Unconventionality in Solid State Chemistry Douglas A. Vander Griend Department of Chemistry & Biochemistry Calvin College Grand Rapids, Michigan July 7,

Slides:



Advertisements
Similar presentations
Site occupancies in the R 2-x Fe 14+2x Si 3 (R = Ce, Nd, Gd, Dy, Ho, Er, Lu, Y) compounds studied by Mössbauer spectroscopy A. Błachowski 1, K. Ruebenbauer.
Advertisements

Division of Materials Science & Engineering
Relations between crystal structures
Structural Properties of Electron Beam Deposited CIGS Thin Films Author 1, Author 2, Author 3, Author 4 a Department of Electronics, Erode Arts College,
Kitaoka lab. Takayoshi SHIOTA M1 colloquium N. Fujiwara et al., Phys. Rev. Lett. 111, (2013) K. Suzuki et al., Phys. Rev. Lett. 113, (2014)
Crystal Structural Behavior of CoCu₂O₃ at High Temperatures April Jeffries*, Ravhi Kumar, and Andrew Cornelius *Department of Physics, State University.
The Double Pervoskite NaTbMnWO 6 : A Likely Multiferroic Material † Alison Pawlicki, ‡ A. S. Sefat, ‡ David Mandrus † Florida State University, ‡ Oak Ridge.
Search for high temperature superconductivity of Sr 2 VO 4 under high pressure Shimizu Lab Kaide Naohiro.
Short range magnetic correlations in spinel Li(Mn Co ) 2 O 4.
University of California at Berkeley – Physics Department – Hellman Lab Application of “Calorimetry-on-a- Chip” Technology to Heat Capacities of Quenched.
H. C. Ku Department of Physics, National Tsing Hua University, Hsinchu, Taiwan 300, R.O.C. with: B. N. Lin, P. C. Guan, Y. C. Lin, T. Y. Chiu, M. F. Tai.
Superconductor Ceramics
Transient Liquid Phase Bonding as a Potential Substitute for Soldering with High-Lead Alloys A.A. Kodentsov Laboratory of Materials and Interface Chemistry,
Abnormal thermal expansion in NaZn 13 -type La(Fe 1-x Co x ) 11.4 Al 1.6 compounds Results Yuqiang Zhao 1,2, Rongjin Huang 1,*, Shaopeng Li 1,2, Wei Wang.
Lanthanides Actinides 1 st Row Transition M 2 nd Row Transition M How do the electrons fill for Rare Earths?
Periodic Table – Filling Order
Magnetic transition in the Kondo lattice system CeRhSn2
Metals, Nonmetals, Metalloids. Metals and Nonmetals Li 3 He 2 C6C6 N7N7 O8O8 F9F9 Ne 10 Na 11 B5B5 Be 4 H1H1 Al 13 Si 14 P 15 S 16 Cl 17 Ar 18 K 19 Ca.
MgB2 Since 1973 the limiting transition temperature in conventional alloys and metals was 23K, first set by Nb3Ge, and then equaled by an Y-Pd-B-C compound.
Inorganic Material Lab. SKKU Selective Intercalation of Various Muconates into [LiAl 2 (OH) 6 ]Cl  H 2 O Layered Double Hydroxide (LDH)
A study of Fe – substituted (La 0.8 Sr 0.2 ) 0.95 MnO 3-y as cathode material for solid oxide fuel cells B. N. Wani, Mrinal Pai, S.J. Patwe, S. Varma,
Study of the Sn-Zn-X alloys for solder applications in the electronic industry Study of the Sn-Zn-X alloys for solder applications in the electronic industry.
Trends of the Periodic Table
Periodic Table Of Elements
NOVEL MIXED-VALENT TRANSITION METAL OXIDES Mas A. Subramanian, Oregon State University, DMR This is an exploratory research project on the identification,
s p d (n-1) f (n-2) 6767 Periodic Patterns 1s1s1s1s 2s2s2s2s 3s3s3s3s 4s4s4s4s 5s5s5s5s 6s6s6s6s 7s7s7s7s 3d3d3d3d 4d4d4d4d 5d5d5d5d 6d6d6d6d 1s1s1s1s.
An Introduction to Fe-based superconductors
Sept. 14 th 2004 Montauk, Long Island, NY Jason S. Gardner NIST, Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg,
