Time-propagation algorithms in molecular dynamics

In molecular dynamics simulations, the ionic positions [math]\displaystyle{ \mathbf{r}_{i}(t) }[/math] and velocities [math]\displaystyle{ \mathbf{v}_{i}(t) }[/math] are monitored as functions of time [math]\displaystyle{ t }[/math]. This time dependence is obtained by integrating Newton's equations of motion. When integrating the equations of motions it is important to use symplectic algorithms which conserve the phase-space volume. To solve the equations of motion under symplectic conditions, various integration algorithms have been developed. The time dependence of a particle can be expressed in a Taylor expansion

[math]\displaystyle{ \mathbf{r}_{i}(t+\Delta t) = \mathbf{r}_{i}(t) + \mathbf{v}_{i}(t)\Delta t + \frac{\mathbf{F}_{i}}{2m}(t)\Delta t^{2} + \frac{\partial^{3} \mathbf{r}_{i}(t)}{\partial t^{3}}\Delta t^{3} + \mathcal{O}(\Delta t^{4}) }[/math]

A backward propagation in time by a time step [math]\displaystyle{ \Delta t }[/math] can be obtained in a similar way

[math]\displaystyle{ \mathbf{r}_{i}(t-\Delta t) = \mathbf{r}_{i}(t) - \mathbf{v}_{i}(t)\Delta t + \frac{\mathbf{F}_{i}}{2m}(t)\Delta t^{2} - \frac{\partial^{3} \mathbf{r}_{i}(t)}{\partial t^{3}}\Delta t^{3} + \mathcal{O}(\Delta t^{4}) }[/math]

Adding these two equation gives and rearrangement gives the Verlet algorithm

[math]\displaystyle{ \mathbf{r}_{i}(t+\Delta t) = 2\mathbf{r}_{i}(t)-\mathbf{r}_{i}(t-\Delta t)+\frac{\mathbf{F}_{i}}{2m}(t)\Delta t^{2}+\mathcal{O}(\Delta t ^{3}) }[/math]

The Verlet algorithm can be rearranged to the Velocity-Verlet algorithm by inserting [math]\displaystyle{ \mathbf{v}_{i}(t)=\frac{\mathbf{r}_{i}(t)-\mathbf{r}_{i}(t-\Delta t)}{\Delta t} }[/math]

[math]\displaystyle{ \mathbf{r}_{i}(t+\Delta t) = \mathbf{r}_{i}(t)+ \mathbf{v}_{i}(t)\Delta t+\frac{\mathbf{F}_{i}}{2m}(t)\Delta t^{2}. }[/math]

Velocity-Verlet integration scheme

The Velocity-Verlet algorithm can be decomposed into the following steps:

1. [math]\displaystyle{ \mathbf{v}_{i}(t + \frac{1}{2}\Delta t)=\mathbf{v}_{i}(t)+\frac{\mathbf{F}_{i}(t)}{2m_{i}}\Delta t }[/math]
2. [math]\displaystyle{ \mathbf{r}_{i}(t + \Delta t) = \mathbf{r}_{i}(t) + \mathbf{v}_{i}(t + \frac{1}{2}\Delta t)\Delta t }[/math]
3. compute forces [math]\displaystyle{ \mathbf{F}_{i}(t) }[/math] from density functional theory or machine learning
4. [math]\displaystyle{ \mathbf{v}_{i}(t + \Delta t)=\mathbf{v}_{i}(t+\frac{1}{2}\Delta t)+\frac{\mathbf{F}_{i}(t+\Delta t)}{2m_{i}}\Delta t }[/math]

From these equations it can be seen that the velocity and the position vectors are synchronous in time.

Leap-Frog integration scheme

Another form of the Verlet algorithm can be written in the form of the Leap-Frog algorithm. The Leap-Frog algorithm consists of the following steps:

1. compute forces [math]\displaystyle{ \mathbf{F}_{i}(t) }[/math] from density functional theory or machine learning
2. [math]\displaystyle{ \mathbf{v}_{i}(t + \frac{1}{2}\Delta t)=\mathbf{v}_{i}(t- \frac{1}{2}\Delta t)+\frac{\mathbf{F}_{i}(t)}{m_{i}}\Delta t }[/math]
3. [math]\displaystyle{ \mathbf{r}_{i}(t + \Delta t) = \mathbf{r}_{i}(t) + \mathbf{v}_{i}(t + \frac{1}{2}\Delta t)\Delta t }[/math]

In this form the velocity and the position vectors are asynchronous in time.

Thermostats and used integrators

MDALGO	thermostat	integration algorithm
0	Nosé-Hoover	Velocity-Verlet
1	Andersen	Leap-Frog
2	Nosé-Hoover	Leap-Frog
3	Langevin	Velocity-Verlet
4	Nosé-Hoover chain	Velocity-Verlet
5	CSVR	Leap-Frog
5	Multiple Andersen	Leap-Frog

Related tags and articles

IBRION, MDALGO, Thermostats