rutile crystal structure z x y. seeing the 1-d chanels in rutile

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RUTILE CRYSTAL STRUCTURE z x y

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Page 1: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

RUTILE CRYSTAL STRUCTURE

z

x

y

Page 2: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

SEEING THE 1-D CHANELS IN RUTILE

Page 3: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

NEW METASTABLE POLYMORPH OF TiO2 BASED ON K2Ti4O9 SLAB STRUCTURE - (010) PROJECTION SHOWN

K+ at y = 3/4

K+ at y = 1/4

Different to rutile, anatase or brookite forms of TiO2

Page 4: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

Finding the number of crystallographically inequivalent oxygen sites in the K2Ti4O9 slab and the number of each

Oxygen count 1/3 + 3/4

Oxygen count 4 + 1/2 +2 +1/3

Oxygen count 1/3 + 3/4 1/3

1/3

1/3 1/41/41/4

1/41/41/4

1/2 1/21/21/2

1 1 1 1

Topotactic loss of H2O from H2Ti4O9 to give “Ti4O8” (TiO2 slabs) plus H2O, where two bridging oxygens in slab are protonated (TiOHTiOTiOH)

[Ti(IV)4O9]2-

Page 5: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

CHIMIE DOUCE: SOFT CHEMISTRY

• Figlarz synthesis of new WO3

• WO3 (cubic form) + 2NaOH Na2WO4 + H2O

• Na2WO4 + HCl (aq) gel

• Gel (hydrothermal) 3WO3.H2O

• 3WO3.H2O (air, 420oC) WO3 (hexagonal tunnel structural form of tungsten trioxide)

• More open tunnel form than cubic ReO3 form of WO3

Page 6: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

Slightly tilted cubic polymorph of WO3 with corner sharing Oh WO6 building blocks, only protons and smaller alkali cations can be injected into cubic shaped voids in structure to form bronzes like NaxWO3 and HxWO3

1-D hexagonal tunnel polymorph of WO3 with corner sharing Oh WO6 building blocks, can inject larger alkali and alkaline earth cations into structure to form bronzes like RbxWO3 and BaxWO3

Page 7: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

Hexagonal tunnels

Injection of larger M+ cations like K+ and Ba2+ than maximum of Li+ and H+ in c-WO3

Apex sharing WO6 Oh building blocks

Structure of h-WO3 showing large 1-D tunnels

Page 8: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

MOLTEN SALT ELECTROCHEMICAL REDUCTIONS OF OXYANIONS: GROWTH OF CRYSTALS

• Molten mixtures of precursors - product crystallizes from melt - inert crucibles and electrodes like Pt, graphite CATHODE

• Reduction of TM oxides to lower oxidation state materials

• CaTi(IV)O3 (perovskite)/CaCl2 (850oC) CaTi(III)2O4 (spinel)

• Na2Mo(VI)O4/Mo(VI)O3 (675oC) Mo(IV)O2 (large crystals)

• Li2B4O7/LiF/Ta(V)2O5 (950oC) Ta(II)B2

• Na2B4O7/NaF/V(V)2O5/Fe(III)2O3 (850oC) Fe(II)V(III)2O4 (spinel)

Page 9: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

SYNTHETIC FORM: SHAPE IS EVERYTHING IN THE MATERIALS WORLD

• When thinking about a solid state synthesis of a particular composition it is also important to plan the form of the material that will ultimately be required for a specific application

• Shape is everything when it comes to designing structure-property-function-utility relations

• Form counts - polycrystalline, nanocrystalline, film, superlattice, wire, single crystal and so forth

Page 10: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

BASICS LSSB: INJECTION-INTERCALATION CATHODES TiO2, NbSe3, WO3, MoS2, V6O13, LixCoO2

• Li+/e- charge equivalents of anode

• Voc, EF(anode-cathode)

• Electrode-electrolyte interfacial kinetics• Polymer segment dynamics

• Polymer Tg controls crystalline vs glassy

• Li+/PEO cooperative motion effects• Goal Li+ RT conductivity• Needs liquid (low MW PEO) plastisizers• Electrode-electrolyte mechanical stability• Electrode-electrolyte chemical stability• Rocking chair architecture• Secondary battery can be cycled• Operational lifetime• Safety, environmentally correct

LiLi3NLixCLixCFLiAlLiSnLixMnO2

PEO

Li+

Li+

Li+ Li+

Li+

Li+

anode electrolyte cathode

SPE

Page 11: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

LiCoO2

LiCoO2

LixC6

Li

ROCKING CHAIR LSSB

Page 12: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

HOW TO SYNTHESIZE A BETTER LSSB?

