Computing free energy: Replica exchange
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1 Computing free energy: Replica exchange
2 Extending the scale Length (m) Potential Energy Surface: {Ri} 10 6 (3N+1) dimensional 10 9 E Thermodynamics: p, T, V, N continuum ls Macroscopic i a t e regime d e average over or m all processes many atoms es Mesoscopic s s e c regime ro p many processes e few atoms or m Microscopic regime few processes {Ri} Time (s) Essentials of computational chemistry: theories and models. 2nd edition. C. J. Cramer, JohnWiley and Sons Ltd (West Sussex, 2004). Ab initio atomistic thermodynamics and statistical mechanics of surface properties and functions K. Reuter, C. Stampfl, and M. Scheffler, in: Handbook of Materials Modeling Vol. 1, (Ed.) S. Yip, Springer (Berlin, 2005).
3 Free energy, one quantity, many definitions (in this page, Helmholtz free energy, F(N,V,T)) Thermodynamics Ab initio if we can calculate E and write analytically on approximation for S for our system, we use this expression. Example: ab initio atomistic thermodynamics. Thermodynamic Integration Ab initio or similar derivatives that yield measurable quantities (in a computer simulation): one can estimate the free energy by integrating such relations. This is the class of the so called thermodynamic integration methods.
4 Free energy, one quantity, many definitions Fundamental statistical mechanics thermodynamics link Classical statistics (for nuclei): Ab initio Probabilistic interpretation of free energy Ab initio
5 Outline Free energy evaluation: Harmonic approximation (solids) Thermodynamic integration. Phase diagrams Thermodynamics perturbation (overlap, umbrella sampling) Accelerated sampling, metadynamics. Replica Exchange MD: finding the optimal dimensionality reduction
6 Energy Parallel tempering: concept Parallel the tempering: the concept T4 T3 T2 T1 Configurational coordinate Exchange rule, ensuring canonical sampling at all temperatures:
7 Parallel tempering: concept Parallel the tempering: the concept
8 Parallel tempering: concept Parallel the tempering: the concept Overlap necessary: the smaller (the system size) the better
9 T4 T3 T2 T1 Swap 2 MD or MC run 3 Swap 1 MD or MC run 2 T5 MD or MC run 1 Parallel tempering: the implementation Parallel Parallel tempering: tempering: the implementation the concept
10 Parallel tempering: monitoring Parallel Parallel tempering: tempering: the implementation the monitoring concept
11 Au4: coexistence of several isomers Parallel Tempering 0.00 ev 0.04 ev 0.36 ev Potential Energy (ev) K 100 K PT (100 ps) 100 K serial (100 ps) (degree)
12 Replica exchange: other than temperature biasing potential means sampling according to distribution:
13 Replica exchange: cluster size
14 Replica exchange: temperature weighted histogram analysis such that
15 Replica exchange: temperature weighted histogram analysis Assuming each count in each histogram as independent, then likelihood of observing the ith histrogram: If all histograms are independent: Maximum likelihood estimate:
16 Au4, relative population Free Energy (Landau): F/kBT = ln [ P (Q) ] 0.04 ev Probability Partition Function (integrated probability) Free Energy [ev] 0.00 ev Angle [degree] Angle [degree]
17 Path collective variables
18 Path collective variables
19 The quest for the right variable(s) : Sketch maps (thanks to Michele Ceriotti, Oxford, for providing figures)
20 Describing structural complexity
21 Dimensionality reduction
22 Dimensionality reduction
23 Dimensionality reduction
24 Dimensionality reduction
25 Dimensionality reduction
26 (Non linear) dimensionality reduction
27 (Non linear) dimensionality reduction
28 (Non linear) dimensionality reduction
29 (Non linear) dimensionality reduction
30 (Non linear) dimensionality reduction
31 Proximity matching
32 Proximity matching
33 Proximity matching
34 Proximity matching
35 Sketch map algorithm (multidimensional scaling)
36 Sketch map algorithm
37 Sketch map algorithm Minimization of the stress function (for a set of landmarks points)
38 Ala12 landscape 24D Gaussian of stdev 0.5 Distribution between pair of ala2 configurations 24D uniform distribution
39 A simplified model for ala12 landscape
40 Projecting the model FES
41 Projecting the model FES
42 Projecting the model FES
43 Sketch map of folded lanscape of ala12
44 Sketch map of folded lanscape of ala12 Is point wise (relative) free energy invariant upon dimensionality reduction? No, only for regions:
45 Sketch map of folded lanscape of ala12
46 Accelerating rare events
47 Accelerating rare events
48 Accelerating rare events
49 Accelerating rare events
50 Accelerating rare events
51 Accelerating rare events
52 Sketch map based metadynamics
53 Sketch map based metadynamics
54 Sketch map based metadynamics
55 Discontinuous trajectories?
56 Discontinuous trajectories?
57 Discontinuous trajectories?
58 Field representation This field replaces the usual representation based on d dimensional points x. The overlap between fields, which measures their similarity, replaces the distance.
59 Field representation
60 Field representation
61 Field overlap metadynamics
62 Field overlap metadynamics
63 Field overlap metadynamics
64 From clusters to defects in bulk
65 From clusters to defects in bulk
66 From clusters to defects in bulk
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