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1.
Journal of Solid State Electrochemistry - We report effectiveness of dopants selected from group 13, such as B, Ga, and In, on the conductivity of Li1.5Al0.5Ge1.5(PO4)3 (LAGP) that is recognized as... 相似文献
2.
A modified sol-gel process was studied as applied to synthesize a lithium-conducting solid electrolyte of composition Li 1.3Al 0.3Ti 1.7(PO 4) 3 (LATP) using water-soluble salts Al(NO 3) 3 · 9H 2O, LiNO 3 · 3H 2O, and (NH 4) 2HPO 4 and a titanium(IV) citrate complex. As-synthesized samples were characterized using X-ray powder diffraction, DSC/TG, SEM, and impedance spectroscopy. Sintering of as-synthesized amorphous powders at 700°C was found to yield LATP with crystallite sizes of 42–48 nm. Ionic conductivity of the electrolyte measured in the frequency range 25–10 6 Hz in disks having 86–90% density that were sintered at 1000°C was (3–4) × 10 ?4 S/cm. Temperature-dependent ionic conductivity was studied in the range 25–200°C. The activation energy of conduction was determined for LATP. 相似文献
3.
Composite polymer electrolyte (CPE) films consisting of PEO, LiClO 4, and Li 1.3Al 0.3Ti 1.7(PO 4) 3 with fixed EO/Li = 8 but different relative compositions of the two lithium salts were prepared by the solution casting method. The CPE films were characterized using SEM, DSC, electrical impedance spectroscopy (EIS), and ion transference number measurement. It was found that the incorporation of LiClO 4 and Li 1.3Al 0.3Ti 1.7(PO 4) 3 into PEO by keeping EO/Li = 8 reduced the crystallinity of PEO from 50.34% to the range of 3.57–15.63% depending upon the relative composition of the two salts. The room temperature impedance spectra of the CPE films all exhibited a shape of depressed semicircle in the high frequency range and inclined line in the low frequency range, but the high temperature ones were mainly inclined lines. The Li + ionic conductivity of the CPE films mildly increased and then decreased with increasing Li 1.3Al 0.3Ti 1.7(PO 4) 3 content, and the maximum conductivities were obtained at Li 1.3Al 0.3Ti 1.7(PO 4) 3 content of 15 wt % for all measuring temperatures, for example, 1.378 × 10 ?3 S/cm at 100 °C and 1.387 × 10 ?5 S/cm at 25 °C. The temperature dependence of the ionic conductivity of the CPE films follows the Vogel–Tamman–Fulcher (VTF) equation The pseudo activation energies (E a) were rather low, 0.053–0.062 eV, indicating an easy migration of Li + in the amorphous phase dominant PEO. The pre‐exponent constant A and ion transference number t Li+ were found to have a similar variation tendency with increasing Li 1.3Al 0.3Ti 1.7(PO 4) 3 content and reached their maximums also at Li 1.3Al 0.3Ti 1.7(PO 4) 3 content of 15 wt %. © 2005 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 43: 743–751, 2005 相似文献
4.
Nano-structured Li 3V 2(PO 4) 3/carbon composite (Li 3V 2(PO 4) 3/C) has been successfully prepared by incorporating the precursor solution into a highly mesoporous carbon with an expanded pore structure. X-ray diffraction analysis, scanning electron microscopy, and transmission electron microscopy were used to characterize the structure of the composites. Li 3V 2(PO 4) 3 had particle sizes of < 50 nm and was well dispersed in the carbon matrix. When cycled within a voltage range of 3 to 4.3 V, a Li 3V 2(PO 4) 3/C composite delivered a reversible capacity of 122 mA h g ? 1 at a 1C rate and maintained a specific discharge capacity of 83 mA h g ? 1 at a 32C rate. These results demonstrate that cathodes made from a nano-structured Li 3V 2(PO 4) 3 and mesoporous carbon composite material have great potential for use in high-power Li-ion batteries. 相似文献
5.
