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Title: Underpotential Deposition Topic Review and


1
Underpotential DepositionTopic Review and
Implementation Considerations Mohan
Karulkar February 2, 2004
2
Outline
  • 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?)

3
Underpotential 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
4
Different 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

5
OPD/UPD Comparison
6
Halide-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)
7
Halide-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)
8
Phenomena 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)
9
UPD 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

10
UPD 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.

11
UPD 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

12
Project 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

13
Project 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
14
Implementation
  • 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

15
Implementation
  • 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

16
Implementation
  • 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

17
Implementation
  • 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

18
Summary
  • 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

19
References
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    Garza, N. Batina, Surface Science, 476, 139
    (2001)
  • C. Lucas, N. Markovic, P. Ross, Physical Review
    B, 56, 3651 (1997)
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    (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
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    Acta, 44, 983, (1998)
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    B, 51, No 4, 2484 (1995)
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    J. Electrochem. Soc. 146, 1035 (1999)
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    Weickowski (Marcel Dekker, New York, 1999), p. 47
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    Principles, (Prentice Hall, New Jersey, 1991).
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    1414 (1996)
  • I. Tidswell, C. Lucas, N. Markovic, P. Ross, Phys
    Rev B, 51, 10205 (1995)

20
References
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    Langmuir, 11, 4098 (1995)
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21
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