05.01.2015 Views

Invited Talks: Transition Metal Oxides - University Blog Service - The ...

Invited Talks: Transition Metal Oxides - University Blog Service - The ...

Invited Talks: Transition Metal Oxides - University Blog Service - The ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

<strong>Invited</strong> <strong>Talks</strong>: <strong>Transition</strong> <strong>Metal</strong> <strong>Oxides</strong>


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

<strong>The</strong> explicit role of O 2p states in high oxidation state transition metal oxides<br />

George A. Sawatzky<br />

<strong>University</strong> of British Columbia<br />

Email: Website:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

For late 3d transition metal oxide with formally high oxidation states like Cu3+,Ni3+, Co4+, Fe4+,5+,<br />

Mn 4+ the charge transfer energy for transferring electrons from O to the transition metal may be negative<br />

resulting in a formally more correct starting point in which the oxidation state is lowered and holes in the<br />

O 2p orbitals are introduced. In this talk we present experimental evidence for this in several systems and<br />

discuss the consequences in terms of magnetic properties and issues such as potential charge<br />

disproportionation. We use x ray spectrosocpies and model cluster like calculations to demonstrate the<br />

importance of considering the hole occupation of the O 2p states explicitly and discuss some popular<br />

materials like the Cuprates Nicalates and Cobaltates from this rather different starting point.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

<strong>The</strong> Verwey phase of magnetite - an old(ish) mystery in transition metal oxides<br />

J. Paul Attfield<br />

Centre for Science at Extreme Conditions and School of Chemistry, <strong>University</strong> of Edinburgh, West Mains Road,<br />

Email: j.p.attfield@ed.ac.uk<br />

Edinburgh, EH9 3JJ, UK.<br />

Website: http://www.chem.ed.ac.uk/staff/academic/attfield.html<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Magnetite (Fe 3 O 4 ) is the eponymous magnetic substance. Its properties have guided the evolution of<br />

magnetoceptive organisms, and of human science and technology over 3000 years. During the twentieth<br />

century magnetite was found to be a ferrimagnetic, inverse spinel-type oxide with applications in magnetic<br />

recording and, more recently, spintronic and multiferroic devices. Spin-spin couplings between<br />

tetrahedrally and octahedrally coordinated Fe-sites follow the Goodenough-Kanamori rules. Magnetite<br />

undergoes a complex structural and electronic transition below 125 K. In 1939, Verwey proposed that this<br />

is driven by a charge ordering of Fe 2+ and Fe 3+ ions, but the low temperature state remained unknown and<br />

contentious, with a variety of models proposed over 70 years of study. <strong>The</strong> full low temperature<br />

superstructure of magnetite was recently solved from high energy x-ray microcrystal diffraction data. 1<br />

Verwey’s hypothesis was found to be approximately correct but an unexpected localization of electrons in<br />

three-Fe ‘trimeron’ units (highly structured small polarons) was discovered – this description is supported<br />

by band structure calculations. 2 Trimerons are proposed to be a type of ‘orbital molecule’; these may be<br />

important quasiparticles in magnetic oxides.<br />

1. M.S. Senn, J.P. Wright and J.P. Attfield, Nature 481, 173 (2012).<br />

2. M.S. Senn, I. Loa, J.P. Wright and J.P. Attfield, Phys. Rev. B (2012).


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

New Iron <strong>Oxides</strong> by Soft Chemistry<br />

Mikio Takano<br />

Institute for Integrated Cell-Material Sciences (WPI-iCeMS), Kyoto <strong>University</strong>, Kyoto 606-8501, Japan<br />

takano@icems.kyoto-u.ac.jp http://www.icems.kyoto-u.ac.jp/<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

1: BaFe 4+ O 3 (BFO) A small class of oxides containing iron in a high valence state of Fe 4+ (d 4 ) have<br />

been known. <strong>The</strong> most representative phase is SrFeO 3 (SFO) which crystallizes in the cubic perovskite<br />

structure (a = 3.850 Å). All the Fe 2+ - and Fe 3+ -oxides are antiferromagnetic insulators in their ground<br />

states, while SFO and related Fe 4+ -oxides commonly exhibit shift toward metallicity and ferromagnetism.<br />

We succeeded in obtaining BaFeO 3 (BFO) crystallizing in the cubic perovskite structure (a = 3.971 Å),<br />

not in the known hexagonal perovskite structure, by flowing ozone over BaFeO 2.5 powder at a low<br />

temperature of 200°C. It has been found that BFO has a spiral spin structure of the A-type below 111 K<br />

but turns ferromagnetic with a large moment of 3.5 μ B /Fe on application of a small external field of ~0.3 T<br />

at 5 K (0.2 T at 77 K). BFO is the very first Fe-oxide that shows ferromagnetism at ambient pressure (N.<br />

Hayashi et al., Angew. Chem. Int. Ed., 43, 12547, 2011). <strong>The</strong> ferromagnetic transition temperature<br />

exceeds 300K as external pressure is increased up to 40 GPa as examined by in-situ Mössbauer<br />

measurements. <strong>The</strong> P-T phase diagram of BFO will be compared with that of SFO which shows pressureinduced<br />

ferromagnetism.<br />

2: Biogenous Iron <strong>Oxides</strong> (BIOX) Prof. J. Takada’s group (Okayama Univ.) has found that the Fe 3+ -<br />

based microtubular deposit produced by a species of water-habitant bacteria, Leptothrix ochracea, shows<br />

interesting unexpected functionalities as a catalyst support, as a starting materials for beautiful red<br />

pigments, and so on. Results of recent studies in which I have been involved will be presented.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Transiton <strong>Metal</strong> <strong>Oxides</strong>: Superconductors, Multiferroics,<br />

and Catalysts for Water Splitting<br />

Martha Greenblatt<br />

Department of Chemistry and Chemical Biology, Rutgers <strong>University</strong><br />

martha@rutchem.rutgers.edu:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Combined experimental and DFT theoretical results on low-dimensional new Ni + /Ni 2+ (d 9 /d 8 ) homologous<br />

series, Ln n+1 Ni n O 2n+2 with n =2 and 3 layered oxides with Ruddlesden-Popper (RP)-related structures and<br />

isostructural and isoelectronic with the high temperature superconducting cuprates are presented.<br />

Temperature variation of magnetization, transport, specific heat and 139 La NMR data in La 4 Ni 3 O 8 evidence<br />

the presence of a transition near ~105 K. DFT calculations suggest similarity of the band structure with that<br />

of the cuprate superconductors and relate the transition at 105 K to a spin density wave nesting instability<br />

of the Fermi surface. More recent experimental and theoretical studies suggest that the transition seen at<br />

105 K could be a high spin-to-low spin transition of Ni 2+ (d8). A quaternary perovskite, PbMn 3 Mn 4 O 12<br />

prepared at high pressure and high temperature, undergoes a structural phase transition at ~380 K from the<br />

room temperature rhombohedral-to-a high temperature cubic phase. Temperature dependence of magnetic<br />

susceptibility, electronic transport and dielectric constant show a transition at ~68 K, which suggest<br />

coupling of a ferroelectric-like and magnetic behavior that is potentially multiferroic. Cheaper efficient<br />

catalysts made from earth abundant (not noble metals) and environmentally green materials are<br />

indispensible for extracting hydrogen from water, the essential precursor to all globally sustainable fuels.<br />

Achieving this goal and the reduction of CO 2 to liquid fuels are necessary to replace fossil fuels. We have<br />

synthesized different polymorphs of LiCoO 2 and compared their catalytic activity in water oxidation. Our<br />

results show that LiCoO 2 is active exclusively in the low-temperature cubic “spinel-like” structure, while<br />

inactive as the high-temperature layered phase, which is thermodynamically more stable. <strong>The</strong> related spinel<br />

LiMn 2 O 4 is transformed from an inactive to a highly efficient water oxidation catalyst (λ-MnO 2 ) upon the<br />

topotactic removal Li + . <strong>The</strong>se spinel phases contain cubical metal-oxo (M 4 O 4 ) subunits (absent in the<br />

layered LiCoO 2 analog) that appear to be the key to catalytic activity. <strong>The</strong> biological basis of the<br />

mechanism for the high activity of the M 4 O 4 -cubical topology of spinels in water oxidation will be<br />

discussed.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering–<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Perovskites of p-block elements: influence of the lone electron pair<br />

José-Antonio Alonso<br />

Instituto de ciencia de Materiales de Madrid, C.S.I.C., Cantoblanco, 28049 Madrid<br />

Email: ja.alonso@icmm.csic.es Website: http://www.icmm.csic.es/matfuelcells/<br />

Perovskite oxides containing p-block elements at the A positions provide the possibility of investigating<br />

the stereochemical effect of the lone electron pair on the crystal structure and properties of these materials.<br />

In this work we will address the singular features of two families of perovskites: Se(Te)MO 3 (M=<br />

Mn,Co,Ni) and Pb 2 (M,Sb)O 6 (M= rare earths). <strong>The</strong> former oxides are only accesses via high-pressure<br />

synthesis, given the small size of Se 4+ (Te 4+ ) and the extremely distorted MO 6 octahedral framework. <strong>The</strong><br />

irregular oxygen environment around Se(Te) is the result of the presence of the Se 4+ (Te 4+ ) non-bonded<br />

lone 4s 2 electron pair, which is thought to be directed towards the apex of each trigonal pyramid.<br />

Additionally, three short Se-O bond lengths, implying very covalent Se-O bonds in a trigonal pyramidal<br />

configuration, are an important ingredient for the stability of this family of SeMO 3 perovskites. <strong>The</strong> highpressure<br />

structural evolution also provides with clues to understand the nature of the chemical bond in<br />

these materials. <strong>The</strong> family of Pb 2 (M,Sb)O 6 oxides, typified by Pb 2 TmSbO 6 , exhibit a room-temperature<br />

structure never observed in double perovskites, and an original sequence of phase transitions with<br />

temperature; in the different structures an asymmetrical distribution of the chemical bonds driven by the<br />

strong interaction between the Pb 2+ non-bonded 6s 2 electron pair and the oxygen p states is observed,<br />

which has been visualized from the electron localization function obtained from DFT calculations by<br />

using accurate structural data for the room temperature crystal structure. Moreover, the presence of an<br />

unexpected hybridization between Y and oxygen has been observed in Pb 2 YSbO 6 . This behavior involves<br />

the oxygen atoms that form the PbO 4 polyhedron, suggesting a strong effect of the chemical pressure of<br />

the non-bonded electron pair of lead in the whole structure of these compounds.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

