tructure - michael goerz
TRANSCRIPT
191. Chemical bonding and crystal structure
Scanning electron microscopy Cleaved surface
Scanning tunneling microscopy
Ni surfaceZnO, TiO2, NiO, NaCl, Si, Ge, GaAs, InP
Crystals are build by „small“repeating units (= basis) like atoms and molecules
201. Chemical bonding and crystal structure
1.1 Atoms
211.1 Atoms
only for s-waves (l=0) Rn0(r = 0) ≠ 0
Hydrogen atom
221.1 Atoms
Polar plot
231.1 Atoms Chemical bonding and Crystal structure
Ni (Z = 28), Zeff = 8, d = 2.49 Å
241.1 Atoms Chemical bonding and Crystal structure
Hydrogen atom
10950 MHz = 0.045 meV, beachte aber ΔE/E ~ Z2α2
251.1 Atoms Chemical bonding and Crystal structure
corresponds to relativistic corrections whichresult from Dirac´s equation
i) Relativistic, kinetic energyii) Spin-orbit coupling (LS – coupling)iIi) Darwin term
(see, e.g., p1/2 - p3/2 splitting in Nickel)
261.1 Atoms Chemical bonding and Crystal structure
i) Relativistic, kinetic energy
Estimate of (v/c)2 via uncertainty relation (a = Bohr radius):
271.1 Atoms Chemical bonding and Crystal structure
ii) Classical Hamiltonian for the spin-orbit interaction B field from the proton in the electron's rest frame is
perturbation Hamiltonian
recall
281.1 Atoms Chemical bonding and Crystal structure
iii) Darwin term
Flickering motion of electron in nucleus leads to average potential
contribution only for s-waves with finite amplitude at x = 0
291.1 Atoms Chemical bonding and Crystal structure
Rumpfniveaus
Valenzniveaus
Nicht die Größe der Bindungsenergiesondern der Grad der Lokalisationder Wellenfunktion entscheidet.
301.1 Atoms Chemical bonding and Crystal structure
Hund‘sche Regeln für teilweise gefüllte Schalen (Valenzelektronen)
1. S maximal2. L maximal3. J = |L-S| für nicht mehr als halbgefüllte Schalen4. J = L+S für mehr als halbgefüllte Schalen
Ni: Ar 3d8 4s2
1. S = 12. L = 33. J = 4
2S+1LJ = 3F4
311.1 Atoms Chemical bonding and Crystal structure
He 1s2 – excited states 2S+1LJ
2s+1 = 1 singulett state antisymmetric2s+1 = 3 triplett state symmetric
attractive Coulombinteraction:
„s-wave in core, p-wave not“
Spatial part accordingly (Hund‘s rules !)
321.1 Atoms Chemical bonding and Crystal structure
Aufbauprinzip
331.2 Molecules
bonding (attraction) due to valence electronsPauli repulsion between neighbouring atoms
equilibrium distance r0 (related to lattice parameter)
r = r0r > r0
r
U(r)
r < r0
Chemical bonding and Crystal structure
341.2 Molecules
Hydrogen ion H2-
Chemical bonding and Crystal structure
351.2 Molecules Chemical bonding and Crystal structure
LCAO – linear combination of atomic orbitals
361.2 Molecules Chemical bonding and Crystal structure
Molecular orbitals (e.g. benzene)
LCAO
371.3 Crystals Chemical bonding and Crystal structure
NaCl CsCl
Ionic bonding (6 -10 eV)Covalent bonding (3-9 eV)
Hydrogen-bridge bonding (0.1 eV)
Van der Waals bonding (< 0.2 eV)
Metalic bonding (1-2 eV)
Si
381.3 Crystals
graphite: planar sp2 structure
diamond, silicon: tetrahedral sp3 structure
Chemical bonding and Crystal structure
Covalent bonding
Electron density (contour plot)
391.3 Ion Crystals Chemical bonding and Crystal structure
Ionic bonding - energetics
ionization energy
(eV)
electron affinity (eV)
ionization energy
(eV)
electron affinity (eV)
Li 5.39 0.62 F 17.4 3.40 Na 5.14 0.55 Cl 13.0 3.61 K 4.34 0.5 Br 11.8 3.36
Rb 4.18 I 10.5 3.06
Na + Cl → Na+ + Cl- + 1.53 eVelectrostatic interaction between ions
Na+ and Cl-: 5.1 eV (r0 ~ 2.8 Å)total energy gain of 3.57 eV
Nearly spherical charge distributions (closed shell)
