1549380323-Statistical Mechanics Theory and Molecular Simulation

(jair2018) #1

314 Monte Carlo


Can this algorithm be used in conjunction with hybrid Monte Carlo? Whyor
why not?

7.6. Write a replica exchange Monte Carlo algorithm to sample the Boltzmann
distribution corresponding to a double-well potentialU(x) of the form

U(x) =D 0

(


x^2 −a^2

) 2


fora= 1 andD 0 values of 5 and 10. For each case, optimize the temperature
ladderT 1 ,...,TM, the number of replicasM, and the frequency of exchange
attempts. Use separate Nos ́e-Hoover chains to control the temperatures on
each of theMreplicas. For each simulation, plot the following measure of
convergence:

ζk=

1


Nbins

N∑bins

i=1

|Pk(xi)−Pexact(xi)|,

wherePexact(x) is the exact probability distribution,Pk(x) is the probability
at thekth step of the simulation, andNbinsis the number of bins used in the
calculation of the histogram of the system with temperatureT 1.

∗7.7 Suppose a non-Hamiltonian molecular dynamics algorithm, such as the Nos ́e-
Hoover chain method of Section 4.10, is used to generate paths in the transi-
tion path sampling algorithm. Assuming symmetry of the rule for generating
shooting points, i.e.,τ(yj∆t|xj∆t)/τ(xj∆t|yj∆t), show that the acceptance rule
in eqn. (7.7.15) must be modified to read

Λ[X(T)|Y(T)] =hA(x 0 )hB(xn∆t)min

[


1 ,


f(x 0 )
f(y 0 )

J(yj∆t; y 0 )
J(xj∆t; x 0 )

]


,


whereJ(xt; x 0 ) is the Jacobian of the transformation from x 0 to xt(x 0 ) de-
termined by eqn. (4.9.2).
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