<strong>Invited</strong> <strong>Talks</strong>: Energy Storage Materials


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Lessons from the early days of Li-ion<br />

Jeff Dahn<br />

Dalhousie <strong>University</strong><br />

Email: Website:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Most early Li‐ion cells used LiCoO2 as the positive electrode material, even though John Goodenough and coworkers<br />

showed that LiNiO2 was also an intercalation electrode. At Moli Energy Ltd, where I was Director of<br />

Research, we "bet the farm" on LiNiO2 around 1988 due to the lower cost of Ni compared to Co. Our early scale<br />

up experiments led to surprises regarding the reactivity of Li(x)NiO2 with electrolyte at elevated temperature.<br />

Using my old research report records, I will describe our successes and ultimate failure using LiNiO2 in Li‐ion cells.<br />

Characterizing charged positive electrode reactivity with electrolyte turns out to be one of the first (not the last!)<br />

experiments one should do when evaluating new electrode materials. <strong>The</strong>se lessons are critical for young (and<br />

old!) researchers moving into Na‐ion and Mg‐ion systems.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Towards the design of new Fe-based polyanionic compounds<br />

from inductive effect guidance.<br />

J-M. Tarascon et al … ,<br />

Laboratoire de Réactivité et Chimie des Solides,<br />

Université de Picardie Jules Verne, UMR-CNRS 6007,<br />

33, rue Saint Leu, Amiens Cedex, 80039, France.<br />

jean-marie.tarascon@u-picardie.fr<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Li-ion batteries are strongly considered for electric transportation or for making the use of<br />

renewable energy the easiest, provided that improvements can be achieved in terms of cost, safety, energy<br />

density and sustainability. This drastically limits the choice of periodic table elements that can be used.<br />

Polyanionic compounds based on either SiO 4 4- , PO 4 3- , or BO 3 3- are being the subject of very intensive<br />

research as they markedly present some of the above benefits we are looking for. <strong>The</strong>refore to increase<br />

their energy density, we have explored, based on the inductive effect concept, the synthesis of compounds<br />

containing both Li and Fe cations together with highly electronegative polyanions with or without the<br />

presence of the most electronegative element, namely fluor.<br />

Combining this strategy with the development of novel low temperature synthesis routes, we have<br />

discovered a new class of Li-based fluorosulphate materials of formulae AMSO 4 F (A=Li, Na, K; M=3d<br />

metals). Among them, LiFeSO 4 F, which presents polymorphism, shows a redox voltage of 3.6 V vs.<br />

Li+/Li° when crystallized in the tavorite form as compared to 3.9 V for the triplite one. This is the highest<br />

potential ever reported for a Fe 3+ /Fe 2+ inorganic compound so far, and simple structural/inductive effect<br />

arguments will be proposed to explain such results.<br />

By mastering the sulphate chemistry we could also prepare new phases such as Li 2 M(SO 4 ) 2<br />

(M=Fe/Co) or new ones whose structure and electrochemical performances will be reported as well.<br />

Within the context of this symposium, the magnetic properties of these phases, which are<br />

antiferromagnetic, will be recapped and the variation of Neel transition temperatures explained in terms of<br />

superexchange interactions.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Lithium Batteries: What Are the Adjusting Screws<br />

Joachim Maier<br />

Max Planck Institute for Solid State Research, Heisenbergstr. 1, D-70569 Stuttgart, Germany<br />

Email: s.weiglein@fkf.mpg.de Website: http://www2.fkf.mpg.de/maier/<br />

<strong>The</strong> contribution focuses on the dominant processes in Li-based batteries and the adjusting screws to<br />

improve the relevant materials. Special emphasis is laid on the significance of point defect chemistry. One<br />

major control parameter that became available in the context of nanotechnology and the exploitation of<br />

which is one of the major drivers in the field, is size. <strong>The</strong> contribution systematically explores the<br />

implication of size on kinetic and thermodynamic issues (nanoionics). <strong>The</strong>se issues refer to improved<br />

electrolytes, improved electrodes, varied cell-voltages and electrochemical performances.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

<strong>The</strong> Rechargeable Aprotic Li-O 2 Battery<br />

Peter G. Bruce<br />

School of Chemistry, <strong>University</strong> of St Andrews, St Andrews, Scotland, UK<br />

Email: pgb1@st-andrews.ac.uk Website: chemistry.st-andrews.ac.uk/staff/pgb/<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

John Goodenough’s immense contribution to lithium battery research has always been characterized by<br />

thinking beyond the current horizon of the technology. He harnesses science in pursuit of next generation<br />

lithium batteries. John investigated oxide-based cathodes at a time when much of the focus was on<br />

sulfides. In this spirit, the talk will consider the rechargeable aprotic lithium-air (O 2 ) battery; a potentially<br />

transformational technology but one that will require scientific advances, even to permit a realistic<br />

assessment of the potential practicality of such an energy storage device.<br />

Aqueous and non-aqueous (aprotic) Li-O 2 batteries are under intense investigation. <strong>The</strong> latter presents us<br />

with scientific challenges associated with the anode, electrolyte and cathode. After summarizing a number<br />

of these challenges, the problem of the electrolyte will be considered in greater depth. Early aprotic Li-O 2<br />

cells employed organic carbonate electrolytes, which have since been shown to exhibit such instability<br />

towards reduced oxygen species at the cathode that there is little or no Li 2 O 2 formation. As a result, the<br />

ability to cycle such a cell is not associated with the reversible electrochemistry of Li 2 O 2<br />

formation/decomposition, as previously thought. Other electrolytes have been investigated and will be<br />

discussed in terms of their ability to support truly reversible Li 2 O 2 electrochemistry at the positive<br />

electrode; something that is essential if the aprotic Li-O 2 cell is ever to succeed as an energy storage<br />

device.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Posters


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Phase Transformation from Vanadium Sulfide to <strong>Oxides</strong> via a New Chemical Route for the Synthesis<br />

of β-Li x V 2 O 5 as a High Performance Cathode<br />

Nina Mahootcheian Asl, Wen Chao Lee, Youngsik Kim *<br />

a<br />

Richard Lugar Center for Renewable Energy, Department of Mechanical Engineering,<br />

Indiana <strong>University</strong> Purdue <strong>University</strong> Indianapolis, Indianapolis, Indiana, USA<br />

*Corresponding Author, Email: yk35@iupui.edu (Y. Kim)<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

High temperature vanadium pentoxide phase, β-Li x V 2 O 5 , was synthesized by a new chemical<br />

route synthesis method, which involved phase transformation from the pure LiVS 2 by heat treatment at<br />

600 °C in atmospheric air. When using this method, well crystalized rod-shaped particles with 20 – 30<br />

µm in length and 3 – 6 µm in width were found. Moreover, the surface of β-Li x V 2 O 5 particles was<br />

found to be coated by an amorphous vanadium oxysulfide film (~20 nm in thickness). In contrast to a low<br />

temperature vanadium pentoxide phase, Li x V 2 O 5 , the electrochemical intercalation of lithium into the high<br />

temperature vanadium pentoxide phase, β-Li x V 2 O 5 , was fully reversible in the range of 0.0 < x < 2.0 and<br />

had a capacity up to 310 mAh/g at 0.07 C between 1.5 V and 4 V. A good capacity retention of more<br />

than 88% was also observed after 50 cycles even at the higher current rate of 2 C. <strong>The</strong> observed<br />

electrochemical performance of the heat-prepared sample was quite surprising when considering its<br />

particle size and comparing it to other vanadium pentoxides prepared using a different synthesis method.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

High-Voltage Spinel Cathodes for Lithium-Ion Batteries<br />

Katharine Chemelewski, Eun Sung Lee, Zach Moorhead-Rosenberg, Il Tae Kim, and Arumugam Manthiram<br />

Materials Science and Engineering Program, <strong>The</strong> <strong>University</strong> of Texas at Austin<br />

Email: manth@austin.utexas.edu Website: http://www.me.utexas.edu/~manthiram<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> high-voltage spinel cathode LiMn 1.5 Ni 0.5 O 4 is a promising candidate for large-scale energy storage solutions of<br />

the future. With fast, 3D lithium-ion diffusion pathways and a robust crystal structure, this cathode material is well<br />

suited for implementation in vehicle and grid storage applications. However, widespread adoption has been<br />

hampered by capacity fade particularly at elevated temperatures, which has been attributed to many factors<br />

including aggressive solid-electrolyte interphase (SEI) reaction, cation ordering, site defects resulting in the<br />

formation of Mn 3+ , and the orientation of the crystal planes facing the surface. We present here investigations to<br />

develop a fundamental understanding of the factors that govern the electrochemical properties of LiMn 1.5 Ni 0.5 O 4 , as<br />

well as novel techniques to characterize the materials quantitatively and surface modification to suppress unwanted<br />

side reactions. <strong>The</strong> solubility of Ni in LiMn 1.5 Ni 0.5 O 4 is dependent on temperature and increases with decreasing<br />

annealing temperature (e.g., 700 o C), eliminating the Li x Ni 1-x O impurity. Additionally, precursor synthesis<br />

conditions including temperature, pH, stir speed, pressure, and annealing conditions affect the morphology and<br />

electrochemical properties of the final cathode material, and the orientation of the crystal planes facing the<br />

electrolyte interface is a critical factor for stabilizing the cathode during high-voltage operation. Also, it is known<br />

that the performance of the undoped LiMn 1.5 Ni 0.5 O 4 spinel is influenced by the Mn 3+ content, and a magnetic method<br />

has been developed, for the first time, to determine quantitatively the Mn 3+ content that agrees closely with the<br />

electrochemical data. Furthermore, the degree of cation ordering could be compared by examining the lithium<br />

insertion reaction below 3 V into the empty 16c sites, which is consistent with the FTIR and electrochemical data.<br />

