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Sample records for li ca tion

  1. Optically pumped cerium-doped LiSrAlF.sub.6 and LiCaAlF.sub.6

    DOE Patents [OSTI]

    Marshall, Christopher D.; Payne, Stephen A.; Krupke, William F.

    1996-01-01

    Ce.sup.3+ -doped LiSrAlF.sub.6 crystals are pumped by ultraviolet light which is polarized along the c axis of the crystals to effectively energize the laser system. In one embodiment, the polarized fourth harmonic light output from a conventional Nd:YAG laser operating at 266 nm is arranged to pump Ce:LiSrAlF.sub.6 with the pump light polarized along the c axis of the crystal. The Ce:LiSrAlF.sub.6 crystal may be placed in a laser cavity for generating tunable coherent ultraviolet radiation in the range of 280-320 nm. Additionally, Ce-doped crystals possessing the LiSrAlF.sub.6 type of chemical formula, e.g. Ce-doped LiCaAlF.sub.6 and LiSrGaF.sub.6, can be used. Alternative pump sources include an ultraviolet-capable krypton or argon laser, or ultraviolet emitting flashlamps. The polarization of the pump light will impact operation. The laser system will operate efficiently when light in the 280-320 nm gain region is injected or recirculated in the system such that the beam is also polarized along the c axis of the crystal. The Ce:LiSrAlF.sub.6 laser system can be configured to generate ultrashort pulses, and it may be used to pump other devices, such as an optical parametric oscillator.

  2. Optically pumped cerium-doped LiSrAlF{sub 6} and LiCaAlF{sub 6}

    DOE Patents [OSTI]

    Marshall, C.D.; Payne, S.A.; Krupke, W.F.

    1996-05-14

    Ce{sup 3+}-doped LiSrAlF{sub 6} crystals are pumped by ultraviolet light which is polarized along the c axis of the crystals to effectively energize the laser system. In one embodiment, the polarized fourth harmonic light output from a conventional Nd:YAG laser operating at 266 nm is arranged to pump Ce:LiSrAlF{sub 6} with the pump light polarized along the c axis of the crystal. The Ce:LiSrAlF{sub 6} crystal may be placed in a laser cavity for generating tunable coherent ultraviolet radiation in the range of 280-320 nm. Additionally, Ce-doped crystals possessing the LiSrAlF{sub 6} type of chemical formula, e.g. Ce-doped LiCaAlF{sub 6} and LiSrGaF{sub 6}, can be used. Alternative pump sources include an ultraviolet-capable krypton or argon laser, or ultraviolet emitting flashlamps. The polarization of the pump light will impact operation. The laser system will operate efficiently when light in the 280-320 nm gain region is injected or recirculated in the system such that the beam is also polarized along the c axis of the crystal. The Ce:LiSrAlF{sub 6} laser system can be configured to generate ultrashort pulses, and it may be used to pump other devices, such as an optical parametric oscillator. 10 figs.

  3. CUSSSFIC4TION CMUXLLq

    Office of Legacy Management (LM)

    CUSSSFIC4TION CMUXLLq RITE AUG 1 7 1962 Fcx the Atomic. Energy Commisaion~ Chief. Declaseifle@tlon Brar\qh F-mm A. B. Grsaingsr (Other ends tifmtioel) The die wae foutq3 to workvery satiafactorilywiti thlanew Qpeof incert, andncm,of tbepmvLouedsfeotaofeoo+tH&' iOitYwaslmd. D&e& ._: . . ..YG ~Kl.3. i>ro;rid3 -&I:: clcsuro on bct.k.mds of the .plece m & Die #l, is also to be tried outoo 4zgust22. Barr~l~or~~~Die~~hadalaobeenawlLfiedta' plwidesd~do~-

  4. CLASSIFICdTION CAWXL~ DAm

    Office of Legacy Management (LM)

    CLASSIFICdTION CAWXL~ DAm NAR 6 1969 For the Atomic EhergY hDh=+= ,' ROBERT L JACKSON /(\' t' for the Chief, Declassification B~Jx~

  5. Progress in the material development of LiCaAlF sub 6 :Cr sup 3+ laser crystals

    SciTech Connect (OSTI)

    Michelle D. Shinn.; Chase, L.L.; Caird, J.A.; Payne, S.A.; Atherton, L.J.; Kway, W.L.

    1990-03-01

    High Cr{sup 3+} doping levels, up to 8 mole percent, and low losses have been obtained with the tunable solid-state laser material LiCaAlF{sub 6}:Cr{sup 3+} (Cr:LiCAF). Measurements and calculations show that high pumping and extraction efficiencies are possible with the improved material. 13 refs., 4 figs., 1 tab.

  6. Photoluminescence performance of thulium doped Li{sub 4}SrCa(SiO{sub 4}){sub 2} under irradiation of ultraviolet and vacuum ultraviolet lights

    SciTech Connect (OSTI)

    Wang, Zhaofeng; Li, Yezhou; Liu, Xiong; Wei, Xingmin; Chen, Yueling; Zhou, Fei; Wang, Yuhua

    2014-11-15

    Highlights: A novel blue-emitting phosphor Li{sub 4}SrCa(SiO{sub 4}){sub 2}:Tm{sup 3+} was reported. Li{sub 4}SrCa(SiO{sub 4}){sub 2}:Tm{sup 3+} exhibited excellent thermal and irradiation stability. Li{sub 4}SrCa(SiO{sub 4}){sub 2}:Tm{sup 3+} was found to possess high color purity. - Abstract: In this work, we synthesized Tm{sup 3+} doped Li{sub 4}SrCa(SiO{sub 4}){sub 2} phosphors and investigated their photoluminescence properties under the excitation of ultraviolet and vacuum ultraviolet lights. The crystal structure analysis and variation of cell parameters confirm that Tm{sup 3+} ions have been successfully doped in the structure of Li{sub 4}SrCa(SiO{sub 4}){sub 2} host by occupying the sites of Ca{sup 2+} with the coordination number of 6. The luminescence results suggest that Li{sub 4}SrCa(SiO{sub 4}){sub 2}:Tm{sup 3+} is a good blue-emitting phosphor when excited by ultraviolet and vacuum ultraviolet irradiations. In addition, it is observed that there is nearly no degradation for Li{sub 4}SrCa(SiO{sub 4}){sub 2}:Tm{sup 3+} after undergoing thermal and irradiation treatments. Possible mechanisms for the luminescence processes are proposed on the basis of the discussion of excitation and emission spectra. In particular, the emission color of Li{sub 4}SrCa(SiO{sub 4}){sub 2}:Tm{sup 3+} by excitation of 147 and 172 nm irradiations is very close to the standard blue color, suggesting that it could be potentially applied in plasma display panels and mercury-free fluorescence lamps.

  7. LI

    Office of Legacy Management (LM)

    \ LI g. / This document con&s of lf pages. No. 1 &of #copies, Series fl . .! ' \ ' > .b P .--r ' i ' ./' MJDIFICATION NO. k sUPPLEMENTALAMw24ENrto CONTRACT NO. A T (30-l)-1335 M O D IFICATION NO. 4 CONTRACTOR AND A D D m S : KIDIFICATION TO: -EINESTIEUTED CCSTOFWORKr TOTAT,ESTIIUTEDC~T OFWRKI INCREASEIN C O M K rSSI~ OBLlDATIONt NEMTOTALCOMMISSION OBLIOaTIONt PAYl%NTTDBEMADEBY: HORIZONS, INCORPOlZATED R-inceton, New Jersey AIBNDSCOPEOFK#tK,EXTENDTR?M AND OTflER CHANOES $&31,lbOO

  8. Performance and discharge characteristics of Ca/LiCl, LiNO/sub 3//LiNO/sub 3/, AgNO/sub 3//Ni thermal battery cells

    SciTech Connect (OSTI)

    McMains, G.E.; Fletcher, A.N.; Miles, M.H.

    1984-02-01

    Thermal battery cells utilizing molten LiNO/sub 3/ as an oxidizing electrolyte with calcium anodes have been characterized for high rate discharge conditions. The presence of small amounts of AgNO/sub 3/ greatly improves the cathode reaction. Half-cell studies of anode characteristics show little variation of anode potential with temperature. Gassing at the anode-electrolyte interface increases with temperature and current density. Overall anode consumption rates increase with increasing temperature, while anode coulombic efficiencies drop at high rates of discharge (300 mA/cm/sup -2/). Cathode half-cell data reveal that high rate reduction of AgNO/sub 3/ dissolved in LiNO/sub 3/ yields masses of dendritic growth at low temperatures (260/sup 0/-275/sup 0/C) while at higher temperatures (>400/sup 0/C) correspondingly fewer dendritic structures are observed. Cell experiments show anticipated current-voltage-temperature relationships, effectively mirroring half-cell experiments. Cell voltages sustain over 2V at 75 mA/cm/sup -2/ for periods which vary according to temperature of discharge.

  9. Viscosity and density of aqueous solutions of LiBr, LiCl, ZnBr[sub 2], CaCl[sub 2], and LiNO[sub 3]; 1: Single salt solutions

    SciTech Connect (OSTI)

    Wimby, J.M.; Berntsson, T.S. . Dept. of Heat and Power Technology)

    1994-01-01

    New experimental data for the viscosity and density of the binary systems lithium chloride + water, lithium bromide + water, calcium chloride + water, lithium nitrate + water, and zinc bromide + water are presented. Densities are presented in tabular form and as 10-parameter correlations, while kinematic and dynamic viscosities are presented in tabular form. Data are presented in the concentration range from intermediate dilution to close to room temperature crystallization concentration. The temperature ranges are 20--70 C for density and 25--90 C for viscosity. When available, literature data are compared with the new data, and some disagreement is found. New thermogravimetric curves are presented for the dehydration of CaCl[sub 2], ZnBr[sub 2], and LiBr in order to enable evaluation of drying as a composition determination technique.

  10. Ca

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    P O. Box 3090 Ca rlsbad, New Mexico 88221 Mr. John Kieling , Acting Bureau Chief Hazardous Waste Bureau MAY 1 6 2012 New Mexico Environment Department 2905 E. Rodeo Park Drive, Bldg . 1 Santa Fe, New Mexico 87505-6303 Subject: Transmittal of the Waste Isolation Pilot Plant Revised Calendar Year 2005-2008 Culebra Potentiometric Surface Map Package Dear Mr. Kieling: On August 5 , 2011 , the New Mexico Environmental Department (NMED) approved the Groundwater Work Plan submitted as a condition to

  11. Effects of Ti-Based Additives on the Hydrogen Storage Properties of aLiBH4/CaH2Destabilized System

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Yang, Hongwei; Ibikunle, Adeola; Goudy, Andrew J.

    2010-01-01

    The hydrogen storage properties of a destabilizedLiBH4/CaH2system ball-milled withTiCl3,TiF3, andTiO2additives have been investigated. It is found that the system withTiCl3additive has a lower dehydrogenation temperature than the ones with other additives. Further study shows that a higher amount ofTiCl3is more effective in reducing the desorption temperature of theLiBH4/CaH2system, since it leads to a lower activation energy of dehydrogenation. The activations energies for mixtures containing 4, 10, and 25?mol% ofTiCl3are 141, 126, and 110?kJ/mol, respectively. However, the benefits of higher amounts ofTiCl3are offset by a larger reduction in hydrogen capacity of the mixtures.

  12. 07Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li Thermal Neutron Capture Evaluated Data Measurements 1967RA24: 6Li(n, γ), E = thermal; measured Eγ; deduced Q. 1968SP01: 6Li(n, γ), E = thermal; measured Eγ, Iγ; deduced Q. 7Li deduced levels, branchings. 1970MEZS: 6Li(n, γ), E = thermal; measured σ. 1970SP02: 6Li(n, γ), E = thermal; measured Eγ, Iγ; deduced Q. 1972OP01: 6Li(n, γ), E = thermal; measured Eγ, Iγ. 1973JUZT, 1973JUZU: 6Li(n, γ), E = thermal; measured σ(Eγ). 7Li deduced γ-branching. 1985KO47: 6Li(n, γ), E =

  13. First principles DFT study of ferromagnetism in SnO{sub 2} induced by doped group 1A and 2A non-magnetic elements X (X=Li, Na, K, Be, Mg, Ca)

    SciTech Connect (OSTI)

    Chakraborty, Brahmananda Ramaniah, Lavanya M.

    2014-04-24

    Transition metal - free - ferromagnetism in diluted magnetic semiconductors (DMS) is of much current interest in the search for more efficient DMS materials for spintronic applications. Here, we report the results of our first principles density functional theory (DFT) study on impurity - induced ferromagnetism in non-magnetic SnO{sub 2} by a non-magnetic impurity. The impurities considered are sp-type of group 1A and 2A elements X (X = Li, Na, K, Be, Mg, Ca). Even a single atom of the group 1A elements makes the system magnetic, whereas for the group 2A elements Ca and Mg, a higher doping is required to induce ferromagnetism. For all the elements studied, the magnetic moment appears to increase with the doping concentration, at least at certain impurity separations, which is a positive indicator for practical applications.

  14. Structure and microwave dielectric characteristics of lithium-excess Ca{sub 0.6}Nd{sub 0.8/3}TiO{sub 3}/(Li{sub 0.5}Nd{sub 0.5})TiO{sub 3} ceramics

    SciTech Connect (OSTI)

    Zhou, Changrong; Chen, Guohua; Cen, Zhenyong; Yuan, Changlai; Yang, Yun; Li, Weizhou

    2013-11-15

    Graphical abstract: - Highlights: Dense ceramics were fabricated by the conventional solid-state route. Excess-Li addition lowers sintering temperature. Excess-Li addition improves the relative density and microwave dielectric properties. - Abstract: Compositions based on (1?x)Ca{sub 0.6}Nd{sub 8/3}TiO{sub 3}?x(Li{sub 1/2}Nd{sub 1/2})TiO{sub 3} + yLi (CNLNTx + yLi, x = 0.300.60, y = 00.05), suitable for microwave applications have been developed by systematically adding excess lithium in order to tune the microwave dielectric properties and lower sintering temperature. Addition of 0.03 excess-Li simultaneously reduced the sintering temperature and improved the relative density of sintered CNLNTx ceramics. The excess Li addition can compensate the evaporation of Li during sintering process and decrease the secondary phase content. The CNLNTx (x = 0.45) ceramics with 0.03 Li excess sintered at 1190 C have single phase orthorhombic perovskite structure, together with the optimum combination of microwave dielectric properties of ?{sub r} = 129, Q f = 3600 GHz, ?{sub f} = 38 ppm/C. Obviously, excess-Li addition can efficiently decrease the sintering temperature and improve the microwave dielectric properties. The high permittivity and relatively low sintering temperatures of lithium-excess Ca{sub 0.6}Nd{sub 0.8/3}TiO{sub 3}/(Li{sub 0.5}Nd{sub 0.5})TiO{sub 3} ceramics are ideal for the development of low cost ultra-small dielectric loaded antenna.

  15. 5Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    abstracted; deduced nuclear properties. 1968TA11: 2H(, p), E 29.2 MeV; measured (Ep, E, ). 5Li deduced resonances. 1968VI03: 6Li(3He, p), E 2 MeV; 5Li; measured...

  16. 9Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    deduced log ft, Gamow-Teller transition strength, level width, di-neutron, neutron halo roles. 1991LUZZ: 9Li(-); measured T12. 1992LI24: 9Li(-); measured NMR...

  17. 4Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li Ground-State Decay Evaluated Data Measured Ground-State Γcm(T1/2) for 4Li Adopted value: 91 ± 9 ys (2003AU02) Measured Mass Excess for 4Li Adopted value: 25320 ± 210 keV (2003AU02) Measurements 1960BR05: 4Li; measured not abstracted; deduced nuclear properties. 1960BR10: 4Li; measured not abstracted; deduced nuclear properties. 1960BR19: 4Li; measured not abstracted; deduced nuclear properties. 1960RO11: 4Li; measured not abstracted; deduced nuclear properties. 1963WE10: 4Li; measured not

  18. 11Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li β--Decay Evaluated Data Measurements 1969KL08: 11Li; measured T1/2. 1974RO31: 11Li; measured Eγ, Iγ, T1/2, delayed neutrons, βγ-coin, Eβ. 1975TH08: 11Li; measured neutron binding energy, delayed neutron branching ratio, T1/2; deduced log ft. 1979ANZZ: 11Li; 11Li deduced evidence for β-delayed 2n emission. 1979AZ03: 11Li; measured β-delayed En, nn-coin. 11Be levels deduced 1n, 2n decay probabilities. 1979DEYX, 1980DE39, 1980DEZF: 11Li; measured Eγ, Iγ, Iβ, β-delayed En, In; deduced

  19. 08Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Thermal Neutron Capture Evaluated Data Measurements 1967RA24: 7Li(n, γ), E = thermal; measured Eγ; deduced Q. 1973JUZT, 1973JUZU: 7Li(n, γ), E = thermal; measured σ(Eγ). 7Li deduced γ-branching. 1991LY01: 7Li(n, γ), E = thermal; measured Eγ, Iγ, capture σ. 1996BL10: 7Li(n, γ), E = 1.5-1340 eV; measured Eγ, Iγ, γ yield, absolute σ(E). 1997HEZW, 1998HE35: 7Li(n, γ), E ≈ 5 meV, 54 keV; measured σ. 1999ZHZM, 2000ZHZP: 7Li(n, γ), E = thermal; compiled, evaluated prompt γ-ray

  20. 10Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li Ground-State Decay Evaluated Data Measured Ground-State Γcm(T1/2) for 10Li Adopted value: 2.0 ± 0.5 zs (2003AU02) Measured Mass Excess for 10Li Adopted value: 33051 ± 15 keV (2003AU02) Measurements 1975WI26: 9Be(9Be, 8B), E = 121 MeV; measured σ(E(8B), θ); deduced Q. 10Li deduced mass excess. 1990AM05: 11B(π-, X), E at rest; measured inclusive p-, d-, t-spectra, X = 10Li production. 10Li deduced level, Γ. 1992AMZY: 11B(π-, X), E at rest; measured pion, deuteron, triton spectra. 10Li

  1. NMR Studies of the Vanadium Spin Dynamics and Spin Structure in LiV2O4, CaV2O4, and (LixV1-x)3BO5 (x is almost equal to 0.33, 0.40)

    SciTech Connect (OSTI)

    Xiaopeng Zong

    2007-12-01

    Strong electron correlation is believed to be an essential and unifying factor in diverse properties of condensed matter systems. Ground states that can arise due to electron correlation effects include Mott insulators, heavy fermion, ferromagnetism and antiferromagnetism, spin glasses, and high-temperature superconductivity. The electronic systems in transition metal oxide compounds are often highly correlated. In this thesis, the author presents experimental studies on three strongly correlated vanadium oxide compounds: LiV{sub 2}O{sub 4}, (Li{sub x}V{sub 1-x}){sub 3}BO{sub 5}, and CaV{sub 2}O{sub 4}, which have completely different ground states.

  2. 8Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    -asymmetry, NMR; deduced polarization. 1986WA01: 8Li(-); analyzed -delayed breakup -spectra; deduced intruder states role. 8Be deduced level, , Gamow-Teller matrix...

  3. A=9Li (1974AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 9Li) GENERAL: See also Table 9.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1966BA26). Special reactions: (1965DO13, 1966GA15, 1966KL1C, 1967AU1B, 1967CA1J, 1967HA10, 1968DO1C, 1972VO06, 1973KO1D, 1973MU12, 1973WI15). Other topics: (1972CA37, 1972PN1A, 1973JU2A). Ground state properties: (1966BA26, , 1969JA1M). Mass of 9Li: From the Q-value of 18O(7Li, 16O)9Li, the atomic mass excess of 9Li is 24.9654 ± 0.005 MeV (1969NE1E; prelim.

  4. Jennifer Li | Photosynthetic Antenna Research Center

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Jennifer Li Jennifer Li Jennifer Li E-mail: jennifer.li

  5. Anodic reactions in the Ca/CaCrO/sub 4/ thermal battery

    SciTech Connect (OSTI)

    Guidotti, R.A.; Reinhardt, F.W.

    1985-09-01

    The reaction of Ca with a CaCrO/sub 4/-(LiCl-KCl eutectic) solution at temperatures of 400/sup 0/C to 500/sup 0/C was studied to better understand the nature of the chemical reactions and electrochemical processes that occur in the Ca/CaCrO/sub 4/ thermal battery at the anode during activation and discharge. Limited tests also were conducted with a CaCrO/sub 4/-(CaCl/sub 2/-NaCl-KCl eutectic) solution at 550/sup 0/C. Ca/CaCrO/sub 4/ and CaLi/sub 2//CaCrO/sub 4/ single cells were tested to observe the relative performance differences of Ca and CaLi/sub 2/ anodes. The discharged cells were analyzed by optical microscopy, electron microprobe, Auger electron spectroscopy, and secondary-ion mass spectroscopy. These analytical data were used in conjunction with the results of chemical-reaction experiments to propose a discharge mechanism for the Ca/CaCrO/sub 4/ thermal battery, consistent with experimental observations.