Single-phase LiVPO 4F and LiVPO 4F/Li 3V 2(PO 4) 3 nanostructured composite cathode materials were prepared by heating of the VPO 4?+?LiF mechanochemically activated mixture to 700 °C and subsequent quick or slow cooling to room temperature, respectively. The formation of the composites was proved by a combination of different physico-chemical methods, including XRD, FTIR, 6Li and 31P NMR, SEM, TEM, and HRTEM. It has been shown that in the composites LiVPO 4F and Li 3V 2(PO 4) 3 nanocrystals well inset into each other resulting in the nanodomain composite formation. Charge–discharge curves of the composites have a sloping profile both in the high-voltage (3.0–4.5 V) and in the low-voltage (1.3–2.5 V) ranges, noticeably different from plateaus for a phase-pure LiVPO 4F, thus indicating a probable change of a two-phase regime of lithium intercalation for a single-phase one. Enhanced rate capability of the LiVPO 4F/Li 3V 2(PO 4) 3 composites is associated with their microstructure and high ionic conductivity of Li 3V 2(PO 4) 3. 相似文献
6.
The alluaudite lithiated phases Li(0.5)Na(0.5)MnFe(2)(PO(4))(3) and Li(0.75)Na(0.25)MnFe(2)(PO(4))(3) were prepared via a sol-gel synthesis, leading to powders with spongy characteristics. The Rietveld refinement of the X-ray and neutron diffraction data coupled with ab initio calculations allowed us for the first time to accurately localize the lithium ions in the alluaudite structure. Actually, the lithium ions are localized in the A(1) and A(1)' sites of the tunnel. M?ssbauer measurements showed the presence of some Fe(2+) that decreased with increasing Li content. Neutron diffraction revealed the presence of a partial Mn/Fe exchange between the two transition metal sites that shows clearly that the oxidation state of the element is fixed by the type of occupied site. The electrochemical properties of the two phases were studied as positive electrodes in lithium batteries in the 4.5-1.5 V potential window, but they exhibit smaller electrochemical reversible capacity compared with the non-lithiated NaMnFe(2)(PO(4))(3). The possibility of Na(+)/Li(+) ion deintercalation from (Na,Li)MnFe(2)(PO(4))(3) was also investigated by DFT+U calculations. 相似文献
7.
In view of a known structural phase transition at 800—875 °C and the by 10 times increased luminescence of Mn 2+ in the high‐temperature phase, low‐ (LT) and high‐temperature (HT) polymorphs of CaMn 0.5Zr 1.5(PO 4) 3 are prepared by sol—gel reaction of Mn(O‐Ac) 2, Ca(NO 3) 2, ZrOCl 2, and NH 4H 2PO 4 in ethylene glycol followed by a final annealing (700 or 900 °C, 20 h, resp.). 相似文献
8.
Journal of Solid State Electrochemistry - The free-standing PAN/PVdF/LiClO4/Li0.5La0.5TiO3 nanocomposite solid polymer electrolytes have been prepared by solution casting technique. The thermal... 相似文献
9.
Journal of Solid State Electrochemistry - Aqueous rechargeable lithium-air batteries are candidates for next-generation high energy and power density batteries. The key material of this type... 相似文献
10.
The effect of Al 2O 3 -coating on Li 3V 2(PO 4) 3/C cathode material for lithium-ion batteries has been investigated. The crystalline structure and morphology of the synthesized powders have been characterized by XRD, SEM, and HRTEM, and their electrochemical performances are evaluated by CV, EIS, and galvanostatic charge/discharge tests. It is found that Al 2O 3 -coating modification stabilizes the structure of the cathode material, decreases the polarization of electrode and suppresses the rise of the surface film resistance. Electrochemical tests indicate that cycling performance and rate capability of Al 2O 3-coated Li 3V 2(PO 4) 3/C are enhanced, especially at high rates. The Al 2O 3-coated material delivers discharge capacity of 123.03 mAh g ?1 at 4 C rate, and the capacity retention of 94.15 % is obtained after 5 cycles. The results indicate that Al 2O 3 -coating should be an effective way to improve the comprehensive properties of the cathode materials for lithium-ion batteries. 相似文献
11.
