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The Structure and Dynamics of Solids
The Muppet’s Guide to: The Structure and Dynamics of Solids 4. Phase Transitions & Crystal Growth
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Phase Transitions The change from one state (or phase) or another is associated with a phase transition and a critical point. In this example it is a structural phase transition that occurs abruptly at a critical temperature, Tc.
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Phase Transition ORDERED DISORDERED At the phase transition the Gibbs free energy of the two states is identical
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Describing Phase Transitions
Ordering Parameter, h: This is the parameter which shows a change at the transition temperature or pressure. Order parameter is a derivative of the Gibbs free energy with respect to a thermodynamic variable Chemical potential Applied Field
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1st Order Phase Transitions
Ehrenfest classification: Discontinuity in the 1st derivative of Gibbs free energy Transitions that exhibit LATENT HEAT – Energy must be supplied to change the local environment. This results in no temperature change.
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Boiling Water First-order transitions are associated with "mixed-phase regimes" Some parts of the system have completed the transition whilst others have not. Water does not instantly change from liquid to gas. Instead it forms a mixture of water and steam bubbles. Similarly it does not instantly freeze.
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First Order h Discontinuity Transitions in liquid crystals
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1st order Phase Transitions…
BaTiO3: Volume change at Tc Thus expect first order phase change with discontinuity in Ps at Tc LaTaO3 shows second order phase transition
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Phase Transitions in BaTiO3
[001] [011] [111] PHONONS Tcf , Introduction to Solid State Physics, 6th Ed., Kittel
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KxNa1-xNbO3 monoclinic cubic tetragonal
Dan Baker, PhD Thesis 2009, University of Warwick
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2nd Order Phase Transitions
Ehrenfest classification: Discontinuity in the 2nd derivative of Gibbs free energy Transitions that exhibit NO latent heat correspond to divergences in the susceptibility, an infinite correlation length, and a power law decay of correlations
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2nd Order – FM transition
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Magnetic Ordering Critical Point Critical Exponents:
h Critical Point Critical Exponents: b=0.326(1) MFA, b=0.5 g=1.2378(6) MFA, g=1
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Phase Transitions A phase change can occur for thermodynamic reasons:
- Ordering of ground state to reduce H BUT Kinetics may produce a non-thermodynamic (metastable) state during growth. Thermodynamically this should decay to the ground state (eventually).
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Metastable State
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Final Structures: Thermo vs. Kinetics
Energy to remain on surface, Ea Energy to diffuse on surface, Ed Cohesive energy, Ec Strain Energy – modification of U
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Carbon structures are stable under different bonding configurations
Allotropes - Carbon Graphite In-plane sp2 & van der Waals Diamond 3D - sp3 Fullerenes sp2: Hexagons & pentagons Carbon structures are stable under different bonding configurations
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Activation Energy Activation Energy
Thermodynamically lowest energy state is the most stable, but must overcome the energy barrier to reach it. Multiple structures of the same material with an energy barrier separating the two.
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Tin Disease – Buttons, Cathedral organ pipes
Allotropes - Sn T<13.2°C Tin Disease – Buttons, Cathedral organ pipes
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HPHT Synthetic Diamonds
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Hexagonal, hcp like, different number of 2nd nearest neighbours
Polymorphs - ZnS Zincblende Cubic, Diamond like Wurtzite Hexagonal, hcp like, different number of 2nd nearest neighbours
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Calcite Polymorphs: CaCO3
Aragonite Vaterite Trigonal Orthorhombic Hexagonal
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Silica Polymorphs: SiO2
Amorphous Tetragonal Rhombohedral
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Paracetamol
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MnSb – polymorph structures
n-MnSb(hexagonal) Niccolite (P63/mmc) c-MnSb (cubic) Zincblende (F-43m) w-MnSb (hexagonal) Wurtzite (P63mc) Mn Sb MnSb(0001) GaAs (111)B MnSb on GaAs(111)B MnSb on GaAs(111)A Cubic MnSb GaAs
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Crystal Growth Different methods needed for different materials
All growth processes require conditions that promote formation of a crystal such as: Condensing from a supersaturated solution Freezing from a melt Evaporation Different methods needed for different materials
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Crystal growth happens at steps
(001) (111) (101) (011) 5μm CdTe in N2 -adatom
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Ce0.5Zr0.5O2 Figures adapted from W.D. McAllister, Materials Science and Engineering, 7th edition, Wiley. Figures after M. Boudart Kinetics of Heterogeneous Catalytic Reactions, Princeton University Press,1984 and W.J. Stark et al. Chem Comm (2003)
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Blocking of step flow by impurities
Cohesive energy, Ec -adatom -Impurity species
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Growth from Solution Evaporation of the solvent causes super-saturation and hence the solute comes out of solution
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