  6. F LI

    Office of Legacy Management (LM)

    >"- -- F LI c ------- RADIATION SURVEY REPORT OF THE M IDDLESEX LANDFILL SITE RADIATION SURVEY REPORT OF THE ~IDDLESEX LfiMDFI.LL S I:TE it%RCH 25 - AFRiL 4, 1374 ;)UNE 27, 1974 T.!BLE OF CONTENTS Introduction and Summary . . . . . . . . . . . . . . . 1 Conclusions. . . . . . w . . . . . . , . . . , . . . . 2 Histohcal Background0 . . . . . . . . . . . . b (I . . 2 Description of Area Surveyed . . . . . . . . I . . . * 3 Survey Findings. * *,. a . . . , . . . . . . . . . . . 4 Surface

  7. 6Li General Tables

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li General Table The General Table for 6Li is subdivided into the following categories: Ground State Properties of 6Li Special States Theoretical Shell Model Cluster Models Complex...

  8. 7Li Cross Section

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    7Li(, '): emission yield 1.0 - 3.4 1 01182012 2011YA02 7Li(, ): elastic scattering differential 1.0 - 4.5 cm 170 07192011 7Li(, p): differential...

  9. X-ray absorption studies of mixed salt polymer electrolytes: ZnBr{sub 2}/CaBr{sub 2}-PEO, ZnBr{sub 2}/LiBr-PEO, and ZnBr{sub 2}/RbBr-PEO complexes

    SciTech Connect (OSTI)

    McBreen, J.; Yang, X.Q.; Lee, H.S.; Okamoto, Y.

    1995-02-01

    Polyethylene oxide (PEO)-salt systems are an important new class of electrolytes that are being considered for many uses. X-ray absorption (XAS) studies of ZnBr{sub 2}-PEO complexes, at the Zn K edge, at temperatures between 25 and 120 C, indicate that additions of bromide salts of Li, Rb, or Ca result in the formation of ZnBr{sub 4}{sup {minus} 2} complexes with a Zn-Br bond length of 2.42 {angstrom}. XAS, at the Rb K edge, in mixed RbBr/ZnBr{sub 2}-PEO complexes with an excess of ZnBr{sub 2}, shows that the ZnBr{sub 2} causes the RbBr to dissolve in the polymer. The Rb{sup +} ions are weakly complexed with the PEO with an Rb-O bond distance of 2.93 {angstrom}.

  10. CA.0

    Office of Legacy Management (LM)

    offergy Washington, DC 20545 *. CA.0 MAY 2 9 1987 .r ,. Hr. Carl Schafer Director of Environmental Poli,cy Office of the Deputy Assistant Secretary of Defense for Installations ...

  11. CA.0

    Office of Legacy Management (LM)

    of_f$ergy Washington, DC 20545 *. CA.0 MAY 2 9 1987 .r ,. Hr. Carl Schafer Director of Environmental Poli,cy Office of the Deputy Assistant Secretary of Defense for Installations Pentagon . ..&&&.@.&&;-D.C. 20301 Dear Mr.~:Schafer: As you know, the Department of Ene,rgy (DOE) is implementing a program to identify sites that may be radiologically contaminated as a result of DOE predecessor operations and to correct any pioblems associated with this contamination if there is

  12. 5Li General Tables

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Table for 5Li is subdivided into the folowing categories: Ground State Properties Cluster Model Shell Model Special States Model Calculations Model Discussions Complex...

  13. THE HIGH TEMPERATURE CHEMICAL REACTIVITY OF LI2O

    SciTech Connect (OSTI)

    Kessinger, G.; Missimer, D.

    2009-11-13

    The ultimate purpose of this study was to investigate the use of a Li-Ca mixture for direct reduction of actinide oxides to actinide metals at temperatures below 1500 C. For such a process to be successful, the products of the reduction reaction, actinide metals, Li{sub 2}O, and CaO, must all be liquid at the reaction temperature so the resulting actinide metal can coalesce and be recovered as a monolith. Since the established melting temperature of Li{sub 2}O is in the range 1427-1700 C and the melting temperature of CaO is 2654 C, the Li{sub 2}O-CaO (lithium oxidecalcium oxide) pseudo-binary system was investigated in an attempt to identify the presence of low-melting eutectic compositions. The results of our investigation indicate that there is no evidence of ternary Li-Ca-O phases or solutions melting below 1200 C. In the 1200-1500 C range utilizing MgO crucibles, there is some evidence for the formation of a ternary phase; however, it was not possible to determine the phase composition. The results of experiments performed with ZrO{sub 2} crucibles in the same temperature range did not show the formation of the possible ternary phase seen in the earlier experiment involving MgO crucibles, so it was not possible to confirm the possibility that a ternary Li-Ca-O or Li-Mg-O phase was formed. It appears that the Li{sub 2}O-CaO materials reacted, to some extent, with all of the container materials, alumina (Al{sub 2}O{sub 3}), magnesia (MgO), zirconia (ZrO{sub 2}), and 95% Pt-5% Au; however, to clarify the situation additional experiments are required. In addition to the primary purpose of this study, the results of this investigation led to the conclusions that: (1) The melting temperature of Li{sub 2}O may be as low as 1250 C, which is considerably lower than the previously published values in the range 1427-1700 C; (2) Lithium oxide (Li{sub 2}O) vaporizes congruently; (3) Lithium carbonate and Li2O react with 95% Pt-5% Au, and also reacts with pure Pt; and (4

  14. 7Li General Tables

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li General Table The General Table for 7Li is subdivided into the following categories: Reviews Ground State Properties Shell Model Cluster Model Other Theoretical Work Model Calculations Photodisintegration Polarization Fission and Fusion Elastic and Inelastic Scattering Projectile Fragmentation and Multifragmentation Astrophysical Hyperfine Structure b-decay Muons Hypernuclei and Mesons Hypernuclei and Baryons Pion, Kaon and Eta-Mesons Other Work Applications

  15. 8Li General Tables

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li General Tables The General Table for 8Li is subdivided into the following categories: Reviews Ground State Properties Shell Model Cluster Model Other Models Photodissociation Fusion and Fission Elastic and Inelastic Scattering Fragmentation Reactions Astrophysical b Decay Hypernuclei Pions, Kaons and h-mesons

  16. 9Li General Tables

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li General Table The General Table for 9Li is subdivided into the following categories: Shell Model Cluster Model Theoretical Ground State Properties Special States Other Model Calculations Complex Reactions Beta-Decay Pions Muons Photodisintegration Elastic and Inelastic Scattering Electromagnetic Transitions Astrophysical

  17. Presence of Li clusters in molten LiCl-Li

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Merwin, Augustus; Phillips, William C.; Williamson, Mark A.; Willit, James L.; Motsegood, Perry N.; Chidambaram, Dev

    2016-05-05

    Molten mixtures of lithium chloride and metallic lithium are of significant interest in various metal oxide reduction processes. These solutions have been reported to exhibit seemingly anomalous physical characteristics that lack a comprehensive explanation. ln the current work, the physical chemistry of molten solutions of lithium chloride and metallic lithium, with and without lithium oxide, was investigated using in situ Raman spectroscopy. The Raman spectra obtained from these solutions were in agreement with the previously reported spectrum of the lithium cluster, Li8. Furthermore, this observation is indicative of a nanofluid type colloidal suspension of Li8, in a molten salt matrix.more » It is suggested that the formation and suspension of lithium clusters in lithium chloride is the cause of various phenomena exhibited by these solutions that were previously unexplainable.« less

  18. Characterization of cathodic corrosion products in the Ca/CaCrO/sub 4/ thermal battery

    SciTech Connect (OSTI)

    Guidotti, R.A.; Reinhardt, F.W.; Venturini, E.L.; Rogers, J.W. Jr.; Cathey, W.N.

    1985-05-01

    Using thermal analysis techniques, we investigated the corrosion process resulting from the reaction of iron, nickel, and stainless steel (used as current collectors in Ca/CaCrO/sub 4/ thermal batteries) with CaCrO/sub 4/ dissolved in LiCl-KCl eutectic. The reaction product for iron was synthesized in bulk external to the battery and was characterized by chemical analysis, X-ray diffraction, Moessbauer spectroscopy, X-ray photoelectron spectroscopy, static magnetization, and electrical conductivity. This characterization provides a better understanding of the cathodic corrosion processes that occur in the Ca/CaCrO/sub 4/ thermal battery, and how the properties of the reaction layer at the catholyte-current collector interface influence battery performance.

  19. 6Li Cross Section

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    α, X) (Current as of 02/01/2016) NSR Reaction Eα (MeV) Cross Section File X4 Dataset Date Added 1985NE05 6Li(α, γ): γ thick target yield resonance X4 02/15/2012 1966FO05 6Li(α, γ): σ 0.9 - 3.0 2 < Eγ < 4 MeV, 4 < Eγ < 7 MeV, thick target capture γ-ray yield, capture γ-ray yield of 2.43 MeV resonance 02/29/2012 1989BA24 6Li(α, γ): σ 1.085, 1.175 X4 02/15/2012 1979SP01 6Li(α, γ): thick target yield curve for 718 keV γ-rays 1140 - 1250 keV 1175 keV resonance 07/19/2011

  20. 6Li Cross Section

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    p, X) (Current as of 03012016) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 2004TU02 6Li(p, ): coincidence yields, deduced S-factors low 1, S-factors from ...

  1. 7Li Cross Section

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    p, X) (Current as of 12162015) NSR Reaction Ep (MeV) Cross Section File X4 Dataset Date Added 1997GO13 7Li(pol. p, ): total , S-factor for capture to third-excited state 0 - ...

  2. Li-Z

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Analysis of Cloud Spectral Radiance/Irradiance at the Surface and Top-of-the-Atmosphere from Modeling and Observations Z. Li and A. Trishchenko Canada Centre for Remote Sensing Ottawa, Ontario, Canada M. Cribb Intermap Technologies Ltd. Ottawa, Ontario, Canada Introduction In view of some reported discrepancies concerning cloud parameter retrievals and cloud absorption (Stephens and Tsay 1990; Li et al. 1999; Rossow and Schiffer 1999) it is useful to compare cloud spectral signatures derived

  3. 10Li General Tables

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li General Table The General Table for 10Li is subdivided into the following categories: Reviews Theoretical Ground State Properties Shell Model Cluster Model Other Models Special States Astrophysical Electromagnetic Transitions Hypernuclei Photodisintegration Light-Ion and Neutron Induced Reactions These General Tables correspond to the 2003 preliminary evaluation of ``Energy Levels of Light Nuclei, A = 10''. The prepublication version of A = 10 is available on this website in PDF format: A =

  4. A=6Li (1984AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 6Li) GENERAL: See also (1979AJ01) and Table 6.2 [Table of Energy Levels] (in PDF or PS). Shell model: (1978CH1D, 1978ST19, 1979CA06, 1980MA41, 1981BO1Y, 1982BA52, 1982FI13, 1982LO09). Cluster and α-particle models: (1978OS07, 1978PL1A, 1978RE1A, 1978SI14, 1979BE39, 1979CA06, 1979LU1A, 1979WI1B, 1980BA04, 1980KU1G, 1981BE1K, 1981HA1Y, 1981KR1J, 1981KU13, 1981VE04, 1981ZH1D, 1982AH09, 1982CH10, 1982GO1G, 1982JI1A, 1982KA24, 1982KR1B, 1982KR09, 1982KU05,

  5. Development of electrically insulating CaO coatings

    SciTech Connect (OSTI)

    Natesan, K.; Reed, C.B.; Uz, M.; Rink, D.L.

    1998-09-01

    A systematic study has been initiated to develop electrically insulating CaO coatings by vapor phase transport and by in-situ formation in a liquid Li environment. Several experiments were conducted in vapor transport studies with variations in process temperature, time, specimen location, specimen surface preparation, and pretreatment. Several of the coatings obtained by the method exhibited Ca concentration in the range of 60--95 wt.% on the surface. However, coating thickness has not been very uniform among several samples exposed in the same run or even within the same sample. The coatings developed in these early tests degraded after 24 h exposure to Li at 500 C. Additional experiments are underway to develop better-adhering and more dense coatings by this method. A program to develop in-situ CaO coatings in Li has been initiated, and the first set of capsule tests at 800 C in three different Li-Ca mixtures will be completed in early July. Specimens included in the run are bare V-4Cr-4Ti alloy, specimens with a grit-blasted surface and O-precharged in 99.999% Ar, polished specimens precharged in a 99.999% Ar and 5000 ppm O{sub 2}-N{sub 2} mixture, and prealuminized V-5Cr-5Ti alloy preoxidized in a 5000 ppm O{sub 2}-N{sub 2} mixture. Additional experiments at lower temperatures are planned.

  6. The SpallaTion

    Office of Environmental Management (EM)

    The Science Behind Cheaper Biofuels The Science Behind Cheaper Biofuels August 15, 2011 - 11:50am Addthis Brookhaven National Laboratory is modeling the metabolic processes in rapeseed plants to optimize production of plant oils for biofuels. Shown above are developing embryos extracted from a growing rapeseed plant. The embryos accumulate seed oils which represent the most energy-dense form of biologically stored sunlight, and have great potential as renewable resources for fuel and industrial

  7. Li Tec | Open Energy Information

    Open Energy Info (EERE)

    Drezden, Germany Product: Based in Kamez, near Dresden, Li-Tec produces components for lithium-ion batteries. References: Li-Tec1 This article is a stub. You can help OpenEI by...

  8. I!' L;I)

    Office of Legacy Management (LM)

    ".>;jy i.~jp.~[~~ i,Zz>-c C,+;) ir,i:%J :' 0 p 'd-i I /) f) ic.c iq -.I ,'c i - * w. 3'2 , phi ': r-t;, ; *.i .; I!' L;I) --, -II s;.,yE;J-~,~;~* I' ;, f: >,p.yg ,p ' .L (3 i!>;' !i.3 y/y!-; x>:-y rJgbf;..qp: \' :sF*:l,' 5-".13, -9 _ ..-;~c~-' ~;Li;-~~~~;, 3h' ;[;i-y ; c; ' 1' 1.b y&k' 2 1 , . ..l =i. 1; G.1 ;Tr.; .j. i-:. I qr:i.gky, M,C. Jp, 2.1 F... ii, Ross CENTRAL F ILES ~"CTIVE OF TXIP m --w- The 0' 0 jet% ive Of this trip xas to evaluate tkie !- .zalth

  9. Chemical stability and Ce doping of LiMgAlF6 neutron scintillator

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Du, M. H.

    2014-11-13

    We perform density functional calculations to investigate LiMgAlF6 as a potential neutron scintillator material. The calculations of enthalpy of formation and phase diagram show that single-phase LiMgAlF6 can be grown but it should be more difficult than growing LiCaAlF6 and LiSrAlF6. Moreover, the formation energy calculations for substitutional Ce show that the concentration of Ce on the Al site is negligible but a high concentration (>1 at.%) of Ce on the Mg site is attainable provided that the Fermi level is more than 5 eV lower than the conduction band minimum. Acceptor doping should promote Ce incorporation in LiMgAlF6.

  10. 7Li MRI of Li batteries reveals location of microstructural lithium...

    Office of Scientific and Technical Information (OSTI)

    SciTech Connect Search Results Journal Article: 7Li MRI of Li batteries reveals location of microstructural lithium Citation Details In-Document Search Title: 7Li MRI of Li ...

  11. Recent developments in Li(Si)/FeS/sub 2/ thermal battery technology

    SciTech Connect (OSTI)

    Searcy, J.Q.; Quinn, R.K.; Saxton, H.J.

    1982-01-01

    The Li(Si)/FeS/sub 2/ electrochemical system has been under development for thermal battery applications as an alternative to Ca/CaCrO/sub 4/ for several years at Sandia National Laboratories (SNL). The new technology differs from the old in that the anode is a pressed powder (44 wt % lithium in Li(Si) alloy) as opposed to sheet calcium or bimetal; and a separator composed of LiCl.KCl eutectic electrolyte and MgO binder is required with a separate cathode pellet composed of FeS/sub 2/ and electrolyte to replace the DEB pellet; and current collectors which may actually function as temperature moderators are always used. The applications require high reliability (typically, a success probability of 0.995) and a twenty-five year shelf-life. Consequently, a substantial materials effort has been necessary to assess degradation and deleterious reactions during storage and to determine necessary production specifications and controls. Experience with several applications has indicated that Li(Si)/FeS/sub 2/ thermal batteries are easier to develop and produce than those which use Ca/CaCrO/sub 4/. Furthermore, the new system is more capable and more forgiving. Therefore, an effort has been initiated to develop the new technology for all SNL thermal battery applications. This paper reviews both the materials-related development and the progress toward utilization of Li(Si)/FeS/sub 2/ for all SNL thermal battery applications.

  12. UJ LiJ

    Office of Legacy Management (LM)

    o >- tD o UJ :> LiJ o W ~ Central Nevada-23 UNITED STATES DEPARTMENT OF THE INTERIOR GEOLOGICAL SURVEY Federal Center, Denver, Colorado 80225 ANALYSIS OF HYDRAULIC TESTS IN HOT CREEK VALLEY, NEVADA June 1970 Open-file report Prepared Under Contract AT(29-2)-474 for the Nevada Operations Office U.S. Atomic Energy Commission USGS-474-82 DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor

  13. A=11Li (2012KE01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    E(11Li) 246 MeVA, analysis of a complete three-body kinematical measurement of 11Li breakup on a 12C target indicates the reaction mechanism is 11Li inelastic scattering to...

  14. A=5Li (1974AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 5Li) GENERAL: See also (1966LA04) and Table 5.5 [Table of Energy Levels] (in PDF or PS) here. Shell model calculations: (1966FR1B, 1968GO01, 1969GO1G, 1970RA1D, 1971RA15, 1972LE1L, 1973HA49). Cluster calculations: (1965NE1B, 1971HE05). Special levels: (1970HE1D, 1971HE05, 1971RA15, 1973JO1J). Electromagnetic transitions:(1973HA49). General reviews: (1966DE1E). Special reactions: (1971CH31). Other topics: (1968GO01, 1970RA1J, 1971CH50, 1971ZA1D, 1972CA37,

  15. A=6Li (1988AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 6Li) GENERAL: See also (1984AJ01) and Table 6.2 [Table of Energy Levels] (in PDF or PS). Shell model: (1983LE14, 1983VA31, 1984AS07, 1984PA08, 1984REZZ, 1984VA06, 1984ZW1A, 1985ER06, 1985FI1E, 1985LO1A, 1986AV08, 1986LE21, 1987KI1C, 1988WO04). Cluster and α-particle models: (1981PL1A, 1982WE15, 1983CA13, 1983DZ1A, 1983FO03, 1983GA12, 1983GO17, 1983SA39, 1983SM04, 1984BE37, 1984CO08, 1984DU17, 1984GL02, 1984JO1A, 1984KH05, 1984KR10, 1984KU03, 1984LA33,

  16. A=7Li (1979AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    9AJ01) (See Energy Level Diagrams for 7Li) GENERAL: See also (1974AJ01) and Table 7.2 [Table of Energy Levels] (in PDF or PS). Shell model: (1974KA11, 1975DI04, 1977ST04, 1978BO31). Collective, rotational or deformed models: (1974BO25, 1976BR26). Cluster and α-particle models: (1973HO1A, 1974GR24, 1974KA11, 1975KU1H, 1975GR26, 1975MI09, 1975PA11, 1975RO1B, 1977BE50, 1977MI03, 1977SA22, 1978RA09). Astrophysical questions: (1973BA1H, 1973CA1B, 1973CO1B, 1973IB1A, 1973SM1A, 1973TI1A, 1973TR1B,

  17. A=9Li (1979AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    9AJ01) (See Energy Level Diagrams for 9Li) GENERAL: See also (1974AJ01) and Table 9.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1974IR04, 1976IR1B, 1977JA14). Special reactions: (1975AB1D, 1975ZE01, 1976AL1F, 1976BE67, 1976BU16, 1977YA1B). Pion and kaon reactions (See also reaction 3.): (1973CA1C, 1976TR1A, 1977BA1Q, 1977DO06, 1977SH1C). Other topics: (1970KA1A, 1973TO16, 1974IR04, 1975BE56, 1976IR1B). Ground state properties: (1975BE31). μ = 3.4359 ± 0.0010 nm (1976CO1L;

  18. Lithium salts for advanced lithium batteries: Li-metal, Li-O2, and Li-S

    SciTech Connect (OSTI)

    Younesi, Reza; Veith, Gabriel M.; Johansson, Patrik; Edstrom, Kristina; Vegge, Tejs

    2015-06-01

    Presently lithium hexafluorophosphate (LiPF6) is the dominant Li-salt used in commercial rechargeable lithium-ion batteries (LIBs) based on a graphite anode and a 3-4 V cathode material. While LiPF6 is not the ideal Li-salt for every important electrolyte property, it has a uniquely suitable combination of properties (temperature range, passivation, conductivity, etc.) rendering it the overall best Li-salt for LIBs. However, this may not necessarily be true for other types of Li-based batteries. Indeed, next generation batteries, for example lithium-metal (Li-metal), lithium-oxygen (Li-O2), and lithium sulphur (Li-S), require a re-evaluation of Li-salts due to the different electrochemical and chemical reactions and conditions within such cells. Furthermore, this review explores the critical role Li-salts play in ensuring in these batteries viability.