Electron density (contour plot)
401.3 Ion Crystals Chemical bonding and Crystal structure
Ionic bonding - electrostatic energy (Born-Mayer potential)
A Madelung constant, z coordination number
NaCl (z = 6): A = 1.747565
CsCl (z=8): A = 1.762675
411.3 Ion Crystals Chemical bonding and Crystal structure
Parameters ρ and B of the repulsive potential determined by equilibrium distance r0 and compressibility κ
stability depends on the ratio rA /rB of ionic radii:CsCl ↔ NaCl ↔ ZnS
1.37 < rA /rB < 2.44
Different structures of ionic crystals:
421.3 Crystals - metals Chemical bonding and Crystal structure
Metallic bonding
Overlapping wave functions form delocalized states (Bloch states)
- s – electrons of Alkali metals Li, Na, K, Cs, Rb (bcc)- s,p – electrons of 3d metals Fe (bcc), Co (hcp), Ni (fcc), Cu (fcc)
(d-electrons add covalent character)
bcc fcchexagonal
hcp
431.3 Crystals
Hydrogen-bridge bonding
proton position (on A-B)
pote
ntia
l en
ergy
μ
104.5o
Hδ+ O
δ-2
Hδ+
Hydrogen: 1s1, Ip = 15.6 eV, ‘ion core’ (proton) with radius ~10-15 m
- Electron transfer to strongly electronegative atoms (F, O, ...)- Small size of proton leads to hydrogen bond A-H...B between two negatively charged atoms (double well potential)
Water
Chemical bonding and Crystal structure
441.3 Crystals
Ice
DNA
Chemical bonding and Crystal structure
Hydrogen-bridge bonding
451.3 Van der Waals Crystals
Origin: Interplay between attractive (van der Waals) and repulsive forces- van der Waals interaction:
zero point fluctuations of electrons lead to induced dipole forces- Short range repulsive interaction due to Pauli exclusion principle
´Model potential: Lennard-Jones potential
Chemical bonding and Crystal structure
461.3 Rare gas crystals
closed packedfcc (ABC – stacking)A12 = 12.13; A6 = 14.45hcp (AB – stacking)
hcpfccfccfccfcc
Chemical bonding and Crystal structure
471.3 Crystal binding energy / atom
metals: ~1 - 2 eV/atomcovalent: ~3 - 9 eV/atomionic: ~6-10 eV/atom
van der Waals: 20-200 meV/atomhydrogen: ~100 meV/bond
Chemical bonding and Crystal structure
481.4 Bravais lattice
fcc
bcc
diamond
Chemical bonding and Crystal structure
491.4 2d - Bravais lattice Chemical bonding and Crystal structure
- choice of unit cell is not unique- primitive unit cell contains only one point
501.4 14 Bravais lattices Chemical bonding and Crystal structure
511.4 Cubic Bravais lattices Chemical bonding and Crystal structure
face-centered cubic
body-centered cubic
simple cubic
521.4 Cubic Bravais lattices Chemical bonding and Crystal structure
Wigner-Seitz cell2 - dim.
bcc fcc
Wigner-Seitz cell reflects symmetry of point group
C4
C3
C2
531.4 Crystal lattice Chemical bonding and Crystal structure
32 crystallographic point groups
Schönflies symbols
Diamond point group Td ; fcc and bcc point group Oh
C4
C3
C2
541.5 Crystal structure Chemical bonding and Crystal structure
Hexagonal close-packedstacking ABABAB...
stacking ABCABC...
fcc
hcp
hexagonal
hcp
551.5 Crystal structure Chemical bonding and Crystal structure
Diamond structure C, Si, Ge Zink sulfid structure ZnS, GaAs, AgI
NaCl CsCl, NiAl, CuBe
561.5 Crystal structure Chemical bonding and Crystal structure
Quasicrystalslong-range orientational, but non-periodic order
Penrose tiles
Al65Cu20Fe15produced by cooling with 106 K/s
fivefold symmetry
571.5 Crystal structure Chemical bonding and Crystal structure
Substitutional binary alloysGe/Si
Two elements crystallizingwith the same structure
30% Ag/ 70% Cu
86 % Ag
Rasterelektronenmikroskop
95 % Cu