Finally, surface modification with graphene and AlPO 4 is shown to improve the cyclability and rate capability of<br />

high-voltage spinel cathodes.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Direct Methanol Fuel Cells: New Materials and Stack Development<br />

Thom Cochell, Wei Li, Xinsheng Zhao, Zhongqing Jiang, Zincheng & Arumugam Manthiram<br />

Materials Science and Engineering Program and Texas Material Institute,<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, TX 78712, United States<br />

Email: rmanth@mail.utexas.edu; Website: http://www.me.utexas.edu/~manthiram/index.htm<br />

Direct Methanol Fuel Cells (DMFCs) are promising electrochemical energy conversion devices for mobile<br />

and portable applications. However, several technical barriers must be overcome including sluggish<br />

methanol oxidation and oxygen reduction reactions, methanol fuel crossover through the proton exchange<br />

membrane from the anode to the cathode, and dissolution of the anode PtRu catalyst. To overcome these<br />

barriers of DMFC commercialization, we have developed new materials and implemented novel<br />

manufacturing processes. <strong>The</strong> new anode catalyst PtRuSnCe/C was shown to have superior durability<br />

compared to the commercial PtRu/C anode catalyst. An optimized low-cost cathode catalyst Pd 4 Co/C was<br />

found to exhibit better performance than Pt/C in DMFC. <strong>The</strong> blend membrane SPEEK + PSf-NBlm shows<br />

lower methanol crossover than Nafion 115, and the home-made graphite bipolar plates show superior<br />

single cell performance to commercial graphite plates. Additionally, novel PtPdCu-based catalysts have<br />

been designed that show enhanced oxygen reduction activity, and several different SPEEK-based<br />

membranes have been tailored to lower methanol crossover and increase proton conductivity. Inkjet<br />

printing and autospray processing methods were used for fabrication of uniform catalyst layers. Together<br />

these novel materials and processing techniques were utilized to prepare an 18 W 20-cell and an 11 W 10-<br />

cell DMFC stack.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Materials and Interfacial Chemistry for Next Generation Electrical Energy Storage<br />

S. Dai, 1 M. P. Paranthaman, 1 C. A. Bridges, 1 R. R. Unocic, 1 X. G. Sun, 1 D.-E. Jiang, 1 G. M. Veith, 1<br />

J. B. Goodenough, 2 and A. Manthiram 2<br />

1 Oak Ridge National Laboratory, Oak Ridge, TN 37831<br />

2 <strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, TX 78712<br />

Email: dais@ornl.gov<br />

Abstract:<br />

<strong>The</strong> overarching goal is to investigate fundamental principles governing energy storage through<br />

integrated synthesis and advanced characterization. Our current research is focused on fundamental<br />

investigation of electrolytes based on ionic liquids and rational synthesis of novel electrode architectures<br />

through Fermi level engineering of anode and cathode redox levels by employing porous structures and<br />

surface modifications as well as advanced operando characterization techniques including neutron<br />

diffraction and scattering. <strong>The</strong> key scientific question concerns the relationship between chemical<br />

structures and their energy-storage efficacies. A novel approach based on small angle neutron scattering<br />

(SANS) enables the observation of electrochemical processes during the cycling of high capacity lithium<br />

ion batteries. Changes in neutron scattering intensity associated with mesopore ordering show the<br />

processes of solid-electrolyte interphase (SEI) formation and lithium intercalation. Using a lithium-ion<br />

half-cell and different solvent deuteration levels, our results demonstrate that SANS can be employed to<br />

better understand complicated electrochemical processes occurring in rechargeable batteries. We will also<br />

report our recent results on ionic liquid electrolytes, and mesoporous architectures for high performance<br />

lithium ion batteries.<br />

Research Sponsored by the U.S. Department of Energy, Basic Energy Sciences, Materials Sciences and<br />

Engineering Division. Research supported by Oak Ridge National Laboratory’s SHaRE User Facility and<br />

Spallation Neutron Source, which are sponsored by the Scientific User Facility Division, Office of Basic<br />

Energy Sciences, U.S. Department of Energy.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Molecular Concepts of Inorganic Structures with Emphasis on Noncentrosymmetry<br />

and Local Geometry.<br />

Martin D. Donakowski*, Romain Gautier, Anastasiya I. Vinokur, Kenneth R. Poeppelmeier<br />

Northwestern <strong>University</strong>; 2145 Sheridan Rd; Evanston, IL; 60208<br />

*Email: martindonakowski@u.northwestern.edu Website: http://chemgroups.northwestern.edu/poeppelmeier/<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

This poster describes coordination environments of vanadium oxyfluoride (VOFs) materials; specifically,<br />

the structural implications of the variable nucleophilicities of VOF anions. <strong>The</strong> VOF basic building unit<br />

(BBU) [VOF 5 ] 2- has been noted for its low nucleophilicity in comparison to the similar anion [NbOF 5 ] 2- .<br />

To examine the coordination of VOF we present the compounds I) CuMOF 5 (H 2 O) 4 (pyz) 2 and<br />

CuMOF 5 (H 2 O)(pyz) 3 (M = V V , Nb V ), II) MVOF 4 (H 2 O) 7 (M II = Co, Ni, Cu, Zn), and III)<br />

Na 2 (M(H 2 O) 2 )(V 2 F 6 O 4 ) (M II = Co, Ni, Cu). Compounds (I) present order or disorder of the oxide and<br />

fluoride ligands owing to the nucleophilicity of the VOF BBU [VOF 5 ] 2- and the use of an organic<br />

molecule present (pyrazine). Compounds (II) display an interesting phenomenon: the anion<br />

[VOF 4 (H 2 O)] 2- is only able to coordinate to the cation [M(H 2 O) 6 ] 2+ when M II = Cu. This results in the<br />

hydrated compound CuVOF 4 (H 2 O) 7 comprised of lambda (Λ)-shaped BBUs that crystallize in a<br />

noncentrosymmetric space group for reasons that will be described. Compounds (III) exhibit a rarely<br />

ordered dioxo vanadium fluoride [VO 2 F 4 ] 3- that dimerizes into the new BBU [V 2 O 4 F 6 ] 4- . In comparison to<br />

[VOF 5 ] 2- This dioxo vanadium fluoride has increased nucleophilicity of the oxide ligands owing to the<br />

division of the pi-bonding orbitals of the V V cation amongst two oxide ligands and the geometry of the<br />

dimeric VOF BBU. Implications of the nucleophilicity of the VOF will be explained in terms of synthetic<br />

strategies to create materials for purposes of nonlinear optical (NLO) activity with analogies to organic<br />

chemistry methodology.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Electrodeposition of Amorphous Silicon Anode for Lithium Ion Batteries<br />

Rigved Epur a , Madhumati Ramanathan b , Faith R. Beck a,c ,<br />

A. Manivannan c and Prashant N. Kumta a,b,d,†<br />

aDepartment of Mechanical Engineering and Materials Science, <strong>University</strong> of Pittsburgh,<br />

Pittsburgh, PA 15261, USA<br />

bDepartment of Bioengineering, <strong>University</strong> of Pittsburgh, Pittsburgh, PA 15261, USA<br />

cUS Department of Energy, National Energy Technology Laboratory, Morgantown, WV 26507, USA<br />

dDepartment of Chemical and Petroleum Engineering, <strong>University</strong> of Pittsburgh, Pittsburgh, PA 15261,<br />

USA<br />

Email: pkumta@pitt.edu, manivana@netl.doe.gov<br />

Amorphous silicon has been successfully electrodeposited on copper using a SiCl4 based organic<br />

electrolyte under galvanostatic conditions. <strong>The</strong> electrodeposited silicon films were characterized for their<br />

composition, morphology and structural characteristics using glancing angle x-ray diffraction (GAXRD),<br />

scanning electron microscopy (SEM), and Raman spectroscopy. GAXRD and Raman analyses clearly<br />

confirm the amorphous state of the deposited silicon film. <strong>The</strong> deposited films were tested for possible<br />

application as anodes for Li-ion battery. <strong>The</strong> results indicate that this binder less amorphous silicon anode<br />

exhibits a reversible capacity of ~1300 mAh g -1 with a columbic efficiency of > 99.5% up to 100 cycles.<br />

Impedance measurements at the end of each charge cycle show a non-variable charge transfer resistance<br />

which contributes to the excellent cyclability over 100 cycles observed for the films. This approach of<br />

developing thin amorphous silicon films directly on copper eliminates the use of binders and conducting<br />

additives, rendering the process simple, facile and easily amenable for large scale manufacturing.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Electronic structure effects in platinum/valve-metal thin film alloys,<br />

that exhibit enhanced oxygen reduction reaction rates<br />

Charles C. Hays<br />

4800 Oak Grove Drive<br />

Jet Propulsion Laboratory<br />

California Institute of Technology, Pasadena, CA 91109<br />

Email: cchays@jpl.nasa.gov<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

In an effort to reduce the platinum group metal (PGM) loading for the cathode in hydrogen-air fuel cells,<br />

we have examined the electrochemical performance of Pt-based alloys, in the form of crystallographically<br />

oriented (111) thin films. Using a multi-electrode technique developed at JPL, we have examined the<br />

electrochemical performance of Pt alloyed with valve metals (Ti, V, and Zr) and the late transition metals<br />

(Co, Ni). Our results indicate that alloys with as little as 30 atomic % Pt, are stable in perchloric and<br />

sulfuric acid electrolytes. <strong>The</strong> alloys are electrochemically active for the major reactions; e.g., the<br />

hydrogen-oxidation-reaction (HOR), hydrogen-evolution-reaction (HER), oxygen-reduction-reaction<br />

(ORR), and oxygen-evolution-reaction (OER). In this contribution, we will focus on results, which show<br />

that significantly enhanced ORR rates are exhibited in the Pt-Co-Zr and Pt-Ni-V composition manifolds,<br />

where the measured ORR rates exceed those of Pt (111) thin films tested in the same cell, by factors as<br />

large as 86X. In each system, a strong dependence on the Pt content is displayed; with peaks in the ORR<br />

current density exhibited, when the Pt-metal content is near 90 atomic % and 30 atomic %. We will<br />

discuss the physical origins of this improved ORR performance, and relate it to the composition dependent<br />

variation in Pt 5d-band filling.<br />

Acknowledgements: <strong>The</strong> research described in this presentation was carried out at the Jet Propulsion<br />

Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space<br />

Administration. We acknowledge support from the Department of Energy (DE-PS36-08GO98101).