  19. Lithium salts for advanced lithium batteries: Li-metal, Li-O2, and Li-S

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Younesi, Reza; Veith, Gabriel M.; Johansson, Patrik; Edstrom, Kristina; Vegge, Tejs

    2015-06-01

    Presently lithium hexafluorophosphate (LiPF6) is the dominant Li-salt used in commercial rechargeable lithium-ion batteries (LIBs) based on a graphite anode and a 3-4 V cathode material. While LiPF6 is not the ideal Li-salt for every important electrolyte property, it has a uniquely suitable combination of properties (temperature range, passivation, conductivity, etc.) rendering it the overall best Li-salt for LIBs. However, this may not necessarily be true for other types of Li-based batteries. Indeed, next generation batteries, for example lithium-metal (Li-metal), lithium-oxygen (Li-O2), and lithium sulphur (Li-S), require a re-evaluation of Li-salts due to the different electrochemical and chemical reactions andmore » conditions within such cells. Furthermore, this review explores the critical role Li-salts play in ensuring in these batteries viability.« less

  20. Lithium Salts for Advanced Lithium Batteries: Li-metal, Li-O2, and Li-S

    SciTech Connect (OSTI)

    Younesi, Reza; Veith, Gabriel M; Johansson, Patrik; Edstrom, Kristina; Vegge, Tejs

    2015-01-01

    Presently lithium hexafluorophosphate (LiPF6) is the dominant Li-salt used in commercial rechargeable lithium-ion batteries (LIBs) based on a graphite anode and a 3-4 V cathode material. While LiPF6 is not the ideal Li-salt for every important electrolyte property, it has a uniquely suitable combination of properties (temperature range, passivation, conductivity, etc.) rendering it the overall best Li-salt for LIBs. However, this may not necessarily be true for other types of Li-based batteries. Indeed, next generation batteries, for example lithium-metal (Li-metal), lithium-oxygen (Li-O2), and lithium sulphur (Li-S), require a re-evaluation of Li-salts due to the different electrochemical and chemical reactions and conditions within such cells. This review explores the critical role Li-salts play in ensuring in these batteries viability.

  1. Recovery of Li from alloys of Al- Li and Li- Al using engineered scavenger compounds

    DOE Patents [OSTI]

    Riley, W. D.; Jong, B. W.; Collins, W. K.; Gerdemann, S. J.

    1994-01-01

    A method of producing lithium of high purity from lithium aluminum alloys using an engineered scavenger compound, comprising: I) preparing an engineered scavenger compound by: a) mixing and heating compounds of TiO2 and Li2CO3 at a temperature sufficient to dry the compounds and convert Li.sub.2 CO.sub.3 to Li.sub.2 O; and b) mixing and heating the compounds at a temperature sufficient to produce a scavenger Li.sub.2 O.3TiO.sub.2 compound; II) loading the scavenger into one of two electrode baskets in a three electrode cell reactor and placing an Al-Li alloy in a second electrode basket of the three electrode cell reactor; III) heating the cell to a temperature sufficient to enable a mixture of KCl-LiCl contained in a crucible in the cell to reach its melting point and become a molten bath; IV) immersing the baskets in the bath until an electrical connection is made between the baskets to charge the scavenger compound with Li until there is an initial current and voltage followed by a fall off ending current and voltage; and V) making a connection between the basket electrode containing engineered scavenger compound and a steel rod electrode disposed between the basket electrodes and applying a current to cause Li to leave the scavenger compound and become electrodeposited on the steel rod electrode.

  2. A=14Li (1986AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    86AJ01) (Not illustrated) 14Li has not been observed. The calculated mass excess is 72.29 MeV: see (1981AJ01). 14Li is then particle unstable with respect to decay into 13Li + n and 12Li + 2n by 3.88 and 3.22 MeV, respectively

  3. A=15Li (1981AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    1AJ01) (Not illustrated) 15Li has not been observed: its atomic mass excess is calculated to be 81.60 MeV. It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.24 and 3.90 MeV, respectively (1974TH01). See also 13Li

  4. DOE - Office of Legacy Management -- Berkeley CA Site - CA 03

    Office of Legacy Management (LM)

    FUSRAP Considered Sites Berkeley, CA Alternate Name(s): University of California Gilman Hall, University of California CA.03-1 Location: Gilman Hall, University of California, ...

  5. Microsoft Word - li_abstract

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    will be served at 3:30 pm A few new issues regarding the density dependence of nuclear symmetry energy Professor Bao-An Li Department of Physics and Astronomy, Texas A&M ...

  6. Women @ Energy: Yan Li | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Yan Li Women @ Energy: Yan Li March 12, 2013 - 9:23am Addthis Yan Li is a Computational Physicist at the Computational Science Center at Brookhaven National Laboratory. Yan Li is a Computational Physicist at the Computational Science Center at Brookhaven National Laboratory. Yan Li is a Computational Physicist at the Computational Science Center at Brookhaven National Laboratory. Her work is mainly focused on developing and applying advanced computational tools to investigate material properties

  7. Liang Li | Argonne National Laboratory

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Liang Li Postdoctoral Appointee (Supervisor, Maria Chan) Current research focuses on ab-initio theoretical studies on hybrid lithium-ion/lithium-oxygen battery materials and photocatalytic reduction of CO2. News Visualizing Redox Dynamics of a Single Ag/AgCl Heterogeneous Nanocatalyst at Atomic Resolution Telephone 630.252.2788 Fax 630.252.4646 E-mail liangli@anl.gov CV/Resume PDF icon Liang_Li

  8. Anion Coordination Interactions in Solvates with the Lithium Salts LiDCTA and LiTDI

    SciTech Connect (OSTI)

    McOwen, Dennis W.; Delp, Samuel A.; Paillard, Elie; Herriot, Cristelle; Han, Sang D.; Boyle, Paul D.; Sommer, Roger D.; Henderson, Wesley A.

    2014-04-17

    Lithium 4,5-dicyano-1,2,3-triazolate (LiDCTA) and lithium 2-trifluoromethyl-4,5-dicyanoimidazole (LiTDI) are two salts proposed for lithium battery electrolyte applications, but little is known about the manner in which the DCTA- and TDI- anions coordinate Li+ cations. To explore this in-depth, crystal structures are reported here for two solvates with LiDCTA: (G2)1:LiDCTA and (G1)1:LiDCTA with diglyme and monoglyme, respectively, and seven solvates with LiTDI: (G1)2:LiTDI, (G2)2:LiTDI, (G3)1:LiTDI, (THF)1:LiTDI, (EC)1:LiTDI, (PC)1:LiTDI and (DMC)1/2:LiTDI with monoglyme, diglyme, triglyme, tetrahydrofuran, ethylene carbonate, propylene carbonate and dimethyl carbonate, respectively. These latter solvate structures are compared with the previously reported acetonitrile (AN)2:LiTDI structure. The solvates indicate that the LiTDI salt is much less associated than the LiDCTA salt and that the ions in LiTDI, when aggregated in solvates, have a very similar TDI-...Li+ cation mode of coordination through both the anion ring and cyano nitrogen atoms. Such coordination facilitates the formation of polymeric ion aggregates, instead of dimers. Insight into such ion speciation is instrumental for understanding the electrolyte properties of aprotic solvent mixtures with these salts.

  9. A=12Li (1975AJ02)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    75AJ02) (Not illustrated) 12Li is not observed in the 4.8 GeV proton bombardment of a uranium target: it is particle unstable (1974BO05). Its atomic mass excess is therefore > 49.0 MeV. (1974TH01) calculate the mass excess of 12Li to be 52.92 MeV. 12Li would then be unstable with respect to 11Li + n, 10Li + 2n and 9Li + 3n by 3.9, 3.68 and 3.74 MeV, respectively. See also (1972TH13, 1973BO30, 1974IR04

  10. A=12Li (1990AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    90AJ01) (Not illustrated) 12Li is not observed in the 4.8 GeV proton bombardment of a uranium target: it is particle unstable. The calculated value of its mass excess is 52.93 MeV [see (1980AJ01)]: 12Li would then be unstable with respect to 11Li + n ,10Li + 2n and 9Li + 3n by 4.01, 2.96 and 3.76 MeV, respectively. The ground state of 12Li is predicted to have Jπ = 2- (1988POZS, 1985PO10; theor.). See also (1980AJ01

  11. A=4Li (1992TI02)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li (1992TI02) (See Energy Level Diagrams for 4Li) GENERAL: The stability of 8B against particle decay (1988AJ01), in particular against decay into 4He + 4Li, sets an upper limit of 1.7 MeV on the separation energy of 4Li into p + 3He (1952SH44). The instability of 4H against particle decay (see 4H, GENERAL section) makes the particle stability of 4Li very unlikely, since the Coulomb energy of 4Li is approximately 1.7 MeV larger than that of 4H (1963WE10), and the nuclear energies should be

  12. Magnetic and electrode properties, structure and phase relations of the layered triangular-lattice tellurate Li{sub 4}NiTeO{sub 6}

    SciTech Connect (OSTI)

    Zvereva, Elena A.; Nalbandyan, Vladimir B.; Evstigneeva, Maria A.; Koo, Hyun-Joo; Whangbo, Myung-Hwan; Ushakov, Arseni V.; Medvedev, Boris S.; Medvedeva, Larisa I.; Gridina, Nelly A.; Yalovega, Galina E.; Churikov, Alexei V.; Vasiliev, Alexander N.; Büchner, Bernd

    2015-05-15

    We examined the magnetic properties of layered oxide Li{sub 4}NiTeO{sub 6} by magnetic susceptibility, magnetization and ESR measurements and density functional calculations, and characterized phase relations, crystal structure and electrochemical properties of Li{sub 4}NiTeO{sub 6}. The magnetization and ESR data indicate the absence of a long-range magnetic order down to 1.8 K, and the magnetic susceptibility data the presence of dominant antiferromagnetic interactions. These observations are well accounted for by density functional calculations, which show that the spin exchanges of the LiNiTeO{sub 6} layers in Li{sub 4}NiTeO{sub 6} are strongly spin frustrated. The electrochemical charging of Li{sub 4}NiTeO{sub 6} takes place at constant potential of ca. 4.2 V vs. Li/Li{sup +} indicating two-phase process as confirmed by X-rays. The starting phase is only partially recovered on discharge due to side reactions. - Graphical abstract: No long-range magnetic order due to frustration in 2D triangular lattice antiferromagnet Li{sub 4}NiTeO{sub 6}. - Highlights: • Li{sub 4}NiTeO{sub 6} is 2D triangular lattice magnet with no long-range order down to 1.8 K. • Intralayer exchange interactions are antiferromagnetic and strongly spin frustrated. • The electrochemical Li extraction proceeds in a two-phase mode at 4.2 V vs. Li/Li{sup +}. • The electrochemical charge–discharge is only partially reversible. • Li{sub 2}O–NiO{sub y}–TeO{sub x} phase relations are reported; Li{sub 4}NiTeO{sub 6} is essentially stoichiometric.

  13. A=11Li (1980AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    80AJ01) (See the Isobar Diagram for 11Li) 11Li has been observed in the bombardment of iridium by 24 GeV protons. Its mass excess is 40.94 ± 0.08 MeV (1975TH08). The cross section for its formation is ~ 50 μb (1976TH1A). 11Li is bound: Eb for break up into 9Li + 2n and 10Li + n are 158 ± 80 and 960 ± 250 keV, respectively [see (1979AJ01) for discussions of the masses of 9Li and 10Li]. The half-life of 11Li is 8.5 ± 0.2 msec (1974RO31): it decays to neutron unstable states of 11Be [Pn =

  14. A=10Li (2004TI06)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    2004TI06) (See Energy Level Diagrams for 10Li) GENERAL: References to articles on general properties of 10Li published since the previous review (1988AJ01) are grouped into...

  15. Construction Consultants, L.I., Inc.

    Office of Environmental Management (EM)

    Mr. Eric Baumack Senior Project Manager Construction Consultants L.I., Inc. 36 East 2 nd ... worker employed by a subcontractor to Construction Consultants L.I., Inc. (CCLI) at the ...

  16. A=18Li (1995TI07)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li (1995TI07) (Not illustrated) 18Li has not been observed. Shell model calculations described in (1988POZS) predict the ground-state magentic dipole moment and charge and matter radii.

  17. A=20Li (1998TI06)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li (1998TI06) (Not observed) See (1977CE05, 1983ANZQ, 1986AN07, 1987SIZX).

  18. A=14Li (1976AJ04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    76AJ04) (Not illustrated) 14Li has not been observed: it is calculated to be particle unstable with a binding energy of -2.66 MeV for decay into 13Li + n and of -3.23 MeV for decay into 12Li + 2n. The calculated mass excess is 72.29 MeV (1974TH01)

  19. A=15Li (1976AJ04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    76AJ04) (Not illustrated) 15Li has not been observed: its atomic mass excess is calculated to be 81.60 MeV. It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.24 and 3.90 MeV, respectively (1974TH01)

  20. A=15Li (1986AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    6AJ01) (Not illustrated) 15Li has not been observed. Its atomic mass excess is calculated to be 81.60 MeV: see (1981AJ01). It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.24 and 3.90 MeV, repsectively

  1. A=11Li (1975AJ02)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    by GeV protons. Its mass excess is 40.9 0.1 MeV (1973KL1C). 11Li is bound: Eb for breakup into 9Li + 2n and 10Li + n are 0.2 and 0.3 MeV, respectively see (1974AJ01) for a...

  2. A=13Li (1976AJ04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    13Li is predicted to have an atomic mass excess of 61.56 MeV: it is then unstable for breakup into 12Li + n and 11Li + 2n by 0.6 and 4.5 MeV, respectively (1974TH01). The modified...

  3. A=13Li (1981AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    13Li is predicted to have an atomic mass excess of 61.56 MeV: it is then unstable for breakup into 12Li + n and 11Li + 2n by 0.6 and 4.5 MeV, respectively (1974TH01). The modified...

  4. A=8Li (2004TI06)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    p)8Li Qm 0.80079 Angular distributions have been obtained at Et 23 MeV for the proton groups to 8Li*(0, 0.98, 2.26, 6.54 0.03); cm for 8Li*(2.26, 6.54) are 35 10 and 35...

  5. A=8Li (66LA04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    to the geometric value, supports the hypothesis that 7Li may be described as an ( + t) cluster (RO62C). See also (AL63N, BA63O, BR63M, VA64G). 9. 7Li(d, p)8Li Qm -0.192...

  6. Recovery of Li from alloys of Al-Li and Li-Al using engineered scavenger compounds

    SciTech Connect (OSTI)

    Riley, W.D.; Jong, B.W.; Collins, W.K.; Gerdemann, S.J.

    1992-01-01

    The invention relates to a process for obtaining Li metal selectively recovered from Li-Al or Al-Li alloy scrap by: (1) removing Li from aluminum-lithium alloys at temperatures between about 400 C-750 C in a molten salt bath of KC1-LiCl using lithium titanate (Li2O.3TiO2) as an engineered scavenger compound (ESC); and (2) electrodepositing of Li from the loaded ESC to a stainless steel electrode. By use of the second step, the ESC is prepared for reuse. A molten salt bath is required in the invention because of the inability of molten aluminum alloys to wet the ESC.

  7. A=12Li (1985AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    5AJ01) (Not illustrated) 12Li is not observed in the 4.8 GeV proton bombardment of a uranium target: it is particle-unstable. The calculated value of its mass excess is 52.93 MeV [see (1980AJ01)]: 12Li would then be unstable with respect to 11Li + n, 10Li + 2n and 9Li + 3n by 3.92, 2.96 and 3.76 MeV, respectively. See also (1980AJ01) and (1982KA1D, 1983ANZQ, 1984VA06

  8. A=13Li (1986AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    86AJ01) (Not illustrated) 13Li has not been observed. The calculated value of its mass excess is 60.34 MeV [see (1981AJ01)]: 13Li would then be unstable with respect to 11Li + 2n by 3.26 MeV. (1980BO31) have not observed 13Li in the bombardment of 124Sn by 6.7 GeV protons but state that the statistics were poor in the region of interest and that it is not excluded that 13Li may be stable. See also (1983ANZQ

  9. A=11Li (1985AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    5AJ01) (See the Isobar Diagram for 11Li) GENERAL: The mass excess of 11Li is 40.94 ± 0.08 MeV (1975TH08). [(A.H. Wapstra, private communication) suggests 40.91 ± 0.11 MeV.] Using the value reported by (1975TH08) 11Li is bound with respect to 9Li + 2n by 156 ± 80 keV and with respect to 10Li + n by 966 ± 260 keV [see (1984AJ01) for the masses of 9Li and 10Li]. Systematics suggest Jπ = 1/2- for 11Lig.s.. See also (1979AZ03, 1980AZ01, 1980BO31, 1981BO1X, 1982BO1Y, 1982OG02), (1981HA2C),

  10. A=9Li (59AJ76)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    59AJ76) (Not illustrated) Mass of 9Li: From the threshold for 9Be(d, 2p)9Li, Ed = 19 ± 1 MeV (GA51C), the mass excess of 9Li is determined as M - A = 28.1 ± 1 MeV. 1. 9Li(β-)9Be* --> 8Be + n Qm = 12.4 9Li decays to excited states of 9Be which decay by neutron emission. The mean of the reported half-lives is 0.169 ± 0.003 sec (GA51C, HO52B). See also (SH52, FR53A, BE55D, FL56, TA58B). 2. 9Be(d, 2p)9Li Qm = -15.5 The threshold is 19 ± 1 MeV (GA51C). 3. 11B(γ, 2p)9Li Qm = -31.4 See (SH52,

  11. A=9Li (66LA04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 9Li) GENERAL: See (GR64C). See also Table 9.1 [Table of Energy Levels] (in PDF or PS). Mass of 9Li: From the Q-value for 7Li(t, p)9Li: Q = -2.397 ± 0.020 MeV, the mass excess of 9Li is 24.965 ± 0.020 MeV (MI64E, MA65A). 1. 9Li(β-)9Be Qm = 13.615 9Li decays to the ground state (25 ± 15 %) and to the 2.43 MeV, neutron-unstable state of 9Be (75 ± 15 %). The β-endpoints are 13.5 ± 0.3 MeV and 11.0 ± 0.4 MeV; log ft = 5.5 ± 0.2 and 4.7 ± 0.2,

  12. CA.O-O

    Office of Legacy Management (LM)

    3sR L C, C II Department of Energy -e\ ' Washington, DC 20545 CA.O-O - 0 MAY 2 9 1987 Mr. Carl Schafer Director of Environmental Policy Office of the Deputy Assistant Secretary of Defense for Installations Pentagon Washington, D.C. 20301 Dear Mr. Schafer: As you know, the Department of Energy (DOE) is implementing a program to identify sites that may be radiologically contaminated as a result of DOE predecessor operations and to correct any problems associated with this contamination if there is

  13. Ca rlsbad Field Office

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    En ergy Ca rlsbad Field Office P. O . Box 3090 Carlsbad , New Mexico 88221 AUG 2 9 2013 Mr. John E. Kieling , Chief Hazardous Waste Bureau New Mexico Environment Department 2905 Rodeo Park Drive East, Building 1 Santa Fe, New Mexico 87505-6303 Subject: Notification of Class 1 Permit Modification to the Waste Isolation Pilot Plant Hazardous Waste Facility Permit Number: NM4890139088-TSDF Dear Mr. Kieling: Enclosed is a Class 1 Permit Modification Notification for the fo ll owing items: * Revise a

  14. li(1)-98.pdf

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    23 Radiative Forcing by Smoke Aerosols Determined from Satellite and Surface Measurements Z. Li Canada Centre for Remote Sensing Ottawa, Ontario, Canada L. Kou Intermap Technologies Ottawa, Ontario, Canada Introduction As a potential offsetting agent to the greenhouse effect, aerosols are receiving increasing attention in the atmospheric science community. Notwithstanding, our knowledge of the impact of aerosols on radiation and climate is rather poor and falls well behind that of the greenhouse

  15. li(1)-99.PDF

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Consistency Check of Cloud Optical Properties Derived from Satellite and Surface Observations Z. Li, A. P. Trishchenko, and F.-L. Chang Canada Center for Remote Sensing Ottawa, Canada H. W. Barker Atmospheric Environmental Service Downsview, Canada W. B. Sun Dalhousie University Halifax, Nova Scotia, Canada Introduction Much work has been done to retrieve both cloud and radiative variables using space-borne observations. Several recent studies also attempted to retrieve cloud optical depth using

  16. li(2)-98.pdf

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    7 A Consistency Analysis of ARESE Measurements Regarding Cloud Absorption Z. Li and A. Trishchenko Canada Centre for Remote Sensing Ottawa, Ontario, Canada H. W. Barker Atmospheric Environment Service Downsview, Ontario, Canada G. L. Stephens and P. Partain Colorado State University Fort Collins, Colorado P. Minnis NASA-Langley Research Center Hampton, Virginia Introduction In an attempt to resolve the recent debate over the cloud absorption anomaly, the U.S. Department of Energy sponsored a

  17. A=12Li (1980AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    0AJ01) (Not illustrated) 12Li is not observed in the 4.8 GeV proton bombardment of a uranium target: it is particle unstable. Its atomic mass excess would then be > 49.0 MeV. (1974TH01) calculate the mass excess of 12Li to be 52.92 MeV, while (1975JE02) calculate 52.94 MeV. Taking the average of these two values, 12Li would then be unstable with respect to 11Li + n, 10Li + 2n and 9Li + 3n by 3.92, 2.96 and 3.76 MeV, respectively. See also (1975AJ02) and (1975BE31, 1976IR1B

  18. A=14Li (1991AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    91AJ01) (Not illustrated) 14Li has not been observed. The calculated mass excess is 72.29 MeV: see (1981AJ01). 14Li is then particle unstable with respect to decay into 13Li + n and 12Li + 2n by 3.9 and 3.2 MeV, respectively [see, however, 13Li]. (1985PO10) calculate [in a (0 + 1)ℏω model space] that the first four states of 14Li at 0, 0.75, 1.22 and 1.48 MeV have, respectively, Jπ = 2-, 4-, 3- and 1-. See also (1986AL09, 1989OG1B) and (1988POZS; theor.)

