Title: Underpotential Deposition Topic Review and
1Underpotential DepositionTopic Review and
Implementation Considerations Mohan
Karulkar February 2, 2004
2Outline
- Underpotential Deposition (UPD) Topic Review
- (What is UPD?)
- Literature Review
- (What work has been done?)
- Project Review
- (Why is it important to our group?)
- Implementation
- (What are the implementation issues?)
3Underpotential Deposition Characteristics
- Occurs at Potentials positive of the Nernst
Potential 7 - Occurs with metal deposition onto a foreign metal
substrate 24 - Depends strongly on
- potential
- electrolyte composition
- local coverage
- Deposits only up to one monolayer (ML)
- Proceeds slower than bulk deposition
Figure 1 CV for Tl Deposition onto Ag
Figure 1 D. M. Kolb, in Advances in
Electrochemistry and Electrochemical Engineering,
edited by H. Gerischer and C. W. Tobias, (Wiley,
New York, 1978), Vol. 11, p. 141
4Different UPD Mechanisms
- Additive-Free 7
- More anodic potentials ordered structures
(islands), up to 0.5 ML - More cathodic potentials, phase transitions
marked by onset of lateral, metal-like
attractions, up to Full ML 1 - Additive-Assisted 1,-3,9-11,15,16,18,19,29-32,36,3
7,39 - Three-region, two-step mechanism.
- Most anodic region hexagonal layer of additive
- Mid-range potentials replacement of some
additive with metal, into hexagonal structure - Most cathodic Formation of metal monolayer with
additive on top - Described in detail shortly
5OPD/UPD Comparison
6Halide-assisted UPD
3-Region, 2-Stage mechanism (Figure 2)
- Region III Substrate covered by halide
hexagonal structure formed - Region II Stage 1 of UPD begins at most anodic
peak some halide is displaced, eventually
forming Region II intermediate hexagonal
structure with both Metal and halide present - Region I Stage 2 begins at less-anodic peak
halide further displaced by metal. Region I
structure consists of pseudomorphic monolayer of
Metal covered by ordered halide layer
Figure 2 CV of Cu UPD on Pt(111) 0.001M
Cu(ClO4)2 and 0.01M NaCl. Shows 3 regions of
UPD. Measured vs. SCE.
Figure 2 Tidswell, C. Lucas, N. Markovic, P.
Ross, Phys Rev B 51, 10205 (1995)
7Halide-assisted UPD Example
End of Region II
Region III
Region I
Start of Region II
Figure 3 Various Stages of halide-assisted UPD
Figure 3 N. Markovic, C. Lucas, H. Gasteiger, P.
Ross, Surface Science 372, 239 (1997)
8Phenomena to Capture
- Geometry
- Region 3 (additive case) is hexagonal, region 2
is hexagonal, region 1 is pseudomorphic, etc - Necessary geometry affects what sites can
experience adsorption
- Potential
- Growth regions separated by potential
- Coverage
- Deposit forms in each growth region only up to a
certain local coverage
Fig 4 Examples of different geometric
interactions
Figure 4 M. Itoh, G. Bell, A. Avery, T. Jones,
B. Joyce, D. Vvedensky, Physical Review Letters
81, 633 (1998)
9UPD Literature Review
Review of Cu UPD Experimental Work
- Surfaces
- Pt(111) and (001) 2,10,15-17,29-32,36
- Au(111) and (001) 1,3,9,11,18,19,37,39
- Additives
- Halide, Sulphate, Perchlorate
- Results
- Same general 2-stage mechanism seen for all
single-additive systems - Differences in threshold concentrations, detailed
structure of metal/additive intermediate,
additive layer in Region I, etc
10UPD Literature Review
Review of Cu UPD Simulation Work
- Pade approximants (Cu on Au(111)) 21, 22
- Interpolated between Langmuir isotherm and Ising
model to derive coverage as function of potential
or electrovalence - Lattice Gas Model (LGM) (Cu on Au(111))
- Simulated two-component adsorption system to
study lateral adsorbate-adsorbate interactions up
to fourth-nearest neighbors.
