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List of symbols | p. xxvii |
Glossary | p. xxix |
Interfacial Structure | |
The geometry of interfaces | p. 3 |
Introduction | p. 3 |
All the group theory we need | p. 4 |
The relationship between two crystals | p. 5 |
Crystals and lattices | p. 5 |
Vector and coordinate transformations | p. 6 |
Descriptions of lattice rotations | p. 8 |
Vector and matrix representations | p. 8 |
The Frank-Rodrigues map | p. 10 |
Fundamental zones | p. 12 |
Quaternions | p. 17 |
Geometrical specification of an interface | p. 20 |
Macroscopic and microscopic geometrical degrees of freedom | p. 20 |
Macroscopic geometrical degrees of freedom of an arbitrary interface | p. 21 |
Grain boundaries in cubic materials | p. 21 |
The median lattice and the mean boundary plane | p. 21 |
Tilt and twist components | p. 23 |
Symmetric and asymmetric tilt boundaries | p. 24 |
Bicrystallography | p. 25 |
Introduction | p. 25 |
Outline of crystallographic methodology | p. 26 |
Introduction to Seitz symbols | p. 30 |
Symmetry of dichromatic patterns | p. 30 |
Symmetry of dichromatic complexes | p. 38 |
Symmetry of ideal bicrystals | p. 40 |
Symmetry of real bicrystals | p. 41 |
Two examples | p. 42 |
Lattice matched polar-non-polar epitaxial interfaces | p. 42 |
Lattice matched metal-silicide silicon interfaces | p. 45 |
Classification of isolated interfacial line defects | p. 46 |
General formulation | p. 48 |
Interfacial dislocations | p. 51 |
DSC dislocations | p. 51 |
Supplementary displacement dislocations | p. 52 |
Relaxation displacement dislocations | p. 55 |
Non-holosymmetric crystals and interfacial defects | p. 56 |
Interfacial disclinations and dispirations | p. 58 |
The morphologies of embedded crystals | p. 58 |
Quasiperiodicity and incommensurate interfaces | p. 62 |
References | p. 68 |
Dislocation models for interfaces | p. 70 |
Introduction | p. 70 |
Classification of interfacial dislocations | p. 74 |
The Frank-Bilby equation | p. 86 |
Comments on the Frank-Bilby equation and the dislocation content of an interface | p. 92 |
Frank's formula | p. 95 |
The O-lattice | p. 96 |
The geometry of discrete dislocation arrays in interfaces | p. 101 |
The general interface | p. 101 |
Application to a grain boundary with arbitrary geometrical parameters | p. 104 |
Grain boundaries containing one and two sets of dislocations | p. 105 |
Epitaxial interfaces | p. 108 |
Local dislocation interactions | p. 110 |
Two examples | p. 111 |
Pt-NiO interfaces | p. 111 |
A1-A1[subscript 3] Ni eutectic interfaces | p. 113 |
Elastic fields of interfaces | p. 115 |
Introduction | p. 115 |
Stress and distortion fields of grain boundaries in isotropic elasticity | p. 116 |
Grain boundary energies | p. 120 |
Stress fields of heterophase interfaces in isotropic elasticity | p. 125 |
Dislocation arrays at interfaces in anisotropic elasticity | p. 129 |
Isotropic elastic analysis of epitaxial interfaces | p. 129 |
Stress fields of precipitates and non-planar interfaces | p. 131 |
Degree of localization of the cores of interfacial dislocations | p. 132 |
Introduction | p. 132 |
Lattice theories of dislocation arrays | p. 133 |
Introduction | p. 133 |
Peierls-Nabarro model for an isolated edge dislocation | p. 135 |
Peierls-Nabarro model for a symmetrical tilt boundary | p. 136 |
The van der Merwe model for a symmetrical tilt boundary | p. 138 |
Atomistic models using computer simulation and interatomic forces | p. 139 |
Experimental observations of arrays of interfacial dislocations | p. 139 |
Mainly room-temperature observations | p. 139 |
High-temperature observations | p. 146 |
References | p. 147 |
Models of interatomic forces at interfaces | p. 149 |
Introduction | p. 149 |
Density functional theory | p. 152 |
The variational principle and the Kohn-Sham equations | p. 152 |
The Harris-Foulkes energy functional | p. 158 |
Valence and core electrons: pseudopotentials | p. 160 |
The force theorem and Hellmann-Feynman forces | p. 163 |
Cohesion and pair potentials in sp-bonded metals | p. 165 |
Effective medium theory | p. 174 |
The embedded atom method | p. 177 |
Tight binding models | p. 181 |
Introduction | p. 181 |
The diatomic molecule | p. 181 |
Bands, bonds, and Green functions | p. 185 |
Moments of the spectral density matrix | p. 196 |
The tight binding bond (TBB) model | p. 202 |
The second moment approximation | p. 207 |
