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MoleculeMolecule Intermolecular Potentials on a Gold Surface

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In partner with Howard Mayne and Greg Bubnis. 2. Introduction ... Each atom on the rotor induces a potential on the atoms of the neighboring rotors ... – PowerPoint PPT presentation

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Title: MoleculeMolecule Intermolecular Potentials on a Gold Surface


1
Molecule-Molecule Intermolecular Potentials on a
Gold Surface
  • By Jacob Harvey, RPI
  • In partner with Howard Mayne and Greg Bubnis

2
Introduction
  • Molecules on gold surface pivot around center
    point
  • Each atom on the rotor induces a potential on the
    atoms of the neighboring rotors

3
Morse Potential
  • Potential is calculated using the Morse Equation
  • Parameters B tightness factor
  • Re Optimal distance
  • R actual distance
  • D energy parameter

4
Graph of Morse Potential Energy
  • Two particle system with one being stationary
  • Parameters D 10000
  • Re .7
  • B 5

5
Quick Look at Parameters
  • Larger B value tightens the well
  • Smaller B value widens the well

B10 Re.7
B1 Re.7
6
Quick Look at Parameters
  • A larger Re value shifts the graph right
  • A smaller Re value shifts the graph left

Re.2 B5
Re1.0 B5
7
Two Rotor System
  • Each rotor is allowed to spin on central point
    and is affected by other rotors
  • Therefore each atom feels a potential from two
    other atoms
  • What are the optimal orientations?
  • What parameters lead to these orientations?

8
Adjusting value of Re
  • What happens when you adjust the value of Re?
  • The parameter B is set equal to 5 and is held
    constant
  • When 0ltRelt.8
  • Optimal orientations exist when rotors exist at
    an angle of 0 or any multiple of 180

9
Adjusting Value of Re
  • When Regt.8
  • Optimal orientations now exist when both rotors
    are at 90

10
Adjusting Value of Re
  • What about when Re .8, B5?
  • Here the system appears to be in a transition
    state with many minimums

11
Re .8
  • Where are the optimal orientations for Re.8?
  • They can be found using the process called
    Simulated Annealing

12
Adjusting the Parameter of B
  • The parameter B can also be adjusted to obtain
    various orientations. Re is set equal to .7 and
    is held constant.
  • When Bgt1.5 the optimal orientation is 180

Bgt1.5
13
Adjusting the Parameter B
  • When Blt1.5 the optimal orientation is 90

Blt1.5
14
B 1.5
  • Again the system appears to be in transition

15
B 1.5
  • Using the same process as before the optimal
    orientations can be found

16
Adjusting the length of Rotor
  • Finally the last parameter to adjust is the
    length of the rotor
  • Is it optimal to have a long rotor?
  • Is it optimal to have a short rotor?

17
Short Rotor
  • What does the system look like for a short rotor?
  • Parameters B5, Re.7, Rotor Length.25

18
Long Rotor
  • What does the system look like for a longer
    rotor?
  • Parameters B5,Re.7,Rotor Length1.0

19
Long or Short?
  • The minima for longer rotors actually yield a
    lower energy
  • It is more practical to have the rotors form a
    line
  • Lower Energy More
    Practical

20
Which Parameter Drives the System
  • What happens when a B value that is favorable to
    a 180 orientation is used with a Re value that
    is favorable to a 90 orientation?

B5 Re1.0
21
Big Picture
  • How can this research be used?
  • More Rotors
  • Rotors can potentially be aligned to form
    pseudo nano-wires

Work by Greg Bubnis
22
Organic Rotors
  • What might a rotor look like?
  • Molecule can potentially rotate in its position
    on a gold surface
  • Potential created by the polar ends of the
    molecule

Fullerene compound synthesized by Miller group
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