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  • 1
    Online Resource
    Online Resource
    Japanese Society for Food Science and Technology ; 2024
    In:  Food Science and Technology Research Vol. 30, No. 1 ( 2024), p. 25-36
    In: Food Science and Technology Research, Japanese Society for Food Science and Technology, Vol. 30, No. 1 ( 2024), p. 25-36
    Type of Medium: Online Resource
    ISSN: 1344-6606 , 1881-3984
    Language: English
    Publisher: Japanese Society for Food Science and Technology
    Publication Date: 2024
    detail.hit.zdb_id: 2061913-3
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  • 2
    Online Resource
    Online Resource
    American Chemical Society (ACS) ; 2013
    In:  Journal of the American Chemical Society Vol. 135, No. 16 ( 2013-04-24), p. 5938-5941
    In: Journal of the American Chemical Society, American Chemical Society (ACS), Vol. 135, No. 16 ( 2013-04-24), p. 5938-5941
    Type of Medium: Online Resource
    ISSN: 0002-7863 , 1520-5126
    RVK:
    Language: English
    Publisher: American Chemical Society (ACS)
    Publication Date: 2013
    detail.hit.zdb_id: 1472210-0
    detail.hit.zdb_id: 3155-0
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  • 3
    In: Chemistry of Materials, American Chemical Society (ACS), Vol. 32, No. 1 ( 2020-01-14), p. 139-147
    Type of Medium: Online Resource
    ISSN: 0897-4756 , 1520-5002
    Language: English
    Publisher: American Chemical Society (ACS)
    Publication Date: 2020
    detail.hit.zdb_id: 1500399-1
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  • 4
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2016-02, No. 7 ( 2016-09-01), p. 1028-1028
    Abstract: 1. Introduction Olivine phosphates have long been investigated as cathode material in Li-ion batteries. In particular, lithium iron phosphate (LiFePO 4 ) has attracted the attention of many researchers because of its high theoretical capacity of 170 mAh g -1 , low cost and high electrochemical/thermal stabilities of the phosphate (PO 4 3- ) anion. [1] However, the large volume difference during two-phase reaction between Li-rich Li 1-a FePO 4 (LFP) and Li-poor Li b FePO 4 (FP) phases leads to lattice mismatch at the LFP/FP boundary which induces a low Li-ion diffusion coefficient of 10 -14 cm 2 s -1 . [2] Such 1D Li + diffusivity in the olivine-LFP is much slower (by 5-8 orders of magnitude) as compared with that of LCO (10 -9 cm 2 s -1 ) and LMO (10 -5 cm 2 s -1 ) cathodes. As a result, this slow lithium ion diffusion and the relatively poor electronic conductivity (10 -10 to 10 -7 Ω -1 cm -1 ) of the olivine-LFP in the absence of a doping cation, limit the power capability of the LFP material. To overcome these limitations, we have proposed new concept of three-phase structure containing a core of crystalline LFP, a shell of amorphous LFP, and graphitic carbon derived from Ketjen Black (KB) synthesized using our original in-situ ultracentrifugation process (UC process) [3]. The peculiar core-shell structure of LFP nanoparticle within the graphitic carbon prepared by UC-process improves the electronic conductivity in the whole LFP/graphitic carbon composites, while the amorphous LFP phase at the particle surface (shell) can achieve excellent rate performance owing to its high Li-ion diffusion coefficient. 2. Experimental A precursor solution was prepared by mixing KB and H 3 PO 4 aq. in ultra-pure water. The precursor solution was treated by UC process after an addition of iron acetate and lithium acetate. After drying at 80°C in vacuum for 12 h, the precursor composite powder was obtained. The powder was lastly annealed at 700 ◦C under N 2 flow for 5 min and the final product (LFP/ graphitic carbon composite powder) was obtained. The LFP/graphitic carbon composite electrode was electrochemically characterized using a 2032 coin half-cell with Li metal in 1M LiPF 6 /EC+DEC (vol. 1:1). 3. Results and Discussion The electron microscopy observations show that LFP/graphitic carbon composite has a highly crystalline phase of LFP core of ca. 12-15 nm diameter with a distance of d=0.32 nm corresponding to (110) plane of the olivine LFP. This crystalline core, that we called “core 1”, is entirely covered with amorphous layers (referred as “core 2”) in light grey in the TEM image. The combination of TEM observation together with XRD, XPS and Mössbauer analysis, supports the hypothesis that amorphous LFP contains Fe 3+ defect. The most outer layer (“shell”) is composed of random carbon (KB) fragments/sheets stacked onto each other. The thickness of the shell is about 5 nm. An interlayer distance of d=0.35 nm was measured which is a little larger than that of graphene. This LFP/graphitic carbon