• 제목/요약/키워드: intercalation

검색결과 388건 처리시간 0.029초

BDMI+ 양이온을 함유한 이온성 액체로부터 흑연으로의 전기화학적 리튬 삽입 (Electrochemical Lithium Intercalation within Graphite from Ionic Liquids containing BDMI+ Cation)

  • 이유신;정순기;이헌영;김지수
    • 전기화학회지
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    • 제13권3호
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    • pp.186-192
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    • 2010
  • 흑연과 1-buthyl-2,3-dimethylimidazolium(BDMI)계 이온성 액체의 계면 반응을 이해하기 위하여 lithium bis(fluorosulfonyl)imide(LiTFSI)가 용해된 BDMI-TFSI 용액 중에서 전기화학 원자간력 현미경(electrochemical atomic force microscopy, ECAFM)을 이용하여 순환 전압전류법 전후에 있어서의 고배향성 열분해 흑연(highly oriented pyrolytic graphite, HOPG)의 표면을 in-situ로 관찰하였다. HOPG 전극에서 리튬의 가역적인 삽입과 탈리반응은 진행되지 않았으며, $BDMI^+$ 양이온의 삽입에 의한 blister의 형성 및 그라펜 층의 파괴만이 관찰되었다. 한편, $BDMI^+$ 양이온의 삽입 반응은 농도가 4.90 mol/kg인 LiTFSI-propylene carbonate(PC)를 15 wt% 함유하고 있는 BDMI-TFSI계에서는 일어나지 않았으며, 이 경우에는 가역적인 리튬의 삽입과 탈리반응이 진행 되었다. ECAFM 결과는 고농도의 PC계 용액이 solid electrolyte interface(SEI)를 형성함으로 인해 $BDMI^+$ 양이온의 삽입을 막는 매우 효과적인 첨가제임을 나타내었다.

리튬-탄소층간화합물의 Deintercalation에 따른 구조변이와 전기적 성질과의 관계(I) : Li-GFDICs와 Li-PCDICs의 생성에 대하여 (The relation of structural transition and electrical property by deintercalation of Li-Carbon intercalation compounds (I) : For the formation of Li-GFDICs and Li-PCDICs)

  • 오원춘;백대진;고영신
    • 분석과학
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    • 제8권2호
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    • pp.131-138
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    • 1995
  • 가온 가압법으로 합성한 리튬-흑연섬유간화합물(Li-Graphite Fiber Intercalation Compounds, Li-GFICs)과 리튬-석유코크스층간화합물(Li-Petroleum Cokes Intercalation Compounds, Li-PCICs)을 공기 순환에 의하여 자발적으로 deintercalation시키고, 이 deintercalation의 분해 과정으로 나타나는 Li-GFDICs와 Li-PCICs의 구조를 전기적 성질에 미치는 영향에 대하여 논의하였다. 이에 대한 분석은 X-선 회절과 전기 비저항 측정에 의해 수행되었다. X-선 회절 분석에 의하면 Li-GFDICs의 경우 주로 2 stage가 형성되었고 Li-PCICs의 경우에는 1 stage와 2 stage가 주된 회절선으로 나타났다. 또한 deintercalatlon 반응 결과에 의하면 Li-GFDICs의 경우 5주 이후에, Li-GFDICs의 경우 3주 후에 deintercalation 반응이 각각 멈췄다. 전기 비저항 측정 결과에 의하면 Li-GFDICs의 경우 3주까지는 거의 변화가 없었고 그 후 완만한 상승곡선을 나타내었으며, Li-PCDICs의 경우에는 3주를 정점으로 하향곡선을 나타내었다. 따라서 본 연구결과에 의하면 기질로 사용된 흑연섬유와 석유 코크스의 경우 리튬의 원활한 intercalation-deintercalation 작용이 잘 이루어지므로 두 물질 모두 전지의 양극재로 사용될 수 있을 것으로 기대되어진다.