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Novel Energy Storage with Solid Oxide Rechargeable <strong>Metal</strong>-Air Batteries<br />

Kevin Huang<br />

Department of Mechanical Engineering, <strong>University</strong> of South Carolina<br />

300 Main Street, Columbia, SC29201<br />

Email: kevin.huang@sc.edu Website: www.sofccenter.com<br />

Cost effective and large scale energy storage is critical to renewable energy integration and smart-grid<br />

energy infrastructure. Rechargeable batteries have a great potential to become a class of cost effective<br />

technology suited for large scale energy storage. In this presentation we report our recent progress in<br />

understanding the energy storage characteristics of a newly developed solid oxide rechargeable iron-air<br />

battery. Investigations of the battery performance under various current densities and cycle durations show<br />

that iron utilization plays a determining role in storage capacity and round-trip efficiency. Further studies<br />

of the battery’s cycle life reveal a unique charge-cycle originated degradation mechanism that can be<br />

interpreted by a combined vapor-phase transport and electrochemical condensation model. Overall, the<br />

energy capacity of the new solid oxide iron-air storage battery can be properly balanced with the roundtrip<br />

efficiency at optimized iron utilization.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Thin Film Solar Cells - Fundamental investigations and Device Applications<br />

B. Reeja Jayan, Chih-Liang Wang, K. L. Harrison, and A. Manthiram<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Materials Science and Engineering Program<br />

Email: manth@austin.utexas.edu Website: http://www.me.utexas.edu/~manthiram<br />

Abstract:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Our research explores charge generation and transfer processes at interfaces within thin film solar cells by<br />

combining data from photovoltaic device performance tests with characterization experiments conducted<br />

directly on the device. Our work spans polymer-based organic-inorganic hybrid solar cells, which<br />

combine the processing flexibility of organics (P3HT) with the low-cost and safety benefits offered by<br />

inorganic materials (TiO 2 ). Bilayer interfacial prototypes with tunable efficiency values ranging from<br />

around 0.01 to 1.6 % have been demonstrated. <strong>The</strong> simple bilayer design and stability of these devices are<br />

beneficial to investigate various device optimization steps, using a host of characterization techniques<br />

directly on a working device. Examples include X-ray photoelectron spectroscopic (XPS) depth profiling<br />

analysis of metal-P3HT and P3HT-TiO 2 interfaces and Raman analysis of bonding between metal sulfide<br />

interlayers like Sb 2 S 3 and P3HT. We also study Kesterite Cu 2 ZnSnS 4 based inorganic solar cells, a<br />

promising material derived entirely from earth-abundant raw materials. <strong>The</strong> solution-based approach using<br />

Cu 2 ZnSnS 4 employed in a low-cost superstrate-type device structure has been demonstrated with 0.4 %<br />

device efficiency under simulated AM 1.5 G illumination conditions. With the goal of developing a<br />

fundamental understanding of the way in which thin film solar cells work, we have developed novel<br />

microwave-assisted low temperature film growth techniques and fabrication approaches to create<br />

functional solar cells that are low-cost, efficient, and stable.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

First-Principles Study of Li Defect in Solid Electrolyte (γ-Li 3 PO 4 ) and in<br />

Electrode/Electrolyte (Li/γ-Li 3 PO 4 ) interface<br />

Santosh KC 1 , Ka Xiong 1 , Roberto C. Longo 1 , and Kyeongjae Cho 1, 3 *<br />

1 Department of Materials Science and Engineering, <strong>University</strong> of Texas at Dallas, Richardson, TX 75080, USA<br />

3 Department of Physics, <strong>University</strong> of Texas at Dallas, Richardson, TX, 75080, USA<br />

*Email: kjcho@utdallas.edu<br />

Abstract:<br />

In this work, we present our results of first-principles calculations of defects in solid electrolyte γ-Li 3 PO 4<br />

and in negative electrode/electrolyte interface (Li/γ-Li 3 PO 4 ). Our results show that Li interstitial defect<br />

dominates over the vacancy defect. <strong>The</strong> Li vacancy-interstitial pair defect formation energy of the<br />

interface model is comparable to the sum of Li vacancy defect at the electrode and Li ion (Li + ) interstitial<br />

defect in the electrolyte. Our study shows that the high Li + defect formation energy is the determining<br />

factor for low ionic conductivity of this Li metal/electrolyte interface. Thus, the study of the Li<br />

metal/electrolyte interface provides information on Li defect formation and migration, which will help us<br />

to improve the ionic conductivity in future Li-ion battery.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Scanning Probe Microscopy Studies in Correlated Electron Systems<br />

Jeehoon Kim, R. Baumbach, F. Ronning, L. Civale, J. D. Thompson, and Roman Movshovich<br />

Los Alamos National Laboratory, NM 87545, USA<br />

Email: jeehoon@lanl.gov Website:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Room-temperature scanning probe microscopy (RT-SPM) is widely used to study electronic and magnetic<br />

properties at the sub-micron scale in basic and applied science. By analogy with RT-SPM, lowtemperature<br />

SPM (LT-SPM) is a key tool to investigate phase transitions at low temperature, such as<br />

ferromagnetism and superconductivity. In this talk, I will present a variety of LT-SPM techniques to<br />

directly image magnetic and electric properties in ferro- and ferri-magnetic materials, and metal insulator<br />

transition materials. Recently, we developed a novel technique to measure the absolute value of the<br />

magnetic penetration in superconductors by magnetic force microscopy (MFM). This technique has been<br />

applied to unconventional superconductors, such as borocarbides and pnictides, to investigate<br />

superconducting properties. Also, direct visualization of the interaction between magnetism and<br />

superconductivity will be present in a ferromagnet-superconductor hybrid.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Dual-Electrolyte Li-Air Batteries<br />

Longjun Li and Arumugam Manthiram<br />

Materials Science and Engineering Program and Texas Material Institute<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, TX 78712, United States<br />

Email: rmanth@mail.utexas.edu; Website: http://www.me.utexas.edu/~manthiram/index.htm<br />

Lthium-air cells based on aprotic electrolytes suffer from clocking of the porous air electrode by insoluble<br />

products like Li 2 O 2 or Li 2 O and attack of the aprotic electrolyte by moisture or carbon dioxide from the<br />

ambient air. To solve these problems, a novel dual-electrolyte Li-air battery with high capacity and<br />

voltage has been developed. <strong>The</strong> lithium anode is protected from contaminates in the air by a Li-ion solid<br />

electrolyte and the discharge products are soluble in the catholyte. But the Li-ion solid electrolyte is not<br />

stable in strong acidic or alkaline solutions. A phosphate buffer solution with a moderate pH has been<br />

developed as a possible catholyte to keep the Li-ion solid electrolyte stable and reduce internal resistance<br />

and overpotential. All the three protons of the phosphoric acid can be effectively utilized to achieve a high<br />

capacity of 740 mAh g -1 at an average cell voltage of 3.3 V with good rechargeability and stability. Nanocrystalline<br />

IrO 2 has been utilized as the oxygen evolution catalyst to lower the charge overpotential. <strong>The</strong><br />

large internal resistance has been decreased by elevating the operating temperature or increasing the ionic<br />

conductivity of the Li-ion solid electrolyte. After optimization, the maximum power density reaches 40<br />

mW cm -2 and the battery conversion efficiency reaches 80 % ( 2 mA cm -2 ) at 40 °C.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Local structure and orbital ordering in YTiO 3<br />

Bing Li and Despina Louca<br />

Department of Physics, <strong>University</strong> of Virginia, Charlottesville, VA 22904<br />

Email: dl4f@virginia.edu<br />

Website: http://www.phys.virginia.edu/People/personal.aspUID=dl4f<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> local atomic structure of YTiO 3 has been investigated by using neutron diffraction and the pair<br />

density function analysis from 10 to 350 K. Upon warming from base temperature, deviations are<br />

observed of the local from the average crystal symmetry and these are attributed to distortions involving<br />

the Y and O atoms. In the case of Y, the in-plane x-y displacements result in an antiferrodistortive motion<br />

exerting influence on Y-O1 (apical sites of octahedral) bonds seen in the temperature dependence. At the<br />

same time, the O ion site in the basal plane of the octahedron is split to two (O2 and O3), giving rise to<br />

two unequivalent Ti-O bonds. <strong>The</strong> splitting of the oxygen site is in contrast to the equivalent sites in the<br />

corresponding average structure and calls for a lower symmetry than the Pnma currently used to describe<br />

the crystal structure. <strong>The</strong> oxygen displacements are of the order of 0.05 to 0.07 Å and lead to bending of<br />

the octahedra. <strong>The</strong> distortion of the in-plane O ions leads to quite different O-Ti-O bond angles. This may<br />

in turn have consequences on the linear combination of the atomic orbitals, where the proportion of the d zy<br />

to d xy components may be affected. However, it is expected that the antiferro-orbital ordering be<br />

preserved.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Electrochemical and electronic properties of tetrahedral silicates Li2MSiO4 as cathode<br />

materials for Li-ion batteries<br />

R. C. Longo, K. Xiong, Santosh KC and K. Cho<br />

Department of Materials Science & Engineering, <strong>The</strong> <strong>University</strong> of Texas at Dallas, 800 W. Campbell<br />