Introduction to Mineralogy Dr. Tark Hamilton Chapter 3: Lecture 7 The Chemical Basis of Minerals (sizes, shapes & directions) Camosun College GEOS 250.
16th International Conference on composite Materials July 8-13,2007 Kyoto International Conference Center, Kyoto, Japan Synthesis of 0.95MgTiO CaTiO.
(Nb-O) (Nb=O) 570 (m) 942 (s) 919 (s) (Te-O) 644 (s) (V=O) [VO 3 ] n n- 944 (s) 900 (sh) n (Mo=O) Mo 8 O (sh) (Mo=O) Mo 7 O (s) 893.
Correlated Electron State in Ce 1-x Yb x CoIn 5 Stabilized by Cooperative Valence Fluctuations Brian M. Maple, University of California, San Diego, DMR.
The Structure and Dynamics of Solids
Phase transition in the H 2 O-H 2 system at pressures up to 10 kbar V. Efimchenko (1), M. Kuzovnikov (1) and M. Tkacz (2) (1) Institute of Solid State.
n n n Group I Group I Metallofullerenes Donate 1 electron to cage M 2n − Distribution similar to empty cages C 60 and C 70 dominant.
Solid State Synthesis, Phase Diagrams and Solid Solutions Chemistry 123 Spring 2008 Dr. Woodward.
Periodic Table Li 3 He 2 C6C6 N7N7 O8O8 F9F9 Ne 10 Na 11 B5B5 Be 4 H1H1 Al 13 Si 14 P 15 S 16 Cl 17 Ar 18 K 19 Ca 20 Sc 21 Ti 22 V 23 Cr.
Chapter 6 Solid-State Chemistry. Problems n n 6.9, 6.13, 6.14.
2n 2n 2n 2n 2n 2n n
Y.C. Hu 1, X.S. Wu 1, J.J. Ge 1, G.F. Cheng 2 1. Nanjing National Laboratory of Microstructures, Department of Physics, Nanjing University, Nanjing ,
Trends of the Periodic Table. Electronegativity ElectronegativityyElectronegativityy.
(a) Ca 14 Au 45 Sn 6 (b) CaAg 3.5 In 1.9 (c) SrAu 4.3 In 1.7 Hexagonal Au star Honeycomb- like template Disorder in tunnel Gold-Rich Complex Intermetallic.
Thermodynamics and the Phase Rule
International University for Science & Technology College of Pharmacy General Chemistry (Students of Dentistry) Prof. Dr. M. H. Al-Samman.
CHAPTER FIFTEEN Copyright © Tyna L. Gaylord All Rights Reserved 1.
Overview of 133/219 class Condensed Matter/Materials Science Laboratory TA : Sooyoung Jang Inho Jeon Welcome to 133/219 class.
Overview of 133/219 class Condensed Matter/Materials Science Laboratory TA : Sooyoung Jang Veronica Burnett Welcome to 133/219 class.
When and who? In 1869 Russian Chemist Dimitri Mendeleev and German chemist Lothar Meyer published nearly identical ways of classifying.
CHEMICAL THERMODYNAMICS CHEM171 – Lecture Series Three : 2012/01  Spontaneous processes  Enthalpy (H)  Entropy (S)  Gibbs Free Energy (G)  Relationship.
Periodic Table Li 3 He 2 C6C6 N7N7 O8O8 F9F9 Ne 10 Na 11 B5B5 Be 4 H1H1 Al 13 Si 14 P 15 S 16 Cl 17 Ar 18 K 19 Ca 20 Sc 21 Ti 22 V 23 Cr.
Thermodynamics and the Phase Rule
13/11/
electrochemical stability of the siliceous brass ЛК80-3
Thermodynamics and the Phase Rule
Effects of sintering temperature on the physical and
Introduction To Chemistry
OXYGEN MEMBRANE CATALYTIC FUEL REFORMING
Non-stoichiometry in CaCu3Ti4O12 (CCTO) ceramics
Trends of the Periodic Table
Periodic Table Kelter, Carr, Scott, Chemistry A Wolrd of Choices 1999, page 74.
Periodic Table of the Elements
4.2 IONIZATION ENERGY 4.6 TABLE 4.2 Ionization Energy of the Elements
PERIODIC TABLE OF ELEMENTS
Dale Clouser Jr., Samantha Schmuecker, Dr. Brian Leonard
THE BIGGER PICTURE - TRENDS IN REAL SYSTEMS
Equilibrium Studies of Self-Assembly Events
Supercell Crystal Structure of Na2Ga2(BO3)2O
DETECTION LIMITS < 1 ppt ng/L 1-10 ppt ng/L ppt ng/L
Hydration and structural properties of mixed conductor Ba1‑xGd0. 8La0
Electron Configurations and the Periodic Table
Presentation transcript:

Unconventionality in Solid State Chemistry Douglas A. Vander Griend Department of Chemistry & Biochemistry Calvin College Grand Rapids, Michigan July 7, 2004

Unconventional ŭn΄kën-věn΄shë-nël/ adjective 1.not bound by or in accordance with convention 2.being out of the ordinary 3.existing without precedent

Conventional Solid State Structures

Conventional Compositions

Idealized Subcell for La 3 Cu 2 VO 9 [La] [(Cu/V)O 2+3/3 ] [La] [A] [BO 2+3/3 ]

La 3 Cu 2 VO 9 Superstructure P6 3 /m a = (1) Å c = (1) Å Cu II V O 2- 87% Cu

La 3 Cu 2 VO 9 : Frustrated Antiferromagnetism Inverse Molar Susceptibility (per copper) Temperature (K)  B 1.14  B 1.68  B 54% Paramagnetic 100% Paramagnetic 16%

La x Ln 3-x Cu 2 VO 9 Lattice Parameters

Idealized Subcell of La 4 Cu 3 MoO 12 [La] [(Cu/Mo)O 2+3/3 ] [La] [A] [BO 2+3/3 ]

Electron Diffraction La 4 Cu 3 MoO 12 Ordering of the B-cations leads to a monoclinic supercell (  = 90.03(1)º) which is 4 times larger than the conventional hexagonal subcell. La 3 Cu 2 VO 9 * Ordering of the B-cations leads to a hexagonal supercell which is 13 times larger than the conventional hexagonal subcell. *K. Jansson, I. Bryntse, Y. Teraoka Mater. Res. Bull., 1996, 31, 827.

La 4 Cu 3 MoO 12 : B-cation Ordering

La 4 Cu 3 MoO 12 : Frustrated Antiferromagnetism Temperature (K) Inverse Molar Susceptibility (per copper) 100% Paramagnetic 35% Paramagnetic 1.02  B 1.73  B

Ln 4 Cu 3 MoO 12 Powder X-ray Diffraction

Ln 4 Cu 3 MoO 12 Lattice Parameters

Rare-earth Hexagonal Structure Type Versatility *Prog. Solid St. Chem. 1993, 22, 197. "Many new and novel compositions and structures remain to be discovered by more traditional means." -J.D. Corbett Ln 4 Cu 3 MoO 12 Ln = La, Pr, Nd, Sm - Tm Ln 3 Cu 2 VO 9 Ln = La, Pr, Nd, Sm - Gd Ln 2 CuTiO 6 Ln = Tb – Lu*

Formation of Single Phases The primary goal of state synthesis is to form single phases Single phases form if and only if their  G is less than all possible multiphase mixtures at the reaction temperature. The following examples demonstrate the importance of stoichiometric analysis in the search for novel materials.