  19. Local field effects at Li K edges in electron energy-loss spectra of Li, Li{sub 2}O and LiF

    SciTech Connect (OSTI)

    Mauchamp, V.; Moreau, P.; Ouvrard, G.; Boucher, F.

    2008-01-15

    Local field effects (LFEs) in low-losses of electron energy-loss spectra of Li, Li{sub 2}O, and LiF were calculated using the density functional theory under the generalized gradient approximation. By including the lithium 1s semicore state in the pseudopotentials, the amplitude of LFE was assessed all the way up to the Li K edge (from 0 to 80 eV). They are found to be much larger for semicore levels (2s of oxygen, 2s of fluorine, and 1s of lithium) than for the valence electron energy-loss region. LFEs at the Li K edge are studied in detail. In particular, for q=0 they are shown to increase with the inhomogeneities of the compounds (from Li to LiF). The influence of the magnitude and the direction of q is also presented. Both parameters have negligible effect in the case of Li metal but changes are quite substantial for Li{sub 2}O and LiF. This is in agreement with the isotropy and the delocalization of the metallic bonding as compared to the ionic one. LFEs at the Li K edge are, however, whatever the compound, much smaller than those observed at transition metal M{sub 2,3} edges situated at similar energy positions. This result can be accounted for by considering the wave functions associated with the initial and final states involved in both edges. For lithium battery materials, most often presenting a transition metal edge close to the Li K edge, these findings imply significant consequences with respect to the interpretation of their electron energy-loss spectroscopy spectra. In particular, LFE can be expected to be stronger in positive electrodes than in negative ones.

  20. Microsoft PowerPoint - Electrolytic T Extraction in Molten Li-LiT_2.pptx

    Office of Environmental Management (EM)

    Electrolytic Tritium Extraction in Molten Li-LiT Luke Olson Brenda L. García-Díaz Hector Colon-Mercado Joe Teprovich Dave Babineau Savannah River National Laboratory Fall 2015 Tritium Focus Group Meeting November 3-5, 2015 SRNL-STI-2015-00605 This presentation does not contain any proprietary, confidential, or otherwise restricted information LiT Electrolysis Options LiT Electrolysis Maroni Process (Baseline Option) Improve Liquid-Liquid Extraction & Electrolysis Process Intensification

  1. Li-rich anti-perovskite Li3OCl films with enhanced ionic conductivity

    SciTech Connect (OSTI)

    Lu, XJ; Wu, G; Howard, JW; Chen, AP; Zhao, YS; Daemen, LL; Jia, QX

    2014-08-13

    Anti-perovskite solid electrolyte films were prepared by pulsed laser deposition, and their room-temperature ionic conductivity can be improved by more than an order of magnitude in comparison with its bulk counterpart. The cyclability of Li3OCl films in contact with lithium was evaluated using a Li/Li3OCl/Li symmetric cell, showing self-stabilization during cycling test.

  2. A=16Li (1993TI07)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Li (1993TI07) (Not illustrated) This nucleus has not been observed. Shell model studies (1988POZS) are used to predict J and the magnetic dipole moment....

  3. A=5Li (2002TI10)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    2002TI10) (See Energy Level Diagrams for 5Li) GENERAL: References to articles on general properties of 5Li published since the previous review (1988AJ01) are grouped into categories and listed, along with brief descriptions of each item, in the General Tables for 5Li located on our website at (www.tunl.duke.edu/NuclData/General_Tables/5li.shtml). See also Table Prev. Table 5.3 preview 5.3 [Table of Energy Levels] (in PDF or PS). See also the A = 5 introductory discussion titled A = 5 resonance

  4. A=9Li (2004TI06)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    2004TI06) (See Energy Level Diagrams for 9Li) GENERAL: References to articles on general properties of 9Li published since the previous review (1988AJ01) are grouped into categories and listed, along with brief descriptions of each item, in the General Tables for 9Li located on our website at (www.tunl.duke.edu/nucldata/General_Tables/9li.shtml). See also Table Prev. Table 9.1 preview 9.1 [Table of Energy Levels] (in PDF or PS). Ground state properties: μ = 3.4391 ± 0.0006 μN (1983CO11). See

  5. Nanoscale LiFePO4 and Li4Ti5O12 for High Rate Li-ion Batteries

    SciTech Connect (OSTI)

    Jaiswal, A.; Horne, C.R.; Chang, O.; Zhang, W.; Kong, W.; Wang, E.; Chern, T.; Doeff, M. M.

    2009-08-04

    The electrochemical performances of nanoscale LiFePO4 and Li4Ti5O12 materials are described in this communication. The nanomaterials were synthesized by pyrolysis of an aerosol precursor. Both compositions required moderate heat-treatment to become electrochemically active. LiFePO4 nanoparticles were coated with a uniform, 2-4 nm thick carbon-coating using an organic precursor in the heat treatment step and showed high tap density of 1.24 g/cm3, in spite of 50-100 nm particle size and 2.9 wtpercent carbon content. Li4Ti5O12 nanoparticles were between 50-200 nm in size and showed tap density of 0.8 g/cm3. The nanomaterials were tested both in half cell configurations against Li-metal and also in LiFePO4/Li4Ti5O12 full cells. Nano-LiFePO4 showed high discharge rate capability with values of 150 and 138 mAh/g at C/25 and 5C, respectively, after constant C/25 charges. Nano-Li4Ti5O12 also showed high charge capability with values of 148 and 138 mAh/g at C/25 and 5C, respectively, after constant C/25 discharges; the discharge (lithiation) capability was comparatively slower. LiFePO4/Li4Ti5O12 full cells deliver charge/discharge capacity values of 150 and 122 mAh/g at C/5 and 5C, respectively.

  6. TOUGH2/EOS7CA

    Energy Science and Technology Software Center (OSTI)

    003504MLTPL00 EOS7CA Version 1.0: TOUGH2 Module for Gas Migration in Shallow Subsurface Porous Media Systems

  7. Antiperovskite Li 3 OCl superionic conductor films for solid...

    Office of Scientific and Technical Information (OSTI)

    Antiperovskite Li 3 OCl superionic conductor films for solid-state Li-ion batteries Citation Details In-Document Search Title: Antiperovskite Li 3 OCl superionic conductor films ...

  8. Electrochemistry of LiCl-Li2O-H2O Molten Salt Systems

    SciTech Connect (OSTI)

    Natalie J. Gese; Batric Pesic

    2013-03-01

    Uranium can be recovered from uranium oxide (UO2) spent fuel through the combination of the oxide reduction and electrorefining processes. During oxide reduction, the spent fuel is introduced to molten LiCl-Li2O salt at 650 degrees C and the UO2 is reduced to uranium metal via two routes: (1) electrochemically, and (2) chemically by lithium metal (Li0) that is produced electrochemically. However, the hygroscopic nature of both LiCl and Li2O leads to the formation of LiOH, contributing hydroxyl anions (OH-), the reduction of which interferes with the Li0 generation required for the chemical reduction of UO2. In order for the oxide reduction process to be an effective method for the treatment of uranium oxide fuel, the role of moisture in the LiCl-Li2O system must be understood. The behavior of moisture in the LiCl-Li2O molten salt system was studied using cyclic voltammetry, chronopotentiometry and chronoamperometry, while reduction to hydrogen was confirmed with gas chromatography.

  9. A=11Li (68AJ02)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    68AJ02) (See the Isobar Diagram for 11Li) 11Li has been identified in the 5.3 GeV proton bombardment of uranium. It is particle stable (PO66H). See also (GA66C, CO67A

  10. A=10Li (74AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    10B: see (HA68V), the mass excess of 10Li, (M - A) 33.10 0.06 MeV (AB73D). The breakup energy into 9Li + n is then -0.06 0.06 MeV. Using the calculated values suggested...

  11. A=8Li (59AJ76)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    one event corresponding to the transition to an excited state at 0.7 0.2 MeV. 3. 7Li(n, )8Li Qm 2.035 The thermal capture cross section is 33 5 mb (HU47A), 42 10 mb...

  12. Atsun Solar Electric Technology Co Ang Li Tiansheng | Open Energy...

    Open Energy Info (EERE)

    Co (Ang Li Tiansheng) Place: Zaozhuang, Shandong Province, China Product: Chinese PV cell and module maker. References: Atsun Solar Electric Technology Co (Ang Li...

  13. Enabling Future Li-Ion Battery Recycling | Argonne National Laboratory

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Future Li-Ion Battery Recycling Title Enabling Future Li-Ion Battery Recycling Publication Type Presentation Year of Publication 2014 Authors Gaines, LL Abstract Presentation made...

  14. Key Parameters Governing the Energy Density of Rechargeable Li...

    Office of Scientific and Technical Information (OSTI)

    of Rechargeable LiS Batteries Citation Details In-Document Search Title: Key Parameters Governing the Energy Density of Rechargeable LiS Batteries Authors: Gao, Jie ; ...

  15. Nanoscale imaging of fundamental Li battery chemistry: solid...

    Office of Scientific and Technical Information (OSTI)

    Nanoscale imaging of fundamental Li battery chemistry: solid-electrolyte interphase ... Citation Details In-Document Search Title: Nanoscale imaging of fundamental Li battery ...

  16. Electrode Materials for Rechargeable Li-ion Batteries: a New...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Electrode Materials for Rechargeable Li-ion Batteries: a New Synthetic Approach ... multiple cycles which enables Li-ion batteries with exceptionally high-power.

    This ...

  17. Li2Se as a Neutron Scintillator

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Du, Mao-Hua; Shi, Hongliang; Singh, David J.

    2015-06-23

    We show that Li2Se:Te is a potential neutron scintillator material based on density functional calculations. Li2Se exhibits a number of properties favorable for efficient neutron detection, such as a high Li concentration for neutron absorption, a small effective atomic mass and a low density for reduced sensitivity to background gamma rays, and a small band gap for a high light yield. Our calculations show that Te doping should lead to the formation of deep acceptor complex VLi-TeSe, which can facilitate efficient light emission, similar to the emission activation in Te doped ZnSe.

  18. A=6Li (2002TI10)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    2002TI10) (See Energy Level Diagrams for 6Li) GENERAL: References to articles on general properties of 6He published since the previous review (1988AJ01) are grouped into categories and isted, along with brief descriptions of each item, in the General Tables for 6Li located on our website at (www.tunl.duke.edu/NuclData/General_Tables/6li.shtml). See also Table Prev. Table 6.4 preview 6.4 [Table of Energy Levels] (in PDF or PS). Ground State Properties: μ = +0.8220473(6) nm, +0.8220567(3) nm:

  19. Southern CA Area | Open Energy Information

    Open Energy Info (EERE)

    CA Area Jump to: navigation, search Contents 1 Clean Energy Clusters in the Southern CA Area 1.1 Products and Services in the Southern CA Area 1.2 Research and Development...

  20. Antiperovskite Li 3 OCl superionic conductor films for solid-state Li-ion batteries

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Lü, Xujie; Howard, John W.; Chen, Aiping; Zhu, Jinlong; Li, Shuai; Wu, Gang; Dowden, Paul; Xu, Hongwu; Zhao, Yusheng; Jia, Quanxi

    2016-02-02

    We prepared antiperovskite Li3OCl superionic conductor films via pulsed laser deposition using a composite target. A significantly enhanced ionic conductivity of 2.0 × 10-4 S cm-1 at room temperature is achieved, and this value is more than two orders of magnitude higher than that of its bulk counterpart. Moreover, the applicability of Li3OCl as a solid electrolyte for Li-ion batteries is demonstrated.

  1. A=13Li (1991AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    91AJ01) (Not illustrated) 13Li has not been observed: see (1986AJ01). The calculated value of its mass excess is 60.34 MeV [see (1981AJ01)]: 13Li would then be unstable with respect to 11Li + 2n by 3.34 MeV. (1985PO10) calculate [in a (0 + 1)ℏω model space] that the first four states of 13Li at 0, 1.42, 2.09 and 2.77 MeV have, respectively, Jπ = 3/2-, 7/2-, 1/2-, 5/2-. See also (1987PE1C, 1989OG1B) and (1988POZS, 1988ZV1A

  2. A=15Li (1991AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    91AJ01) (Not illustrated) 15Li has not been observed. Its atomic mass excess is calculated to be 81.60 MeV: see (1981AJ01). It is then unstable with respect to decay into 14Li + n and 13Li + 2n by 1.2 and 5.1 MeV, respectively. (1985PO10) calculate [in a (0 + 1)ℏω model space] that the first four states of 15Li at 0, 0.73, 2.39 and 2.77 MeV have, respectively, Jπ = 3/2-, 1/2-, 7/2- and 5/2-. See also (1988POZS; theor.)

  3. Microsoft Word - li_z.doc

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    of Cloud Liquid Water Path and Its Potential for Rain Detection Z. Li, R. Chen, and F-L Chang Earth System Science Interdisciplinary Center, University of Maryland College Park,...

  4. A=11Li (1990AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    increase in matter radii with increasing A and do not support the idea of a neutron halo in 11Li (1988POZS; prelim.). See, however, (1988TA1A). Fragmentation cross sections of...

  5. A=8Li (74AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    cross section, comparable to the geometric value, is understood in terms of the ( + t) cluster nature of 7Li (RO62C). Cross sections for this reaction have recently been...

  6. A=7Li (59AJ76)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    59AJ76) (See the Energy Level Diagram for 7Li) GENERAL: See also Table 7.1 [Table of Energy Levels] (in PDF or PS). Theory: See (AU55, DA55, LA55A, AB56, FE56, KU56, ME56, FE57C, FR57, LE57F, MA57E, MA57J, SO57, HA58D, SK58). 1. 3H(α, γ)7Li Qm = 2.465 For Eα = 0.5 to 1.9 MeV, capture radiation is observed to 7Li(0) and 7Li*(0.48), with intensity ratio 5 : 2. The smooth rise of the cross section suggests a direct capture process. The angular distribution is not isotropic, indicating l > 0

  7. Materials Data on LiCaSn (SG:156) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  8. Materials Data on LiCaN (SG:62) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  9. Materials Data on LiCaPrTeO6 (SG:7) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  10. Construction Consultants, L.I., Inc.

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Mr. Eric Baumack Senior Project Manager Construction Consultants L.I., Inc. 36 East 2 nd Street Riverhead, New York 11901 WEL-2015-05 Dear Mr. Baumack: The Office of Enterprise Assessments' Office of Enforcement has completed an investigation into an electrical shock incident involving a worker employed by a subcontractor to Construction Consultants L.I., Inc. (CCLI) at the Brookhaven National Laboratory (BNL). CCLI is a first-tier subcontractor to Brookhaven Science Associates, LLC (BSA),

  11. Excitation functions of {sup 6,7}Li+{sup 7}Li reactions at low energies

    SciTech Connect (OSTI)

    Prepolec, L.; Soic, N.; Blagus, S.; Miljanic, D.; Siketic, Z.; Skukan, N.; Uroic, M.; Milin, M.

    2009-08-26

    Differential cross sections of {sup 6,7}Li+{sup 7}Li nuclear reactions have been measured at forward angles (10 deg. and 20 deg.), using particle identification detector telescopes, over the energy range 2.75-10.00 MeV. Excitation functions have been obtained for low-lying residual-nucleus states. The well pronounced peak in the excitation function of {sup 7}Li({sup 7}Li,{sup 4}He){sup 10}Be(3.37 MeV,2{sup +}) at beam energy about 8 MeV, first observed by Wyborny and Carlson in 1971 at 0 deg., has been observed at 10 deg., but is less evident at 20 deg. The cross section obtained for the {sup 7}Li({sup 7}Li,{sup 4}He){sup 10}Be(g.s,0{sup +}) reaction is about ten times smaller. The well pronounced peak in the excitation function of {sup 7}Li({sup 7}Li,{sup 4}He){sup 10}Be(3.37 MeV,2{sup +}) reaction could correspond to excited states in {sup 14}C, at excitation energies around 30 MeV.

  12. Ca

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ... Month selection is based on the least perturbation to the natural groundwater sytem due to well testingpumping, oil field activities, or other unnatural events causing ...

  13. Ca

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    James Bearzi, Chief Hazardous Waste Bureau New Mexico Environment Department 2905 Rodeo Park Drive East, Building 1 Santa Fe, New Mexico 87505-6303 April 27, 2010 Subject:...

  14. Ca

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    John Kieling , Acting Bureau Chief Hazardous Waste Bureau New Mexico Environment Department 2905 Rodeo Park Drive East, Bldg. 1 Santa Fe, NM 87505-6303 FEB 2 3 2012 Subject: Transmittal of the Final Audit Report for SRS/CCP Certification Audit A-1 2-04 Dear Mr. Kieling : This letter transmits the Final Audit Report for Carlsbad Field Office Audit A-12-04 of the Savannah River Site Central Chara cterization Project (SRS/CCP) processes performed to characterize and certify waste , as required by

  15. Ca

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    James Bearzi, Chief Hazardous Waste Bureau New Mexico Environment Department 2905 Rodeo Park Drive East, Building 1 Santa Fe, New Mexico 87505-6303 April 27, 2010 Subject: Notification of Sampling Line Loss, Waste Isolation Pilot Plant Permit Number NM4890139088-TSDF Dear Mr. Bearzi: The purpose of this letter is to transmit notification to the New Mexico Environment Department (NMED) of the loss of a hydrogen and methane monitoring sampling line and the results of the associated evaluation as

  16. A=5Li (1979AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    9AJ01) (See Energy Level Diagrams for 5Li) GENERAL: See also (1974AJ01) and Table 5.3 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1975KR1A). Special states: (1974GO13, 1974IR04, 1976IR1B). Astrophysical questions: (1974RA1C, 1978ME1C). Special reactions: (1975BR1A, 1976VA29, 1978ME1C). Reactions involving pions: (1973AR1B, 1974AM01). Applied topics: (1975HU1A). Other topics: (1974GO13, 1974IR04, 1976IR1B, 1978GO1D). Ground state of 5Li: (1975BE31). 1. 3He(d, γ)5Li Qm =

  17. A=5Li (59AJ76)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    59AJ76) (See the Energy Level Diagram for 5Li) See Table 5.3 [Table of Energy Levels] (in PDF or PS). 1. 3H(3He, n)5Li Qm = 10.297 Not reported. 2. 3He(d, γ)5Li Qm = 16.555 The excitation curve measured from Ed = 0.2 to 2.85 MeV shows a broad maximum at Ed = 0.45 ± 0.04 MeV (Eγ = 16.6 ± 0.2, σ = 50 ± 10 μb, Γγ = 11 ± 2 eV). Above this maximum, non-resonant capture is indicated by a slow rise of the cross section. The radiation appears to be isotropic to ± 10% at Ed = 0.58 MeV,

  18. A=6Li (1979AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    79AJ01) (See Energy Level Diagrams for 6Li) GENERAL: See also (1974AJ01) and Table 6.2 [Table of Energy Levels] (in PDF or PS) here. Shell model: (1974KA11, 1975DI04, 1975GO1B, 1975VE01, 1976CE03, 1976GH1A). Collective, rotational and deformed models: (1974BO25). Cluster and α-particle models: (1972KR1A, 1973DO09, 1973LI23, 1974BA30, 1974GR24, 1974JA1K, 1974KA11, 1974NO03, 1974PA1B, 1974SH08, 1974WO1B, 1975BL1C, 1975GO08, 1975GR26, 1975HA48, 1975KR1A, 1975LE1A, 1975LI1C, 1975MI09, 1975NO03,

  19. Re-evaluation of the eutectic region of the LiBr-KBr-LiF system

    SciTech Connect (OSTI)

    Redey, L.; Guidotti, R.A.

