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Contents An overview Literature
The electronic structure of materials 1Quantum mechanics 2 - Lecture 8
Igor Lukacevic
UJJS, Dept. of Physics, Osijek
December 13, 2012
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
1 An overview
2 Literature
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Contents
1 An overview
2 Literature
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
Ground state
cohesive energy
equilibrium crystal structure
phase transitions betweenstructures
elastic constants
charge density
magnetic order
static dielectric susceptibility
static magnetic susceptibility
nuclear vibrations (in theadiabatic approximation)
...
Excited state
low-energy excitations
Pauli spin susceptibility
transport
electrical conductivity
optical properties
thermal excitation of electrons
spectra for adding electrons
spectra for removing electrons
...
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
Interplay:
electronic ground state ! spatial structure of the nuclei
⇓
bonding
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
1 closed-shell systemsrare gasesmolecular solidsvan der Waals interaction
2 ionic bonding
3 covalent bonding
4 metallic bonding
5 hydrogen bonding
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
1 closed-shell systems
2 ionic bondingelectronegativity differencecharge transferhcp, fcc or bccinsulators
3 covalent bonding
4 metallic bonding
5 hydrogen bonding
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
1 closed-shell systems
2 ionic bonding
3 covalent bondingcomplete change of theelectronic statesopen structures
4 metallic bonding
5 hydrogen bonding
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
1 closed-shell systems
2 ionic bonding
3 covalent bonding
4 metallic bondingpartially filled bandsclose-packed structures
5 hydrogen bonding
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electronic ground state
1 closed-shell systems
2 ionic bonding
3 covalent bonding
4 metallic bonding
5 hydrogen bondingp-e attractionno core repulsionintra- and inter- molecular
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electron density in the ground state
n(r) can be:measured experimentally
- x-ray scettering- high-energy electron scattering
calculated theoretically
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electron density in the ground state
n(r) can be:measured experimentally
- x-ray scettering- high-energy electron scattering
calculated theoretically
n(r) reveals:
core density
atomic-like
Debye-Waller factor
smearing of theaverage density due tothermal and zero-pointmotion
“outer” density
changes in density dueto bonding and chargetransfer
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electron density in the ground state
core density
atomic-like
Debye-Waller factor
smearing of theaverage density dueto thermal andzero-point motion
“outer” density
changes in densitydue to bonding andcharge transfer
A question
How would you reveal (calculate) the covalent bond density?
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Electron density in the ground state
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Volume or pressure as the fundamental variables
Equation of state: E = E(p,T )
E = E(V ,T = 0) very easy to calculate
99K one of the most important tests of the theory (e-e interaction)
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Volume or pressure as the fundamental variables
Fundamental quantities
E = E(V ) = Etotal(V ) ,
p = − dE
dV,
B = −V dp
dV= V
d2p
dV 2
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Volume or pressure as the fundamental variables
Fundamental quantities
E = E(V ) = Etotal(V ) ,
p = − dE
dV,
B = −V dp
dV= V
d2p
dV 2
How to test the theory using these variables:
1 equilibrium volume V0 =⇒ E0 , p = 0
2 equilibrium bulk modulus B0 =⇒ E0 , p = 0
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Volume or pressure as the fundamental variables
For example,
1 calc. E for several V
2 fit with analytic eq. of states
3dE
dVgives V0 and E0
4d2p
dV 2gives B
Accuracy within few percent ofexp.
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
Experiments can now easily measure materials’ properties under pressure
“Bridgman” era: 1905. - 20th century40’s
DAC (diamond anvil cell) - C. E. Weir(1959)
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
Pressure can change manymaterials’ properties
Band structure of K under pressure [2].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
Pressure can change manymaterials’ properties
The shift of optical absorption spectra under pressure [3].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
Pressure can change manymaterials’ properties
Existance of superconducting phases under pressure [4].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
Pressure can change manymaterials’ properties
E(V ) of various Si phases [5].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
How to calculate the pressureat which phase transitionoccurs?
1 G(T = 0) = H
stable structure enthalpy minimum
2 Gibbs construction oftangent lines betweenE(V ) curves
Enthalpies of various InP phases [6].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
How to calculate the pressureat which phase transitionoccurs?
1 G(T = 0) = H
stable structure enthalpy minimum
2 Gibbs construction oftangent lines betweenE(V ) curves
E(V ) of various Si phases [5].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phase transitions under pressure
How to calculate the pressureat which phase transitionoccurs?
1 G(T = 0) = H
stable structure enthalpy minimum
2 Gibbs construction oftangent lines betweenE(V ) curves
So, how accurate are thesemethods?