11UPD Literature Review
Review of Cu UPD Simulation Work
- Dynamic Monte Carlo Method (Cu on Au(111)) 13
- Combined with LGM to simulate thermally activated
motion of particles adsorbing, desorbing, and
diffusing - Used LG Hamiltonian to get free energies for
different geometric configurations - Kinetic Monte Carlo Method (homoepitaxy,
GaAs(001)) 25 - Included Ga deposition, hopping, As2 deposition
and desorption - Used to obtain energy barriers for different
surface interactions
12Project Review
- Experimental study and Simulation of Metallic
Nanoclusters - Potential gradient along resistive strip
- UPD-like conditions at deposition nose
- Detailed in 2003 NIRT Proposal
- Bohn group (Brian Coleman) experiments
- Experimental setup is a resistive strip
- Investigation of deposition nose
Fig 5 Deposition along linear potential gradient
13Project Review
- Dima Lubomorskys Cell
- Mono-electrode
- Must calculate potential distribution
- Feng Xuis Cell
- Bi-potential
- Known potential distribution
- Both cells will exhibit regions of underpotential
deposition
Fig 6Lubomorsky Cell design
14Implementation
- Need Rate Law to use for KMC algorithm
- Rate law must obey detailed balance
- Rate of going from state c to c in equilibrium
is same as c going to c. - Simplest rate law 13
- state2 and state1 are the energy of state 1 and 2
- u attempt frequency, D free-energy barrier
- Obtain energy of a state from Hamiltonian
15Implementation
- Energy of a particular configuration given by
Grand-canonical lattice-gas Hamiltonian12, 13
- m electrochemical potential
- ci concentration of adsorbate at site i (1 or
0) - Index n represents separation between sites
- represents sum over all pairs of neighbors
of rank - F 2-body interaction energy
16Implementation
- Can combine Hamiltonian with simple rate law to
obtain KMC-ready rate expression - Can be extended to 2-component systems by using a
two-component lattice gas Hamiltonian 12 - Hamiltonian can be extended to include more
components
17Implementation
- Recall important phenomena
- Potential
- Hamiltonian has a potential-dependent term, which
carries over to the rate law. At more negative
potentials, this overpowers body-interaction term
- Geometry
- Hamiltonian has term for 2-body interactions,
which can be adjusted for certain orientations - Coverage
- Body-interaction term overpowers potential term
at less negative potentials, leading to lower
coverage
Fig 7 Recall different geometric interactions
18Summary
- UPD
- Deposition at potentials more positive than
Nernst Potential - Important aspects Potential, Geometry, Coverage
- 3-stage, 2-step mechanism
- UPD Regions Separated by potential characterized
by geometry and maximum coverage - Literature Review
- Experiments Pt and Au, (111) and (001) Halide,
Sulphate, Perchlorate additives - Simulation Pade Approximants, Lattice Gas
Models, Dynamic Monte Carlo, Kinetic Monte Carlo - Projects
- Bi-potential and mono-electrode cells (Feng and
Dima) - Implementation
- Basic Arrhenius rate law
- Energy of states obtained from Lattice Gas
Hamiltonian
19References
- A. Matrinez-Ruiz, J. Valenzuela-Benavides, L.
Garza, N. Batina, Surface Science, 476, 139
(2001) - C. Lucas, N. Markovic, P. Ross, Physical Review
B, 56, 3651 (1997) - C. Sanchez. E. Leiva, Elecrochemica Acta, 45, 691
(1999) - D. Huckaby, J. Kowalski, J. Chem. Phys, 80, 2163
(1984) - D. Huckaby, L. Blum, Langmuir 11, 4583 (1995)
- D. Kolb, Z. Phys. Chem. N.F. 154, 179 (1987)
- D. M. Kolb, in Advances in Electrochemistry and
Electrochemical Engineering, edited by H.