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Exfoliation of Dion-Jacobson Layered Perovskite into Macromolecular Nanoplatelet

  • Lee, Won-Jae;Yeo, Hyun Jung;Kim, Do-Yun;Paek, Seung-Min;Kim, Young-Il
    • Bulletin of the Korean Chemical Society
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    • 제34권7호
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    • pp.2041-2043
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    • 2013
  • A layered perovskite of Dion-Jacobson phase, $RbLaTa_2O_7$, was successfully exfoliated into colloidal suspension via successive ion-exchange and intercalation reaction. The pristine perovskite $RbLaTa_2O_7$ was synthesized by conventional solid-state reaction, and then, it was ion-exchanged with hydrochloric acid to obtain a protonic form of perovskite. The resulting proton-exchanged perovskite was reacted with ethylamine to increase interlayer spaces for further intercalation reaction. Finally, the ethylamine-intercalated form was exfoliated into nanosheets via an intercalation of bulky organic cations (tetrabutylammonium). According to X-ray diffraction (XRD) analysis, the TBA-intercalated form showed remarkably increased interlayer spacing (${\Delta}d$ = 1.67 nm) in comparison with that of the pristine material. Transmission electron microscopic image of exfoliated perovskite clearly revealed that the present exfoliated perovskite were composed of very thin layers. This exfoliated perovskite nanosheets could be applicable as building blocks for fabricating functional nanocomposites.

유기화제 구조가 열가소성 나노복합체의 제조에 미치는 영향 (Effects of Organosilicate Structure on Melt Intercalation of Thermoplastic Polymers)

  • 어태식;김성수;송기국;김준경
    • 폴리머
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    • 제24권6호
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    • pp.794-801
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    • 2000
  • Static 용융 삽입에 의하여 열가소성 고분자의 나노복합체를 제조할 때 유기화 점토에 치환된 유기화제의 길이와 packing 밀도, 그리고 열처리 온도와 시간 등이 고분자의 점토 층간 삽입에 미치는 영향에 대하여 x-ray와 FTIR spectroscopy를 이용하여 조사하였다. 초기 유기화제의 배열형태가 lateral monolayer일 때는 고분자들의 용융 삽입이 일어나지 않았으며 그 외의 경우 유기화제의 종류 및 구조 등에 따라 최종 점토 층간 간격은 큰 변화를 보이지 않았다. 열처리 시간에 따라서 층간 간격은 증가하며 더욱 규칙적으로 변하는 것을 알 수 있었고, 온도가 증가함에 따라서는 점토 층간 간격은 증가하지만 불규칙적으로 배열이 되어가는 것을 관찰하였다.

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Lithium intercalation into a plasma-enhanced-chemical-vapour-deposited carbon film electrode

  • Pyun Su-II
    • 전기화학회지
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    • 제2권1호
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    • pp.38-45
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    • 1999
  • Electrochemical lithium intercalation into a PECVD (plasma enhanced chemical vapour deposited) carbon film electrode was investigated in 1 M $LiPF_6-EC$ (ethylene carbonate) and DEC (diethyl carbonate) solution during lithium intercalation and deintercalation, by using cyclic voltammetry supplemented with ac-impedance spectroscopy. The size of the graphitic crystallite in the a- and c-axis directions obtained from the carbon film electrode was much smaller than those of the graphite one, indicating less-developed crystalline structure with hydrogen bonded to carbon, from the results of AES (Auger electron spectroscopy), powder XRD (X-ray diffraction) method, and FTIR(Fourier transform infra-red) spectroscopy. It was shown from the cyclic voltammograms and ac-impedance spectra of carbon film electrode that a threshold overpotential was needed to overcome an activation barrier to entrance of lithium into the carbon film electrode, such as the poor crystalline structure of the carbon film electrode showing disordered carbon and the presence of residual hydrogen in its structure. The experimental results were discussed in terms of the effect of host carbon structure on the lithium intercalation capability.

A Study on the Initial Irreversible Capacity of Lithium Intercalation Using Gradually Increasing State of Charge

  • Doh, Chil-Hoon;Jin, Bong-Soo;Park, Chul-Wan;Moon, Seong-In;Yun, Mun-Soo
    • KIEE International Transactions on Electrophysics and Applications
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    • 제3C권5호
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    • pp.189-193
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    • 2003
  • Initial irreversible capacity (IIC) can be defined by means of the initial intercalation Ah efficiency (IIE) and the initial irreversible specific capacity at the surface (IICs) with the linear-fit range of the intercalation so as to precisely express the irreversibility of an electrode-electrolyte system. Their relationship was IIC = Qc - Q$_{D}$ = (IIE$^{-1}$ - 1) Q$_{D}$ + IICs in the linear-fit range of IIE. Here, Qc and Qd signify charge and discharge capacity, respectively, based on a complete lithium ion battery cell. Charge indicates lithium insertion to carbon anode. Two terms of IIE and IICs depended on the types of active materials and compositions of the electrode and electrolyte but did not change with charging state. In an ideal electrode-electrolyte system, IIE and IICs would be 100%, 0 mAh/g for the electrode and mAh for the cell, respectively. These properties can be easily obtained by the Gradual Increasing of State of Charge (GISOC).OC).