Lowest transition pressures of several semisonductors [6].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Elasticity: stress-strain relation
A question
What happens with the electronic ground state when strain is applied?
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Elasticity: stress-strain relation
A question
What happens with the electronicground state when strain is applied?
“Streckung des Grundgebietes”.
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Elasticity: stress-strain relation
Stress-strain relation
σαβ = − 1
V
∂Etot
∂uαβ
σαβ → stress tensor
uαβ → strain tensor
Stress-strain relation in Si [7].
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Magnetism and electron-electron interaction
What are magnetic systems?Ones in which the ground state has a broken symmetry with spin and/or orbitalmoments of the electrons.
Examples:
1 ferromagnets
2 antiferromagnets...
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Magnetism and electron-electron interaction
What are magnetic systems?Ones in which the ground state has a broken symmetry with spin and/or orbitalmoments of the electrons.
Explanation:
spin + orbital moment + Hund’s rules
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Magnetism and electron-electron interaction
Explanation:
spin + orbital moment + Hund’s rules
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Magnetism and electron-electron interaction
Basic equations
E(Vm) = Etot(Vm) ,
m(r) = − dE
dVm(r),
χ(r, r′) = − dm(r)
dVm(r′)=
d2E
dVm(r)dVm(r′)
m = n↑ − n↓ - magnetization
Vm = µHZeeman - effective Zeeman field which replaces e-e interaction
A question
What is m if we ignore the e-e interaction? What is m in a ferromagnet or aantiferromagnet?
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Magnetism and electron-electron interaction
Stoner parameter:
I · N(0)→ 1⇒ χ→∞
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phonons and displacive phase transitions
Experiments
Vibrational spectra:
infrared absorptionspectroscopy
light scattering
inelastic neutron scattering
Theory
E({RI}) = Etot({RI}) ,
FI = − dE
dRI,
CIJ = − dFI
dRJ= − d2E
dRIdRJ
A question
These equations hold only in adiabatic orBorn-Oppenheimer approximation. Can youremember what they say?
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phonons and displacive phase transitions
Experiments
Vibrational spectra:
infrared absorptionspectroscopy
light scattering
inelastic neutron scattering
Great synergy betweenexperiments and theory!
Theory
E({RI}) = Etot({RI}) ,
FI = − dE
dRI,
CIJ = − dFI
dRJ= − d2E
dRIdRJ
From these we get:
interatomic force constants
static dielectric constants
piezoelectric constants
effective charges
electron-phonon interaction...
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phonons and displacive phase transitions
Two approaches:
1 “frozen phonon”method
2 response functionmethod
Left: Two optic mode displacements in MgB2. Right: Two optic mode displacements of Ti
atoms in BaTiO3.
A question
What does the left figure reminds you of?
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Phonons and displacive phase transitions
Two approaches:
1 “frozen phonon”method
2 response functionmethod
Phonon dispersion curves for GaAs.
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Thermal properties
QMD = Quantum MolecularDynamics (Car-Parrinello MD)
liquids as a function of T
solids as a function of T
melting
chemical reactions of moleculesin solution
adsorption processes...
Phase diagram of carbon.
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Thermal properties
Water tough test for the theory (hydrogen bonding)
Radial density distributions in water molecule.
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Thermal properties
Water tough test for the theory (hydrogen bonding)
Proton transfer in water under high-temeprature/high-pressure conditions.
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Surfaces, interfaces and defects
Experiments
Powerfull techniques:
STM
x-ray diffraction
electron diffraction...
STM image of GaN (000-1) surface.
Theory
Supercell method - repeat supercells,not unit cells
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Surfaces, interfaces and defects
Surfaces Defects Molecules
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Surfaces, interfaces and defects
Electrolyses of water on metal surfaces - Pt(111)
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Contents
1 An overview
2 Literature
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1
Contents An overview Literature
Literature
1 R. M. Martin, “Electronic Structure - Basic Theory and PracticalMethods”, Cambridge University Press, Cambridge, 2004.
2 M. Alouani et al., Phys. Rev. B 39, 8096 (1989).
3 M. Moakafi et al., Eur. Phys. J. B 64, 35 (2008).
4 V. V. Struyhkin et al., Nature 390, 382 (1997).
5 M. T. Yin et al., Phys. Rev. B 26, 5668 (1982).R. Biswas et al., Phys. Rev. B 30, 3210 (1984).
6 A. Mujica et al., Rev. Mod. Phys. 75, 863 (2003).
7 O. H. Nielsen et al., Phys. Rev. Lett. 50, 697 (1983).
8 http://www.youtube.com/watch?v=UjXvI2w0VAU
Igor Lukacevic UJJS, Dept. of Physics, Osijek
The electronic structure of materials 1