An Expected Result

An Unexpected Result

Thermodynamic Hierarchy  G(La 2 MoO 6 + Ho 2 Cu 2 O 5 ) <  G(Ho 2 MoO 6 + La 2 Cu 2 O 5 ) Ln 2 Cu 2 O 5 is more stable for smaller lanthanides, and/or Ln 2 MoO 6 is more stable for larger lanthanides. GG

Ln' 2 Ln" 2 Cu 3 MoO 12 Synthesis Results

Why does La 4 Cu 3 MoO 12 Form? Structure is unconventional. –A-cation coordination is low (6-7). –B-cation coordination is atypical (trigonal bipyramidal). But La 2+2n Cu 4+n O 7+4n (n = 2) is worse! –“It is remarkable that, given the simple ratio of the constituent elements, such complex structures form instead of the structurally simpler Ruddleson-Popper series.” - Cava et al Ln 2 Cu 2 O 5 is not even known for Ce – Gd. 75% copper is sufficient to promote single phase. La 4 Cu 3 MoO 12 forms so that La 2 Cu 2 O 5 doesn’t.

The La 2 Cu 2 O 5 Umbrella Stoichiometry

La 4 Cu 3+x Mo 1-x O 12

Why does Ho 4 Cu 3 MoO 12 Form? Ho 2 Cu 2 O 5 isn’t the problem anymore. Ho 2 MoO 6 + CuO is the problem! Ln 2 MoO 6 changes structure between Nd and Sm. 25% molybdenum is sufficient to promote single phase. Ho 4 Cu 3 MoO 12 forms so that Ho 2 MoO 6 doesn’t.

Ln 2 MoO 6 Structural Shift Nd 2 MoO 6 (I-42m) a = Å c = Å Sm 2 MoO 6 (I2/a) a = Å b = Å c = Å 2  (copper K  )

Ln 4 (Cu/Mo) 4 O 12 Thermodynamic Stability

More Examples La 2 CuSnO 6 vs. La 2 Cu 2 O 5 + La 2 Sn 2 O 7 –La 2 Sn 2 O 7, stable pyrochlore, infamous thermodynamic sink –La 2 CuSnO 6, lone example of a layered double perovskite that forms at ambient pressure. La 2 Ba 2 Cu 2 Ti 2 O 11 vs. La 2 Cu 2 O 5 + 2BaTiO 3 –La 2 Ba 2 Cu 2 Ti 2 O 11, layered quadruple perovskite –BaTiO 3, well known for centuries. All known phases exist because at least one of the phases in every multiphase alternative has a sufficiently high  G. Identifying and applying these Umbrella Stoichiometries is the key to a more rational search for novel matierals.

Conclusions – searching for unconventionality Umbrella stoichiometries promote single phase results by destabilizing multiphase alternatives. Umbrella stoichiometries facilitate substitutions that shift compositions towards them. Example: La 4 Cu 3+x Mo 1-x O 12-2x 0  x  0.12 Undiscovered phases likely exist near umbrella stoichiometries. Phases discovered near umbrella stoichiometries will tend to be unconventional because they can be structurally discontent and still be the thermodynamic product of a solid state reaction.

Acknowledgements Chemistry Department Kenneth R. Poeppelmeier Dr. Kenji Otzschi Dr. Donggeun Ko Dr. Sophie Boudin Dr. Vincent Caignaert Dr. Sylvie Malo Dr. Antoine Maignan Tony Wang Noura Dabbouseh Scott Barry Materials Science Department Prof. Thomas Mason Dr. Yanguo Wang Prof. Vinayak Dravid Kyoto University Prof. Mikio Takano Dr. Masaki Azuma Hiroki Toganoh Argonne National Laboratory Dr. Simine Short Dr. Zhongbo Hu Dr. James Jorgensen Funding Science and Technology Center for Superconductivity Japan Society for the Promotion of Science National Science Foundation Graduate Fellowship