composite enabled a 100C rate (36 seconds) discharge with 60 mAh g -1 per composite corresponding to 70% of the capacity obtained at the slowest discharge rate (1C). An amorphous LFP containing Fe 3+ defects enhances lithium ion diffusion coefficient probably by switching from one-dimensional to three-dimensional diffusion. Then, the electron utilized in Fe redox reaction can be fast transferred by the covering graphitic carbon coating the particles. Such an ultrafast charge–discharge performance opens the possibility of using LiFePO 4 as a cathode material for ultrafast hybrid capacitor with a stable cycle performance over 2,000 cycles at a 10C rate, maintaining 90% of the initial capacity. References 1) A. K. Padhi, et al., J. Electrochem. Soc. , 1997, 144 , 1188-1194. 2) G. Kobayashi, et al., Adv. Funct. Mater. , 2009, 19 , 395-403. 3) K. Naoi, et al., J. Electrochem. Soc. , 2015, 162 (6) , A1-A7.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2016
    detail.hit.zdb_id: 2438749-6
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  • 5
    Online Resource
    Online Resource
    The Electrochemical Society ; 2020
    In:  ECS Meeting Abstracts Vol. MA2020-02, No. 68 ( 2020-11-23), p. 3502-3502
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2020-02, No. 68 ( 2020-11-23), p. 3502-3502
    Abstract: In laboratory charge-discharge tests of lithium-ion battery electrodes is often used half-cell with a lithium metal anode, which can supply enough lithium ions. On the other hand, practical lithium-ion batteries do not contain lithium metal and use full-cell configuration with almost similar capacities between cathode and anode. Limited number of lithium ions supplied by the cathode contributes as carrier ions, which determines the actual charge-discharge capacity. Since the degradation behavior observed in full-cell is different from in half-cell [1, 2], it is important to understand the problems that occur during charge-discharge in full-cell to maximize battery performance. In this study, we investigated the irreversibility in full-cell with lithium iron phosphate (LiFePO 4 ) cathode and lithium titanate (Li 4 Ti 5 O 12 ) anode as an unnatural case, where both active materials show two-phase reaction in almost all composition. The potential changes of cathode and anode were tracked using the three-electrode full-cell with a lithium metal reference electrode. In addition to the electrochemical measurements, the charge-discharge state was analyzed from the X-ray absorption spectroscopy (XAS), which provides the valence change information. Half-cell charge-discharge tests of LiFePO 4 and Li 4 Ti 5 O 12 at 0.1C result in reversible charge-discharge profile. However, the distinct irreversible capacity is observed in the LiFePO 4 / Li 4 Ti 5 O 12 full-cell configuration. The initial charge and discharge capacity are 162 nd 126 mAh g -1 , respectively and this irreversibility is continuously observed in the subsequent cycle. The three-electrode test indicates that the potential of Li 4 Ti 5 O 12 anode sharply increases despite in the middle of the discharge. Fe K-edge XAS shows similar edge energy for the half-charged and half-discharged LiFePO 4 cathode. However, Ti K-edge XAS of half-charged Li 4 Ti 5 O 12 anode shows the different edge energy from that of the half-discharged. The full-discharged LiFePO 4 cathode does not reach the lithiated state even after discharging, which agrees with the results from the three-electrode test. At the end of the charge, little edge-energy shift in the Li 4 Ti 5 O 12 anode is observed, indicating that the insertion reaction of lithium ions does not progress. Therefore, the irreversible capacity is caused by a side reaction at the Li 4 Ti 5 O 12 anode in end of the charge. [1] Bjorklund, D. Brandell, M. Hahlin, K. Edstrom, R. Younesi, J. Electrochem. Soc . , 164 (2017) A3054-A3059. [2] H. Kim, N.P.W. Pieczonka, Z.C. Li, Y. Wu, S. Harris, B.R. Powell, Electrochim. Acta. , 90 (2013) 556-562.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2020
    detail.hit.zdb_id: 2438749-6
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  • 6
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2018-02, No. 4 ( 2018-07-23), p. 178-178
