Li local environments and the dynamics in the Li1+xV3O8 insertion electrode

The structural and electronic properties of the Li1+xV3O8 insertion electrode system with nominal range of have been explored through measurements of x-ray diffraction, magnetization and nuclear magnetic resonance (NMR) for 7Li. The system prepared electrochemically exhibits two kinds of phase depen...

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Veröffentlicht in:Journal of physics. Condensed matter 2005-07, Vol.17 (26), p.4057-4071
Hauptverfasser: Onoda, Masashige, Miyasaka, Shintaro, Mutoh, Tomohiro, Nichogi, Katsuhiro
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container_issue 26
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container_title Journal of physics. Condensed matter
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creator Onoda, Masashige
Miyasaka, Shintaro
Mutoh, Tomohiro
Nichogi, Katsuhiro
description The structural and electronic properties of the Li1+xV3O8 insertion electrode system with nominal range of have been explored through measurements of x-ray diffraction, magnetization and nuclear magnetic resonance (NMR) for 7Li. The system prepared electrochemically exhibits two kinds of phase depending on the composition: the gamma1-phase with has the octahedral (Li1) and tetrahedral (Li2) coordinations for the Li sites, and the gamma2-phase with has the octahedral coordination alone. These phases coexist for 1.5 < x < 3.5. Application of the one-dimensional chain model to the susceptibility data for the gamma2-phase provides reasonable results for the Li concentration and the exchange constant. For x = 0, the quadrupole parameters are determined precisely. Both the gamma1-phase and the gamma2-phase indicate the activation energies for the long-range motion of Li ions to be of 3 X 103 K at temperatures above 300 K, and the gamma2-phase has another narrowing process below 100 K. Magic-angle spinning (MAS) NMR spectra for the gamma1-phase reflect the site differentiation for Li; the Li1 shift originates from a negative spin transfer, while the effect for Li2 is less significant. The spin-lattice relaxation for x = 0 is explained with the quadrupole interaction mechanism. For Li1.25V3O8, which exhibits variable-range hopping-type transport anomalies at K, the phase transition for the Li local environments takes place at around Tc. The spectra for the gamma2-phase are different from those for the gamma1-phase, and the complicated relaxations likely originating from Li ions located in the cathode and the acetylene black, and the boundary between these substances, are observed.
doi_str_mv 10.1088/0953-8984/17/26/006
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The system prepared electrochemically exhibits two kinds of phase depending on the composition: the gamma1-phase with has the octahedral (Li1) and tetrahedral (Li2) coordinations for the Li sites, and the gamma2-phase with has the octahedral coordination alone. These phases coexist for 1.5 &lt; x &lt; 3.5. Application of the one-dimensional chain model to the susceptibility data for the gamma2-phase provides reasonable results for the Li concentration and the exchange constant. For x = 0, the quadrupole parameters are determined precisely. Both the gamma1-phase and the gamma2-phase indicate the activation energies for the long-range motion of Li ions to be of 3 X 103 K at temperatures above 300 K, and the gamma2-phase has another narrowing process below 100 K. Magic-angle spinning (MAS) NMR spectra for the gamma1-phase reflect the site differentiation for Li; the Li1 shift originates from a negative spin transfer, while the effect for Li2 is less significant. The spin-lattice relaxation for x = 0 is explained with the quadrupole interaction mechanism. For Li1.25V3O8, which exhibits variable-range hopping-type transport anomalies at K, the phase transition for the Li local environments takes place at around Tc. 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Both the gamma1-phase and the gamma2-phase indicate the activation energies for the long-range motion of Li ions to be of 3 X 103 K at temperatures above 300 K, and the gamma2-phase has another narrowing process below 100 K. Magic-angle spinning (MAS) NMR spectra for the gamma1-phase reflect the site differentiation for Li; the Li1 shift originates from a negative spin transfer, while the effect for Li2 is less significant. The spin-lattice relaxation for x = 0 is explained with the quadrupole interaction mechanism. For Li1.25V3O8, which exhibits variable-range hopping-type transport anomalies at K, the phase transition for the Li local environments takes place at around Tc. 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The spin-lattice relaxation for x = 0 is explained with the quadrupole interaction mechanism. For Li1.25V3O8, which exhibits variable-range hopping-type transport anomalies at K, the phase transition for the Li local environments takes place at around Tc. The spectra for the gamma2-phase are different from those for the gamma1-phase, and the complicated relaxations likely originating from Li ions located in the cathode and the acetylene black, and the boundary between these substances, are observed.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/0953-8984/17/26/006</doi><tpages>15</tpages></addata></record>
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subjects Condensed matter: electronic structure, electrical, magnetic, and optical properties
Condensed matter: structure, mechanical and thermal properties
Diffusion in solids
Exact sciences and technology
Magnetic resonances and relaxations in condensed matter, mössbauer effect
Nuclear magnetic resonance and relaxation
Physics
Self-diffusion and ionic conduction in nonmetals
Transport properties of condensed matter (nonelectronic)
title Li local environments and the dynamics in the Li1+xV3O8 insertion electrode
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