    1996-05-01

    The separator pellet in a thermal battery consists of electrolyte immobilized by a binder (typically, MgO powder). The melting point of the electrolyte determines the effective operating window for its use in a thermal battery. The development of a two-hour thermal battery required the use of a molten salt that had a lower melting point and larger liquidus range than the LiCl-KCl eutectic which melts at 352 C. Several candidate eutectic electrolyte systems were evaluated for their suitability for this application. One was the LiCl-LiBr-KBr eutectic used at Argonne National Laboratories for high-temperature rechargeable batteries for electric-vehicle applications. Using a custom-designed high-temperature conductivity cell, the authors were able to readily determine the liquidus region for the various compositions studied around the original eutectic for the LiBr-KBr-LiF system. The actual eutectic composition was found to be 60.0 m/o LiBr-37.5 m/o KBr-2.5 m/o LiF with a melting point of 324 {+-} 0.5 C.

  20. Low energy detectors: 6Li-glass scintillators (Conference) |...

    Office of Scientific and Technical Information (OSTI)

    Low energy detectors: 6Li-glass scintillators Citation Details In-Document Search Title: Low energy detectors: 6Li-glass scintillators You are accessing a document from the ...

  1. Hydrogen storage in LiH: A first principle study

    SciTech Connect (OSTI)

    Banger, Suman Nayak, Vikas Verma, U. P.

    2014-04-24

    First principles calculations have been performed on the Lithium hydride (LiH) using the full potential linearized augmented plane wave (FP-LAPW) method within the framework of density functional theory. We have extended our calculations for LiH+2H and LiH+6H in NaCl structure. The structural stability of three compounds have been studied. It is found that LiH with 6 added Hydrogen atoms is most stable. The obtained results for LiH are in good agreement with reported experimental data. Electronic structures of three compounds are also studied. Out of three the energy band gap in LiH is ∼3.0 eV and LiH+2H and LiH+6H are metallic.

  2. Shanghai Shen Li High Tech Co Ltd | Open Energy Information

    Open Energy Info (EERE)

    Shen Li High Tech Co Ltd Jump to: navigation, search Name: Shanghai Shen-Li High Tech Co Ltd Place: Shanghai, Shanghai Municipality, China Zip: 201400 Product: Focused on the...

  3. Predicting Reaction Sequences for Li-S Batteries - Joint Center...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    May 2, 2014, Research Highlights Predicting Reaction Sequences for Li-S Batteries Computed ... polysulfide species will be used to identify more stable electrolytes for Li-S batteries. ...

  4. Enforcement Letter, Construction Consultants L.I., Inc. | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Energy Construction Consultants L.I., Inc. Enforcement Letter, Construction Consultants L.I., Inc. December 4, 2015 Worker Safety and Health Enforcement Letter issued to Construction Consultants L.I., Inc. On December 4, 2015, the U.S. Department of Energy (DOE) Office of Enterprise Assessments' Office of Enforcement issued an Enforcement Letter (WEL-2015-05) to Construction Consultants L.I., Inc., relating to an electrical shock suffered by a subcontractor while working on a meteorological

  5. Predictive Models of Li-ion Battery Lifetime (Presentation) (Conference) |

    Office of Scientific and Technical Information (OSTI)

    SciTech Connect Predictive Models of Li-ion Battery Lifetime (Presentation) Citation Details In-Document Search Title: Predictive Models of Li-ion Battery Lifetime (Presentation) Predictive models of Li-ion battery reliability must consider a multiplicity of electrochemical, thermal and mechanical degradation modes experienced by batteries in application environments. Complicating matters, Li-ion batteries can experience several path dependent degradation trajectories dependent on storage

  6. Optimized Operating Range for Large-Format LiFePO4/Graphite Batteries

    SciTech Connect (OSTI)

    Jiang, Jiuchun; Shi, Wei; Zheng, Jianming; Zuo, Pengjian; Xiao, Jie; Chen, Xilin; Xu, Wu; Zhang, Jiguang

    2014-06-01

    e investigated the long-term cycling performance of large format 20Ah LiFePO4/graphite batteries when they are cycled in various state-of-charge (SOC) ranges. It is found that batteries cycled in the medium SOC range (ca. 20~80% SOC) exhibit superior cycling stability than batteries cycled at both ends (0-20% or 80-100%) of the SOC even though the capcity utilized in the medium SOC range is three times as large as those cycled at both ends of the SOC. Several non-destructive techniques, including a voltage interruption approach, model-based parameter identification, electrode impedance spectra analysis, ΔQ/ΔV analysis, and entropy change test, were used to investigate the performance of LiFePO4/graphite batteries within different SOC ranges. The results reveal that batteries at the ends of SOC exhibit much higher polarization impedance than those at the medium SOC range. These results can be attributed to the significant structural change of cathode and anode materials as revealed by the large entropy change within these ranges. The direct correlation between the polarization impedance and the cycle life of the batteries provides an effective methodology for battery management systems to control and prolong the cycle life of LiFePO4/graphite and other batteries.

  7. Probing the failure mechanism of nanoscale LiFePO₄ for Li-ion batteries

    SciTech Connect (OSTI)

    Gu, Meng; Shi, Wei; Zheng, Jianming; Yan, Pengfei; Zhang, Ji-guang; Wang, Chongmin

    2015-05-18

    LiFePO4 is a high power rate cathode material for lithium ion battery and shows remarkable capacity retention, featuring a 91% capacity retention after 3300 cycles. In this work, we use high-resolution transmission electron microscopy (HRTEM), energy dispersive x-ray spectroscopy (EDS), and electron energy loss spectroscopy (EELS) to study the gradual capacity fading mechanism of LiFePO4 materials. We found that upon prolonged electrochemical cycling of the battery, the LiFePO4 cathode shows surface amorphization and loss of oxygen species, which directly contribute to the gradual capacity fading of the battery. The finding is of great importance for the design and improvement of new LiFePO4 cathode for high-energy and high-power rechargeable battery for electric transportation.

  8. Thermal Stability of LiPF 6 Salt and Li-ion Battery Electrolytes...

    Office of Scientific and Technical Information (OSTI)

    In the presence of water (300 ppm) in the carrier gas, its decomposition onset temperature is lowered as a result of direct thermal reaction between LiPF 6 and water vapor to form ...

  9. 6Li foil thermal neutron detector

    SciTech Connect (OSTI)

    Ianakiev, Kiril D; Swinhoe, Martyn T; Favalli, Andrea; Chung, Kiwhan; Macarthur, Duncan W

    2010-01-01

    In this paper we report on the design of a multilayer thermal neutron detector based on {sup 6}Li reactive foil and thin film plastic scintillators. The {sup 6}Li foils have about twice the intrinsic efficiency of {sup 10}B films and about four times higher light output due to a unique combination of high energy of reaction particles, low self absorption, and low ionization density of tritons. The design configuration provides for double sided readout of the lithium foil resulting in a doubling of the efficiency relative to a classical reactive film detector and generating a pulse height distribution with a valley between neutron and gamma signals similar to {sup 3}He tubes. The tens of microns thickness of plastic scintillator limits the energy deposited by gamma rays, which provides the necessary neutron/gamma discrimination. We used MCNPX to model a multilayer Li foil detector design and compared it with the standard HLNCC-II (18 {sup 3}He tubes operated at 4 atm). The preliminary results of the {sup 6}Li configuration show higher efficiency and one third of the die-away time. These properties, combined with the very short dead time of the plastic scintillator, offer the potential of a very high performance detector.

  10. A=10Li (1988AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    MeV) corresponds to the ground state. 10Lig.s. would then be unbound with respect to breakup into 9Li + n by 0.80 0.25 MeV: see (1979AJ01). See also (1986GI10, 1987AB15),...

  11. A=10Li (1979AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    width of the ground state is 1.2 0.3 MeV. 10Lig.s. is unbound with respect to breakup into 9Li + n by 0.80 0.25 MeV (1975WI26). See also (1974BA15, 1974CE1A, 1974TH01,...

  12. A=10Li (1984AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    MeV) corresponds to the ground state. 10Lig.s. would the be unbound with respect to breakup into 9Li + n by 0.80 0.25 MeV (1975WI26). However (1979AB11, 1980AB16), on the...

  13. Epitaxial thin film growth of LiH using a liquid-Li atomic template

    SciTech Connect (OSTI)

    Oguchi, Hiroyuki; Ikeshoji, Tamio; Orimo, Shin-ichi; Ohsawa, Takeo; Shiraki, Susumu; Hitosugi, Taro; Kuwano, Hiroki

    2014-11-24

    We report on the synthesis of lithium hydride (LiH) epitaxial thin films through the hydrogenation of a Li melt, forming abrupt LiH/MgO interface. Experimental and first-principles molecular dynamics studies reveal a comprehensive microscopic picture of the crystallization processes, which sheds light on the fundamental atomistic growth processes that have remained unknown in the vapor-liquid-solid method. We found that the periodic structure that formed, because of the liquid-Li atoms at the film/MgO-substrate interface, serves as an atomic template for the epitaxial growth of LiH crystals. In contrast, films grown on the Al{sub 2}O{sub 3} substrates indicated polycrystalline films with a LiAlO{sub 2} secondary phase. These results and the proposed growth process provide insights into the preparation of other alkaline metal hydride thin films on oxides. Further, our investigations open the way to explore fundamental physics and chemistry of metal hydrides including possible phenomena that emerge at the heterointerfaces of metal hydrides.

  14. Correlation of anisotropy and directional conduction in β-Li3PS4 fast Li+ conductor

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Chen, Yan; Cai, Lu; Liu, Zengcai; dela Cruz, Clarina R.; Liang, Chengdu; An, Ke

    2015-07-06

    Our letter reports the correlation of anisotropy and directional conduction in the fast Li+ conductor β-Li3PS4, one of the low-symmetry crystalline electrolyte candidates. The material has both high conductivity and good stability that serves well for the large-scale energy storage applications of all-solid-state lithium ion batteries. The anisotropic physical properties, demonstrated here by the thermal expansion coefficients, are crucial for compatibility in the solid-state system and battery performance. Neutron and X-ray powder diffraction measurements were done to determine the crystal structure and thermal stability. Moreover, the crystallographic b-axis was revealed as a fast expansion direction, while negligible thermal expansion wasmore » observed along the a-axis around the battery operating temperatures. The anisotropic behavior has its structural origin from the Li+ conduction channels with incomplete Li occupancy and a flexible connection of LiS4 and PS4 tetrahedra within the framework. This indicates a strong correlation in the direction of the ionic transport in the low-symmetry Li+ conductor.« less

  15. Making Li-air batteries rechargeable: material challenges

    SciTech Connect (OSTI)

    Shao, Yuyan; Ding, Fei; Xiao, Jie; Zhang, Jian; Xu, Wu; Park, Seh Kyu; Zhang, Jiguang; Wang, Yong; Liu, Jun

    2013-02-25

    A Li-air battery could potentially provide three to five times higher energy density/specific energy than conventional batteries, thus enable the driving range of an electric vehicle comparable to a gasoline vehicle. However, making Li-air batteries rechargeable presents significant challenges, mostly related with materials. Herein, we discuss the key factors that influence the rechargeability of Li-air batteries with a focus on nonaqueous system. The status and materials challenges for nonaqueous rechargeable Li-air batteries are reviewed. These include electrolytes, cathode (electocatalysts), lithium metal anodes, and oxygen-selective membranes (oxygen supply from air). The perspective of rechargeable Li-air batteries is provided.

  16. Electrolyte effects in Li(Si)/FeS{sub 2} thermal batteries

    SciTech Connect (OSTI)

    Guidotti, R.A.; Reinhardt, F.W.

    1994-10-01

    The most common electrochemical couple for thermally activated (``thermal``) batteries is the Li-alloy/FeS{sub 2} system. The most common Li-alloys used for anodes are 20% Li-80% Al and 44% Li-56% Si (by weight); liquid Li immobilized with iron powder has also been used. The standard electrolyte that has been used in thermal batteries over the years is the LiCl-KCl eutectic that melts at 352{degrees}C. The LiCl-LiBr-LiF eutectic had the best rate and power characteristics. This electrolyte melts at 436{degrees}C and shows very low polarization because of the absence of Li+ gradients common with the LiCl-KCl eutectic. The low-melting electrolytes examined included a KBr-LiBr-LiCl eutectic (melting at 321{degrees}C), a LiBr-KBr-LiF eutectic (melting at 313{degrees}C), and a CsBr-LiBr-KBr eutectic (melting at 238{degrees}C). The CsBr-based salt had poor conductivity and was not studied further. The LiBr-KBr-LiF eutectic outperformed the KBr-LiBr-LiCl eutectic and was selected for more extensive testing. Because of their lower melting points and larger liquidi relative to the LiCl-KCl eutectic, the low-melting electrolytes are prime candidates for long-life applications (i.e., for activated lives of one hour or more). This paper will detail the relative performance of the Li(Si)/FeS{sub 2} couple using primarily the LiCl-KCl (standard) eutectic, the LiCl-LiBr-LiF (all-Li) eutectic, and the LiBr-KBr-LiF (low-melting) eutectic electrolytes. Most of the tests were conducted with 5-cell batteries; validation tests were also carried out with appropriate full-sized batteries.

  17. Solution-processable glass LiI-Li4SnS4 superionic conductors for all-solid-state Li-ion batteries

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Kern Ho Park; Oh, Dae Yang; Choi, Young Eun; Nam, Young Jin; Han, Lili; Kim, Ju -Young; Xin, Huolin; Lin, Feng; Oh, Seung M.; Jung, Yoon Seok

    2015-12-22

    The new, highly conductive (4.1 × 10–4 S cm–1 at 30 °C), highly deformable, and dry-air-stable glass 0.4LiI-0.6Li4SnS4 is prepared using a homogeneous methanol solution. Furthermore, the solution process enables the wetting of any exposed surface of the active materials with highly conductive solidified electrolytes (0.4LiI-0.6Li4SnS4), resulting in considerable improvements in electrochemical performances of these electrodes over conventional mixture electrodes.

  18. A=5Li (1984AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    84AJ01) (See Energy Level Diagrams for 5Li) GENERAL: See also (1979AJ01) and Table 5.3 [Table of Energy Levels] (in PDF or PS) here. Model calculations:(1978RE1A, 1979MA1J, 1980HA1M, 1981BE10, 1982FI13). Special states:(1981BE10, 1981KU1H, 1982EM1A, 1982FI13, 1982FR1D). Complex reactions involving 5Li:(1979BR02, 1979RU1B). Reactions involving pions:(1978BR1V, 1979SA1W, 1983AS02). Reactions involving antiprotons:(1981YA1B). Hypernuclei:(1980IW1A, 1981KO1V, 1981KU1H, 1983GI1C). Other

  19. A=5Li (66LA04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 5Li) GENERAL: See Table 5.4 [Table of Energy Levels] (in PDF or PS). See also (BA59N, MI59B, PE60C, PH60A, VA61K, DI62B, IN62, KU63I, BA64HH, GR64C, SA64G, ST64). 1. 3He(d, γ)5Li Qm = 16.388 The excitation curve measured from Ed = 0.2 to 2.85 MeV shows a broad maximum at Ed = 0.45 ± 0.04 MeV (Eγ = 16.6 ± 0.2 MeV, σ = 50 ± 10 μb, Γγ = 11 ± 2 eV). Above this maximum, non-resonant capture is indicated by a slow rise of the cross section. The

  20. A=8Li (1984AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 8Li) GENERAL: See also (1979AJ01) and Table 8.2 [Table of Energy Levels] (in PDF or PS). Special states: (1980OK01). Complex reactions involving 8Li: (1978BO1B, 1978DU1B, 1979BO22, 1979IV1A, 1980AN1T, 1980BO31, 1980GR10, 1980WI1L, 1981BO1X, 1981MO20, 1982BO35, 1982BO1Y, 1982GO1E, 1982GU1H, 1982MO1N). Muon and neutrino interactions: (1978BA1G). Reactions involving pions and other mesons: (1977VE1C, 1979BA16, 1980HA29, 1981JU1A, 1981NI03, 1982HA57).

  1. A=8Li (1988AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 8Li) GENERAL: See also (1984AJ01) and Table 8.2 [Table of Energy Levels] (in PDF or PS) here. Nuclear models: (1983KU17, 1983SH38, 1984MO1H, 1984REZZ, 1984VA06, 1988WO04). Special states: (1982PO12, 1983KU17, 1984REZZ, 1984VA06, 1986XU02). Electromagnetic transitions: (1983KU17). Astrophysics: (1987MA2C). Complex reactions involving 8Li: (1983FR1A, 1983GU1A, 1983OL1A, 1983WI1A, 1984GR08, 1984HI1A, 1984LA27, 1985JA1B, 1985MA02, 1985MA13, 1985MO17, 1986AV1B,

  2. A=9Li (1984AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 9Li) GENERAL: See also (1979AJ01) and Table 9.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1979LA06). Complex reactions involving 9Li: (1978DU1B, 1979AL22, 1979BO22, 1979JA1C, 1980BO31, 1980WI1L, 1981BO1X, 1981MO20, 1982BO1Y). Muon and neutrino capture and reactions: (1980MU1B). Reactions involving pions and other mesons (See also reaction 3.): (1978FU09, 1979BO21, 1979PE1C, 1979WI1E, 1980NI03, 1980ST15, 1981YA1A). Hypernuclei: (1978DA1A,

  3. A=9Li (1988AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 9Li) GENERAL: See also (1984AJ01) and Table 9.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1983KU17, 1984CH24, 1984VA06). Special states: (1983KU17, 1984VA06). Electromagnetic interactions: (1983KU17). Astrophysical questions: (1987MA2C). Complex reactions involving 9Li: (1983OL1A, 1983WI1A, 1984GR08, 1985JA1B, 1985MA02, 1985MO17, 1986CS1A, 1986HA1B, 1986SA30, 1986WE1C, 1987BA38, 1987CH26, 1987JA06, 1987KO1Z, 1987SH1K, 1987TAZU, 1987WA09,

  4. FIRST_Research Perspective_Li

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    1. Structure factor obtained from MD (a) and SAXS (b) at different temperatures: comparison of spatial heterogeneity from snapshots (c) of DILs (top) and MILs (bottom) FIRST Center Research Perspective: Nanoscale Heterogeneity and Dynamics of Room Temperature Ionic Liquids Song Li Vanderbilt University Jianchang Guo, Kee Sung Han, Jose L. Bañuelos, Edward W. Hagaman, Robert W. Shaw Oak Ridge National Laboratory Research Summary: An increase of the alkyl chain length of the cation of room

  5. Li2OHCl crystalline electrolyte for stable metallic lithium anodes

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Hood, Zachary D.; Wang, Hui; Samuthira Pandian, Amaresh; Keum, Jong Kahk; Liang, Chengdu

    2016-01-22

    In a classic example of stability from instability, we show that Li2OHCl solid electrolyte forms a stable solid electrolyte interface (SEI) with metallic lithium anode. The Li2OHCl solid electrolyte can be readily achieved through simple mixing of air-stable LiOH and LiCl precursors with a mild processing temperature under 400 °C. Additionally, we show that continuous, dense Li2OHCl membranes can be fabricated at temperatures less than 400 °C, standing in great contrast to current processing temperatures of over 1600 °C for most oxide-based solid electrolytes. The ionic conductivity and Arrhenius activation energy were explored for the LiOH-LiCl system of crystalline solidmore » electrolytes where Li2OHCl with increased crystal defects was found to have the highest ionic conductivity and reasonable Arrhenius activation energy. The Li2OHCl solid electrolyte displays stability against metallic lithium, even in extreme conditions past the melting point of lithium metal. Furthermore, to understand this excellent stability, we show that SEI formation is critical in stabilizing the interface between metallic lithium and the Li2OHCl solid electrolyte.« less

  6. Microsoft Word - Household Energy Use CA

    U.S. Energy Information Administration (EIA) Indexed Site

    0 20 40 60 80 100 US PAC CA Site Consumption million Btu $0 $500 $1,000 $1,500 $2,000 $2,500 US PAC CA Expenditures dollars ALL ENERGY average per household (excl. transportation) 0 2,000 4,000 6,000 8,000 10,000 12,000 US PAC CA Site Consumption kilowatthours $0 $250 $500 $750 $1,000 $1,250 $1,500 US PAC CA Expenditures dollars ELECTRICITY ONLY average per household  California households use 62 million Btu of energy per home, 31% less than the U.S. average. The lower than average site

  7. Microsoft Word - Household Energy Use CA

    Gasoline and Diesel Fuel Update (EIA)

    0 20 40 60 80 100 US PAC CA Site Consumption million Btu $0 $500 $1,000 $1,500 $2,000 $2,500 US PAC CA Expenditures dollars ALL ENERGY average per household (excl. transportation) 0 2,000 4,000 6,000 8,000 10,000 12,000 US PAC CA Site Consumption kilowatthours $0 $250 $500 $750 $1,000 $1,250 $1,500 US PAC CA Expenditures dollars ELECTRICITY ONLY average per household  California households use 62 million Btu of energy per home, 31% less than the U.S. average. The lower than average site

  8. UTICA 4, NEW YORK COFIPOR~TION

    Office of Legacy Management (LM)

    H. J. Zmjian, GE", of the ncmbers of our orzaniza- has a "Q" cl:arance and our President is rcqueoting an 'L" clearance for some of us. -'n would appreciate it very much if you ...