    Abstract: Introduction Li-excess metal oxide having high charge-discharge capacity has been expected to realize higher energy density in lithium-ion batteries. Several lithium-excess metal oxides have been studied extensively in order to use effectively the charge compensation by redox reaction of oxide ions. [1-5] In 4 d and 5 d metal oxides such as Li 2 RuO 3 [1] and Li 2 IrO 3 -based systems [2] , high covalent bond between 4 d orbital of transition-metal and 2 p orbital of oxygen enables charge compensation by the oxidation of oxide ions to peroxo-like dimer. On the other hand, in a 3 d transition-metal oxide, Li 1.2 Ni 0.13 Co 0.13 Mn 0.54 O 2 exhibits formation of isolated holes on oxide ions because highly ionized 3 d transition-metal ions stabilize the isolated holes on the oxide ions surrounded by lithium ions. [3, 4] Other 3 d transition-metal oxides such as Li 1.2 Ti 0.4 Mn 0.4 O 2 , also exhibit stable oxide ions redox. [5] According to the previous studies, covalent character or ionic character between transition-metal ions and oxide ions in Li-excess metal oxides is a key factor to stabilize oxide ions redox. However, behavior of oxide ions redox in Li-excess metal oxides with different covalent character or ionic character has not been systematically examined. In this study, we focus on four different Li-excess metal oxides, Li 2 MeO 3 (Me = Mn and Ru) and Li 1.2 Ti 0.4 Me 0.4 O 2 (Me = Mn and Fe), as models with different covalent character or ionic character. Developing a new operando soft X-ray absorption spectroscopy, we observed directly the electronic state of the oxide ions in these materials during charge process via the technique. [6] Experimental operando soft X-ray absorption spectroscopy measurements were performed at BL27SU in SPring-8, Japan. The absorption spectra were collected with partial fluorescence mode using home-made cell. Composite electrodes were pasted on aluminum sputtered-Si 3 N 4 window. For Li 1.2 Ti 0.4 Mn 0.4 O 2 , half charged-LiFePO 4 was used as a counter electrode, and 4.2 mol dm -3 lithium bis(trifluoromethanesulfonyl)amide/ acetonitrile was used as an electrolyte solution. Two electrode cells were assembled in the Ar-filled grovebox. XAS spectra were collected during galvanostatic measurement at rate of 1/20 C rate at 55°C. Results and Discussion The charge and discharge profiles of the Li 1.2 Ti 0.4 Mn 0.4 O 2 showed that the voltage gradually increased at initial stage under charging process, then a plateau was observed at approximately 4.2 V. The first discharge profile was similar to the first charge one. The first discharge capacity was 270 mAh/g, which was comparable to the first charge capacity of 300 mAh/g. operando Mn L -edge XAS spectra of the Li 1.2 Ti 0.4 Mn 0.4 O 2 showed that a board peak was observed at 642 eV before charge process. The peak separated to two peaks and shifted higher energy in the slope region of charge process, and the two peaks unchanged with subsequent charge process. The peak separation and shift toward higher energy in the slope region were caused by spin multiplicity and crystal field effect with oxidation Mn ions. No change of the spectra in the subsequently charge process means that the Mn ions did not contribute to the charge compensation. operando O K -edge XAS spectra of Li 1.2 Ti 0.4 Mn 0.4 O2 showed a board peak was observed around 531 eV before charge process. The peak was divided into two peaks during charge process. These peaks reflect transition from O 1s orbitals to hybridized states between 3d orbital of transition-metal and 2p orbital of oxygen. The integrated intensity of the peak at the lower energy increased in the slope region of charge process, whereas the integrated intensity of the peak at the higher energy increased with subsequent charge process. The change of the spectrum in the slope region was caused by oxidation Mn ions (Mn 3+ to Mn 4+ ) as observed in the Mn- L XANES spectra. The increase of the integrated intensity at the higher energy in the subsequently charge process was caused by oxidization of oxygen ions. References: [1] Sathiya, M. et al. , and Tarascon, J.-M. Nat. Mater. 2013 , 12, 827. [2] McCalla, E. et al. , and Tarascon, J.-M. Science 2015 , 350, 1516. [3] Luo, K. et al. , and Bruce, P. G. Nat. Chem. 2016 , 8, 684. [4] Seo, D.-H. et al. , and Ceder, G. Nat. Chem. 2016 , 8, 692. [5] Yabuuchi, N. et al. , and Ohta, T. Nat. Commun. 2016 . 7, 13814. [6] Yamamoto, K. et al. , and Uchimoto, Y. submitted . Acknowledgement This research was financially supported by the Japan Science and Technology Agency (JST), Advanced Low Carbon Technology Research and Development Program (ALCA), Specially Promoted Research for Innovative Next Generation Batteries (SPRING) Project.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2018
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  • 7
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2016-02, No. 53 ( 2016-09-01), p. 4042-4042
