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Scientific Report 2007-2009<br />

Condensed matter physics and biophysics<br />

C22. Computer simulation of rare events and non-equilibrium<br />

phenomena<br />

Computational physics, in particular molecular dynamics<br />

(MD), adopts an atomistic representation of matter,<br />

with model or ab initio interaction potentials, and<br />

solves numerically the evolution equations of the system.<br />

Statistical mechanics links the microscopic evolution to<br />

macroscopic properties and provides the framework to<br />

employ simulations to understand and control materials<br />

by acting at the nano-scale. Our group develops<br />

methods to make simulations more effective theoretical<br />

tools and applies them to investigate condensed matter.<br />

Two important areas of research are rare events and nonequilibrium<br />

MD.<br />

Rare events are characterized by time-scales much<br />

longer than those accessible by brute force MD. In an<br />

appropriate set of collective variables, they can be described<br />

as transitions, over barriers higher than the thermal<br />

energy of the system, among metastable states of<br />

the free energy landscape. Chemical reactions, phase<br />

transformations, nucleation processes, and conformational<br />

changes related to the functionality of proteins<br />

are just a few examples of rare events. In collaboration<br />

with Eric Vanden-Eijnden (Courant Institute for Mathematical<br />

Studies), our group has contributed to establishing<br />

a set of methods that, appropriately combined,<br />

determine the most relevant aspects of rare events: free<br />

energy landscape, rate, mechanism. Recently, we used<br />

these methods to characterize the short-range diffusion<br />

of hydrogen in sodium alanates [1], prototypical materials<br />

for building safe and cost-effective storage devices for<br />

using hydrogen to fuel sustainable vehicles. The same<br />

kinetics of phase transitions in the Ising model [2].<br />

Non-equilibrium MD. Perturbing a system from<br />

equilibrium is a common experimental method to study<br />

its properties. Transport coefficients (shear and bulk<br />

viscosity, thermal conductivities etc.) are often measured<br />

by creating a flow (of momentum, energy, etc.)<br />

in the material. Standard MD cannot be used directly<br />

to simulate a system in non-equilibrium conditions. A<br />

few years ago, we introduced a method, the dynamical<br />

approach to non-equilibrium (D-NEMD), that allows<br />

to obtain rigorous ensemble averages for properties of<br />

a non-stationary system out of equilibrium via MD<br />

trajectories. D-NEMD can be used to study both the<br />

steady state and the transient evolution of a system<br />

out of an initial stationary state and it can be applied<br />

also in the presence of a time-dependent perturbation<br />

that takes the system to a non-equilibrium final state.<br />

Calculations of the bulk viscosity of the triple point<br />

Lennard-Jounes fluid were performed [3] to prove the<br />

accuracy of the method compared with Green-Kubo<br />

estimates. More recently, the method has been applied<br />

Figure 2: Snapshots of the velocity field in the 2d fluid at<br />

successive times during the D-NEMD simulation [4]. The<br />

development of the velocity roll in panel (d) reflects the response<br />

of the system, initially in a steady state under the<br />

effect of a thermal gradient (panel (a)), to the ignition of<br />

gravity. The system here is heated from below.<br />

to study the transient leading to the formation of a<br />

convective cell which appears in a two dimensional fluid<br />

under the combined action of a thermal gradient and of<br />

gravity[4].<br />

Figure 1: CO diffusion in myoglobin. The yellow curves are<br />

the most likely migration paths, while the arrows locate CO<br />

exits to the solvent. The white and black spheres indicate,<br />

respectively, the free energy barriers and minima along the<br />

pathways. The protein backbone is represented as ribbons<br />

and the heme as sticks.<br />

methods were employed to map the exit pathways and<br />

the binding sites of CO in myoglobin and to study the<br />

References<br />

1. M. Monteferrante et al., Sc. Model. Sim. 35, 187 (2008).<br />

2. M. Venturoli et al., J. Math. Chem. 45, 188 (2009).<br />

3. P. L. Palla et al., Phys. Rev. E 78, 021204 (2008).<br />

4. M. L. Mugnai et al., J. Chem. Phys. 131, 064106 (2009).<br />

Authors<br />

G. Ciccotti 7 , S. Caprara, S. Bonella 7 , M. Monteferrante<br />

http://abaddon.phys.uniroma1.it/<br />

<strong>Sapienza</strong> Università di Roma 75 Dipartimento di Fisica

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