Gerischer and C. W. Tobias, (Wiley, New York,
1978), Vol. 11, p. 125 - D.M. Kolb in Scherling Lecture, (Sherling
Lecture Publications, Berlin, 1991), Vol. 1 - E. Chabala, J. Cairns, T. Rayment, J Electroanal.
Chem., 412, 77 (1996) - E. Herrero, L. Buller, A. Finnefrock, A. Salomon,
C. Alonso, J. Brock, H Abruna, Electrochemica
Acta, 44, 983, (1998) - F. Moller, O. Magnussen, R. Behm, Physical Review
B, 51, No 4, 2484 (1995) - G. Brown, P. Rikvold, M. Novotny, A. Wieckowski,
J. Electrochem. Soc. 146, 1035 (1999) - G. Brown, P. Rikvold, S. Mitchell, M. Novotny, in
Interfacial Electrochemistry, edited by A.
Weickowski (Marcel Dekker, New York, 1999), p. 47 - G. Prentice, Electrochemical Engineering
Principles, (Prentice Hall, New Jersey, 1991). - H. Bludau, K. Wu, M.S. Zei, M. Eiswirth, H. Over,
G. Ertl, Surface Science, 402-404, 786 (1998) - H. Gasteiger, N. Markovic, P. Ross, Langmuir, 12,
1414 (1996) - I. Tidswell, C. Lucas, N. Markovic, P. Ross, Phys
Rev B, 51, 10205 (1995)
20References
- J. Hotlos, O.M. Magnussen, R. J. Behm, Surface
Science, 335, 129 (1995) - J. Xu, X. W. Wang, Surface Science, 408, 317
(1998) - J. Zhang, Y. Sung, P. Rikvold, A. Wieckowski, J.
Chem. Phys. 104, 14 (1996) - L. Blum, D Huckaby, Electrochemica Acta, 41, 2207
(1996) - L. Blum, D Huckaby, J. Chem. Phys. 94, 10 (1991)
- L. Blum, D Huckaby, J. Electroanal. Chem. 315,
255 (1991) - L. Blum, M. Legault, D. Huckaby, in Interfacial
Electrochemisty, edited by A. Weickowski (Marcel
Dekker, New York, 1999), p. 19 - M. Itoh, G. Bell, A. Avery, T. Jones, B. Joyce,
D. Vvedensky, Physical Review Letters, 81, 633
(1998) - M. Legault, L. Blum, D. Huckaby, J. Analytical
Chem., 409, 79 (1996) - M.S. Zei, G. Qiao, G. Lempfuhl, D. M. Kolb, Ber.
Bunsenges. Phys. Chem. 91, 349 (1987) - Martinez, J. Valenzuela-Benavides, L. Garza, N.
Batina, Surface Science, 476, 139 (2001) - N. Markovic, C. Lucas, H. Gasteiger, P. Ross,
Surface Science, 372, 239 (1997) - N. Markovic, H. Gasteiger, C. Lucas, P. Ross,
Langmuir, 11, 4098 (1995) - N. Markovic, H. Gasteiger, C. Lucas, P. Ross,
Surface Science, 335, 91 (1995) - N. Markovic, P. Ross, Langmuir, 9, 580 (1993)
- P. Rikvold, Electrochemica Acta, 36, 1689 (1991)
- P. Rikvold, G. Brown, M. Novotny, A. Wieckowski,
Colloids and Surfaces A, 134, 3 (1998) - P. Rikvold, M. Deakin, Surface Science, 249, 180
(1991)
21References
- R. Michaelis, M.S. Zei, R. S. Zhai, J.
Electroanal. Chem, 339, 299 (1992) - S. Manne, P. Hansma, J. Massie, V. Elings,
A.Gewirth, Science, 251, 183 (1991) - Y. Nakai, M.S. Zei, D. M. Kolb, G. Lempfuhl, Ber.
Bunsenges. Phys. Chem. 88, 340 (1984) - Z. Shi, J. Lipkowski, Journal of
Electroanalytical Chemistry 365, 303 (1994)