BasicMD
A collection of basic routines for Molecular Dynamics simulations written in Julia. These include
 Euler–Maruyama (EM)
 Random Walk Metropolis (RWM)
 Metropolis Adjusted Langevin (MALA)
 Brünger, Brooks and Karplus (BBK)
 GrønbechJensen and Farago (GJF)
 ABOBA, BAOAB
 Hamiltonian/Hybrid Monte Carlo (HMC)
This is intended to be a collection for small scale problems and code development. Larger problems will best be handled with LAMMPS or OpenMM
Overview
This module has been significantly reorganized to better take advantage of
multiple dispatch. The older versions are still available in deprecated.jl
as a part of the module OldBasicMD
, if needed.
This module can be added with the command:
(@v1.XYZ) pkg> add BasicMD
This package was previously named JuBasicMD
, but has since been renamed to
conform with Julia package naming recommendations.
Sampling
Each sampler is first initialized as
> sampler = RWM(V, β, Δt);
or
> sampler = HMC(V, gradV!, β, M, Δt, nΔt);
depending on the type of sampler that is chosen. Information about what is needed to define each sampler can be obtained in the REPL by calling ?
with the sampler name (i.e., ?HMC
).
Once a sampler is constructed, sampling is then performed with either sample_trajectory!
or sample_trajectory
. The former performs an in place transformation on the input state, while the latter records values along the trajectory:
sample_trajectory!(X, sampler, options=opts);
and
Xvals = sample_trajectory(X₀, sampler);
For Metropolis methods, the latter form also returns the running acceptance rate,
Xvals, avals = sample_trajectory(X₀, sampler);
The sample_observables
routine is also included to allow for the computation of the observables directly. This avoids storing an entire trajectory, which may be computationally expensive. Given some set of observables, f₁
, f₂
, etc., storing these as a tuple, obs=(f₁,f₂)
, they are computed directly with the command X
obs_vals = sample_observables(X₀ , sampler, obs)
This can otpionaly take the MDOptions
in as an argument.
MDOptions
The number of iterations performed is determined by the optional options
argument. This takes as its argument a data structure which is formatted using
the MDOptions
function:
opts = MDOptions(n_iters=n_iters,n_save_iters=n_save_iters)
n_iters
is the number of iterations performed by the sampler. n_save_iters
is the frequency with which samples are saved. If n_save_iters=1, every
iteration is saved. If n_save_iters=n_iters, only the final iteration is saved.
All of these methods have two versions, Integrator
and Integrator!
. The Integrator!
routine performs an in place transformation on the starting position (and momentum, where appropriate), while Integrator
copies over the initial condition. Integrator
also accepts the optional argument return_trajectory=true/false
, which will return the entire time series data.
Examples
Example codes include:
 1D Harmonic potential
 1D Double Well Potential
 2D Muller Potential
These examples assume that the active environment includes the BasicMD
package.
Caveats
 The code assumes that the state space is vector valued. Thus, even if the problem is one dimensional, you should have initial points and functions formatted appropriately, i.e.
> x0 = [1.0]

The mass matrix,
M
, used in the inertial Langevin integrators and Hamiltonian methods must be diagonal and provided either as a scalar (in the isotropic case) or a vector (in the anisotropic case). This restriction is in place for performance purposes. 
BBK is currently implemented for a slightly different version of the Langevin SDE than ABOBA/BAOAB. BBK requires inverting the mass matrix while ABOBA/BAOAB require its square root.

GJF is implemented in (q,p) coordinates as opposed to (x,v) coordinates. Consequently, the mass term appears slightly differently than in the literature.
Both will sample the associated Boltzmann distribution, but the SDE trajectories will differ when M≂̸I
.
TO DO
Before reaching a 1.0, the goals are:
 Include GHMC samplers.
 Add to the package registry
Acknowledgements
This work was supported in part by the US National Science Foundation Grant DMS1818716.