A new zero-dimensional (0D) aluminophosphate monomer [ dl-Co(en) 3] 2[Al(HPO 4) 2(H 1.5PO 4) 2(H 2PO 4) 2](H 3PO 4) 4 (designated AlPO-CJ38) with Al/P ratio of 1/6 has been solvothermally prepared by using racemic cobalt complex dl-Co(en) 3Cl 3 as the template. The Al atom is octahedrally linked to six P atoms via bridging oxygen atoms, forming a unique [Al(HPO 4) 2(H 1.5PO 4) 2(H 2PO 4) 2] 6? monomer. Notably, there exists intramolecular symmetrical O?H?O bonds, which results in pseudo-4-rings stabilized by the strong H-bonding interactions. The structure is also featured by the existence of four different types of monophosphates that have been confirmed by 31P NMR and 1H NMR spectra. The crystal data are as follows: AlPO-CJ38, [ dl-Co(en) 3] 2[Al(HPO 4) 2(H 1.5PO 4) 2(H 2PO 4) 2](H 3PO 4) 4, M = 1476.33, monoclinic, C2/ c (No. 15), a = 36.028(7) Å, b = 8.9877(18) Å, c = 16.006(3) Å, β = 100.68(3)°, U = 5093.2(18) Å 3, Z = 4, R1 = 0.0509 ( I > 2 σ( I)) and wR2 = 0.1074 (all data). CCDC number 689491. 相似文献
12.
The Raman spectra for Sr 3(PO 4) 2 and Ba 3(PO 4) 2 were investigated in the temperature range from 80 to 1623 K at atmospheric pressure. An unexpected melting of each sample was observed around 1573–1583 K in this study. In the temperature range from 80 to 1323 K, the Raman wavenumbers of all observed bands for Sr 3(PO 4) 2 and Ba 3(PO 4) 2 continuously decrease with increasing temperature. A quantitative analysis on the wavenumbers of Raman bands for both samples reveals that the ν3 antisymmetric stretching vibrations show the strongest temperature dependence and the ν2 symmetric bending vibration displays the weakest temperature dependence. The effects of cations on Raman bands are discussed. The reason for the unexpected melting of both samples is mainly attributed to the significant contribution from excess surface energy and the grain-boundary energy that has apparently lowered the melting points of the small samples, i.e., Gibbs–Thomson effect. 相似文献
13.
Na-doped Li 3V 2(PO 4) 3/C (LVP/C) cathode materials are prepared by a sol–gel method. X-ray diffraction results show that the Na ion has been well doped into the crystal structure of LVP/C and does not disturb the extraction–insertion behavior of lithium ion seriously. The initial discharge capacity of the Na-doped LVP/C is 112.2?mA?h g ?1 at 5?C, and the capacity retention reaches 98.3?% over 80 cycles. Cyclic voltammetry and electrochemical impedance spectra indicate that the reversibility of electrochemical redox reaction and the charge-transfer resistance of LVP/C cathode material have been significantly improved by Na doping. The improved performances can be attributed to the more convenient route for lithium ion diffusion and the lower activation energy of the extraction–insertion of lithium ion due to the weakness of Li-O bond. 相似文献
14.
采用溶胶凝胶及高能球磨制得Li 3Fe 2(PO 4) 3/C材料,利用多种物理及其电化学技术观察材料形貌,表征材料结构及电化学性能,用电化学原位XAFS等初步研究Li 3Fe 2(PO 4) 3/C超理论容量电化学反应机理. 结果显示,Li 3Fe 2(PO 4) 3/C的结构为单斜晶系,空间群P21/n. 2.0 ~ 4.0 V电位区间,10 mAh·g -1电流密度,Li 3Fe 2(PO 4) 3/C电极的首周期放电比容量为129 mAh·g -1,达到其理论容量. 若电位区间拓宽至2.0 ~ 4.95 V,其首周期放电比容量高达165 mAh·g -1,超出理论的“额外”容量30%. 电化学原位XAFS测试未观察到明显的Fe 3+/Fe 4+氧化还原对参与电化学反应,初步推测“额外”容量可能来自于该复合材料的高浓度表面缺陷. 相似文献
15.
The electrochemical lithium insertion reaction of monoclinic Li(3)Fe(2)(PO(4))(3) as cathode materials of lithium-ion batteries was investigated from the viewpoint of the electronic structure around Fe and the polyanion unit (PO(4)). Fe K-edge and L(III,II)-edge XAS measurements revealed that Fe(3+) was reduced to Fe(2+) upon Li insertion. In addition, O K-edge and P K-edge XAS also showed spectral changes upon Li insertion, which corresponded to changes in the electronic structure of the PO(4) polyanion unit. The ab initio density functional calculation was performed within the GGA and LDA+U methods. The LDA+U method reproduced well the cell potential upon lithium intercalation into Li(3)Fe(2)(PO(4))(3), whereas the GGA method underestimated the intercalation. The calculated electronic structure of Li(3)Fe(2)(PO(4))(3) described strong P 3p-O 2p covalent bonding, while weak hybridization was indicated in Fe 3d-O 2p. Moreover, the difference in electronic density between Li(3)Fe(2)(PO(4))(3) and the lithiated model indicated that the polarization effect between inserted Li and oxygen induced the changes in the electronic structure around the polyanion unit. 相似文献
16.
