Crystal Structures of Interest • Elemental solids: – Face-centered cubic (fcc) – Hexagonal close-packed (hcp) – Body-centered cubic (bcc) – Diamond cubic (dc) • Binary compounds – Fcc-based (Cu3Au,NaCl, ß-ZnS) – Hcp-based (α-ZnS) – Bcc-based (CsCl, Nb3Sn) MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley The Common Crystal Structures: Body-Centered Cubic (BCC) • Atoms at the corners of a cube plus one atom in the center • Common in MSE 200A Fall, 2008 – Is a Bravais lattice, but drawn with 2 atoms/cell to show symmetry – Bcc is not ideally close-packed – Closest-packed direction: <111> – Closest-packed plane: {110} – Alkali metals (K, Na, Cs) – Transition metals (Fe, Cr, V, Mo, Nb, Ta) J.W. Morris, Jr. University of California, Berkeley The Face-Centered Cubic (fcc) and Hexagonal Close-Packed (hcp) Structures • Fcc: atoms at the corners of the cube and in the center of each face • Hcp: close-packed hexagonal planes stacked to fit one another – Is a Bravais lattice, but drawn with 4 atoms/cell to show symmetry – Found in natural and noble metals: Al, Cu, Ag, Au, Pt, Pb – Transition metals: Ni, Co, Pd, Ir – Does not have a primitive cell (two atoms in primitive lattice of hexagon) – Divalent solids: Be, Mg, Zn, Cd – Transition metals and rare earths: Ti, Zr, Co, Gd, Hf, Rh, Os MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley fcc and hcp from Stacking Close-Packed Planes A A B A A A B B C A A A B C A A BB C A A C C → C A B A AB A A A B → C C A A B A B C A A ABA = hcp A B C C A A A B B C A A A • There are two ways to stack spheres • The sequence ABA creates hcp • The sequence ABC creates fcc MSE 200A Fall, 2008 The image cannot be displayed. Your computer may not have enough memory to open the image, or the image may ABC = fcc J.W. Morris, Jr. University of California, Berkeley Hexagonal Close-Packed MSE 200A Fall, 2008 • HCP does not have a primitive cell • Common in • Anisotropy limits engineering use of these elements – 2 atoms in primitive cell of hexagonal lattice – 6 atoms in cell drawn to show hexagonal symmetry – Divalent elements: Be, Mg, Zn, Cd – Transition metals and rare earths: Ti, Zr, Co, Gd, Hf, Rh, Os J.W. Morris, Jr. University of California, Berkeley Face-Centered Cubic Structure ABC stacking Fcc cell View along diagonal (<111>) • FCC is cubic stacking of close-packed planes ({111}) • Common in – 1 atom in primitive cell; 4 in cell with cubic symmetry – <110> is close-packed direction – Natural and noble metals: Cu, Ag, Au, Pt, Al, Pb – Transition metals: Ni, Co, Pd, Ir MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Interstitial Sites: Octahedral Voids in fcc MSE 200A Fall, 2008 • Octahedral interstitial site is equidistant from six atoms • There are 4 octahedral voids per fcc cell – “Octahedral void” – Located at {1/2,1/2,1/2} and {1/2,0,0} – One per atom J.W. Morris, Jr. University of California, Berkeley Interstitial Sites: Tetrahedral Voids in FCC • Tetrahedral site is equidistant from four atoms – “tetrahedral void” – Located at {1/4,1/4,1/4} - center of cell octet • There are 8 tetrahedral voids per fcc cell – Two per atom MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Interstitial Sites: Voids between Close-packed Planes A B C C A A A B B C A A A A B C C A A A B B C A A • In both FCC and HCP packing: • Stacking including voids: A – Tetrahedral void above and below each atom (2 per atom) – Octahedral void in third site between planes – Fcc: ...(aAa)c(bBb)a(cCc)b(aAa)… – Hcp: ...(aAa)c(bBb)c(aAa)… (octahedral voids all on c-sites) ⇒ Size and shape of voids are the same in fcc and hcp MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley The Diamond Cubic Structure • Fcc plus atoms in 1/2 of tetrahedral voids • DC is the structure of the Group IV elements – Close-packed plane stacking is ...AaBbCc… or ... aAbBcC... - Each atom has four neighbors in tetrahedral coordination - Natural configuration for covalent bonding – C, Si, Ge, Sn (grey) – Are all semiconductors or insulators MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Solid Solutions and Compounds • Solid solution – Solute distributed through solid - Substitutional: solutes on atom sites - Interstitial: solutes in interstitial sites - Ordinarily small solutes (C, N, O, …) • Ordered solution (compound) – Two or more atoms in regular pattern (AxBy) – Atoms may be substitutional or interstitial on parent lattice – “Compound” does not imply distinguishable molecules MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Atomic Resolution Image of Gum Metal • “Gum metal”: Ti-23Nb-0.7Ta-2Zr-1.2O MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Binary Compounds: Examples • Substitutional: – Bcc: CsCl – Fcc: Cu3Au • Interstitial: – – – – MSE 200A Fall, 2008 Fcc octahedral: NaCl Fcc tetrahedral: ß-ZnS Hcp tetrahedral: α-ZnS Bcc tetrahedral: Nb3Sn (A15) J.W. Morris, Jr. University of California, Berkeley BCC Substitutional: CsCl • BCC parent – – – – Stoichiometric formula AB A-atoms on edges B-atoms in centers