Improved Performance Cathode, Anode and Electrolyte

Page 13: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

TEMPLATE SYNTHESIS OF NANOSCALE BATTERY CATHODE MATERIALS

Page 14: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

A BETTER BATTERY CATHODE USING NANOSCALE MATERIALS - NANODIFFUSION LENGTHS FOR Li+

DIFFUSIVE INTERCALATION

• Template synthesis is a versatile nanomaterial fabrication method used to make monodisperse nanoparticles of a variety of materials including metals, semiconductors, carbons, and polymers.

• The template method has been used to prepare nanostructured lithium-ion battery electrodes in which nanofibers or nanotubes of the electrode material protrude from an underlying current-collector surface like the bristles of a brush.

• Nano-structured electrodes of this type composed of carbon, LiMn2O4, V2O5, Sn, TiO2 and TiS2 have been prepared.

Page 15: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

A BETTER BATTERY CATHODE USING NANOSCALE MATERIALS - NANODIFFUSION LENGTHS FOR Li+

DIFFUSIVE INTERCALATION

• In all cases, the nanostructured electrode showed dramatically improved rate capabilities relative to thin-film control electrodes composed of the same material.

• The rate capabilities are improved because the distance that Li must diffuse in the solid state (the current- and power-limiting step in Li-ion battery electrodes) is significantly smaller in the nanostructured electrode.

• For example, in a nanofiber-based electrode, the distance that Li must diffuse is restricted to the radius of the fiber, which may be as small as 50 nm.

Page 16: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

A BETTER BATTERY CATHODE USING NANOSCALE MATERIALS - NANODIFFUSION LENGTHS FOR Li+

DIFFUSIVE INTERCALATION

• Beating mechanical stability problem of repeated intercalation-deintercalation expansion-contraction cycles

• In addition to improved rate capabilities, the nanostructured electrodes do not suffer from poor cyclability observed for conventional electrodes.

• This is because the absolute volume changes in the nanofibers are small, and because of the brush-like configuration, there is room to accommodate the volume expansion around each nanofiber.

• Improved cycle life results show nanostructured electrode can be driven through 1400 charge/discharge cycles without loss of capacity.

Page 17: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

nc-TiO2

Nanocrystal-PEO electrolytes solid plasticisers for LSSB

Ti(IV)-X- surface coordinated anion

Li+ cation

Ti(IV)-O surface coordinated oxygen of PEO polymer chain

PEO polymer chain coordinated to Li+ cation and surface Ti(IV)

Page 18: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

LiClO4-PEO-nc-TiO2

• LiClO4-PEO-nc-TiO2 -high surface area nanocrystalline ceramic

• Brnsted and Lewis acid-base sites - surface Ti(IV) coordination to O(CH2CH2)-

• Surface Ti(IV) binding to counteranion X-

• Polymer-particle crosslinking - no 60oC glass transition

• nc-TiO2 stabilizes glassy polymer state at RT

• Domains of local polymer disorder at PEO-nc-TiO2 interface

• Optimal anchoring promotes local structural and dynamical modifications• High RT Li+ conductivity• Excellent mechanical stability, improved stress-strain curves• Reduced reactivity with solid compared to liquid plasticizer• Less cooperative PEO segmental motion with enhanced interfacial mobility of

Li+

• Transport number t(Li+), 0.3 pristine LiClO4-PEO, 0.6 in LiClO4-PEO-nc-TiO2

nc-TiO2

Page 19: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

nc-CERAMIC OXIDES: SOLID PLASTICISERS IN POLYMER-ELECTROLYTE LITHIUM BATERIES

• LiClO4 : PEO = 1 : 8, 10 wt% nc-TiO2 or Al2O3,

• anchoring PEO oxygens and counteranions to Brnsted/Lewis acid surface sites,

• enhanced corrosion resistance of electrodes,

• better mechanical stability PEO,

• higher Li+ conductivity & transport number,

• local disorder of polymer, loss of Tg, stabilizes RT glassy state,

• discards need for PEO-Li+ cooperative segmental motion

Page 20: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

METHODS FOR SYNTHESIZING NANOCLUSTERS AND NANOCRYSTALS

• Vaporization of metals (thermal, laser ablation) in inert gas - condensation of mixture - Pt, Au

• Supersonic molecular beams - Knudsen cell vaporization with inert gas expansion - condensation into vacuum and mass selection and mass spectroscopy detection - Si, GaAs

• Plasma-arc vaporization - condensation - WC, SiC

• Aerosol spray pyrolysis of salt, sol-gel precursor solution - Y3Fe5O12, Mn0.8Zn0.2FeO4, PbZr0.52Ti0.48O3, YBa2Cu3O7, ZrO2, TiO2

• Microemulsions, micelles, zeolites - precursors - confined nucleation and arrested nanocluster growth - capped CdSe, FePt, TiO2, YBa2Cu3O7

Page 21: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

LENGTH SCALES IN CHEMISTRY, PHYSICS

AND BIOLOGY

Peter Day, Chemistry in Britain

Page 22: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

Spatial and quantum confinement and dimensionality

Page 23: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

WHEN IS SMALL GOOD?