Beyond the second moment approximation | p. 210 |
Temperature dependence of atomic interactions | p. 211 |
Ionic bonding | p. 224 |
Interatomic forces at heterophase interfaces | p. 229 |
References | p. 236 |
Models and experimental observations of atomic structure | p. 240 |
Introduction: classification of interfaces | p. 240 |
Diffuse interfaces | p. 241 |
Heterophase interfaces in systems with a miscibility gap | p. 243 |
Antiphase domain boundaries in systems with long-range order | p. 247 |
Displacive transformation interfaces in systems near a mechanical instability | p. 249 |
Sharp homophase interfaces: large-angle grain boundaries | p. 252 |
Large-angle grain boundaries in metals | p. 253 |
The significance of the rigid body displacement parallel to the boundary plane | p. 253 |
The significance of the expansion normal to the boundary plane | p. 259 |
Testing the analytic model | p. 264 |
The significance of individual atomic relaxation | p. 265 |
Discussion: singular, vicinal, and general interfaces | p. 272 |
Methods of computer simulation | p. 277 |
The polyhedral unit model | p. 284 |
The structural unit model | p. 286 |
Three-dimensional grain boundary structures | p. 305 |
The influence of temperature | p. 311 |
Grain boundaries in ionic crystals | p. 318 |
Grain boundaries in covalent crystals | p. 324 |
Sharp heterophase interfaces | p. 327 |
Introduction | p. 327 |
Metal-metal interfaces | p. 330 |
Metal-insulator interfaces | p. 332 |
Metal-semiconductor interfaces | p. 338 |
References | p. 341 |
Interfacial Thermodynamics | |
Thermodynamics of interfaces | p. 349 |
Introduction | p. 349 |
The interface free energy | p. 349 |
Additional interface thermodynamic quantities and relationships between them | p. 353 |
Introduction of the interface stress and strain variables | p. 359 |
Introduction of the geometric thermodynamic variables | p. 366 |
Dependence of [sigma] on the interface inclination | p. 367 |
The Wulff plot | p. 367 |
Equilibrium shape (Wulff form) of embedded second-phase particle | p. 369 |
Faceting of initially flat interface | p. 372 |
The capillarity vector, [xi] | p. 375 |
Capillary pressure associated with smoothly curved interface | p. 378 |
Equilibrium lattice solubility at a smoothly curved heterophase interface | p. 379 |
Equilibrium solubility at embedded second-phase particle | p. 381 |
Equilibrium interface configurations at interface junction lines | p. 382 |
Further thermodynamic relationships involving changes in interface inclination | p. 383 |
Dependence of [sigma] on the crystal misorientation | p. 384 |
Dependence of [sigma] on simultaneous variations of the interface inclination and crystal misorientation | p. 386 |
Chemical potentials and diffusion potentials, M[subscript i], in non-uniform systems containing interfaces | p. 387 |
Introduction | p. 387 |
Analysis of system at equilibrium; introduction of the diffusion potential, M[subscript i] | p. 387 |
Incoherent interface | p. 389 |
Coherent interface | p. 392 |
Summary | p. 392 |
Diffusional transport in non-equilibrium systems | p. 393 |
References | p. 394 |
Interface phases and phase transitions | p. 396 |
Introduction | p. 396 |
Interface phase equilibria | p. 397 |
Interface phase transitions | p. 400 |
Non-congruent phase transitions | p. 400 |
Faceting of initially flat interfaces | p. 400 |
Faceting of embedded particle interfaces | p. 401 |
Interface dissociation | p. 402 |
Congruent phase transitions | p. 404 |
Various transitions induced by changes in temperature, composition, or crystal misorientation | p. 405 |
Interface wetting by a solid phase | p. 409 |
Interface wetting by a liquid phase in alloy systems | p. 410 |
Grain boundary melting in a one-component system | p. 410 |
References | p. 412 |
Segregation of solute atoms to interfaces | p. 414 |
Introduction | p. 414 |
Overview of some of the main features of interface segregation in metals | p. 414 |
Physical models for the interaction between solute atoms and interfaces | p. 424 |
Introduction | p. 424 |
Elastic interaction models | p. 426 |
Size accommodation model | p. 426 |
Hydrostatic pressure (P[Delta]V) and elastic inhomogeneity models | p. 427 |
Further elastic models | p. 430 |
Atomistic models at 0 K | p. 430 |
Electronic interaction models | p. 433 |
Statistical mechanical models of segregation | p. 435 |
Introduction | p. 435 |
Regular solution model | p. 436 |
Mean field models | p. 438 |