  9. Predictive Materials Modeling for Li-Air Battery Systems | Argonne

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Leadership Computing Facility Predictive Materials Modeling for Li-Air Battery Systems PI Name: Larry Curtiss PI Email: curtiss@anl.gov Institution: Argonne National Laboratory Allocation Program: INCITE Allocation Hours at ALCF: 50 Million Year: 2015 Research Domain: Materials Science A rechargeable lithium-air (Li-air) battery can potentially store five to ten times the energy of a lithium-ion (Li-ion) battery of the same weight. Realizing this enormous potential presents a challenging

  10. Properties of (Ga,Mn)As codoped with Li

    SciTech Connect (OSTI)

    Miyakozawa, Shohei; Chen, Lin; Matsukura, Fumihiro; Ohno, Hideo

    2014-06-02

    We grow Li codoped (Ga,Mn)As layers with nominal Mn composition up to 0.15 by molecular beam epitaxy. The layers before and after annealing are characterized by x-ray diffraction, transport, magnetization, and ferromagnetic resonance measurements. The codoping with Li reduces the lattice constant and electrical resistivity of (Ga,Mn)As after annealing. We find that (Ga,Mn)As:Li takes similar Curie temperature to that of (Ga,Mn)As, but with pronounced magnetic moments and in-plane magnetic anisotropy, indicating that the Li codoping has nontrivial effects on the magnetic properties of (Ga,Mn)As.

  11. Electrical conduction of LiF interlayers in organic diodes

    SciTech Connect (OSTI)

    Bory, Benjamin F.; Janssen, Ren A. J.; Meskers, Stefan C. J.; Gomes, Henrique L.; Leeuw, Dago M. de

    2015-04-21

    An interlayer of LiF in between a metal and an organic semiconductor is commonly used to improve the electron injection. Here, we investigate the effect of moderate bias voltages on the electrical properties of Al/LiF/poly(spirofluorene)/Ba/Al diodes by systematically varying the thickness of the LiF layer (2-50?nm). Application of forward bias V below the bandgap of LiF (V?LiF/poly(spirofluorene) hetero-junction. Electrons are trapped on the poly(spirofluorene) side of the junction, while positively charged defects accumulate in the LiF with number densities as high as 10{sup 25}/m{sup 3}. Optoelectronic measurements confirm the built-up of aggregated, ionized F centres in the LiF as the positive trapped charges. The charged defects result in efficient transport of electrons from the polymer across the LiF, with current densities that are practically independent of the thickness of the LiF layer.

  12. Predictive Models of Li-ion Battery Lifetime (Presentation) Smith...

    Office of Scientific and Technical Information (OSTI)

    Predictive Models of Li-ion Battery Lifetime (Presentation) Smith, K.; Wood, E.; Santhanagopalan, S.; Kim, G.; Shi, Y.; Pesaran, A. 25 ENERGY STORAGE; 33 ADVANCED PROPULSION...

  13. Degradation Mechanisms in Li-Ion Battery Electrolytes Uncovered...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Degradation Mechanisms in Li-Ion Battery Electrolytes Uncovered by In-Situ Scanning ... to evaluate stability and degradation in battery electrolytes Developed a rapid method ...

  14. Notices FOR FURTHER INFORMATION CONTACT: Michael Li, Policy Advisor...

    Office of Environmental Management (EM)

    12, 2016 Notices FOR FURTHER INFORMATION CONTACT: Michael Li, Policy Advisor, Office of Energy Efficiency and Renewable Energy, U.S. Department of Energy, 1000 Independence Ave. ...

  15. Characterization of Materials for Li-ion Batteries: Success Stories...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Success Stories from the High Temperature Materials Laboratory (HTML) User Program Characterization of Materials for Li-ion Batteries: Success Stories from the High...

  16. Nanoscale imaging of fundamental Li battery chemistry: solid...

    Office of Scientific and Technical Information (OSTI)

    Nanoscale imaging of fundamental Li battery chemistry: solid-electrolyte interphase formation and preferential growth of lithium metal nanoclusters Prev Next Title: Nanoscale ...

  17. Prediction of superconductivity in Li-intercalated bilayer phosphorene

    SciTech Connect (OSTI)

    Huang, G. Q.; Xing, Z. W.; Xing, D. Y.

    2015-03-16

    It is shown that bilayer phosphorene can be transformed from a direct-gap semiconductor to a BCS superconductor by intercalating Li atoms. For the Li-intercalated bilayer phosphorene, we find that the electron occupation of Li-derived band is small and superconductivity is intrinsic. With increasing the intercalation of Li atoms, both increased metallicity and strong electron-phonon coupling are favorable for the enhancement of superconductivity. The obtained electron-phonon coupling λ can be larger than 1 and the superconducting temperature T{sub c} can be increased up to 16.5 K, suggesting that phosphorene may be a good candidate for a nanoscale superconductor.

  18. Construction of a Li Ion Battery (LIB) Cathode Production Plant...

    Broader source: Energy.gov (indexed) [DOE]

    Process for Low Cost Domestic Production of LIB Cathode Materials Process for Low Cost Domestic Production of LIB Cathode Materials Construction of a Li Ion Battery (LIB) Cathode ...

  19. Li ion Motors Corp formerly EV Innovations Inc | Open Energy...

    Open Energy Info (EERE)

    Vegas, Nevada Zip: 89110 Sector: Vehicles Product: Las Vegas - based manufacturer of lithium-powered plug-in vehicles. References: Li-ion Motors Corp (formerly EV Innovations...

  20. LiDAR (Lewicki & Oldenburg, 2005) | Open Energy Information

    Open Energy Info (EERE)

    Technique LiDAR Activity Date Usefulness useful DOE-funding Unknown References Jennifer L. Lewicki, Curtis M. Oldenburg (2005) Strategies To Detect Hidden Geothermal Systems...

  1. LiDAR (Lewicki & Oldenburg, 2004) | Open Energy Information

    Open Energy Info (EERE)

    Technique LiDAR Activity Date Usefulness useful DOE-funding Unknown References Jennifer L. Lewicki, Curtis M. Oldenburg (2004) Strategies For Detecting Hidden Geothermal Systems...

  2. Characterization of Li-ion Batteries using Neutron Diffraction...

    Broader source: Energy.gov (indexed) [DOE]

    Materials Characterization Capabilities at the High Temperature Materials Laboratory and HTML User Program Success Stories Characterization of Materials for Li-ion Batteries: ...

  3. Measuring Li+ inventory losses in LiCoO2/graphite cells using Raman microscopy

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Snyder, Chelsea Marie; Apblett, Christopher A.; Grillet, Anne; Thomas Edwin Beechem; Duquette, David

    2016-03-25

    Here, the contribution from loss of Li+ inventory to capacity fade is described for slow rates (C/10) and long-term cycling (up to 80 cycles). It was found through electrochemical testing and ex-situ Raman analysis that at these slow rates, the entirety of capacity loss up to 80 cycles can be explained by loss of Li+ inventory in the cell. The Raman spectrum of LiCoO2 is sensitive to the state of lithiation and can therefore be leveraged to quantify the state of lithiation for individual particles. With these Raman derived estimates, the lithiation state of the cathode in the discharged statemore » is compared to electrochemical data as a function of cycle number. High correlation is found between Raman quantifications of cycleable lithium and the capacity fade. Additionally, the linear relationship between discharge capacity and cell overpotential suggests that the loss of capacity stems from an impedance rise of the electrodes, which based on Li inventory losses, is caused by SEI formation and repair.« less

  4. Predicted Structure, Thermo-Mechanical Properties and Li Ion Transport in LiAlF4 Glass

    SciTech Connect (OSTI)

    Stechert, T. R.; Rushton, M. J. D.; Grimes, R. W.; Dillon, A. C.

    2012-08-15

    Materials with the LiAlF{sub 4} composition are of interest as protective electrode coatings in Li ion battery applications due to their high cationic conductivity. Here classical molecular dynamics calculations are used to produce amorphous model structures by simulating a quench from the molten state. These are analysed in terms of their individual pair correlation functions and atomic coordination environments. This indicates that amorphous LiAlF{sub 4} is formed of a network of corner sharing AlF{sub 6} octahedra. Li ions are distributed within this network, primarily associated with non-bridging fluorine atoms. The nature of the octahedral network is further analysed through intra- and interpolyhedral bond angle distributions and the relative populations of bridging and non-bridging fluorine ions are calculated. Network topology is considered through the use of ring statistics, which indicates that, although topologically well connected, LiAlF{sub 4} contains an appreciable number of corner-linked branch-like AlF{sub 6} chains. Thermal expansion values are determined above and below the predicted glass transition temperature of 1340 K. Finally, movement of Li ions within the network is examined with predictions of the mean squared displacements, diffusion coefficients and Li ion activation energy. Different regimes for lithium ion movement are identified, with both diffusive and sessile Li ions observed. For migrating ions, a typical trajectory is illustrated and discussed in terms of a hopping mechanism for Li transport.

  5. Characterization of low-melting electrolytes for potential geothermal borehole power supplies: The LiBr-KBr-LiF eutectic

    SciTech Connect (OSTI)

    Guidotti, R.A.; Reinhardt, F.W.

    1998-05-01

    The suitability of modified thermal-battery technology for use as a potential power source for geothermal borehole applications is under investigation. As a first step, the discharge processes that take place in LiSi/LiBr-KBr-LiF/FeS{sub 2} thermal cells were studied at temperatures of 350 C and 400 C using pelletized cells with immobilized electrolyte. Incorporation of a reference electrode allowed the relative contribution of each electrode to the overall cell polarization to be determined. The results of single-cell tests are presented, along with preliminary data for cells based on a lower-melting CsBr-LiBr-KBr eutectic salt.

  6. Primordial Li abundance and massive particles

    SciTech Connect (OSTI)

    Latin-Capital-Letter-Eth apo, H.

    2012-10-20

    The problem of the observed lithium abundance coming from the Big Bang Nucleosynthesis is as of yet unsolved. One of the proposed solutions is including relic massive particles into the Big Bang Nucleosynthesis. We investigated the effects of such particles on {sup 4}HeX{sup -}+{sup 2}H{yields}{sup 6}Li+X{sup -}, where the X{sup -} is the negatively charged massive particle. We demonstrate the dominance of long-range part of the potential on the cross-section.

  7. A=3Li (2010PU04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    2010PU04) GENERAL: The previous A = 3 evaluations (1975FI08, 1987TI07) identified reactions 1 through 4 below as possible candidates for the observation of a bound or resonant state of three protons. An additional possibility would be the double charge exchange reaction 3H(π+, π-)3Li. There is a report of this reaction (2001PA47), but the pion energy was high, 500 MeV, and the focus of the experiment was on the role of the Δ component in the 3H ground state, not on the possible presence of a

  8. Advanced Li-Ion Polymer Battery Cell Manufacturing Plant in USA...

    Broader source: Energy.gov (indexed) [DOE]

    MB) More Documents & Publications Advanced Li-Ion Polymer Battery Cell Manufacturing Plant in USA Li-Ion Battery Cell Manufacturing 2010 DOE, Li-Ion Battery Cell Manufacturing

  9. Update on Performance Improvement of Sandia-Built Li/(CFx)n and...

    Office of Scientific and Technical Information (OSTI)

    Update on Performance Improvement of Sandia-Built Li(CFx)n and LiFePO4 Cells. Citation Details In-Document Search Title: Update on Performance Improvement of Sandia-Built Li...

  10. Update on Performance Improvement of Sandia-Built Li/(CFx)n and...

    Office of Scientific and Technical Information (OSTI)

    Update on Performance Improvement of Sandia-Built Li(CFx)n and LiFePO4 Cells. Citation Details In-Document Search Title: Update on Performance Improvement of Sandia-Built Li(CFx)n ...

  11. Predicting Chemical Pathways for Li-O2 Batteries - Joint Center...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    March 6, 2014, Research Highlights Predicting Chemical Pathways for Li-O2 Batteries ... figure) and (LiO2)6 (red curve, upper figure) to Li2O2 using quantum chemical theory. ...

  12. Selected test results from the LiFeBatt iron phosphate Li-ion battery.

    SciTech Connect (OSTI)

    Ingersoll, David T.; Hund, Thomas D.

    2008-09-01

    In this paper the performance of the LiFeBatt Li-ion cell was measured using a number of tests including capacity measurements, capacity as a function of temperature, ohmic resistance, spectral impedance, high power partial state of charge (PSOC) pulsed cycling, pulse power measurements, and an over-charge/voltage abuse test. The goal of this work was to evaluate the performance of the iron phosphate Li-ion battery technology for utility applications requiring frequent charges and discharges, such as voltage support, frequency regulation, and wind farm energy smoothing. Test results have indicated that the LiFeBatt battery technology can function up to a 10C{sub 1} discharge rate with minimal energy loss compared to the 1 h discharge rate (1C). The utility PSOC cycle test at up to the 4C{sub 1} pulse rate completed 8,394 PSOC pulsed cycles with a gradual loss in capacity of 10 to 15% depending on how the capacity loss is calculated. The majority of the capacity loss occurred during the initial 2,000 cycles, so it is projected that the LiFeBatt should PSOC cycle well beyond 8,394 cycles with less than 20% capacity loss. The DC ohmic resistance and AC spectral impedance measurements also indicate that there were only very small changes after cycling. Finally, at a 1C charge rate, the over charge/voltage abuse test resulted in the cell venting electrolyte at 110 C after 30 minutes and then open-circuiting at 120 C with no sparks, fire, or voltage across the cell.

  13. DOE - Office of Legacy Management -- Electro Circuits Inc - CA 08

    Office of Legacy Management (LM)

    Electro Circuits Inc - CA 08 FUSRAP Considered Sites Site: Electro Circuits, Inc. (CA.08 ) Eliminated from consideration under FUSRAP Designated Name: Not Designated Alternate Name: None Location: 401 East Green Street , Pasadena , California CA.08-1 Evaluation Year: 1994 CA.08-2 Site Operations: Conducted ultrasonic tests on uranium ingots in the early 1950s. CA.08-3 CA.08-4 Site Disposition: Eliminated - Potential for contamination remote based on limited operations at the site CA.08-2

  14. A=07Li (66LA04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 7Li) GENERAL: See (HU57D, BA59K, BA59N, BR59M, FE59E, MA59E, MA59H, KU60A, PE60E, PH60A, SH60C, TA60L, BA61H, BA61N, BL61C, CL61D, KH61, TA61G, TO61B, CL62E, CR62A, IN62, CH63, CL63C, KL63, SC63I, BE64H, GR64C, MA64HH, NE64C, OL64A, SA64G, BE65F, FA65A, JA65H, NE65, PR65). See also Table 7.1 [Table of Energy Levels] (in PDF or PS). Ground state: Q = -45 ± 5 mb (KA61F, VA63F, WH64); μ = +3.2564 nm (FU65E). 1. 4He(t, γ)7Li Qm = 2.467 Excitation functions

  15. Enabling the Future of Li-Ion Batteries | Argonne National Laboratory

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Enabling the Future of Li-Ion Batteries Title Enabling the Future of Li-Ion Batteries Publication Type Presentation Year of Publication 2015 Authors Gaines, LL Abstract...

  16. Significant Cost Improvement of Li-Ion Cells Through Non-NMP...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Significant Cost Improvement of Li-Ion Cells Through Non-NMP Electrode Coating, Direct Separator Coating, and Fast Formation Technologies Significant Cost Improvement of Li-Ion ...

  17. Localization of vacancies and mobility of lithium ions in Li{sub 2}ZrO{sub 3} as obtained by {sup 6,7}Li NMR

    SciTech Connect (OSTI)

    Baklanova, Ya. V., E-mail: baklanovay@ihim.uran.ru [Institute of Solid State Chemistry, Ural Branch of the Russian Academy of Sciences, 91 Pervomaiskaya str., 620990 Ekaterinburg (Russian Federation); Arapova, I. Yu.; Buzlukov, A.L.; Gerashenko, A.P.; Verkhovskii, S.V.; Mikhalev, K.N. [Institute of Metal Physics, Ural Branch of the Russian Academy of Sciences, 18 Kovalevskaya str., 620990 Ekaterinburg (Russian Federation); Denisova, T.A.; Shein, I.R.; Maksimova, L.G. [Institute of Solid State Chemistry, Ural Branch of the Russian Academy of Sciences, 91 Pervomaiskaya str., 620990 Ekaterinburg (Russian Federation)

    2013-12-15

    The {sup 6,7}Li NMR spectra and the {sup 7}Li spinlattice relaxation rate were measured on polycrystalline samples of Li{sub 2}ZrO{sub 3}, synthesized at 1050 K and 1300 K. The {sup 7}Li NMR lines were attributed to corresponding structural positions of lithium Li1 and Li2 by comparing the EFG components with those obtained in the first-principles calculations of the charge density in Li{sub 2}ZrO{sub 3}. For both samples the line width of the central {sup 7}Li transition and the spinlattice relaxation time decrease abruptly at the temperature increasing above ?500 K, whereas the EFG parameters are averaged (??{sub Q}?=42 (5) kHz) owing to thermally activated diffusion of lithium ions. - Graphical abstract: Path of lithium ion hopping in lithium zirconate Li{sub 2}ZrO{sub 3}. - Highlights: Polycrystalline samples Li{sub 2}ZrO{sub 3} with monoclinic crystal structure synthesized at different temperatures were investigated by {sup 6,7}Li NMR spectroscopy. Two {sup 6,7}Li NMR lines were attributed to the specific structural positions Li1 and Li2. The distribution of vacancies was clarified for both lithium sites. The activation energy and pathways of lithium diffusion in Li{sub 2}ZrO{sub 3} were defined.

  18. Polymer electrolytes for a rechargeable li-Ion battery

    SciTech Connect (OSTI)

    Argade, S.D.; Saraswat, A.K.; Rao, B.M.L.; Lee, H.S.; Xiang, C.L.; McBreen, J.

    1996-10-01

    Lithium-ion polymer electrolyte battery technology is attractive for many consumer and military applications. A Li{sub x}C/Li{sub y}Mn{sub 2}O{sub 4} battery system incorporating a polymer electrolyte separator base on novel Li-imide salts is being developed under sponsorship of US Army Research Laboratory (Fort Monmouth NJ). This paper reports on work currently in progress on synthesis of Li-imide salts, polymer electrolyte films incorporating these salts, and development of electrodes and cells. A number of Li salts have been synthesized and characterized. These salts appear to have good voltaic stability. PVDF polymer gel electrolytes based on these salts have exhibited conductivities in the range 10{sup -4} to 10{sub -3} S/cm.

  19. Tuning complexity by lithiation: A family of intergrowth structures using condensed hypho-icosahedra in the Li-doped Ca–Zn system

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Lin, Qisheng; Zhu, Ran; Miller, Gordon J.

