Title: DENSITY FUNCTIONAL CALCULATIONS OF BONDING AND ADHESION AT METAL
1DENSITY FUNCTIONAL CALCULATIONS OF BONDING AND
ADHESION AT METAL CERAMIC INTERFACES
Newton Ooi newton.ooi_at_asu.edu Ph.D student in
Materials Science Engineering Computational
Materials Science group of Dr. J. B.
Adams http//ceaspub.eas.asu.edu/cms/
ASU workshop on Quantum and Many-body effects in
nano-scale devices October 24 25, 2003
2OUTLINE
- Uses and properties of aluminum
- Adhesion to aluminum
- Computational approaches
- Density functional theory
- VASP
- Methodology
- Results
- Future work
- Acknowledgements and references
3ALUMINUM
- Uses
- Interconnects in IC chips
- Circuit board material
- Electrolytic capacitors
- Properties
- High thermal and electrical conductivity
- Forms stable oxide
- Low cost and low weight
- Reasonable electro-migration resistance
- Aluminum forms interfaces with other materials
when used in microelectronics - Need to understand bonding and structure at these
interfaces
http//www.ssmc.co.jp
http//www.dselectronicsinc.com
4ADHESION TO ALUMINUM
- Measure using wetting experiments
- Oxidation and surface contamination
- No insight into atomic bonding
- Difficult to quantify results
- Examine using computer simulation
- No concern about oxidation and contamination
- Find ideal work of separation
? work of separation - Assumes no plastic deformation
- Interfacial bonding and geometry is very complex
? need reliable quantum mechanical approaches
5WORK OF SEPARATION
6DENSITY FUNCTIONAL THEORY
- Total energy is functional of electron density
- Proposed first by Thomas and Fermi in 1920s
- Current model proposed by Hohenberg, Kohn and
Sham in 1960s and applicable to ground state - Replace many-electron Schrödinger equation with
single particle Kohn-Sham (KS) equation
Potential energy of non-interacting electrons
- Kinetic energy of
- non-interacting electrons
Electrostatic energy
Exchange correlation energy
7VASP
- Vienna Ab initio Software Package
- Fortran 90 code for Unix / Linux
- Plane wave basis set to span Hilbert space
- Born Oppenheimer approximation
- Pseudopotentials to represent ion electron
interactions - Projector augmented wave (PAW) Blochl. PRB 50,
24 (1994) 17953 - Ultra-soft (US) Vanderbilt. PRB 41 (1990) 7892
- Super cell method ? 3D periodic boundary
conditions - Variational method with free energy as
variational quantity - Exchange correlation energy
- LDA Kohn Sham. Physical Review 140 (1965)
A1133 - GGA Perdew Wang. PRB 33, 12 (1986) 8800
- VASP website http//cms.mpi.univie.ac.at/vasp/
8METHODOLOGY
- Bulk calculations
- Surface calculations
- Generate interface models
- Interface calculations
- Calculate work of separation
- Analyze atomic and electronic structure of
interface
Aluminum single electron trap http//www.nsf.gov/o
d/lpa/priority/nano/
9BULK CALCULATIONS
- Determine irreducible Brillouin zone
- Plane wave convergence to minimize basis set
- Finite temperature smearing to quicken
calculations - Calculate energy as a function of volume
- Fit using equation of state (EOS)
- Determine cohesive energy, bulk modulus and
lattice constants - Used to select best pseudopotential for surface
calculations
Aluminum bulk data a (Ã…) Ec (eV) V (Ã…3) Bo (GPa)
Calculated with LDA 3.971 -4.22 15.66 82.55
Calculated with GGA 4.039 -3.72 16.47 72.75
Experimental 4.045 -3.39 16.60 72.2
10Energy versus volume for Al using GGA-PAW
11SURFACE CALCULATIONS
- Choose surface with lowest value of ?
- Construct slabs with symmetric surfaces
- Determine irreducible Brillouin zone
- Vacuum convergence to minimize interaction
between consecutive slabs
12SURFACE ENERGY CALCULATIONS
- Calculate surface energy via surface thickness
convergence - Fit results to appropriate surface energy
equation - We used equation of Boettger PRB 49, 23 (1994)
16798
13SURFACE ENERGIES
Surface Termination Calculated (J/m2) Experiment (J/m2)
Al (100) Al 0.89 NA
Al (110) Al 1.05 NA
Al (111) Al 0.81 NA
Al2O3 (0001) Al 1.59 NA
Al2O3 (0001) O 7.64 4.45 10.83
WC (0001) W 3.66 3.43 3.88
WC (0001) C 5.92 5.69 6.14
VN (100) VN 0.95 NA
CrN (100) CrN 0.74 NA
14INTERFACE CALCULATIONS
- Generate periodic interfaces
- With or without vacuum?
- Sandwich or bi-layer?
- Lattice mismatch?
- Interface registry?
- Universal Binding Energy Relationship (UBER)
curve - Determine equilibrium interfacial separation
- Rough estimate of Ws
- Works for modeling adsorption
- Relax interface and isolated slabs to minimal
energy geometries - Calculate Ws
- Electronic structure analysis
- Charge density plots
- Electron localization function
15TYPES OF INTERFACE MODELS
- Vacuum or not?