Direction of Intercalation of a bis-Ru(II) Complex to DNA Probed by a Minor Groove Binding Molecule 4',6-Diamidino-2-phenylindole

  • Jang, Yoon Jung;Kim, Raeyeong;Chitrapriya, Nataraj;Han, Sung Wook;Kim, Seog K.;Bae, Inho
    • Bulletin of the Korean Chemical Society
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    • 제34권10호
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    • pp.2895-2899
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    • 2013
  • Direction of intercalation to DNA of the planar dipyrido[3,2-a:2',3'-c]phenazine ligands (dppz) of a bis-Ru(II) complex namely, $[Ru(1,10-phenanthroline)_2dipyrido[3,2-a:2^{\prime},3^{\prime}-c]phenazine]^{2+}$ linkered by a 1,3-bis(4-pyridyl)propane, was investigated by probing the behavior of 4',6-diamidino-2-phenylindole (DAPI) that bound deep in the minor groove. Bis-intercalation of DPPZ resulted in a little blue shift and hyperchromism in DAPI absorption band, and a large decrease in DAPI fluorescence intensity which accompined by an increase in the dppz emission intensity. Diminishing the intenisty of the positive induced circular dichroism (CD) and linear dichroism (LD) were also observed. These spectral changes indicated that insertion of dppz ligand caused the change of the binding mode of DAPI, which probably moved to the exterior of DNA from the minor groove and interacted with the phospghate groups of DNA by electrostatic interaction. At the surface of DNA, DAPI binds at the phosphate groups of DNA by electrostatic attraction. Consequently, this observation indicated that the dppz ligand intercalated from the minor groove.

Cycling Behavior of Binder-Free Graphite-Lithium Intercalation Anode In AICI3-EMIC-LiCI-SOCI2 Room-Temperature Molten Salt

  • Koura, Nobuyuki;Minami, Takuto;Etoh, Keiko;Idemoto, Yasushi;Matsumoto, Futoshi
    • 전기화학회지
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    • 제5권4호
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    • pp.178-182
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    • 2002
  • The electrochemical behavior of binder-free carbon anode, comprising of only artificial and natural graphite (AG and NG) particles, for intercalation and deintercalation of lithium ion $(Li^+)$ in aluminum chloride (AICI_3)-I-ethyl­3-methylimidazolium chloride (EMIC)-lithium chloride (LiCl)-thionyl chloride $(SOCI_2)$ room-temperature molten salt (RTMS) was studied. Binder-free carbon electrodes were fabricated using electrophoretic deposition (EPD) method. The binder-free carbon anodes provided a relatively flat charge and discharge potentials $(0\;to\;0.2V\;vs.\;Li/Li^+)$ and current capabilities $(250-340mAh{\cdot}g^{-1})$ for the intercalation and deintercalation of $Li^+$. Stability of the binder-free carbon anodes for intercalation and deintercalation of 50 cycles was confirmed.

Electronic structure of the Au intercalated monolayer graphene on Ni(111)

  • Hwang, H.N.;Jee, H.G.;Han, J.H.;Tai, W.S.;Kim, Y.D.;Hwang, C.C.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2009년도 제38회 동계학술대회 초록집
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    • pp.342-342
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    • 2010
  • We have investigated an Au intercalated monolayer graphene on Ni(111) using angle-resolved photoemission spectroscopy (ARPES), high resolution photoemission spectroscopy (HRPES), and low energy electron diffraction (LEED) at the 3A2 ARUPS beamline in Pohang Accelerator Laboratory. We find the monolayer graphene is well grown on the Ni(111) surface by the adsorption of acetylene. However, the graphene does not show the characteristic $\pi$ band near the Fermi level due to its strong interaction with the underlying substrate. When Au is adsorbed on the surface and then annealed at high temperature, we observe that Au is intercalated underneath the monolayer graphene. The process of the Au intercalation was monitored by HRPES of corresponding Au 4f and C 1s core levels as well as the electronic structure of the $\sigma$, $\pi$ states at $\Gamma$, K points. The $\sigma$, $\pi$ bands of graphene shift towards the Fermi level and the $\pi$ band is clearly observed at K point after the intercalation of full monolayer Au. The full width at half maximum (FWHM) of the C 1s peak narrows to approximately 0.42 eV after intercalation. These results imply that the interaction between the graphene and substrate is considerably weakened after the Au intercalation. We will discuss the graphene is really closer to ideal free standing graphene suggested recently.

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