# compute mliap command¶

## Syntax¶

```
compute ID group-ID mliap ... keyword values ...
```

ID, group-ID are documented in compute command

mliap = style name of this compute command

two or more keyword/value pairs must be appended

keyword =

*model*or*descriptor*or*gradgradflag**model*values = style style =*linear*or*quadratic*or*mliappy**descriptor*values = style filename style =*sna*filename = name of file containing descriptor definitions*gradgradflag*value = 0/1 toggle gradgrad method for force gradient

## Examples¶

```
compute mliap model linear descriptor sna Ta06A.mliap.descriptor
```

## Description¶

Compute style *mliap* provides a general interface to the gradient
of machine-learning interatomic potentials w.r.t. model parameters.
It is used primarily for calculating the gradient of energy, force, and
stress components w.r.t. model parameters, which is useful when training
mliap pair_style models to match target data.
It provides separate
definitions of the interatomic potential functional form (*model*)
and the geometric quantities that characterize the atomic positions
(*descriptor*). By defining *model* and *descriptor* separately,
it is possible to use many different models with a given descriptor,
or many different descriptors with a given model. Currently, the
compute supports just two models, *linear* and *quadratic*,
and one descriptor, *sna*, the SNAP descriptor used by
pair_style snap, including the linear, quadratic,
and chem variants. Work is currently underway to extend
the interface to handle neural network energy models,
and it is also straightforward to add new descriptor styles.

The compute *mliap* command must be followed by two keywords
*model* and *descriptor* in either order.

The *model* keyword is followed by the model style (*linear*,
*quadratic* or *mliappy*). The *mliappy* model is only available if
LAMMPS is built with the *mliappy* python module. There are
specific installation instructions for that.

The *descriptor* keyword is followed by a descriptor style, and
additional arguments. The compute currently supports two descriptor
styles *sna* and *so3*, but it is is straightforward to add additional
descriptor styles. The SNAP descriptor style *sna* is the same as that
used by pair_style snap, including the linear,
quadratic, and chem variants. A single additional argument specifies
the descriptor filename containing the parameters and setting used by
the SNAP descriptor. The descriptor filename usually ends in the
*.mliap.descriptor* extension. The format of this file is identical to
the descriptor file in the pair_style mliap, and is
described in detail there.

Note

The number of LAMMPS atom types (and the value of *nelems* in the model)
must match the value of *nelems* in the descriptor file.

Compute *mliap* calculates a global array containing gradient information.
The number of columns in the array is \(nelems \times nparams + 1\).
The first row of the array contain the derivative of potential energy w.r.t. to
each parameter and each element. The last six rows
of the array contain the corresponding derivatives of the
virial stress tensor, listed in Voigt notation: *pxx*, *pyy*, *pzz*,
*pyz*, *pxz*, *pxy*. In between the energy and stress rows are
the 3**N* rows containing the derivatives of the force components.
See section below on output for a detailed description of how
rows and columns are ordered.

The element in the last column of each row contains
the potential energy, force, or stress, according to the row.
These quantities correspond to the user-specified reference potential
that must be subtracted from the target data when training a model.
The potential energy calculation uses the built in compute *thermo_pe*.
The stress calculation uses a compute called *mliap_press* that is
automatically created behind the scenes, according to the following
command:

```
compute mliap_press all pressure NULL virial
```

See section below on output for a detailed explanation of the data layout in the global array.

The optional keyword *gradgradflag* controls how the force
gradient is calculated. A value of 1 requires that the model provide
the matrix of double gradients of energy w.r.t. both parameters
and descriptors. For the linear and quadratic models this matrix is
sparse and so is easily calculated and stored. For other models, this
matrix may be prohibitively expensive to calculate and store.
A value of 0 requires that the descriptor provide the derivative
of the descriptors w.r.t. the position of every neighbor atom.
This is not optimal for linear and quadratic models, but may be
a better choice for more complex models.

Atoms not in the group do not contribute to this compute. Neighbor atoms not in the group do not contribute to this compute. The neighbor list needed to compute this quantity is constructed each time the calculation is performed (i.e. each time a snapshot of atoms is dumped). Thus it can be inefficient to compute/dump this quantity too frequently.

Note

If the user-specified reference potentials includes bonded and
non-bonded pairwise interactions, then the settings of
special_bonds command can remove pairwise
interactions between atoms in the same bond, angle, or dihedral. This
is the default setting for the special_bonds
command, and means those pairwise interactions do not appear in the
neighbor list. Because this fix uses the neighbor list, it also means
those pairs will not be included in the calculation. The rerun
command is not an option here, since the reference potential is required
for the last column of the global array. A work-around is to prevent
pairwise interactions from being removed by explicitly adding a
*tiny* positive value for every pairwise interaction that would otherwise be
set to zero in the special_bonds command.

## Output info¶

Compute *mliap* evaluates a global array.
The columns are arranged into
*nelems* blocks, listed in order of element *I*. Each block
contains one column for each of the *nparams* model parameters.
A final column contains the corresponding energy, force component
on an atom, or virial stress component. The rows of the array appear
in the following order:

1 row: Derivatives of potential energy w.r.t. each parameter of each element.

3*

*N*rows: Derivatives of force components. x, y, and z components of force on atom*i*appearing in consecutive rows. The atoms are sorted based on atom ID.6 rows: Derivatives of virial stress tensor w.r.t. each parameter of each element. The ordering of the rows follows Voigt notation:

*pxx*,*pyy*,*pzz*,*pyz*,*pxz*,*pxy*.

These values can be accessed by any command that uses a global array from a compute as input. See the Howto output doc page for an overview of LAMMPS output options. To see how this command can be used within a Python workflow to train machine-learning interatomic potentials, see the examples in FitSNAP.

## Restrictions¶

This compute is part of the ML-IAP package. It is only enabled if
LAMMPS was built with that package. In addition, building LAMMPS with
the ML-IAP package requires building LAMMPS with the ML-SNAP package.
The *mliappy* model also requires building LAMMPS with the PYTHON
package. See the Build package doc page for more
info.

## Default¶

The keyword defaults are gradgradflag = 1