Page 24: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

Sub-dividing or perforating mattermono- or polydispersed particles, crystalline or amorphous, micro (<10 Å),

meso (10-1000 Å) or macro (>1000 Å) length scale, organized or random arrangements, channels or pores, structure-composition-defects, surface

area, sites, charge, hydrophobicity, functionality

Property-function

QSEs, of e, h, or hrelative to materials size, dimensionality, interaction strength of components, interconnection and integration of parts, hierarchy

and system architecture, function

WHEN IS SMALL GOOD?

Properties that are size and shape tunablemechanical, thermal, acoustical, dielectric, surface vs bulk,

electrical, optical, electro-optical, magnetic, photonic, catalytic, photochemical, photophysical, electrochemical, separation, recognition,

composite

Page 25: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

CAPPED MONODISPERSED SEMICONDUCTOR NANOCLUSTERS

nMe2Cd + nnBu3PSe + mnOct3PO (nOct3PO)m(CdSe)n + n/2C2H6 + nnBu3P

EgC = Eg

B + (h2/8R2)(1/me* + 1/mh*) - 1.8e2/R

Coulomb interaction between e-h

Quantum localization term

Page 26: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

ARRESTED GROWTH OF MONODISPERSED

NANOCLUSTERS

CRYSTALS, FILMS ANDLITHOGRAPHIC

PATTERNS

nMe2Cd + nnBu3PSe + mnOct3PO (nOct3PO)m(CdSe)n + n/2C2H6 + nnBu3P

Page 27: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

MONODISPERSED CAPPED CLUSTER SINGLE CRYSTALS

methanol

2-propanol

toluene

Rogach AFM 2002

Page 28: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

THINK SMALL DO BIG THINGS!!!

EgC = Eg

B + (h2/8R2)(1/me* + 1/mh*) - 1.8e2/R

Page 29: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

SELF-ASSEMBLING AUROTHIOL CLUSTERS

HAuCl4(aq) + Oct4NBr (Et2O) Oct4NAuCl4 (Et2O)

nOct4NAuCl4(Et2O) + mRSH + 3nNaBH4 Aun(SR)m

Page 30: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

CAPPED METAL CLUSTER CRYSTAL

CLUSTER SELF-ASSEMBLY DRIVEN BY HYDROPHOBIC INTERACTIONS BETWEEN ALKANE TAILS OF

ALKANETHIOLATE CAPPING GROUPS ON GOLD NANOCRYSTALLITES

Page 31: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE
Page 32: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

CAPPED FePt NANOCLUSTER SUPERLATTICE HIGH-DENSITY DATA STORAGE MATERIALS

Page 33: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

ZEOLATE CAPPED SEMICONDUCTOR CLUSTERS

Page 34: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

ZEOLATE LIGAND

Crown ether - zeolate ligand analogy - metal coordination

chemistry of zeolites

Page 35: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

TOPOTACTIC MOCVD

Intrazeolite reaction of acid zeolite Y (HY) with known amounts of Me2Cd or Me4Sn vapors

Gives anchored MeCdY and Me3SnY, which react with H2S or H2Se to create encapsulated and zeolate capped nanoclusters Cd4S4Y and Sn4S6Y

Defined by Reitveld PXRD structure refinement

Page 36: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

MOCVD TOPOTAXY OF INTRAZEOLITE TIN SULFIDE, CADMIUM SELENIDE AND SILICON AND GERMANIUM NANOCLUSTERS

Page 37: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

INTRAZEOLITE CVD OF SILICON

NANOCLUSTERS

Page 38: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

• Si2H6 + H56Y (Si2H5)8-Y

• (Si2H5)8-Y (Si8)8-Y

• Superlattice of Si8 clusters in ZY

QUANTUM CONFINED SILICON - < 5 nm -MAKING SILICON GLOW THROUGH NANOCHEMISTRY

Page 39: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

INTRAZEOLITE TUNGTEN OXIDE NANOCLUSTERS

Page 40: RUTILE CRYSTAL STRUCTURE z x y. SEEING THE 1-D CHANELS IN RUTILE

NANOWIRES - FABRICATION OR SYNTHESIS

• Top down advanced nanolithography fabrication methods - expensive and time consuming

• Bottom up chemical synthesis methods - economical and fast

• Creation of 1D nanowires - used as functional components and interconnects in building nanodevices and nanocircuitry through self assembly strategies

• Most successful purely synthesis methods involve vapor-solid VS, vapor-liquid-solid VLS, solution-liquid solid SLS and solution-solid SS processes

• These chemical approaches have led to carbon nanotubes, metal and semiconductor nanowires and a range of inorganic materials

• Other approaches involve structure directing templates like channels in porous alumina, hexagonal lyotropic liquid crystals and block copolymers