ChemInform is a weekly Abstracting Service, delivering concise information at a glance that was extracted from about 100 leading journals. To access a ChemInform Abstract of an article which was published elsewhere, please select a “Full Text” option. The original article is trackable via the “References” option. 相似文献
17.
Li(3)V(2)(PO(4))(3)/graphene nanocomposites have been firstly formed on reduced graphene sheets as cathode material for lithium batteries. The nanocomposites synthesized by the sol-gel process exhibit excellent high-rate and cycling stability performance, owing to the nanoparticles connected with a current collector through the conducting graphene network. 相似文献
18.
In this study, spinel LiNi0.5Mn1.5O4 (LNMO) was successfully decorated with Al2O3 thin film by using atomic layer deposition (ALD) approach and evaluated as a cathode material for high-temperature applications in lithium ion batteries (LIBs). To optimize the LNMO-Al2O3 electrodes operated at elevated temperature (55 °C), the effects of Al2O3 thicknesses adjusted by controlling the ALD deposition cycle were systemically investigated. According to the series of electrochemical results, the LNMO coated with the Al2O3 thin layer in the thickness of ca. 2 nm was achieved by using one-cycle ALD and the LNMO-Al2O3 electrode exhibited superior electrochemical stability (capacity retention up to 93.7% after consecutive 150 charge/discharge cycles at 0.5 C to the pristine LNMO electrode at elevated temperature. This can be attributed to two factors: (i) the decoration of Al2O3 thin layer could not contribute remarkably to extra resistance for charge transfer; (ii) Al2O3 thin film deposition could efficiently stabilize the growth of cathode electrolyte interface (CEI) and suppress the dissolution of transition metals. Therefore, these results verify that the LNMO-Al2O3 electrode could be regarded as a promising cathode material for high-voltage LIBs, especially at elevated temperature operation. 相似文献
19.
In the present investigation, we report the transformation of alpha-LiVOPO 4 to alpha-Li 3V 2(PO 4) 3, leading to an enhancement of capacity. The alpha-LiVOPO 4 sample was synthesized by a sol-gel method, followed by sintering at 550-650 degrees C in a flow of 5% H 2/Ar. The structural transformation of a triclinic alpha-LiVOPO 4 structure to a monoclinic alpha-Li 3V 2(PO 4) 3 structure was observed at higher sintering temperatures (700-800 degrees C in a flow of 5% H 2/Ar). The alpha-Li 3V 2(PO 4) 3 phase was characterized by X-ray diffraction, scanning electron microscopy, transmission electron microscopy, thermal gravimetric analysis, and X-ray absorption near edge spectrum (XANES) techniques. The valence shift of vanadium ions from +4 to +3 states was observed using in situ XANES experiments at V K-edge. The structural transformation is ascertained by the shape changes in pre-edge and near edge area of X-ray absorption spectrum. It was observed that the capacity was enhanced from 140 mAh/g to 164 mAh/g via structural transformation process of LiVOPO 4 to Li 3V 2(PO 4) 3. 相似文献
20.
Samples of Li(x)Ni0.5Mn0.5O2 and Li(x)Ni(1/3)Mn(1/3)Co(1/3)O2 were prepared as active materials in electrochemical half-cells and were cycled electrochemically to obtain different values of Li concentration, x. Absorption edges of Ni, Mn, Co, and O in these materials of differing x were measured by electron energy loss spectrometry (EELS) in a transmission electron microscope to determine the changes in local electronic structure caused by delithiation. The work was supported by electronic structure calculations with the VASP pseudopotential package, the full-potential linear augmented plane wave code WIEN2K, and atomic multiplet calculations that took account of the electronic effects from local octahedral symmetry. A valence change from Ni2+ to Ni4+ with delithiation would have caused a 3 eV shift in energy of the intense white line at the Ni L3 edge, but the measured shift was less than 1.2 eV. The intensities of the "white lines" at the Ni L-edges did not change enough to account for a substantial change of Ni valence. No changes were detectable at the Mn and Co L-edges after delithiation either. Both EELS and the computational efforts showed that most of the charge compensation for Li+ takes place at hybridized O 2p states, not at Ni atoms. 相似文献
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