Doc page for compute mliap

This commit is contained in:
Aidan Thompson
2020-07-02 17:09:10 -06:00
parent 07afe1c66d
commit 28bbb6afbc
2 changed files with 158 additions and 4 deletions

154
doc/src/compute_mliap.rst Normal file
View File

@ -0,0 +1,154 @@
.. index:: compute mliap
compute mliap command
====================
Syntax
""""""
.. code-block:: LAMMPS
compute mliap
Examples
""""""""
.. code-block:: LAMMPS
compute mliap model linear nelems nparams descriptor sna InP.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
:doc:`MLIAP pair_style <pair_mliap>` 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
:doc:`pair_style snap <pair_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 a model style, currently limited to
either *linear* or *quadratic*. In both cases,
this is followed by two arguments. *nelems* is the number of elements.
It must be equal to the number of LAMMPS atom types. *nparams*
is the number of parameters per element for this model i.e.
the number of paramter gradients for each element. Note these definitions
are identical to those of *nelems* and *nparams* in the
:doc:`pair_style mliap <pair_mliap>` model file.
The *descriptor* keyword is followed by a descriptor style, and additional arguments.
Currently the only descriptor style is *sna*, indicating the bispectrum component
descriptors used by the Spectral Neighbor Analysis Potential (SNAP) potentials of
:doc:`pair_style snap <pair_snap>`.
The \'p\' in SNAP is dropped, because keywords that match pair_styles are silently stripped
out by the LAMMPS command parser. 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 descriptor file in the
:doc:`pair_style mliap <pair_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 the :math:`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 3\*\ *N* rows containing the derivatives
of the force components.
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 fitting SNAP.
The potential energy calculation uses the built in compute *thermo_pe*.
The stress calculation uses a compute called *snap_press* that is
automatically created behind the scenes, according to the following
command:
.. code-block:: LAMMPS
compute snap_press all pressure NULL virial
See section below on output for a detailed explanation of the data
layout in the global array.
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 you have a bonded system, then the settings of
:doc:`special_bonds <special_bonds>` command can remove pairwise
interactions between atoms in the same bond, angle, or dihedral. This
is the default setting for the :doc:`special_bonds <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. One way to get
around this, is to write a dump file, and use the :doc:`rerun <rerun>`
command to compute the bispectrum components for snapshots in the dump
file. The rerun script can use a :doc:`special_bonds <special_bonds>`
command that includes all pairs in the neighbor list.
----------
**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 per-atom values
from a compute as input. See the :doc:`Howto output <Howto_output>` doc
page for an overview of LAMMPS output options.
Restrictions
""""""""""""
This compute is part of the MLIAP package. It is only enabled if
LAMMPS was built with that package. In addition, building LAMMPS with the MLIAP package
requires building LAMMPS with the SNAP package.
See the :doc:`Build package <Build_package>` doc page for more info.
doc page for more info.
Related commands
""""""""""""""""
:doc:`pair_style snap <pair_mliap>`
**Default:** none

View File

@ -47,9 +47,9 @@ where N is the number of LAMMPS atom types.
The *model* keyword is followed by a model style, currently limited to
either *linear* or *quadratic*. In both cases,
this is followed by a single argument specifying the model filename containing the
linear or quadratic coefficients for a set of elements.
parameters for a set of elements.
The model filename usually ends in the *.mliap.model* extension.
It may contain coefficients for many elements. The only requirement is that it
It may contain parameters for many elements. The only requirement is that it
contain at least those element names appearing in the
*pair_coeff* command.
@ -58,10 +58,10 @@ but follows a strict format after that. The first non-blank non-comment
line must contain two integers:
* nelems = Number of elements
* ncoeff = Number of coefficients
* nparams = Number of parameters
This is followed by one block for each of the *nelem* elements.
Each block consists of *ncoeff* coefficients, one per line.
Each block consists of *nparams* parameters, one per line.
Note that this format is similar, but not identical to that used
for the :doc:`pair_style snap <pair_snap>` coefficient file.
Specifically, the line containing the element weight and radius is omitted,