Either specie may be “A” • Found in: – Ionic solids (CsCl) • Small size difference • RB/RA > 0.732 to avoid like-ion impingement – Intermetallic compounds • CuZn (ß-brass) MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley FCC Substitutional: Cu3Au • FCC parent – Stoichiometric formula A3B – B-atoms on edges – A-atoms on faces • Found in: – Intermetallic compounds (Cu3Au) – As “sublattice” in complex ionics • E.g., “perovskites” – BaTiO3 (ferroelectric) – YBa2Cu3O7 (superconductor) • Lattices of + and - ions must interpenetrate since like ions cannot be neighbors MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley FCC Octahedral Interstitial: NaCl • FCC parent – – – – Stoichiometric formula AB A-atoms on fcc sites B-atoms in octahedral voids Either can be “A” • Found in: – Ionic compounds: • NaCl, MgO (RB/RA ~ 0.5) • “Perovskites” (substitutional ordering on both sites) – Metallic compounds • Carbonitrides (TiC, TiN, HfC) MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley FCC Tetrahedral Interstitial: ß-ZnS • Binary analogue of DC – Stoichiometric formula AB – A-atoms on fcc sites – B-atoms in 1/2 of tetrahedral voids • AaBbCc – Either element can be “A” • Found in: – Covalent compounds: • GaAs, InSb, ß-ZnS, BN – Ionic compounds: • AgCl • Large size difference (RB/RA < .414) MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Hcp Tetrahedral Interstitial: α-ZnS • Hexagonal analogue of ß-ZnS – Stoichiometric formula AB – A-atoms on hcp sites – B-atoms in 1/2 of tetrahedral voids • AaBbAaBb – Either element can be “A” • Found in: – Covalent compounds: • ZnO, CdS, α-ZnS, “Lonsdalite” C – Ionic compounds: • Silver halides • Large size difference (RB/RA < .414) MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Interstitial Sites: “Octahedral” Voids in Bcc Crystals • Octahedral voids in face center and edge center • Octahedral voids in bcc are asymmetric MSE 200A Fall, 2008 – Located at {1/2,1/2,0} and {1/2,0,0} – Each has a short axis parallel to cube edge (Ox, Oy, Oz) – Total of six octahedral voids, three of each orientation J.W. Morris, Jr. University of California, Berkeley Interstitial Sites: “Tetrahedral” Voids in Bcc Crystals • Tetrahedral voids in each quadrant of each face – Located at {1/2,1/4,0} – 12/cell => 6/atom • MSE 200A Fall, 2008 Tetrahedral voids in bcc are asymmetric J.W. Morris, Jr. University of California, Berkeley Bcc Tetrahedral Interstitial: Α15 • Complex BCC derivative – Stoichiometric formula A3B – B-atoms on bcc sites – A-atoms in 1/2 of tetrahedral voids • Form “chains” in x, y, and z • Found in: – A15 compounds: • Nb3Sn, Nb3Al, Nb3Ge, V3Ga – These are the “type-II” superconductors used for wire in high-field magnets, etc. MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Description of Complex Crystal Structures • Most crystals can be referred to a close-packed frame – Fcc or hcp network – Possibly plus small distortions along symmetry axes • Cubic → tetragonal (edge unique), • Cubic → rhombohedral (diagonal unique) • Atoms in ordered configurations in – Substitutional sites – Interstital sites: octahedral or tetrahedral – Vacancies are useful as “atoms” to complete the configuration MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Hierarchical Description of Complex Crystal Structures • Construct planar layers • Identify ordered pattern • Order layers – Network (fcc or hcp) – Interstitial planes that contain atoms – Primary and interstitial planes – Pattern is the same on all planes – Including vacancies, if necessary, as species – Physical pattern (fcc or hcp) – Chemical pattern • composition may change from layer to layer (differentiation) – Stacking pattern is the same for network and interstitial layers MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Substitutional X-Compounds • Undifferentiated – All atoms are the same: fcc, hcp, polytypes (e.g., ABCBABCBA…) • Differentiated – Planes of atoms alternate: CuPt, WC – Note that cubic symmetry is broken in CuPt: rhombohedral ^ ^ ^ ^ ^ MSE 200A Fall, 2008 ^ = Cu =W = Pt =C J.W. Morris, Jr. University of California, Berkeley Octahedral Interstital X-Compounds • Undifferentiated • Differentiated = Na = As = Cl = Ni – Fcc or hcp planes alternate with filled octahedral planes: NaCl, NiAs – Note that o-sites in NiAs are ccc, can tell which atom is in octahedral hole – Alternate lattice or interstitial planes differ – CdI2: like NiAs but octahedral Cd planes alternate with vacant planes MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Tetrahedral(I) X-compounds = Zn = Zn =S =S • Lattice planes plus alternate planes of tetrahedral voids • Examples: – Unary: diamond cubic, hexagonal diamond (Lonsdaleite) – Binary: α-ZnS, β-ZnS MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley Tetrahedral(II) X-Compounds = Ca =F • Lattice planes plus planes on both tetrahedral sites • Fcc-based: CaF2 (flourite) and Li2O • Hcp-based: none known MSE 200A Fall, 2008 J.W. Morris, Jr. University of California, Berkeley