    Abstract: For the widespread use of Polymer Electrolyte Fuel Cell (PEFC), it is needed to reduce the amount of platinum used for electrode catalyst materials from the viewpoint of improving oxygen reduction reaction (ORR) activity of platinum. Recently, it is reported by Erlebacher 1), 2) that the ORR activity of nanoporous NiPt alloy catalysts encapsulated by ionic liquid (IL) is higher than that of this material not encapsulated by. Based on the report 3) that promoting the oxygen solubility at the interface between catalysts and electrolyte improves the ORR activity, this result implies that the high oxygen solubility of IL mainly contributes to high ORR activity. However, the reason of improvement of the ORR activity has not been clarified yet. In this study, we prepared Pd/Pt core shell catalyst, which is one of the most notable nanomaterials showing substantially high ORR activity, and encapsulated the surface of this catalyst with IL. Then we studied on the ORR of IL-encapsulated Pd/Pt core shell nanoparticles (NPs) by operando X-ray absorption spectroscopy (XAS) method. Pd/C (particle diameter of Pd: 3.6 nm) was applied in this study. Cu monolayer has been deposited on Pd NPs using under potential deposition (UPD) of Cu in 10 mM CuSO 4 solution. A single UPD Cu monolayer replacement with Pt in K 2 PtCl 4 solution formed Pt monolayer film on Pd NPs (Pt/Pd/C). The surface of Pt/Pd/C was coated with [MTBD][NTf2] 2), 3) (IL). Convection voltammetry was performed at 25 ˚C in O 2 -saturated 0.1 M HClO 4 aq and H 2 SO 4 aq using rotating disc electrode (RDE). RDE was rotated at 300, 500, 700, 900, 1200, 1600, and 2500 rpm. Electrochemical activity value at 0.9 V vs. Reversible Hydrogen Electrode (RHE) was calculated from Koutecky-Levich plot. Operando XAS measurements for Pt L Ⅲ -edge and L Ⅱ -edge of Pt/Pd/C catalysts were carried out by using the beamline BL14B2 in SPring-8 (Japan). These measurements were performed by fluorescence method in O 2 -saturated 0.1 M HClO 4 aq and H 2 SO 4 aq. Potentials were maintained at 0.5, 0.85, and 1.15 V vs. RHE. Specific activity value of Pt/Pd/C in 0.1 M H 2 SO 4 aq was much lower than that of Pt/Pd/C in 0.1 M HClO 4 aq. Pt-Pt bond distances were calculated by analyzing EXAFS spectra of Pt L Ⅲ -edge. At each potentials, there are no significant differences between Pt-Pt bond distances of Pt/Pd/C in 0.1 M HClO 4 aq and H 2 SO 4 aq. It implied that the irreversible specific adsorption of SO 4 2- on the surface of Pd/Pt NPs decreased the number of active site of catalysts. The specific activity value of IL-encapsulated Pt/Pd/C was 1.31 times higher than that of non-encapsulated Pt/Pd/C in 0.1 M HClO 4 aq. Pt-Pt bond distance estimated by EXAFS spectra of Pt L Ⅲ -edge of IL-encapsulated Pt/Pd/C was definitely longer than that of non-encapsulated Pt/Pd/C. These results suggested that coating with IL on the surface of Pt/Pd/C have lattice strain. The quantitative lattice strain establishes a direct correlation to monolayer Pt shell ORR activity and the strain effect induced d-band shift regulates the adsorption properties of rate-limiting intermediates in catalytic processes. 4) References: (1) J. Snyder, T. Fujita, M.W. Chen, and J. Erlebacher, Nat. Mater. , 9 , 904 (2010). (2) C. Chen, Y. Kang, Z. Huo, Z. Zhu, W. Huang, H. Xin, J. Snyder, D. Li, J. Herron, M. Mavrikakis, M. Chi, K. More, Y. Li, N. Markovic, G. Somorjai, P. Yang, and V. Stamenkovic, Science , 343 , 1339 (2014). (3) J. Maruyama, M. Inaba, T. Morita and Z. Ogumi, J. Electroanal. Chem. , 504 , 208-216 (2001). (4) X. Wang, Y. Orikasa, Y. Takesue, H. Inoue, M. Nakamura, T. Minato, N. Hoshi and Y. Uchimoto,  J. Am. Chem. Soc . , 135 , 5938 – 5941(2013).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2016
    detail.hit.zdb_id: 2438749-6
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  • 8
    In: Energy & Environmental Science, Royal Society of Chemistry (RSC), Vol. 9, No. 6 ( 2016), p. 2143-2151
    Type of Medium: Online Resource
    ISSN: 1754-5692 , 1754-5706
    Language: English
    Publisher: Royal Society of Chemistry (RSC)
    Publication Date: 2016
    detail.hit.zdb_id: 2439879-2
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  • 9
    Online Resource
    Online Resource
    The Electrochemical Society ; 2012
    In:  ECS Meeting Abstracts Vol. MA2012-02, No. 9 ( 2012-06-04), p. 725-725
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2012-02, No. 9 ( 2012-06-04), p. 725-725
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2012
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  • 10
    Online Resource
    Online Resource
    The Electrochemical Society ; 2013
    In:  ECS Meeting Abstracts Vol. MA2013-02, No. 15 ( 2013-10-27), p. 1403-1403
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2013-02, No. 15 ( 2013-10-27), p. 1403-1403
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2013
    detail.hit.zdb_id: 2438749-6
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