/hybridization of SWCNTs and a Cu-based complex and provide a mechanism derives from counterbalancing the electrostatic interactions via molecular-level charge transfer. The Cu-based complex-hybridized SWCNTs self-assemble and demonstrate suitable viscoelastic behaviors for various printing or coating processes. Finally, the nanostructured SWCNTs/Cu nanoparticle exhibits multifunctional electrothermal properties, electromagnetic interference shielding performances, and flexibilities. The proposed metal-complex-hybridized SWCNTs dispersions provide a wet process guideline for producing nanostructured electrodes

    Moisture barrier composites made of non-oxidized graphene flakes

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    Graphene flakes (GFs) with minimized defects and oxidation ratios are incorporated into polyethylene (PE) to enhance the moisture barrier. GFs produced involving solvothermal intercalation show extremely low oxidation rates (3.17%), and are noncovalently functionalized in situ, inducing strong hydrophobicity. The fabricated composite possesses the best moisture barrier performance reported for a polymer-graphene composite. ยฉ 2015 Wile-VCH Verlag GmbH & Co. KGaA.
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