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Rare Event Simulations

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Title: Rare Event Simulations


1
Rare Event Simulations
  • Theory 16.1
  • Transition state theory 16.1-16.2
  • Bennett-Chandler Approach 16.2
  • Diffusive Barrier crossings 16.3
  • Transition path ensemble 16.4

2
Diffusion in porous material
3
Theory macroscopic phenomenological
Chemical reaction
Total number of molecules
Make a small perturbation
Equilibrium
4
Theory microscopic linear response theory
Microscopic description of the reaction
Reaction coordinate
Reaction coordinate
Reactant A
Product B
Lowers the potential energy in A
Increases the concentration of A
Perturbation
Probability to be in state A
5
Theory microscopic linear response theory
Microscopic description of the reaction
Reaction coordinate
Reactant A
Product B
Lowers the potential energy in A
Increases the concentration of A
Perturbation
Probability to be in state A
6
Reaction coordinate
Reaction coordinate
7
Very small perturbation linear response theory
Linear response theory static
Outside the barrier gA 0 or 1 gA (x) gA (x) gA
(x)
Switch of the perturbation dynamic linear
response
Holds for sufficiently long times!
8
Very small perturbation linear response theory
Outside the barrier gA 0 or 1 gA (x) gA (x) gA
(x)
Switch of the perturbation dynamic linear
response
Holds for sufficiently long times!
9
Linear response theory static
10
? has disappeared because of derivative
Derivative
Stationary
For sufficiently short t
11
Stationary
12
Eyrings transition state theory
Only products contribute to the average
At t0 particles are at the top of the barrier
Let us consider the limit t ?0
13
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14
Transition state theory
  • One has to know the free energy accurately
  • Gives an upper bound to the reaction rate
  • Assumptions underlying transition theory should
    hold no recrossings

15
Bennett-Chandler approach
Probability to find q on top of the barrier
Computational scheme
  1. Determine the probability from the free energy
  2. Compute the conditional average from a MD
    simulation

16
Reaction coordinate
17
Ideal gas particle and a hill
q is the true transition state
q1 is the estimated transition state
18
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20
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21
Bennett-Chandler approach
  • Results are independent of the precise location
    of the estimate of the transition state, but the
    accuracy does.
  • If the transmission coefficient is very low
  • Poor estimate of the reaction coordinate
  • Diffuse barrier crossing

22
Transition path sampling
xt is fully determined by the initial condition
Path that starts at A and is in time t in B
importance sampling in these paths
23
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24
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25
Walking in the Ensemble
Shooting
Shifting
26
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