    2016-04-26

    Cluster chemistry of intermetallics with valence electron counts (VECs) in the range of 2.0–3.0 is intriguing. Lithiation of polar intermetallics in this VEC region is found to be an effective chemical route to produce new complex structures with different stability mechanisms. In this work, two new complex intermetallic structures have been discovered in the Ca–Li–Zn system: Ca12LixZn59–x and Ca15LixZn75–x. Ca12LixZn59–x, x ≈ 5.65(3)–14.95(3), forms in the trigonal space group R3m, with a = 9.074(1)–9.1699(2) Å, c = 53.353(1)–53.602(1) Å, and Z = 3. In comparison, Ca15LixZn75–x, x ≈ 19.07(2), crystallizes in the space group P63/mmc, with a ≈ 9.183(1) Å,more » c ≈ 45.191(5) Å), and Z = 2. Both structures are members of a large intergrowth family featuring slabs of dimers (D) and trimers (T) stacking along [001], with the sequences DTDDTDDTD for Ca12LixZn59–x and TDDDTDDD for Ca15LixZn75–x. Each dimer consists of two face-sharing Zn-centered hypho-icosahedra, and each trimer comprises a Li-centered icosahedron sandwiched by two hypho-icosahedra. Furthermore, this intergrowth family includes several known intermetallic structure types involving very electropositive metals, e.g., SrMg5.2, Ba2Li4.21Al4.79, and Sr9Li17.5Al25.5. Because of cluster defects and condensation, both Ca12LixZn59–x and Ca15LixZn75–x are electronically akin to close-packed metals, and their structural stabilities can be interpreted by a Hume-Rothery mechanism rather than the Zintl–Klemm concept.« less

  20. Solution-processable glass LiI-Li4SnS4 superionic conductors for all-solid-state Li-ion batteries

    SciTech Connect (OSTI)

    Kern Ho Park; Oh, Dae Yang; Choi, Young Eun; Nam, Young Jin; Han, Lili; Kim, Ju -Young; Xin, Huolin; Lin, Feng; Oh, Seung M.; Jung, Yoon Seok

    2015-12-22

    The new, highly conductive (4.1 × 10–4 S cm–1 at 30 °C), highly deformable, and dry-air-stable glass 0.4LiI-0.6Li4SnS4 is prepared using a homogeneous methanol solution. Furthermore, the solution process enables the wetting of any exposed surface of the active materials with highly conductive solidified electrolytes (0.4LiI-0.6Li4SnS4), resulting in considerable improvements in electrochemical performances of these electrodes over conventional mixture electrodes.

  1. Additional experiments relative to the shelf life of Li(Si)/FeS/sub 2/ thermal batteries

    SciTech Connect (OSTI)

    Searcy, J.Q.; Armijo, J.R.

    1985-02-01

    Work described in this report is part of a continuing effort to develop a new thermal battery technology based on the Li(Si)/FeS/sub 2/ electrochemical couple. The results reported relate to the long shelf-life requirement for thermal batteries designed by Sandia, and include topics relevant to leakage through the hermetic seal and accelerated aging experiments with materials new to the technology. Conclusions relevant to leakage through the hermetic seal are that the maximum leak rate must not exceed 1.8 x 10/sup -7/ w, where w is the grams of Li(Si) contained by a battery, and that a bomb-type leak test can be designed that is adequate for most Li(Si)/FeS/sub 2/ batteries. Conclusions relevant to long-term compatibility of new materials include the following: nickel is not compatible with the iron disulfide in the cathode; the CaSi/sub 2/ additive used to suppress the initial voltage transient does not react or degrade during accelerated aging experiments, but the use of that material can lead to an increase in the variability of the activated lives, especially for long-life batteries; Grafoil current collectors used with the cathode do not degrade in accelerated aging experiments.

  2. Structure of neutron-rich Isotopes {sup 8}Li and {sup 9}Li and allowance for it in elastic scattering

    SciTech Connect (OSTI)

    Ibraeva, E. T.; Zhusupov, M. A.; Imambekov, O.; Sagindykov, Sh. Sh.

    2008-07-15

    The differential cross sections for elastic proton scattering on the unstable neutron-rich nuclei {sup 8}Li and {sup 9}Li at E = 700 and 60 MeV per nucleon were considered. The {sup 8}Li nucleus was treated on the basis of the three-body {alpha}-t-n model, while the {sup 9}Li nucleus was considered within the {alpha}-t-n and {sup 7}Li-n-n models. The cross sections in question were calculated within Glauber diffraction theory. A comparison of the results with available experimental data made it possible to draw conclusions on the quality of the wave functions and potential used in the calculations.

  3. LiCl Dehumidifier LiBr absorption chiller hybrid air conditioning system with energy recovery

    DOE Patents [OSTI]

    Ko, Suk M.

    1980-01-01

    This invention relates to a hybrid air conditioning system that combines a solar powered LiCl dehumidifier with a LiBr absorption chiller. The desiccant dehumidifier removes the latent load by absorbing moisture from the air, and the sensible load is removed by the absorption chiller. The desiccant dehumidifier is coupled to a regenerator and the desiccant in the regenerator is heated by solar heated hot water to drive the moisture therefrom before being fed back to the dehumidifier. The heat of vaporization expended in the desiccant regenerator is recovered and used to partially preheat the driving fluid of the absorption chiller, thus substantially improving the overall COP of the hybrid system.

  4. Investigation of the Decomposition Mechanism of Lithium Bis(oxalate)borate (LiBOB) Salt in the Electrolyte of an Aprotic LiO2 Battery

    SciTech Connect (OSTI)

    Lau, Kah Chun; Lu, Jun; Low, John; Peng, Du; Wu, Huiming; Albishri, Hassan M.; Al-Hady, D. Abd; Curtiss, Larry A.; Amine, Khalil

    2014-04-01

    The stability of the lithium bis(oxalate) borate (LiBOB) salt against lithium peroxide (Li2O2) formation in an aprotic LiO2 (Liair) battery is investigated. From theoretical and experimental findings, we find that the chemical decomposition of LiBOB in electrolytes leads to the formation lithium oxalate during the discharge of a LiO2 cell. According to density functional theory (DFT) calculations, the formation of lithium oxalate as the reaction product is exothermic and therefore is thermodynamically feasible. This reaction seems to be independent of solvents used in the LiO2 cell, and therefore LiBOB is probably not suitable to be used as the salt in LiO2 cell electrolytes.

  5. New solid-state synthesis routine and mechanism for LiFePO{sub 4} using LiF as lithium precursor

    SciTech Connect (OSTI)

    Wang Deyu; Li Hong; Wang Zhaoxiang; Wu Xiaodong; Sun Yucheng; Huang Xuejie; Chen Liquan . E-mail: lqchen@aphy.iphy.ac.cn

    2004-12-01

    Li{sub 2}CO{sub 3} and LiOH.H{sub 2}O are widely used as Li-precursors to prepare LiFePO{sub 4} in solid-phase reactions. However, impurities are often found in the final product unless the sintering temperature is increased to 800 deg. C. Here, we report that lithium fluoride (LiF) can also be used as Li-precursor for solid-phase synthesis of LiFePO{sub 4} and very pure olivine phase was obtained even with sintering at a relatively low temperature (600 deg. C). Consequently, the product has smaller particle size (about 500nm), which is beneficial for Li-extraction/insertion in view of kinetics. As for cathode material for Li-ion batteries, LiFePO{sub 4} obtained from LiF shows high Li-storage capacity of 151mAhg{sup -1} at small current density of 10mAg{sup -1} (1/15C) and maintains capacity of 54.8mAhg{sup -1} at 1500mAg{sup -1} (10C). The solid-state reaction mechanisms using LiF and Li{sub 2}CO{sub 3} precursors are compared based on XRD and TG-DSC.

  6. Material review of Li ion battery separators

    SciTech Connect (OSTI)

    Weber, Christoph J. Geiger, Sigrid; Falusi, Sandra; Roth, Michael

    2014-06-16

    Separators for Li Ion batteries have a strong impact on cell production, cell performance, life, as well as reliability and safety. The separator market volume is about 500 million m{sup 2} mainly based on consumer applications. It is expected to grow strongly over the next decade for mobile and stationary applications using large cells. At present, the market is essentially served by polyolefine membranes. Such membranes have some technological limitations, such as wettability, porosity, penetration resistance, shrinkage and meltdown. The development of a cell failure due to internal short circuit is potentially closely related to separator material properties. Consequently, advanced separators became an intense area of worldwide research and development activity in academia and industry. New separator technologies are being developed especially to address safety and reliability related property improvements.

  7. A=5Li (1988AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 5Li) GENERAL: See also (1984AJ01) and Table 5.3 [Table of Energy Levels] (in PDF or PS) here. Model discussions: (1984ZW1A, 1985BA68, 1985FI1E, 1985KW02). Special states: (1982PO12, 1983FE07, 1984BE1B, 1984FI20, 1984GL1C, 1984VA1C, 1984ZW1A, 1985BA68, 1985FI1E, 1985PO18, 1985PO19, 1985WI1A, 1987SV1A, 1988BA86, 1988KW02). Electromagnetic transitions: (1985FI1E, 1987KR16). Astrophysical questions: (1984BA74, 1984SU1A, 1985BO1E, 1986HU1D). Complex reactions

  8. A=6Li (1974AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 6Li) GENERAL: See also (1966LA04) and Table 6.2 [Table of Energy Levels] (in PDF or PS). Shell model: (1961KO1A, 1965CO25, 1966BA26, 1966GA1E, 1966HA18, 1966WI1E, 1967BO1C, 1967CO32, 1967PI1B, 1967WO1B, 1968BO1N, 1968CO13, 1968GO01, 1968LO1C, 1968VA1H, 1969GU10, 1969RA1C, 1969SA1C, 1969VA1C, 1970LA1D, 1970SU13, 1970ZO1A, 1971CO28, 1971JA06, 1971LO03, 1971NO02, 1972LE1L, 1972LO1M, 1972VE07, 1973HA49, 1973JO1K, 1973KU03). Cluster and α-particle model:

  9. A=6Li (59AJ76)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    59AJ76) (See the Energy Level Diagram for 6Li) GENERAL: See also Table 6.2 [Table of Energy Levels] (in PDF or PS). Theory: See (MO54F, AD55, AU55, BA55S, IR55, LA55, OT55, FE56, ME56, NE56D, FR57, LE57F, LY57, SO57, TA57, PI58, SK58). 1. (a) 3H(3He, d)4He Qm = 14.319 Eb = 15.790 (b) 3H(3He, p)5He Qm = 11.136 (c) 3H(3He, p)4He + n Qm = 12.093 The relative intensities (43 ± 2, 6 ± 2, 51 ± 2) of reactions (a), (b) and (c), do not vary for E(3He) = 225 to 600 keV. The deuterons are isotropic

  10. A=7Li (1974AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 7Li) GENERAL: See also (1966LA04) and Table 7.1 [Table of Energy Levels] (in PDF or PS). Shell model: (1961KO1A, 1965CO25, 1965KU09, 1965VO1A, 1966BA26, 1966HA18, 1966WI1E, 1967BO1C, 1967BO22, 1967CO32, 1967FA1A, 1969GU03, 1969TA1H, 1969VA1C, 1970ZO1A, 1971CO28, 1972LE1L, 1973HA49, 1973KU03). Cluster model: (1965NE1B, 1968HA1G, 1968KU1B, 1969ME1C, 1969SM1A, 1969VE1B, 1969WI21, 1970BA1Q, 1972HA06, 1972HI16, 1972JA23, 1972KU12, 1972LE1L, 1973KU03, 1973KU12).

  11. A=7Li (1984AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 7Li) GENERAL: See also (1979AJ01) and Table 7.2 [Table of Energy Levels] (in PDF or PS). Shell model: (1978FU13, 1978MI13, 1979MA11, 1981BO1Y, 1982BA52, 1982FI13). Cluster and α-particle models: (1978MI13, 1979MA11, 1979VE08, 1980KA16, 1980SU04, 1981BE27, 1981EL06, 1981FI1A, 1981HA1Y, 1981KR1J, 1981RA1M, 1981SR01, 1982DE12, 1982FI13, 1982MU10, 1983DU1B, 1983KA1K). Special states: (1978MI13, 1979BU14, 1978DU1C, 1979KI10, 1980GO1Q, 1980SH1N, 1981BE27,

  12. A=7Li (1988AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 7Li) GENERAL: See also (1984AJ01) and Table 7.2 [Table of Energy Levels] (in PDF or PS) here. Shell model: (1983BU1B, 1983KU17, 1983SH1D, 1983VA31, 1984CH24, 1984REZZ, 1984VA06, 1984ZW1A, 1985FI1E, 1985GO11, 1986AV08, 1987KA09, 1987KI1C, 1988WO04). Cluster and α-particle models: (1981PL1A, 1983FU1D, 1983HO22, 1983PA06, 1983SH1D, 1983SR1C, 1984BA53, 1984DA07, 1984DU13, 1984DU17, 1984JO1A, 1984KA06, 1984KA04, 1984LO09, 1984MI1F, 1984SH26, 1985FI1E, 1985FU01,

  13. A=8Li (1979AJ01)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    9AJ01) (See Energy Level Diagrams for 8Li) GENERAL: See also (1974AJ01) and Table 8.1 [Table of Energy Levels] (in PDF or PS). Nuclear models: (1975KH1A, 1977ST24). Special states: (1974IR04, 1976IR1B, 1978KH03). Electromagnetic interactions: (1974KU06, 1976KU07). Special reactions: (1973SI38, 1974BA70, 1974BA1N, 1974BO08, 1975FE1A, 1975ZE01, 1976BE67, 1976BO08, 1976BU16, 1977FE1B, 1977PR05, 1977ST1J, 1977YA1B, 1978DI04). Muon and neutrino interactions: (1977BA1P). Pion and kaon reactions (See

  14. California Climate Exchange CaCX | Open Energy Information

    Open Energy Info (EERE)

    CaCX Jump to: navigation, search Name: California Climate Exchange (CaCX) Place: California Product: Aims to reducte CO2 emission in California. References: California Climate...

  15. EA-1798: Abengoa Solar's Mojave Solar Project near Barstow, CA...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    8: Abengoa Solar's Mojave Solar Project near Barstow, CA EA-1798: Abengoa Solar's Mojave Solar Project near Barstow, CA July 1, 2011 EA-1798: Final Environmental Assessment Loan ...

  16. ERSUG Meeting: January 28-29, 1997 (Berkeley, CA)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ERSUG Meeting: January 28-29, 1997 (Berkeley, CA) Dates January 28-29, 1997 Location Lawerence Berkeley Nantional Laboratory Perserverence Hall 1 Cyclotron Road Berkeley, CA 94720...

  17. ERSUG Meeting: June 13 - 14, 1995 (Livermore, CA)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ERSUG Meeting: June 13 - 14, 1995 (Livermore, CA) Dates ERSUG Meeting: June 13 & 14, 1995 Location Lawrence Livermore National Laboratory Livermore, CA Minutes Summary of ERSUG ...

  18. San Diego, CA Liquefied Natural Gas Exports to Mexico (Dollars...

    U.S. Energy Information Administration (EIA) Indexed Site

    San Diego, CA Liquefied Natural Gas Exports to Mexico (Dollars per Thousand Cubic Feet) San Diego, CA Liquefied Natural Gas Exports to Mexico (Dollars per Thousand Cubic Feet) ...

  19. Effects of electrolyte salts on the performance of Li-O2 batteries

    SciTech Connect (OSTI)

    Nasybulin, Eduard N.; Xu, Wu; Engelhard, Mark H.; Nie, Zimin; Burton, Sarah D.; Cosimbescu, Lelia; Gross, Mark E.; Zhang, Jiguang

    2013-02-05

    It is well known that the stability of nonaqueous electrolyte is critical for the rechargeable Li-O2 batteries. Although stability of many solvents used in the electrolytes has been investigated, considerably less attention has been paid to the stability of electrolyte salt which is the second major component. Herein, we report the systematic investigation of the stability of seven common lithium salts in tetraglyme used as electrolytes for Li-O2 batteries. The discharge products of Li-O2 reaction were analyzed by X-ray diffraction, X-ray photoelectron spectroscopy and nuclear magnetic resonance spectroscopy. The performance of Li-O2 batteries was strongly affected by the salt used in the electrolyte. Lithium tetrafluoroborate (LiBF4) and lithium bis(oxalato)borate (LiBOB) decompose and form LiF and lithium borates, respectively during the discharge of Li-O2 batteries. Several other salts, including lithium bis(trifluoromethane)sulfonamide (LiTFSI), lithium trifluoromethanesulfonate (LiTf), lithium hexafluorophosphate (LiPF6), lithium perchlorate (LiClO4) , and lithium bromide (LiBr) led to the discharge products which mainly consisted of Li2O2 and only minor signs of decomposition of LiTFSI, LiTf, LPF6 and LiClO4 were detected. LiBr showed the best stability during the discharge process. As for the cycling performance, LiTf and LiTFSI were the best among the studied salts. In addition to the instability of lithium salts, decomposition of tetraglyme solvent was a more significant factor contributing to the limited cycling stability. Thus a more stable nonaqueous electrolyte including organic solvent and lithium salt still need to be further developed to reach a fully reversible Li-O2 battery.

  20. Ammonium Additives to Dissolve Li2S through Hydrogen Binding for High

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Energy Li-S Batteries - Joint Center for Energy Storage Research July 1, 2016, Research Highlights Ammonium Additives to Dissolve Li2S through Hydrogen Binding for High Energy Li-S Batteries (a) Solubility of Li2S in DMSO solvent with different amounts of NH4NO3 as additive. (b) 1H chemical shifts as a function of Li2S concentration in DMSO-d6 with NH4NO3 additive. (c) DFT-derived structure of Li2S-NH4-NO3-8DMSO system shows the dissolution process of Li2S is enhanced through hydrogen

  1. Materials Data on Li6Ca12W4N16O3 (SG:220) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  2. Electrochemical Investigation of Al–Li/LixFePO4 Cells in Oligo(ethylene glycol) Dimethyl Ether/LiPF6

    SciTech Connect (OSTI)

    Wang, X.J.; Zhou, Y.N.; Lee, H.S.; Nam, K.W.; Yang, X.Q.; Haas, O.

    2011-02-01

    1 M LiPF{sub 6} dissolved in oligo(ethylene glycol) dimethyl ether with a molecular weight, 500 g mol{sup -1} (OEGDME500, 1 M LiPF{sub 6}), was investigated as an electrolyte in experimental Al-Li/LiFePO{sub 4} cells. More than 60 cycles were achieved using this electrolyte in a Li-ion cell with an Al-Li alloy as an anode sandwiched between two Li x FePO{sub 4} electrodes (cathodes). Charging efficiencies of 96-100% and energy efficiencies of 86-89% were maintained during 60 cycles at low current densities. A theoretical investigation revealed that the specific energy can be increased up to 15% if conventional LiC{sub 6} anodes are replaced by Al-Li alloy electrodes. The specific energy and the energy density were calculated as a function of the active mass per electrode surface (charge density). The results reveal that for a charge density of 4 mAh cm{sup -2} about 160 mWh g{sup -1} can be reached with Al-Li/LiFePO{sub 4} batteries. Power limiting diffusion processes are discussed, and the power capability of Al-Li/LiFePO{sub 4} cells was experimentally evaluated using conventional electrolytes.

  3. Charge states of Ca atoms in {beta}-dicalcium silicate

    SciTech Connect (OSTI)

    Mori, Kazuhiro . E-mail: kmori@rri.kyoto-u.ac.jp; Kiyanagi, Ryoji; Yonemura, Masao; Iwase, Kenji; Sato, Takashi; Itoh, Keiji; Sugiyama, Masaaki; Kamiyama, Takashi; Fukunaga, Toshiharu

    2006-11-15

    In order to study the crystal structure of {beta}-bar Ca{sub 2}SiO{sub 4}, time-of-flight neutron powder diffraction experiments were carried out at temperatures between room temperature (RT) and 600 deg. C. Rietveld refinement at RT has shown that {beta}-bar Ca{sub 2}SiO{sub 4} is monoclinic based on P2{sub 1}/n symmetry and two different types of Ca sites, Ca(1) and Ca(2). All interatomic distances within 3A were calculated, with the valences of Ca(1) with seven Ca-O bonds and Ca(2) with eight were estimated to be 1.87+ and 2+ by the Zachariasen-Brown-Altermatt formula (bond valence sum). Applying charge neutrality the two charge states of Ca in {beta}-bar Ca{sub 2}SiO{sub 4} are [Ca(1)SiO{sub 4}]{sup 2-} and Ca(2){sup 2+}, respectively. Furthermore, the [Ca(1)SiO{sub 4}]{sup 2-} unit has the shortest Ca-O distance, and its length kept constant at 2.23A at all temperatures. In the short-range structure analysis at RT, the shortest Ca-O bond was also observed in a radial distribution function. These results imply that the [Ca(1)SiO{sub 4}]{sup 2-} unit has covalency on the shortest Ca-O in addition to Si-O.