Road, Richardson, TX, 75080, USA<br />

Emails: roberto.longo@utdallas.edu and kjcho@utdallas.edu<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Using density functional theory (DFT), we investigate the structural, electronic and electrochemical<br />

properties of different tetrahedral silicate polymorphs recently synthesized and experimentally<br />

characterized. This family of compounds can insert and/or extract two Li atoms in two consecutive<br />

electron redox processes, giving rise to a much higher capacity (330 mAh/g) than that of the current<br />

cathodes (e.g., 160 mAh/g for LiCoO 2 ). Our DFT study includes the lithiated and both semi- and fully<br />

delithiated phases, in order to analyze how the charge/discharge process affects their structural stability.<br />

We also describe the electronic structure of these compounds accurately, trying to point out the main<br />

favorable mechanisms for both ionic and electronic conductivities. Finally, we show that, with suitable<br />

doping, it is possible to tailor the voltage and band gap of these silicates, improving their performance and<br />

making them promosing candidates as new cathode materials of rechargeable Li-ion batteries.<br />

Acknowledgments<br />

<strong>The</strong> authors also acknowledge the Texas Advanced Computing Center (TACC) for providing HPC<br />

resources.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Finding Unusually Strong Spin‐Orbit Coupling in Post‐Perovskite CaIrO 3 via X‐ray<br />

Magnetic Circular Dichroism<br />

Luke G. Marshall 1 , Jinguang Cheng 1,2 , Jianshi Zhou 1 , John B. Goodenough 1 , Daniel Haskel 3 ,<br />

and Michel Van Veenendaal 3,4<br />

1 Texas Materials Institute, <strong>The</strong> <strong>University</strong> of Texas at Austin,<br />

204 E. Dean Keeton St. C2201,<br />

Austin, TX 78712-1591<br />

2 <strong>The</strong> Institute of Physics, Chinese Academy of Sciences<br />

3 Advanced Photon Source, Argonne National Laboratory<br />

4 Department of Physics, Northern Illinois <strong>University</strong><br />

Email: luke.g.marshall@utexas.edu Website: http://lukegmarshall.wordpress.com<br />

Abstract:<br />

Strong spin-orbit coupling (SOC) and strong correlations have been considered essential in understanding<br />

the unusual physical properties of the 4d and 5d transition-metal oxides, such as the SOC driven Mott<br />

insulating state in Sr 2 IrO 4 . Recently, an unusual atomic-like orbital moment and strong SOC have been<br />

confirmed experimentally in 9R-BaIrO 3 through analysis of the branching ratio at the Ir L 2,3 absorption<br />

edges as obtained from x-ray absorption spectroscopy and x-ray magnetic circular dichroism (XMCD)<br />

measurements. We have applied the same techniques to probe unusual ferromagnetism and SOC in the<br />

post-perovskite (pPv) CaIrO 3 , which is an insulator and exhibits weak ferromagnetism below T c ~ 110K.<br />

<strong>The</strong> branching ratio at the Ir L 2,3 absorption edges, which is close to unity in pPv CaIrO 3 , appears to<br />

indicate an even stronger spin-orbit interaction in the pPv CaIrO 3 than in 9R-BaIrO 3 . However, it has been<br />

challenging to model the Ir 5d orbital moment, as probed by the XMCD measurements, due to the<br />

understood local octahedral-site distortions.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering–<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Understanding Interfacial Reactivity of Silicon Nanostructures<br />

Sankaran Murugesan ± , Kjell Schroder*, Justin T. Harris + , Lauren Webb* ,± , Brian A. Korgel* ,+ and Keith J. Stevenson* , ±<br />

± Department of Chemistry & Biochemistry, + Department of Chemical Engineering, *Materials Science and<br />

Engineering Program, <strong>The</strong> <strong>University</strong> of Texas at Austin<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

In recent years Si has drawn considerable interest as an anode material for Lithium ion batteries<br />

(LIB) due to its high gravimetric and volumetric energy density. Si can react with Li and form an alloy of<br />

Li 15 Si 4 , corresponding to a very high charge storage capacity of 3579 mAh/g that is approximately 10<br />

times higher in gravimetric capacity than graphite. However, Si-based anodes face several challenges.<br />

First, crystalline Si anodes undergo a 400% volume expansion during the lithiation process. Typically<br />

large irreversible capacity losses are observed during lithiation/delithiation since volume expansion and<br />

contraction cause pulverization of the Si and loss of electrical contact with the current collector. Secondly,<br />

the electrochemical alloying potential of Si is above the solvent reduction level, which leads to the<br />

formation of a solid electrolyte interface (SEI). <strong>The</strong>se fundamental processes are investigated through high<br />

resolution spectroscopic techniques. What effects volumetric expansion/contraction processes in Si and<br />

how can they be controlled What factors govern charge transfer kinetics and how can charge transfer<br />

resistance be controlled What influence do morphology and surface chemistry have on reversibility and<br />

charge storage capacity What role does SEI play in the charge transfer process between the electrolyte<br />

and electrode


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

MXene - A New Family of Two Dimensional Materials for Use in Lithium Ion Batteries<br />

and Lithium Ion Capacitors<br />

Michael Naguib 1 , Jérémy Come 2 , Yohan Dallagnese, 1 Olha Mashtalir 1 , Volker Presser 1 , Pierre-Louis Taberna 2 ,<br />

Patrice Simon 2 , Michel W. Barsoum 1 , and Yury Gogotsi 1 *<br />

Affiliation & Address<br />

1<br />

Department of Materials Science and Engineering & A.J. Drexel Nanotechnology Institute, Drexel<br />

<strong>University</strong>, Philadelphia, PA 19104, USA<br />

2<br />

Université Paul Sabatier, CIRIMAT UMR CNRS 5085, 31062 Toulouse Cedex 4, France and Réseau<br />

sur le Stockage Electrochimique de l’Energie (RS2E), FR CNRS 3459, France<br />

* gogotsi@drexel.edu<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Recently, we reported on the fabrication of a new family of two-dimensional (2-D) sheets of early<br />

transition metal carbides produced by the exfoliation of the MAX phases [1, 2]. <strong>The</strong> latter are a large<br />

family of machinable, layered ternary carbides and nitrides, where “M” is an early transition metal, “A” is<br />

a group 13 to 16 element and “X” is C and/or N [3]. We labeled this new materials “MXene” to indicate<br />

the selective etching of the A layers from the MAX phases and the similarity of the 2-D layers to graphene.<br />

More recently, we showed that Ti 2 C can be used as an anode material in lithium ion batteries [4]. <strong>The</strong><br />

performance was found similar to titania based anodes; the lithiation and delithiation potentials were<br />

found to be around 1.6 and 2.0V respectively. Already the very first study [4] showed stable capacity of<br />

225 mAh.g -1 was obtained for the Ti 2 C-based MXene anode at C/25. Ti 2 C can be cycled at high rates, for<br />

example at 10C a stable capacity of 70 mAh.g -1 was obtained. Anodes of delaminated MXenes showed a<br />

much higher Li uptake at high cycling rates. <strong>The</strong> ability to charge/discharge Li at such high rates suggests<br />

that Ti 2 C could be used in hybrid cells that combine the advantages of batteries and supercapacitors [5].<br />

References:<br />

[1] M. Naguib, M. Kurtoglu, V. Presser, J. Lu, J. Niu, M. Heon, L. Hultman, Y. Gogotsi, M.W. Barsoum,<br />

Advanced Materials, 23 (2011) 4248–4253.<br />

[2] M. Naguib, O. Mashtalir, J. Carle, V. Presser, J. Lu, L. Hultman, Y. Gogotsi, M.W. Barsoum, ACS<br />

Nano, 6 (2) 1322–1331 (2012).<br />

[3] M.W. Barsoum, Progress in Solid State Chemistry, 28 (2000) 201-281.<br />

[4] M. Naguib, J. Come, B. Dyatkin, V. Presser, P.-L. Taberna, P. Simon, M.W. Barsoum, Y. Gogotsi,<br />

Electrochemistry Communications, 16 (2012) 61-64.<br />

[5] J Come M Naguib P Rozier M W Barsoum Y Gogotsi P -L Taberna M Morcrette P Simon


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Enhanced charge-transfer kinetics by anion surface modification of LiFePO 4<br />

Kyu-Sung Park 1 , Penghao Xiao 2 , Anthony Dylla 2 , Graeme Henkelman 2 , Keith J. Stevenson 2 , John B. Goodenough 1<br />

1 Texas Materials Institute, <strong>University</strong> of Texas at Austin, Austin, Texas 78712, United States<br />

2 Department of Chemistry and Biochemistry, <strong>University</strong> of Texas at Austin, Austin, Texas 78712, United States<br />

Email: kspark37@gmail.com<br />

Abstract<br />

Despite the great achievement in understanding the materials properties and powder engineering of<br />

LiFePO 4 , the chemical bonding at the surface has been almost ignored. Herein, we demonstrate that the<br />

undercoordinated Fe 2+ /Fe 3+ redox couple at the surface gives a high barrier for charge transfer, but it can<br />

be stabilized by nitrogen or sulfur adsorption. <strong>The</strong> surface modification improves greatly the charge<br />

transfer kinetics and the charge/discharge performance of a LiFePO 4 cathode. DFT calculation estimates<br />

the origin of the improvement in terms of an electronic and ionic contribution based on a surface model<br />

probed by TOF-SIMS; the calculation agrees well with an experimental rate-constant analysis.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

In-situ synchrotron high-energy x-ray characterization of advanced materials for<br />

rechargeable batteries<br />

Yang Ren and Zonghai Chen<br />

Argonne National Laboratory, 9700 S. Cass Avenue, Argonne, IL 60439, USA<br />

Email: yren@anl.gov Website:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> increasing demand in safer and higher performance rechargeable batteries for broad applications has<br />

led to global efforts to develop advanced electrode materials, electrolyte components and additives, and<br />

other cell components. <strong>The</strong>re is a critical need in understanding key material issues in batteries under<br />

realistic conditions and in real time. We will present here a recent application of synchrotron high-energy<br />

x-ray diffraction (HEXRD) for in-situ structural characterization of advanced battery materials. Our<br />

experimental work includes in-situ HEXRD studies of cathode materials during solid-state synthesis, timeresolved<br />

measurements during hybrid pulse characteristic test (HPPC) of a full battery, in-situ study of Si-<br />

Li interaction and nondestructive material characterization of commercial 18650 cells during cycling, and<br />

in-situ monitoring reaction pathways of electrodes with electrolytes during thermal runaway. Our results<br />

provide important property-structure-performance information for in-depth understanding of advanced<br />

energy materials and the safety and performance of batteries. (Use of the Advanced Photon Source was<br />

supported by the U. S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under<br />

Contract No. DE-AC02-06CH11357.)