McLean isotherm | p. 442 |
Fowler-Guggenheim isotherm | p. 443 |
Multiple segregation site models | p. 443 |
Beyond mean field models | p. 447 |
Some additional models | p. 449 |
Atomistic models at a finite temperature | p. 450 |
Interface segregation in ionic solids | p. 457 |
References | p. 462 |
Interfacial Kinetics | |
Diffusion at interfaces | p. 467 |
Introduction | p. 467 |
Fast diffusion along interfaces of species which are substitutional in the crystal lattice | p. 468 |
Slab model and regimes of diffusion behaviour | p. 468 |
Mathematical analysis of the diffusant distribution in the type A, B, and C regimes | p. 472 |
Experimental observations | p. 474 |
Some major results for diffusion along interfaces | p. 475 |
Effects of interface structure | p. 481 |
Mechanisms for fast grain boundary diffusion | p. 486 |
Equilibrium point defects in the grain boundary core | p. 487 |
'Ring', vacancy, interstitialcy, and interstitial mechanisms | p. 492 |
Models for grain boundary self-diffusivities via the different mechanisms | p. 495 |
Vacancy mechanism | p. 498 |
Interstitialcy mechanism | p. 498 |
Interstitial mechanism | p. 499 |
General characteristics of the models for boundary self-diffusion | p. 499 |
On the question of the mechanism (or mechanisms) of fast grain boundary diffusion | p. 502 |
Metals | p. 502 |
Ionic materials | p. 506 |
Covalent materials | p. 508 |
Diffusion along interfaces of solute species which are interstitial in the crystal lattice | p. 509 |
Slow diffusion across interfaces in fast ion conductors | p. 513 |
Diffusion-induced grain boundary motion (DIGM) | p. 514 |
References | p. 518 |
Conservative motion of interfaces | p. 522 |
Introduction | p. 522 |
'Conservative' versus 'non-conservative' motion of interfaces | p. 522 |
Driving pressures for conservative motion | p. 523 |
Basic mechanisms: correlated versus uncorrelated processes | p. 525 |
Impediments to interface motion | p. 525 |
Mechanisms and models for sharp interfaces | p. 526 |
Glissile motion of interfacial dislocations | p. 526 |
Small-angle grain boundaries | p. 526 |
Large-angle grain boundaries | p. 531 |
Heterophase interfaces | p. 536 |
Glide and climb of interfacial dislocations | p. 540 |
Small-angle grain boundaries | p. 540 |
Large-angle grain boundaries | p. 543 |
Heterophase interfaces | p. 549 |
Shuffling motion of pure steps | p. 550 |
Uncorrelated atom shuffling and/or diffusional transport | p. 555 |
Uncorrelated atom shuffling | p. 557 |
Uncorrelated diffusional transport | p. 558 |
Solute atom drag | p. 560 |
Experimental observations of non-glissile (thermally activated) grain boundary motion in metals | p. 563 |
General large-angle grain boundaries | p. 563 |
Singular (or vicinal) large-angle grain boundaries | p. 566 |
Solute atom drag effects | p. 569 |
Small-angle grain boundaries | p. 572 |
Mechanisms and models for diffuse interfaces | p. 573 |
Propagation of non-linear elastic wave (or, alternatively, coherency dislocations) | p. 574 |
Self-diffusion | p. 574 |
Equations of interface motion | p. 577 |
Motion when v = v(n) | p. 577 |
Motion of curved interfaces under capillary pressure | p. 580 |
More general conservative motion | p. 582 |
Impediments to interface motion due to pinning | p. 583 |
Pinning effects due to embedded particles | p. 583 |
Pinning at stationary particles at low temperatures | p. 583 |
Thermally activated unpinning | p. 587 |
Diffusive motion of pinned particles along with the interface | p. 587 |
Pinning at free surface grooves | p. 590 |
References | p. 594 |
Non-conservative motion of interfaces: interfaces as sources/sinks for diffusional fluxes of atoms | p. 598 |
Introduction | p. 598 |
General aspects of interfaces as sources/sinks | p. 599 |
'Diffusion-controlled', 'interface-controlled', and 'mixed' kinetics | p. 599 |
Dissipation of energy during source/sink action | p. 603 |
The maximum energy available to drive the source/sink action | p. 604 |
Grain boundaries as sources/sinks for fluxes of atoms | p. 606 |
Introduction | p. 606 |
Small-angle grain boundaries | p. 606 |
Models | p. 606 |
Experimental observations | p. 613 |
Large-angle grain boundaries | p. 614 |
Models for singular or vicinal grain boundaries | p. 614 |
Models for general grain boundaries | p. 617 |
Experimental observations | p. 618 |
Sharp heterophase interfaces as sources/sinks for fluxes of atoms | p. 621 |
Models | p. 621 |