  4. Batteries - Next-generation Li-ion batteries Breakout session

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    to enable Li-metal * Inter-digitated electrodes for improved fast-charge capability * Nano-engineered electrode films to allow for thicker films Research Suggestions * See above ...

  5. Qiaojia River Power Co Ltd Li County | Open Energy Information

    Open Energy Info (EERE)

    Changde City, Hainan Province, China Zip: 415500 Sector: Hydro Product: Hunan-based small hydro developer. References: Qiaojia River Power Co., Ltd, Li County1 This article is a...

  6. Transport and Failure in Li-ion Batteries | Stanford Synchrotron...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    in Li-ion Batteries Monday, February 13, 2012 - 1:30pm SSRL Conference Room 137-322 Stephen J. Harris, General Motors R&D While battery performance is well predicted by the...

  7. Low energy detectors: 6Li-glass scintillators (Conference) |...

    Office of Scientific and Technical Information (OSTI)

    Citation Details In-Document Search Title: Low energy detectors: 6Li-glass scintillators Authors: Lee, Hye Young 1 ; Taddeucci, Terry N 1 + Show Author Affiliations Los Alamos ...

  8. Beijing ChangLi Union Energy Company | Open Energy Information

    Open Energy Info (EERE)

    Municipality, China Product: China-based technology company that research in zinc-air batteries (fuel cells). References: Beijing ChangLi Union Energy Company1 This article is a...

  9. LiDAR (Lewicki & Oldenburg) | Open Energy Information

    Open Energy Info (EERE)

    Technique LiDAR Activity Date Usefulness useful DOE-funding Unknown References Jennifer L. Lewicki, Curtis M. Oldenburg (Unknown) Near-Surface Co2 Monitoring And Analysis To...

  10. Dendrite-Free Li Deposition Using Trace-Amounts of Water as an Electrolyte

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Additive - Joint Center for Energy Storage Research April 25, 2015, Research Highlights Dendrite-Free Li Deposition Using Trace-Amounts of Water as an Electrolyte Additive Dendrite growth leads to low CE and safety issues of Li anode. Trace amount of water enables dendrite-free Li deposition. Scientific Achievement Residual water (H2O) present in nonaqueous electrolytes has been widely regarded as a detrimental factor for lithium (Li) batteries. However, dendrite-free Li film can be obtained

  11. Heteroclite electrochemical stability of an I based Li7P2S8I superionic conductor

    SciTech Connect (OSTI)

    Rangasamy, Ezhiylmurugan; Liu, Zengcai; Gobet, Mallory; Pilar, Kartik; Sahu, Gayatri; Greenbaum, Steve; Liang, Chengdu

    2015-01-01

    Stability from Instability: A Li7P2S8I solid state Li-ion conductor derived from -Li3PS4 and LiI demonstrates exceptional electrochemical stability. The oxidation instability of I is subverted nullified via its incorporation into the coordinated structure. The inclusion of I also creates stability with metallic Li anode while simultaneously improving the interfacial kinetics. Low temperature membrane processability enables facile fabrication of dense membranes, making it suitable for industrial adoption.

  12. ARM - Campaign Instrument - twin-otter-li-prof

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    govInstrumentstwin-otter-li-prof Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Campaign Instrument : Twin Otter Lidar Profiles (TWIN-OTTER-LI-PROF) Instrument Categories Aerosols, Atmospheric Profiling, Cloud Properties Campaigns Tropical Warm Pool - International Cloud Experiment (TWP-ICE) [ Download Data ] Tropical Western Pacific, 2006.01.21 - 2006.02.13 Primary Measurements Taken The following measurements are those considered

  13. LiDAR Technology | netl.doe.gov

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    LiDAR Technology LiDAR Technology Enables the Location of Historic Energy Production Sites Understanding the impact that newly developed novel methods for extracting resources from the Earth has on our environment is important, but this requires baseline data against which potential changes can be measured. In Pennsylvania, as in other parts of the United States, commercial activity has already left environmental impacts that are not readily discernible. Charcoal from a completed burn (image

  14. Predictive Materials Modeling for Li-Air Battery Systems | Argonne

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Leadership Computing Facility electron density obtained from a density functional theory Shown here is the electron density obtained from a density functional theory (DFT) calculation of lithium oxide (Li2O) performed with the GPAW code. This visualization was the result of a simulation run on Intrepid, a supercomputer at the Argonne Leadership Computing Facility. Kah Chun Lau, Aaron Knoll and Larry A. Curtiss, Argonne National Laboratory Predictive Materials Modeling for Li-Air Battery

  15. Fluoro-Carbonate Solvents for Li-Ion Cells

    SciTech Connect (OSTI)

    NAGASUBRAMANIAN,GANESAN

    1999-09-17

    A number of fluoro-carbonate solvents were evaluated as electrolytes for Li-ion cells. These solvents are fluorine analogs of the conventional electrolyte solvents such as dimethyl carbonate, ethylene carbonate, diethyl carbonate in Li-ion cells. Conductivity of single and mixed fluoro carbonate electrolytes containing 1 M LiPF{sub 6} was measured at different temperatures. These electrolytes did not freeze at -40 C. We are evaluating currently, the irreversible 1st cycle capacity loss in carbon anode in these electrolytes and the capacity loss will be compared to that in the conventional electrolytes. Voltage stability windows of the electrolytes were measured at room temperature and compared with that of the conventional electrolytes. The fluoro-carbon electrolytes appear to be more stable than the conventional electrolytes near Li voltage. Few preliminary electrochemical data of the fluoro-carbonate solvents in full cells are reported in the literature. For example, some of the fluorocarbonate solvents appear to have a wider voltage window than the conventional electrolyte solvents. For example, methyl 2,2,2 trifluoro ethyl carbonate containing 1 M LiPF{sub 6} electrolyte has a decomposition voltage exceeding 6 V vs. Li compared to <5 V for conventional electrolytes. The solvent also appears to be stable in contact with lithium at room temperature.

  16. DOE CYBER SECURITY EBK: CORE COMPETENCY TRAINING REQUIREMENTS: CA

    Broader source: Energy.gov [DOE]

    DOE CYBER SECURITY EBK: CORE COMPETENCY TRAINING REQUIREMENTS. Key Cyber Security Role: Certification Agent (CA)

  17. Materials compatibility during the chlorination of molten CaCl/sub 2/. CaO salts. [CaCl/sub 2/. CaO salt

    SciTech Connect (OSTI)

    Rense, C.E.C.; Fife, K.W.; Bowersox, D.F.; Ferran, M.D.

    1987-01-01

    As part of our effort to develop a semicontinuous PuO/sub 2/ reduction process, we are investigating promising materials for containing a 900/sup 0/C molten CaCl/sub 2/ . CaO chlorination reaction. We want the material to contain this reaction and to be reusable. We tested candidate materials in a simulated salt (no plutonium) using anhydrous HCl as the chlorinating agent. Data are presented on the performance of 36 metals and alloys, 9 ceramics, and 3 coatings.

  18. Probing the failure mechanism of nanoscale LiFePO{sub 4} for Li-ion batteries

    SciTech Connect (OSTI)

    Gu, Meng; Yan, Pengfei; Wang, Chongmin; Shi, Wei; Zheng, Jianming; Zhang, Ji-guang

    2015-05-18

    LiFePO{sub 4} is a high power rate cathode material for lithium ion battery and shows remarkable capacity retention, featuring a 91% capacity retention after 3300 cycles. In this work, we use high-resolution transmission electron microscopy and electron energy loss spectroscopy to study the gradual capacity fading mechanism of LiFePO{sub 4} materials. We found that upon prolonged electrochemical cycling of the battery, the LiFePO{sub 4} cathode shows surface amorphization and loss of oxygen species, which directly contribute to the gradual capacity fading of the battery. The finding can guide the design and improvement of LiFePO{sub 4} cathode for high-energy and high-power rechargeable battery for electric transportation.

  19. Efimov physics in {sup 6}Li atoms

    SciTech Connect (OSTI)

    Braaten, Eric; Hammer, H.-W.; Kang, Daekyoung; Platter, Lucas

    2010-01-15

    A new narrow three-atom loss resonance associated with an Efimov trimer crossing the three-atom threshold has recently been discovered in a many-body system of ultracold {sup 6}Li atoms in the three lowest hyperfine spin states at a magnetic field near 895 G. O'Hara and coworkers have used measurements of the three-body recombination rate in this region to determine the complex three-body parameter associated with Efimov physics. Using this parameter as the input, we calculate the universal predictions for the spectrum of Efimov states and for the three-body recombination rate in the universal region above 600 G where all three scattering lengths are large. We predict an atom-dimer loss resonance at 672+-2 G associated with an Efimov trimer disappearing through an atom-dimer threshold. We also predict an interference minimum in the three-body recombination rate at 759+-1 G where the three-spin mixture may be sufficiently stable to allow experimental study of the many-body system.

  20. A=6Li (66LA04)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 6Li) GENERAL: See Table 6.4 [Table of Energy Levels] (in PDF or PS). See also (AU55, LA55, ME56, FR57, HU57D, LE57F, PI58, BA59K, BR59M, FE59E, SK59, UB59, AN60, JA60G, KO60E, PH60A, TA60L, WA60F, BA61N, KO61A, SH61B, TA61G, VA61, CO62B, CR62A, DI62B, FO62E, GA62C, IN62, IN62A, IN62B, JA62, ME62A, NA62C, SA62C, ST62B, WA62H, BO63B, BU63D, DA63D, EL63D, HA63K, JA63C, JO63B, KL63, KU63B, KU63I, MO63C, OL63B, SA63K, SC63E, SC63I, VL63A, WA63, GR64C, JI64,

  1. Structural and Electrochemical Characterization of Pure LiFePO 4 and Nanocomposite C- LiFePO 4 Cathodes for Lithium Ion Rechargeable Batteries

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Kumar, Arun; Thomas, R.; Karan, N. K.; Saavedra-Arias, J. J.; Singh, M. K.; Majumder, S. B.; Tomar, M. S.; Katiyar, R. S.

    2009-01-01

    Pure limore » thium iron phosphate ( LiFePO 4 ) and carbon-coated LiFePO 4 (C- LiFePO 4 ) cathode materials were synthesized for Li-ion batteries. Structural and electrochemical properties of these materials were compared. X-ray diffraction revealed orthorhombic olivine structure. Micro-Raman scattering analysis indicates amorphous carbon, and TEM micrographs show carbon coating on LiFePO 4 particles. Ex situ Raman spectrum of C- LiFePO 4 at various stages of charging and discharging showed reversibility upon electrochemical cycling. The cyclic voltammograms of LiFePO 4 and C- LiFePO 4 showed only a pair of peaks corresponding to the anodic and cathodic reactions. The first discharge capacities were 63, 43, and 13 mAh/g for C/5, C/3, and C/2, respectively for LiFePO 4 where as in case of C- LiFePO 4 that were 163, 144, 118, and 70 mAh/g for C/5, C/3, C/2, and 1C, respectively. The capacity retention of pure LiFePO 4 was 69% after 25 cycles where as that of C- LiFePO 4 was around 97% after 50 cycles. These results indicate that the capacity and the rate capability improved significantly upon carbon coating.« less

  2. Structural and Electrochemical Characterization of PureLiFePO4and Nanocomposite C-LiFePO4Cathodes for Lithium Ion Rechargeable Batteries

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Kumar, Arun; Thomas, R.; Karan, N. K.; Saavedra-Arias, J. J.; Singh, M. K.; Majumder, S. B.; Tomar, M. S.; Katiyar, R. S.

    2009-01-01

    Pure lithium iron phosphate (LiFePO4) and carbon-coatedLiFePO4(C-LiFePO4) cathode materials were synthesized for Li-ion batteries. Structural and electrochemical properties of these materials were compared. X-ray diffraction revealed orthorhombic olivine structure. Micro-Raman scattering analysis indicates amorphous carbon, and TEM micrographs show carbon coating onLiFePO4particles. Ex situ Raman spectrum of C-LiFePO4at various stages of charging and discharging showed reversibility upon electrochemical cycling. The cyclic voltammograms ofLiFePO4and C-LiFePO4showed only a pair of peaks corresponding to the anodic and cathodic reactions. The first discharge capacities were 63, 43, and 13?mAh/g for C/5, C/3, and C/2, respectively forLiFePO4where as in case of C-LiFePO4that were 163, 144,more118, and 70?mAh/g for C/5, C/3, C/2, and 1C, respectively. The capacity retention of pureLiFePO4was 69% after 25 cycles where as that of C-LiFePO4was around 97% after 50 cycles. These results indicate that the capacity and the rate capability improved significantly upon carbon coating.less

  3. Influence of Li ions on the oxygen reduction reaction of platinum electrocatalyst

    SciTech Connect (OSTI)

    Liu, H; Xing, YC

    2011-06-01

    A Li-air battery can provide a much higher theoretical energy density than a Li-ion battery. The use of aqueous acidic electrolytes may prevent lithium oxide deposition from aprotic electrolytes and lithium carbonate precipitation from alkaline electrolytes. The present communication reports a study on the effect of Li ions on the oxygen reduction reaction (ORR) in sulfuric acid electrolytes. It was found that the Li ions have negligible interactions with the active surface of Pt catalysts. However, significantly lower ORR activities were found when Li ions are present in the sulfuric acid. The intrinsic kinetic activities were found to decrease with the increase of Li ion concentrations, but level off when the Li ion concentrations are larger than 1.0 M. The low activities of Pt catalysts in Li ion containing electrolytes were attributed to a constraining effect of Li ions on the diffusion of oxygen in the electrolyte solution. (C) 2011 Elsevier B.V. All rights reserved.

  4. DISCOVERY OF SUPER-Li-RICH RED GIANTS IN DWARF SPHEROIDAL GALAXIES

    SciTech Connect (OSTI)

    Kirby, Evan N.; Fu, Xiaoting; Deng, Licai; Guhathakurta, Puragra

    2012-06-10

    Stars destroy lithium (Li) in their normal evolution. The convective envelopes of evolved red giants reach temperatures of millions of kelvin, hot enough for the {sup 7}Li(p, {alpha}){sup 4}He reaction to burn Li efficiently. Only about 1% of first-ascent red giants more luminous than the luminosity function bump in the red giant branch exhibit A(Li) > 1.5. Nonetheless, Li-rich red giants do exist. We present 15 Li-rich red giants-14 of which are new discoveries-among a sample of 2054 red giants in Milky Way dwarf satellite galaxies. Our sample more than doubles the number of low-mass, metal-poor ([Fe/H] {approx}< -0.7) Li-rich red giants, and it includes the most-metal-poor Li-enhanced star known ([Fe/H] = -2.82, A(Li){sub NLTE} = 3.15). Because most of the stars have Li abundances larger than the universe's primordial value, the Li in these stars must have been created rather than saved from destruction. These Li-rich stars appear like other stars in the same galaxies in every measurable regard other than Li abundance. We consider the possibility that Li enrichment is a universal phase of evolution that affects all stars, and it seems rare only because it is brief.

  5. High performance anode for advanced Li batteries

    SciTech Connect (OSTI)

    Lake, Carla

    2015-11-02

    The overall objective of this Phase I SBIR effort was to advance the manufacturing technology for ASI’s Si-CNF high-performance anode by creating a framework for large volume production and utilization of low-cost Si-coated carbon nanofibers (Si-CNF) for the battery industry. This project explores the use of nano-structured silicon which is deposited on a nano-scale carbon filament to achieve the benefits of high cycle life and high charge capacity without the consequent fading of, or failure in the capacity resulting from stress-induced fracturing of the Si particles and de-coupling from the electrode. ASI’s patented coating process distinguishes itself from others, in that it is highly reproducible, readily scalable and results in a Si-CNF composite structure containing 25-30% silicon, with a compositionally graded interface at the Si-CNF interface that significantly improve cycling stability and enhances adhesion of silicon to the carbon fiber support. In Phase I, the team demonstrated the production of the Si-CNF anode material can successfully be transitioned from a static bench-scale reactor into a fluidized bed reactor. In addition, ASI made significant progress in the development of low cost, quick testing methods which can be performed on silicon coated CNFs as a means of quality control. To date, weight change, density, and cycling performance were the key metrics used to validate the high performance anode material. Under this effort, ASI made strides to establish a quality control protocol for the large volume production of Si-CNFs and has identified several key technical thrusts for future work. Using the results of this Phase I effort as a foundation, ASI has defined a path forward to commercialize and deliver high volume and low-cost production of SI-CNF material for anodes in Li-ion batteries.

  6. High Performance Cathodes for Li-Air Batteries

    SciTech Connect (OSTI)

    Xing, Yangchuan

    2013-08-22

    The overall objective of this project was to develop and fabricate a multifunctional cathode with high activities in acidic electrolytes for the oxygen reduction and evolution reactions for Li-air batteries. It should enable the development of Li-air batteries that operate on hybrid electrolytes, with acidic catholytes in particular. The use of hybrid electrolytes eliminates the problems of lithium reaction with water and of lithium oxide deposition in the cathode with sole organic electrolytes. The use of acid electrolytes can eliminate carbonate formation inside the cathode, making air breathing Li-air batteries viable. The tasks of the project were focused on developing hierarchical cathode structures and bifunctional catalysts. Development and testing of a prototype hybrid Li-air battery were also conducted. We succeeded in developing a hierarchical cathode structure and an effective bifunctional catalyst. We accomplished integrating the cathode with existing anode technologies and made a pouch prototype Li-air battery using sulfuric acid as catholyte. The battery cathodes contain a nanoscale multilayer structure made with carbon nanotubes and nanofibers. The structure was demonstrated to improve battery performance substantially. The bifunctional catalyst developed contains a conductive oxide support with ultra-low loading of platinum and iridium oxides. The work performed in this project has been documented in seven peer reviewed journal publications, five conference presentations, and filing of two U.S. patents. Technical details have been documented in the quarterly reports to DOE during the course of the project.

  7. Degradation Reactions in SONY-Type Li-Ion Batteries

    SciTech Connect (OSTI)

    Nagasubramanian, G.; Roth, E. Peter

    1999-05-04

    Thermal instabilities were identified in SONY-type lithium-ion cells and correlated with interactions of cell constituents and reaction products. Three temperature regions of interaction were identified and associated with the state of charge (degree of Li intercalation) of the cell. Anodes were shown to undergo exothermic reactions as low as 100°C involving the solid electrolyte interface (SEI) layer and the LiPF6 salt in the electrolyte (EC: PC: DEC/LiPF6). These reactions could account for the thermal runaway observed in these cells beginning at 100°C. Exothermic reactions were also observed in the 200°C-300°C region between the intercalated lithium anodes, the LiPF6 salt and the PVDF. These reactions were followed by a high- temperature reaction region, 300°C-400°C, also involving the PVDF binder and the intercalated lithium anodes. The solvent was not directly involved in these reactions but served as a moderator and transport medhun. Cathode exotherrnic reactions with the PVDF binder were observed above 200oC and increased with the state of charge (decreasing Li content). This offers an explanation for the observed lower thermal runaway temperatures for charged cells.

  8. Microsoft Word - Cd-CA.doc

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    The First Cadmium Enzyme - Carbonic Anhydrase 2 from the marine diatom Thalassiosira weissflogii Todd W. Lane 1 , Mak A. Saito 2 , Graham N. George 3 , Ingrid J. Pickering 3 , Roger C. Prince 4 and François M.M. Morel 5 1 Biosystems Research Department, Sandia National Labs, Livermore, CA 2 Marine Chemistry and Geochemistry Department, Woods Hole Oceanographic Institution, Woods Hole, MA 3 Department of Geological Sciences, University of Saskatchewan, Saskatoon, Canada 4 ExxonMobil Research

  9. Operando NMR and XRD study of chemically synthesized LiCx oxidation...

    Office of Scientific and Technical Information (OSTI)

    Title: Operando NMR and XRD study of chemically synthesized LiCx oxidation in a dry room environment We test the stability of pre-lithiated graphite anodes for Li-ion batteries in ...

  10. Xiang Ge Li La Xian Mai Di He Hydro Power Development Co Ltd...

    Open Energy Info (EERE)

    Xiang Ge Li La Xian Mai Di He Hydro Power Development Co Ltd Jump to: navigation, search Name: Xiang Ge Li La Xian Mai Di He Hydro Power Development Co., Ltd. Place: Yunnan...