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Polymer assisted deposition of transition-metal-oxide thin films<br />

Francisco Rivadulla<br />

Center for Research in Biological Chemistry and Molecular Materials (CIQUS), <strong>University</strong> of Santiago de<br />

Email: f.rivadulla@usc.es<br />

Compostela, 15782-Santiago de Compostela, Spain<br />

Website: http://www.usc.es/ciqus/en/research/research-teams/rivadulla-lazzari<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> spectacular advances in physical deposition techniques during the last decades made possible the<br />

fabrication of thin-films of the required quality for either fundamental studies or highly demanding<br />

applications. Chemical methods, although more cost effective, are normally not competitive with physical<br />

techniques of deposition when the final quality required (smoothness, interface roughness, long-range<br />

homogeneity, etc) is important.<br />

I will present results of the epitaxial growth of ultra-thin films of different oxides (LnMnO 3 , LaCoO 3 ,<br />

SrRuO 3 , etc.) on SrTiO 3 and LaAlO 3 by spin-coating of a polymer/metal aqueous solution. <strong>The</strong> films show<br />

morphological and structural parameters similar to the best reported by physical methods, over large areas.<br />

Moreover, the use of aqueous-based solutions of environmentally friendly polymers represents an<br />

important improvement over other methods of chemical deposition.<br />

This simple chemical method produces the high-quality films required for either fundamental studies or<br />

applications, similar to physical deposition techniques.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

LiFePO 4 Electrodes with conductive polymers and no elemental carbon particles.<br />

Steen B. Schougaard<br />

Université du Québec à Montréal 2005 Jeanne Mance, Montréal, QC H2X 2J6, Canada<br />

Email: schougaard.steen@uqam.ca Website: http://www.lab-schougaard.uqam.ca<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Since its original discovery by Prof. Goodenough [1], LiFePO 4 has become a material of choice for<br />

lithium-ion batteries, when toxicity, cycling stability and safety are considered. However, to function in<br />

practical batteries, it requires a conductive coating.<br />

We have in past years developed an alternative technology to the industrial standard of pyrolytic carbon<br />

coating. Our processes [2] uses the intrinsic oxidative power of Li 1-x FePO 4 to polymerize a 2-3 nm thick<br />

conductive coating on the particle surface. This process, unlike the pyrolysis, takes place at low<br />

temperature (


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Greening Digital Systems Requires Better Quantum Models<br />

Bob Schubring<br />

Wonder Funding 1680 Vine Street, Suite 325, Los Angeles, CA 90028<br />

office: 323.733.1000 | mobile: 734.320.3435<br />

Email: rschubring@gmail.com<br />

Website: http://www.wonderfunding.com<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Polarization gradients in compositionally-graded perovskite ferroelectric thin films are known to generate<br />

electrical current by an unexplained mechanism that is not corrosion. Barium strontium titanate thin films<br />

have been engineered by compositional grading to compensate for geometric effects, and function as<br />

commercially nonvolatile random-access memories in microcontrollers. Further advancement requires<br />

elucidation of the mechanism by which the unexplained currents happen. <strong>The</strong> benefits are potentially<br />

enormous. Conventional RAM requires refresh at every clock cycle of the computer. Ferroelectric RAM<br />

holds data indefinitely without refresh, for periods up to 7 years, and does not degrade mechanically as<br />

does flash memory. If feature sizes are reduced and switching speeds increased to match conventional<br />

RAM, the energy and cooling savings will be vast, because most RAM-cached data is not read every clock<br />

cycle. Markets do not price in the cost advantages of these energy savings, because too little is known<br />

about the anomalous current mechanism and how it may limit switching speeds in alternative memory<br />

materials. To overcome this obstacle will require an advanced quantum-mechanical model that accounts<br />

for the anomalous current. <strong>The</strong> current may be the effect of polarization-driven quantum tunneling but this<br />

is unproven. <strong>The</strong>rmoelectric tunneling effects were not measurable by thermometry in graded potassium<br />

tantalate niobate thin films, but new calculations show that the likely temperature differences were within<br />

experimental error of the thermometry study. Thus, a secondary benefit of improved quantum-mechanical<br />

models, is that waste heat may be harvested by resulting ferroelectric RAM devices.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

A-site ordered perovskite-structure oxides with intriguing properties<br />

Yuichi Shimakawa<br />

Institute for Chemical Research, Kyoto <strong>University</strong>, Uji, Kyoto 611-0011, Japan<br />

Email: shimak@scl.kyoto-u.ac.jp Website: http://www.scl.kyoto-u.ac.jp/ ~ shimakgr<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

A very unusual ordered arrangement of the A-site ions in the simple ABO 3 perovskite produces<br />

AA’ 3 B 4 O 12 A-site ordered perovskites. <strong>The</strong> A site accommodates alkaline metals, alkaline-earth metals,<br />

and lanthanides like those in the simple perovskites. At the originally 12-fold coordinated A’ site,<br />

transition-metal ions such as Cu 2+ and Mn 3+ form square coordinated units that align perpendicular to each<br />

other. <strong>The</strong> presence of the transition-metal ions at both A’ and B sites produces A’-A’ and and/or A’-B<br />

interactions in addition to B-B interaction usually seen in the simple perovskite materials. Competitive<br />

and/or cooperative interplay of these interactions gives rise to diverse and intriguing physical properties.<br />

Two new A-site ordered perovskite-structure oxides, CaCu 3 Fe 4 O 12 and LaCu 3 Fe 4 O 12 , are<br />

highlighted. <strong>The</strong>y were synthesized under high-pressure and high-temperature conditions. <strong>The</strong><br />

compounds contain unusually high valence states of iron: Fe 4+ in CaCu 3 Fe 4 O 12 and Fe 3.75+ in<br />

LaCu 3 Fe 4 O 12 . Instabilities of the high oxidation states at low temperatures are resolved in CaCu 3 Fe 4 O 12<br />

by charge disproportionation from Fe 4+ to Fe 3+ and Fe 5+ , and in LaCu 3 Fe 4 O 12 by charge transfer between<br />

A-site Cu and B-site Fe ions. <strong>The</strong> charge disproportionation and the charge transfer are accompanied by<br />

significant changes in structural, transport, and magnetic properties.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Covalency influence on crystal chemistry of some inorganic compounds with<br />

octahedral-site cations<br />

Y. Shirako 1<br />

1 Department of Chemistry, Gakushuin <strong>University</strong>, 1-5-1, Mejiro, Toshima-ku, Tokyo, 171-8588, Japan<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> purpose of this presentation is to explain the local structures which is a network of octahedral<br />

ionic clusters in inorganic compounds using a modification of the methods to predict a shape of severalatomic<br />

molecules [1], and then to restrict the adopted inorganic crystal structure of each composition. This<br />

way is a qualitative rule and yet easily available. In particular, the improved method may be effective to<br />

classify pressure-induced structural phase transition sequences of various compounds.<br />

In the covalency-dominant small molecules such as CO 2 and NH 3 , shape of the molecule depends on<br />

number of electrons in valence shell orbitals of molecule (Walsh’s rule) [1]. Essence of the rule is<br />

delocalization of the lone-pair electrons. <strong>The</strong> author extends the Walsh’s rule to be able to apply to<br />

inorganic crystal structures with frameworks of the octahedra. <strong>The</strong> modified rule can be called “extended<br />

Walsh’s rule”. In the extended rule, number of electrons in outer shell orbitals can be used as a qualitative<br />

parameter to relate stability of the inorganic crystal structures with those compositions. For example, all<br />

M-X-M angles in post-perovskite compounds AMX 3 are more bent to 90 º than those in the perovskite<br />

which is less dense than the post-perovskite. <strong>The</strong> extended Walsh’s rule suggests that, if all 4-electrons on<br />

p orbitals of closed-shell X can be delocalized to t 2g orbitals on M’s, linear M-X-M fragments are stable,<br />

or else bent M-X-M fragments are stable since the electrons can be delocalized through e g orbitals on M’s.<br />

<strong>The</strong>refore, the M-X-M fragments in which the M ions have at least one of d orbitals with inability of<br />

formation of -bond (filled orbitals), unlike Ti 4+ , Nb 4+ and Re 4+ , are expected to be bent by covalent<br />

effect. Actually, post-perovskite compounds containing the -bond ability cations such as Ti 4+ and Zr 4+ in<br />

octahedral-sites are almost not reported.<br />

<strong>The</strong> previous articles have been reported on the similar topic [2, 3, 4]. Goodenough and Kafalas (1973)<br />

[2] described discussion about contribution of covalency, electrostatic energy, and ionic size for crystal


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Interaction-Enhanced Coherence Between Two-Dimensional Dirac Layers<br />

Inti Sodemann, Dmytro Pesin and Allan MacDonald<br />

<strong>University</strong> of Texas at Austin<br />

Email: sodemann@physics.utexas.edu<br />

We estimate the interaction induced coherence gap between parallel layers of two-dimensional Dirac<br />

electron liquids by accounting explicitly for the retardation of the effective inter-layer interaction and selfconsistently<br />

incorporating the influence of the gap on screening. We apply our results to graphene doublelayers<br />

and topological insulator thin films.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Electrode and Cell Configuration Design of Rechargeable Lithium–Sulfur Batteries<br />