Singular or vicinal heterophase interfaces | p. 621 |
General heterophase interfaces | p. 624 |
Experimental observations | p. 624 |
Growth, coarsening, shape-equilibration, and shrinkage of small precipitate particles | p. 624 |
Growth of phases in the form of flat parallel layers | p. 634 |
Annealing of supersaturated vacancies | p. 640 |
Diffusional accommodation of boundary sliding at second phase particles | p. 642 |
Diffuse heterophase interfaces as sources/sinks for solute atoms | p. 644 |
On the question of interface stability during source/sink action | p. 647 |
References | p. 651 |
Interfacial Properties | |
Electronic properties of interfaces | p. 657 |
Introduction | p. 657 |
Metal-semiconductor interfaces | p. 660 |
Introduction | p. 660 |
The Schottky model | p. 660 |
The Bardeen model | p. 663 |
Metal-induced gap states (MIGS) | p. 664 |
The defect model | p. 668 |
The development of the Schottky barrier as a function of metal coverage | p. 669 |
Schottky barriers on Si | p. 671 |
Discussion of models for Schottky barriers | p. 673 |
Inhomogeneous Schottky barriers | p. 673 |
Semiconductor heterojunctions | p. 674 |
Introduction | p. 674 |
The band offsets | p. 676 |
Grain boundaries in metals | p. 684 |
Grain boundaries in semiconductors | p. 689 |
Grain boundaries in high temperature superconductors | p. 695 |
References | p. 700 |
Mechanical properties of interfaces | p. 704 |
Introduction | p. 704 |
Compatibility stresses in bicrystals and polycrystals | p. 704 |
Compatibility stresses caused by applied elastic stress | p. 704 |
Compatibility stresses caused by plastic straining | p. 709 |
Compatibility stresses caused by heating/cooling | p. 710 |
Elastic interactions between dislocations and interfaces | p. 711 |
Interfaces as sinks, or traps, for lattice dislocations | p. 714 |
Introduction | p. 714 |
Small-angle grain boundaries | p. 716 |
Large-angle grain boundaries and heterophase boundaries | p. 721 |
Singular boundaries | p. 721 |
General boundaries | p. 726 |
On the global equilibration of impinged lattice dislocations | p. 729 |
Interfaces as sources of both interfacial and lattice dislocations | p. 730 |
Interfaces as sources of interfacial dislocations | p. 731 |
Interfaces as sources of lattice dislocations | p. 732 |
Singular interfaces | p. 733 |
General interfaces | p. 734 |
Interfaces as barriers to the glide of lattice dislocations (slip) | p. 737 |
Grain boundaries | p. 737 |
Heterophase interfaces | p. 740 |
Effects of interfaces on the plastic deformation of bicrystals and polycrystals at low temperatures | p. 740 |
Homophase bicrystals and polycrystals | p. 741 |
Heterophase bicrystals and polycrystals | p. 744 |
Role of interfaces in the plastic deformation of bicrystals and polycrystals at high temperatures | p. 744 |
Interface sliding | p. 745 |
Sliding at an ideally planar grain boundary | p. 745 |
Sliding at a non-planar grain boundary by means of elastic accommodation | p. 748 |
Sliding at a non-planar grain boundary by means of diffusional accommodation | p. 750 |
Sliding at a non-planar grain boundary by means of plastic flow accommodation in the lattice | p. 752 |
Experimental observations of sliding at interfaces | p. 753 |
Creep of polycrystals | p. 758 |
Creep of homophase polycrystals controlled by diffusional transport | p. 759 |
Creep of homophase polycrystals controlled by boundary sliding | p. 763 |
Creep of homophase polycrystals controlled by movement of lattice dislocations | p. 766 |
Further aspects of the creep of polycrystals | p. 767 |
Fracture at homophase interfaces | p. 768 |
Overview of the different types of fracture observed experimentally in homophase polycrystals | p. 768 |
Propagation of cleavage cracks | p. 772 |
Crack propagation in a single crystal | p. 772 |
Crack propagation along a grain boundary | p. 779 |
Crack propagation in homophase polycrystals | p. 781 |
Growth and coalescence of cavities at grain boundaries at low temperatures by plastic flow due to dislocation glide | p. 785 |
Growth and coalescence of cavities at grain boundaries at high temperatures by diffusion, power-law creep, and boundary sliding | p. 786 |
Initiation of cavities | p. 786 |
Growth of cavities | p. 789 |
Coalescence of cavities and complete intergranular fracture | p. 794 |
Fracture at heterophase interfaces | p. 794 |
References | p. 798 |
Index | p. 805 |
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