- Vacuum allows more room for atoms to relax ?
increases accuracy - Vacuum must be populated by plane waves ?
increases calculation cost
- Sandwich or periodic?
- Dipoles must cancel
- Free surfaces must be paired
16INTERFACE CREATION
- Build interface models
- Minimize lattice mismatch
- Require symmetric interfaces
- Al(111) - graphite (0001)
- Plot out a (32) Al(111) surface, red Al atoms
and blue cell lines - Plot out a (22) C(0001) surface green cell lines
- Rotate the graphite surface so its corners match
up with Al atoms
17LATTICE MISMATCH
- Real materials can have different
- Crystal structures
- Lattice constants
- Lattice angles
- Use of periodic boundary conditions
- Minimize lattice mismatch
- Eliminate dangling bonds and unmatched surfaces
- Solutions
- Rotate surfaces with respect to each other
- Match up different multiples of each surface
- Stretch / compress one or both slabs (strain)
- Examples of lattice strain
- Al (111) Al2O3 (0001) 4.9
- Al (110) WC (0001) 0.4
- Al (100) TiN (100) 5.3
Expand Compress
18INTERFACE GEOMETRY
- Also denoted as interface registry or coherency
- Interface can range from fully coherent to fully
incoherent - Example Al (111) Graphite (0001)
- Black atoms are carbon, gray atoms are aluminum
19UBER CURVES
20NITRIDES AND CARBIDES
- VN a0 4.126 Ã…
- VC a0 4.171 Ã…
- CrN a0 4.140 Ã…
Al surface Ceramic surface Ceramic structure Ws (J/m2)
(100) VC (100) Rock salt 2.14
(100) VN (100) Rock salt 1.73
(100) CrN (100) Rock salt 1.45
(100) TiN (100 Hexagonal 1.52
21SURFACE TERMINATION AFFECT
- WC
- Gray C
- Brown W
- Al2O3
- Black O
- Red Al
Al surface Ceramic surface Calculated Ws (J/m2) Experimental Ws (J/m2)
(111) Al terminated Al2O3 (0001) 1.06 1.13
(111) O terminated Al2O3 (0001) 9.73
(111) W terminated WC (0001) 4.08
(111) C terminated WC (0001) 6.01
22GRAPHITE AND DIAMOND
- Al (111) Diamond (111)
- Clean interface Ws 3.98 4.10 J/m2 depends on
interface model and registry - Hydrogen termination of diamond Ws 0.02 J/m2
for all registries - Calculated results agree with experiments
hydrogen passivation of diamond surfaces lower
its coefficient of friction and adhesion to other
materials - Al (111) Graphite (0001)
- Ws 0.2 0.35 J/m2 depending on interface model
- Different interface registries does not affect Ws
? graphite is great lubricant for Al processing
because graphite basal planes slide easily over
Al surface - Calculations agree with measured adhesion
energies of 0.1 0.4 J/m2
23Al Graphite charge density
Abrupt change at interface negligible Al
graphite bonding
24Al Graphite ELF
- ELF (Electron Localization Function) measures
probability of electrons with same spin being
near each other - Different bonding types are differentiated by
color - Red areas ? bonding pairs ? localized bonding ?
covalent - Blue to green ? unpaired electrons or vacuum
- Yellow to orange ? metallic bonding
25Al Al203 ELF
Abrupt change in bonding at interface
Aluminum --------------------- Al2O3
26SUMMARY
- Modeling of interfaces involves many issues
- Lattice mismatch
- Symmetry and periodicity
- Coherency
- Surface termination and composition
- Adhesion to aluminum increases with the polarity
of opposing material ? polarity increases bond
formation - Adhesion at interface proportional to the surface
energies of contacting surfaces ? surface
reactivity - DFT adhesion calculations give results in good
agreement with available experimental data
System Experiment Ws (J/m2) Calculated Ws (J/m2)
Al Al2O3 1.13 1.06
Al graphite 0.1 0.4 0.2 0.35
27FUTURE WORK
- Aluminum Diamond-like carbon (DLC)
- Influence of surface stresses in carbon
- Effect of sp3/sp2 bonding ratio in carbon
- Aluminum BN
- Hexagonal versus cubic BN
- Influence of surface stoichiometry B or N or BxNy
ELF of 64-atom DLC cubic supercell with gray
iso-surface of 0.53
28CREDITS
- Acknowledgements
- NCSA at UIUC for computational resources
- NSF for funding under grant DMR 9619353
- Dr. D. J. Siegel
- Dr. L. G. Hector and Dr. Y. Qi at GM
- Georg Kresse and authors of VASP
- Newton Ooi and other group members
- References
- Siegel, Hector, Adams. PRB 67 (2003) 092105
- Kittel. Introduction to Solid State Physics 7th
Edition 2000 John Wiley Sons - Adams et al. Journal of Nuclear Materials 216
(1994) 265 - Landry et al. Mat. Science and Engineering A254
(1998) 99 - www.accelrys.com
- www.webelements.com