Yu-Sheng Su, Chenxi Zu, Sheng-Heng Chung, Yongzhu Fu and Arumugam Manthiram*<br />

Electrochemical Energy Laboratory, Materials Science and Engineering Program, <strong>The</strong> <strong>University</strong> of Texas at<br />

Austin, Austin, TX 78712, USA<br />

Email: manth@austin.utexas.edu Website: http://www.me.utexas.edu/~manthiram/index.htm<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> limitations in the cathode capacity compared to the capacity of anode have been an impediment to<br />

make advances in the lithium-ion battery area. <strong>The</strong> lithium–sulfur (Li–S) system is appealing in this<br />

regard as sulfur exhibits an order of magnitude higher capacity (1,675 mAh g -1 ) than the currently used<br />

cathodes. However, low active material utilization and poor cycle life hinder the practicality of Li–S<br />

batteries due to the insulating nature of sulfur/lithium sulfide redox products and dissolution behavior of<br />

polysulfide species. We present here several state-of-the-art designs based on electrode/cell configuration<br />

aspects to tackle the drawbacks in the cathode region. Various carbon–sulfur and polymer–sulfur<br />

composite materials have been developed to retain intermediate polysulfides during charge/discharge,<br />

leading to good cycle stability. Additionally, a simple adjustment to the traditional Li–S battery system<br />

configuration has been designed to achieve high capacity with a long and stable cycle life. Carbon<br />

interlayers with different framework structures act as a liaison between the cathode and the separator,<br />

resulting in a significant improvement not only in the efficiency of active material utilization but also in<br />

capacity retention, without involving complex synthesis. Surface modification applied to the carbon<br />

interlayer can further enhance the cycle performance. Sulfur cathodes with 3D architectures also offer<br />

excellent capacity retention by a single-step processing. <strong>The</strong>se approaches decrease the internal charge<br />

transfer resistance and localize the soluble polysulfide species, facilitating a feasible means of fabricating<br />

commercially viable lithium–sulfur batteries.


Abstract<br />

<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

High Capacity Lithium-<strong>Metal</strong>-Oxide Electrodes: Challenges and Opportunities<br />

Michael M. Thackeray 1 , J. R. Croy 1 , D. Kim 1 , M. Balasubramanian 2 and S.-H. Kang 3<br />

1 Electrochemical Energy Storage Department<br />

Chemical Sciences and Engineering Division<br />

2 X-ray Science Division, Advanced Photon Source, Argonne National Laboratory<br />

Argonne, IL 60439, USA<br />

3 Samsung SDI, Yongin, Gyeonggi-do, Korea<br />

Email: thackeray@anl.gov<br />

It is well known that lithium-manganese-oxide electrodes are significantly more stable than their cobalt<br />

and nickel analogues, particularly at high states of charge, and that some manganese-based structures can<br />

provide a very high rechargeable capacity (~250 mAh/g) between 4.6 and 2.5 V, albeit it a relatively slow<br />

current rate. <strong>The</strong> urgent need to design and develop safe, high energy and power lithium-ion batteries that<br />

are not prone to thermal runaway and fire has therefore placed considerable attention on manganese oxide<br />

systems, particularly for electrically-powered vehicles. On the other hand, lithium-manganese-oxides tend<br />

to suffer from chemical and physical instabilities induced, for example, by oxygen loss at high potentials,<br />

dissolution phenomena, crystallographic changes and voltage decay during charge and discharge; these<br />

phenomena can severely impact the capacity, rate and cycle life of the cells. A significant worldwide<br />

effort is therefore being made to address these chemical, electrochemical and structural limitations.<br />

<strong>The</strong> results of recent research conducted at Argonne National Laboratory in designing and stabilizing high<br />

capacity lithium- and manganese-rich electrode structures for Li-ion cells will be presented. <strong>The</strong><br />

versatility of using a layered Li 2 MnO 3 precursor as a template to synthesize ‘layered-layered’<br />

(xLi 2 MnO 3 [1-x] LiMO 2 ), ‘layered-spinel’ and ‘layered-rocksalt’ composite electrode structures will be<br />

highlighted. Electrochemical data and structural insights of these highly complex materials as determined<br />

by powder X-ray diffraction and absorption techniques at Argonne’s Advanced Photon Source will be<br />

presented.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

H + ↔Li + Ion-Exchange Chemistry of Ceramic Garnet-Type Electrolytes<br />

Lina Truong and Venkataraman Thangadurai*<br />

<strong>University</strong> of Calgary, 2500 <strong>University</strong> Drive NW, Calgary, Alberta, T2N 1N4<br />

Email: vthangad@ucalgary.ca Website: www.chem.ucalgary.ca/research/groups/vthangad/index.html<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Chemical stability and ion-exchange of the garnet-type fast Li ion conducting Li 5+x Ba x La 3-x Nb 2 O 12 (x = 0,<br />

0.5, 1) were studied in various media such as water and organic acids. <strong>The</strong> H + /Li + reaction was found to be<br />

most successful for x = 0, which showed ~89% H + /Li + exchange reaction, while x = 0.5 showed ~46%<br />

and x = 1 showed ~20% in water at room temperature. In Li 5 La 3 Nb 2 O 12 , more of the Li ions occupy the<br />

tetrahedral sites, the ion-exchange reaction occurs readily and to a greater extent. <strong>The</strong> relative population<br />

of Li ions that reside in the octahedral sites increases with increasing Li content in Li 5+x Ba x La 3-x Nb 2 O 12<br />

and the proton-exchange proceeds to a lesser extent in water. <strong>The</strong> reaction was also shown to be<br />

reversible, where ionic conductivity of the reverse Li exchanged product from the H-garnet, for x = 0, was<br />

found to show comparable values to its original solid state synthesized Li 5 La 3 Nb 2 O 12 . Similar trends were<br />

found when the H + /Li + ion-exchange reaction was done at room temperature using weak organic acids,<br />

including CH 3 COOH and C 6 H 5 COOH as proton sources. <strong>The</strong> exchange was almost (100%) completed<br />

using the x = 0 member in CH 3 COOH.


Abstract:<br />

<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

In situ Electron Microscopy of Electrical Energy Storage Materials<br />

R.R. Unocic, X. Sun, L. Baggetto, G.M. Veith, K.A. Unocic, S. Dai, N.J. Dudney, K.L.More<br />

1 Oak Ridge National Laboratory, Oak Ridge, TN 37831<br />

Email: unocicrr@ornl.gov<br />

Electrode/electrolyte interfaces play an active role in controlling the electrochemical energy conversion process in<br />

lithium ion batteries. Of critical importance to the performance and life-cycle is the formation of the solid<br />

electrolyte interphase (SEI), which is a passive interfacial, nm-scale film that forms at the electrode/electrolyte<br />

(solid/liquid) interface as a result of electrolyte decomposition reactions during electrochemical cycling. Due to the<br />

dynamic nature of the SEI, it has proven difficult to design experiments that will reveal details regarding SEI<br />

formation mechanisms as well as how its structure and chemistry evolves during electrochemical cycling. In-situ<br />

transmission electron microscopy provides a viable means for directly correlating structure-property relationships in<br />

materials where dynamically evolving processes can be studied in real-time and at high spatial and temporal<br />

resolution. Here we investigate the formation of the SEI on graphite anodes during electrochemical cycling<br />

experiments with organic liquid electrolytes. <strong>The</strong> unique feature of this method is the capability to wholly contain<br />

volatile and corrosive liquid electrolytes when placed into the high vacuum environment of the TEM. By sealing the<br />

electrodes and electrolytes between silicon nitride membranes, direct imaging of the electrode material, interfaces,<br />

and surfaces under electrochemical charge/discharge cycling is permissible. <strong>The</strong> development and implementation<br />

of this unique tool will enable fundamental research related to electrical energy storage systems.<br />

Research supported by (1) the Office of Vehicle Technologies, Office of Energy Efficiency and Renewable Energy<br />

(2) the Fluid Interface Reactions, Structures and Transport (FIRST) Center, an Energy Frontier Research Center<br />

funded by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences and (3) ORNL's<br />

Shared Research Equipment (ShaRE) User Facility, which is sponsored by the Office of Basic Energy Sciences,<br />

U.S. Department of Energy.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Novel Cathode and Anode Materials for Solid Oxide Fuel Cells<br />

Matthew West, 1 Daeil Yoon, 2 and Arumugam Manthiram 1,2<br />

1 Department of Chemical Engineering and 2 Materials Science and Engineering Program<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, TX<br />

Email: manth@austin.utexas.edu Website: http://www.me.utexas.edu/~manthiram<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Solid oxides fuel cells (SOFCs) offer great promise for future energy production due to their high<br />

efficiencies and fuel flexibility. Despite their benefits, the commercialization of SOFCs is hampered by<br />

severe materials challenges, and there is significant interest in reducing their operating temperatures from<br />

the conventional > 800 o C to an intermediate range of 500 o C – 800 o C and in utilizing hydrocarbon fuels<br />

like natural gas directly instead of hydrogen fuel. We present here the development of new materials and<br />

novel synthesis approaches to address some of these issues. A new series of cathode materials RBaM 4 O 7<br />

(R = rare earth) identified in our group exhibits good catalytic activity with an ideal matching of the<br />

thermal expansion coefficient to that of conventional electrolytes like YSZ. However, the RBaM 4 O 7 series<br />

suffers from long-term stability issues, and attempts to improve stability often come at the expense of<br />

reduced catalytic activity for the oxygen reduction reaction. Through appropriate cationic substitutions<br />

with small amount of dopants in the crystal lattice, we have been able to resolve the stability issues<br />

without significantly sacrificing the electrochemical performance. As for the anode, the oxidation of<br />

hydrocarbon fuels on conventional Ni-YSZ catalyst is accompanied by carbon deposition on Ni, resulting<br />

in a reduction in catalytic activity and overall life expectancy of the cell. To alleviate these problems and<br />

enhance the performance of SOFC anodes, both heterogeneous anode catalysts and new synthesis<br />

techniques for traditional materials are being investigated.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Surprising superexchange interactions in osmate double perovskites<br />

Patrick M. Woodward<br />

Department of Chemistry<br />

Ohio State <strong>University</strong><br />

Email: woodward.55@osu.edu<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> synthesis, structures and magnetic behavior of A 2 MOsO 6 osmate double perovskites are presented in this<br />

poster. <strong>The</strong> compounds A 2 CrOsO 6 , A 2 FeOsO 6 , A 2 CoOsO 6 and A 2 MgOsO 6 (A = Sr, Ca) have been prepared and<br />

characterized. All of the compounds are ordered double perovskites, many of which undergo ocathedral tilting<br />

distortions. All of the compounds studied contain localized electrons and their magnetism is dictated by<br />

superexchange interactions. However, the strength and sign of the superexchange interactions, particularly between<br />

3d transition metal ions and osmium, defy conventional expectations in many cases. For example in Sr 2 CoOsO 6 ,<br />

the Co(II) and Os(VI) ions order independently despite the fact that the two sublattices are completely<br />

interpenetrating. This suggests that the four bond Os–O–Co–O–Os and Co–O–Os–O–Co superexchange<br />

interactions are stronger than the much shorter Os–O–Co superexchange interactions. This surprising conclusion is<br />

supported by DFT calculations. In Sr 2 FeOsO 6 , which contains the d 5 high spin Fe(III) ion and the d 3 Os(V) ion, the<br />

Goodenough-Kanamori rules predict ferromagnetic coupling, but antiferromagnetism is observed. <strong>The</strong> behavior of<br />

this family of compounds highlights the need for deeper understanding of superexchange interactions between<br />

transition metals with very different d-orbital energies and sizes.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Atomic and electronic structures of superionic solid electrolyte Li 10 GeP 2 S 12<br />

K. Xiong a , R. C. Longo a , and Kyeongjae Cho a,b,*<br />

a Materials Science & Engineering Dept, <strong>The</strong> <strong>University</strong> of Texas at Dallas, Richardson, TX 75080, USA<br />

b Physics Dept, <strong>The</strong> <strong>University</strong> of Texas at Dallas, Richardson, TX 75080, USA<br />

Email: ka.xiong@utdallas.edu Website:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Inorganic solid electrolytes have attracted much attention for being used in lithium batteries to replace<br />

conventional liquid electrolytes to achieve better safety and reliability. This has led to intensive research<br />

during the last three decades and many electrolyte candidates have been proposed such as lithium<br />

phosphate oxynitride and Li 2 S-P 2 S 5 -based glasses such as lithium thiophosphate. LiPON has been used as<br />

commercial solid electrolyte in thin-film batteries. However, its ionic conductivity is rather low (10 -6 S<br />

cm -1 ). To improve the performance of the battery cell, the electrolyte material should have high ionic<br />

conductivity. It has been found recently that a superionic conductor, Li 10 GeP 2 S 12 , possesses an extremely<br />

high ion conductivity of 10 mS cm -1 . To date, few theoretical studies have been carried out on<br />

understanding the fundamental properties of this material. For this purpose, we use first principles<br />

calculations to investigate the impact of Li defects on the atomic and electronic structures of Li 10 GeP 2 S 12 .<br />

To understand the mechanisms of ion transport, we investigate the Li ion migration in Li 10 GeP 2 S 12 by<br />

calculating the activation energy barriers of various possible diffusion pathways. In addition, we propose<br />

possible solutions (e.g. doping) to optimize the Li ion migration in these materials. This study will help us<br />

to gain fundamental understanding on the Li ion diffusion process and possible mechanisms to maximize<br />

it.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Flowerlike Co 3 O 4 particles Loaded with Copper Nanoparticle as a Bifunctional<br />

Catalyst for Lithium-Air Batteries<br />

Wei Yang, Jason Salim, Chunwen Sun, LiquanChen, and Youngsik Kim<br />

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing<br />

100190, China<br />

Email: csun@iphy.ac.cn<br />

Website:<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

<strong>The</strong> high cost of energy storage and conversion devices such as PEM fuel cells and metal/air batteries<br />

restrains their practical use. For lithium-air battery, another issue that has to be addressed in the current<br />

technology is the limitations of oxygen reduction reaction (ORR) during discharging process and oxygen<br />

evolution reaction (OER) during charging process. <strong>The</strong> sluggish kinetics of ORR and OER in lithium-air<br />

batteries is ascribed to the low efficiency of catalysts. A low-cost and stable electrocatalysts is the solution<br />

to tackle this problem. In this study, we found that porous flowerlike Co 3 O 4 particles prepared by<br />

hydrothermal method and loaded with copper nanoparticles on their surface have shown to be a high<br />

performance and stable bifunctional electrocatalyst for the ORR and OER reactions. <strong>The</strong> cobalt oxidebased<br />

catalysts show better performance during the discharging and charging process at a current density<br />

of 0.05 mA cm -2 compared with that of the Vulcan XC-72 and close to that of the 50% Pt/carbon-black<br />

catalyst. This electrocatalyst could be used in a metal/air battery or a PEM fuel cell as an efficient and<br />

stable bifunctional catalyst.<br />

5.0<br />

5<br />

4.5<br />

4<br />

Cell Voltage (V)<br />

4.0<br />

V<br />

3.5<br />

3.0<br />

Cell Voltage (V)<br />

3<br />

2<br />

1<br />

50% Pt/C<br />

Vulcan XC-72<br />

2.5<br />

Co 3 O 4<br />

Co 3 O 4 - Cu<br />

2.0<br />

0 2 4 6 8 10<br />

Time (h)<br />

0<br />

0 200 400 600 800 1000 1200 1400<br />

Capacity (mAHg -1 Co 3 O 4 -Cu )<br />

Figure 1 Comparison of the charge and discharge curves of the prepared lithium-air batteries with various catalysts.<br />

Figure 2 Voltage versus discharge/charge capacity for the lithium-air batteries with the Co 3 O 4 -Cu catalyst at a current density of 0.05 mA cm -2 with the active<br />

catalyst (Co 3 O 4 -Cu) mass loading of 0.5 mg/cm 2 .


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Multiscale Simulation Study of Si Anode Material for Li-ion Battery Applications<br />

Hengji Zhang 1 , Janghyuk Moon 2 , Maenghyo Cho 2 , Kyeongjae Cho 1, 2<br />

1 Department of Physics and Department of Materials Science and Engineering, <strong>University</strong> of Texas at Dallas,<br />

Richardson, Texas, 75080, US<br />

2 Division of WCU Multiscale Mechanical Design, School of Mechanical and Aerospace Engineering,<br />

Seoul National <strong>University</strong>, Seoul 151-742, Republic of Korea<br />

Email: hengji@utdallas.edu Website: http://www.utdallas.edu/~hxz083000/<br />

Abstract Body in Space Below:<br />

(Please use single space, Times New Roman or similar font, size 12, and limit to 250 Words. Please DO NOT exceed the space<br />

below.)<br />

Si based anode materials have attracted much interests for Li-ion battery applications because of its known<br />

advantages such as high energy density, high operating voltage, and low cost and toxicity. Despite of these<br />

attractive features, Si based anode materials often shows structure failure caused by rapid volume<br />

expansion during the battery charging process. To understand the mechanism of this structure failure, we<br />

use first principle method to study the kinetics of Li diffusion in Si anode materials, and the mechanical<br />

strength of Li-Si alloy phases. Based on these first principle results, we try to develop Li-Si Reactive<br />

Force Field (Reaxff) potential parameters to run classical MD simulations, which can be useful to<br />

investigate the evolution of structures and compositions for the lithiation of Si anode materials. In this<br />

work, we compare the results predicted both from first principle method and classical MD simulations.


<strong>The</strong> John B. Goodenough Symposium in Materials Science & Engineering –<br />

In Honor of His 90 th Birthday –<br />

<strong>The</strong> <strong>University</strong> of Texas at Austin, Austin, Texas<br />

October 26-27, 2012<br />

Structure – Electrochemical and Magnetic Property Relationships<br />

in <strong>Transition</strong> <strong>Metal</strong> <strong>Oxides</strong> for Energy Applications<br />

Xiao-Dong Zhou<br />

Department of Chemical Engineering, <strong>University</strong> of South Carolina<br />

Email: xiao-dong.zhou@sc.edu Website: www.che.sc.edu/faculty/zhou<br />

<strong>The</strong> aim of this paper is to present a theoretical and practical view of electronic, electrochemical and<br />

magnetic properties of functional oxides, with a focus on correlating structure and properties with the<br />

chemical composition, defect chemistry and microstructures. I will use oxides for solid oxide fuel cells,<br />

thermoelectric converters, and lithium-ion batteries as examples to illustrate the closely coupled structureproperty<br />

relationships in perovskite-type oxides, misfitted layered Ca 3 CO 4 O 9+ , Fe 3 O 4- nanoparticles,<br />

MnO 2 nanowires, and SnO x nanoribbons.<br />

Disproportionation reaction will be discussed in (La,Sr)MnO 3 , while distinct oxidation states (e.g. III, IV,<br />

and V) of Fe in (La,Sr)FeO 3 are observed and presented in this poster. Electronic conductivity will be<br />

correlated with defect and magnetic properties in these compounds. Defect chemistry and transport<br />

properties will be discussed in Ca 3 Co 4 O 9+δ , which adopts a misfit layered structure: the CdI 2 type for the<br />

“CoO 2 ” layer and the rock salt type for the “Ca 2 CoO 3 ” layer. Copper nanoribbon supported Fe 3 O 4 and<br />

SnO x as the negative electrodes for lithium-ion batteries will be discussed to correlate structureelectrochemical<br />

property relationship. Superior recyclability can be achieved by improving the interfacial<br />

structures.<br />

<strong>The</strong> specific attention of this poster will be on the physical understanding of the origin of activity-stability<br />

dichotomy and the engineering solutions to decouple this conjugation.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!