Manual

Please consult with Features for an overview of MLatom capabilities. This page provides details on how to use MLatom for various types of calculations.

Installation and usage

Installation with pip

One way to install MLatom is to use command:

python3 -m pip install -U MLatom

Then you can use MLatom by simply running command:

mlatom [options]

Installation from a zipped package

Alternatively, you can download a zipped package with MLatomPy (requires Python 3.7+) and a statically compiled binary of MLatomF and cs.so for Linux systems. These files can be unpacked in any directory and used directly without any modifications to the environment variables etc. You may need to make files executable by using command line option chmod +x MLatom.py MLatomF cs.so.

You can also add your MLatom path into the $PATH variable with the command (in bash):

export PATH=$PATH:/path/to/MLatom

It is convenient to add this line to .bashrc file.

Installation instructions for enabling interfaced third-party programs, see below.

To run MLatom provide a path to MLatom.py and the necessary command-line options (see in the next section), i.e. in your terminal type:

$pathToMLatom/MLatom.py [command-line options or the name of an input file with options]

In the following, notation mlatom (it is useful to setup such an alias in your shell) is used instead of $pathToMLatom/MLatom.py.

Running MLatom

All options are case insensitive, i.e. you can type either

mlatom help

or

mlatom Help

with the same result (the command will print available options on your computer screen).

In order to run MLatom you have to have several input files as described below. Note that input and output file names are case sensitive! For example, xyz.dat and XYZ.dat are two different file names.

By default, MLatom will use all available threads on your computer. If you want to limit the number of threads to N threads, you can use option nthreads=N.

Getting Help and List of Options for a Current Version

You can directly request your current version of MLatom to print its available options with the command:

mlatom help for an overall help

Input

MLatom can be run by providing it with the input file. Example:

mlatom myinputfile.inp

myinputfile.inp can look like this (with comments followed after # symbol):

estAccMLmodel # one command on one line
# Lines with comments etc.
# createMLmodel # Requests creating ML model
# MLmodelOut=mlmod_E_FCI_Gaussian_20random.unf # saves the model to file
XfileIn=R_451.dat Yfile=E_FCI_451.dat # Several commands on one line
sigma=opt # Requests optimizing sigma parameter

All above options can be given directly to MLatom in a single command:

mlatom estAccMLmodel XfileIn=R_451.dat Yfile=E_FCI_451.dat sigma=opt

Along with options MLatom needs to read various files from disk depending on the task. File names should be specified using the following options:

  • XYZfile=[name of file with molecular XYZ coordinates]
  • XfileIn=[name of file with molecular descriptor (ML input) vectors]
  • Yfile=[name of file with reference values]
  • Yb=[file name with the data obtained with the baseline method for Δ-ML]
  • Yt=[file name with the reference data obtained with the target method for Δ-ML]
  • MLmodelIn=[name of file with ML model]
  • iTrainIn=[name of file with indices of training points]
  • iTestIn=[name of file with indices of test points]
  • iSubtrainIn=[name of file with indices of sub-training points]
  • iValidateIn=[name of file with indices of validation points]
  • iCVtestPrefIn=[prefix of names of files with indices for CVtest]
  • iCVoptPrefIn=[prefix of names of files with indices for CVopt]

In the requested input file does not exist, MLatom will terminate with the request to provide it.  This check is not performed for files with indices involved in cross-validation.

File extensions are arbitrary.

It is sometimes useful to use only part of the big data set. This can be requested by using option Nuse=N, requesting that only N first entries of input files will be used.

File Formats

XYZfile option requires file with XYZ coordinates of molecules one after another, with first line specifying number of atoms in a molecule followed by one blank line and then by Cartesian coordinates of nuclei, e.g. for three molecules:

5

C   0.000  0.000  0.000
Cl  1.776  0.000  0.000
H  -0.342  1.027  0.000
H  -0.342 -0.513 -0.890
H  -0.342 -0.513  0.890
5

C   0.000  0.000  0.000
Cl  1.776  0.000  0.000
H  -0.343  1.027  0.000
H  -0.342 -0.513 -0.890
H  -0.342 -0.513  0.890
5

C   0.000  0.000  0.000
Cl  1.776  0.000  0.000
H  -0.339  1.028  0.000
H  -0.342 -0.513 -0.890
H  -0.342 -0.513  0.890

Nuclear charges can be used instead of element symbols. Coordinates are given in Å.

XfileIn requires file with input vectors, where each vector should be on one line, e.g.:

1.0093 1.0009 1.0009
1.0080 1.0229 1.0004
1.0009 0.9947 0.9738

Yfile, Yb, and Yt requires a file with one reference datum per line, e.g.:

 6.349
23.852
60.872

MLmodelIn requires a file with ML model generated by MLatom, version 1.0 or version 1.1.

Files with indices should contain one index per line.

Output

MLatom prints summary of its calculations to the standard output, i.e. it is recommended to redirect it to a file, e.g.:

mlatom help > mlatom.out

It can also write files to the disk depending on the task. File names should be specified using the following options:

  • XfileOut=[name of file to write input vectors to]
  • XYZsortedFileOut=[name of file to write sorted XYZ coordinates]
  • MLmodelOut=[name of file to write ML model to]
  • YestFile=[name of file with values predicted by ML or with corrections predicted by Δ-ML]
  • YestT=[file name with the Δ-ML predictions estimating the target method]
  • YgradEstFile=[name of file to write gradients predicted by ML to]
  • iTrainOut=[name of file to write training point indices to]
  • iTestOut=[name of file to write test point indices to]
  • iSubtrainOut=[name of file to write sub-training point indices to]
  • iValidateOut=[name of file to write validation point indices to]

If output file with the same name already exists, MLatom will terminate with the request to remove or rename it. This check is not performed for files with indices generated during cross-validation.

File extensions are arbitrary.

Option XYZsortedFileOut only works with optionsmolDescriptor=RE molDescrType=sorted. Option permInvNuclei=[atomic indices separated by '-']can be provided to specify which atoms to sort.

You can request additional output with debug option. It will e.g. print the regression coefficients α when using the ML model.

ML Tasks

estAccMLmodel

You can estimate accuracy of ML models, i.e. estimate its generalization error by using option estAccMLmodel with other options:

mlatom estAccMLmodel [other options]

For default settings and other mandatory options see the corresponding sections below, specically section Model Validation.

Example:

mlatom estAccMLmodel Yfile=y.dat XYZfile=xyz.dat kernel=Gaussian sigma=opt lambda=opt

This command will request estimation of the generalization error of an ML model for molecules provided in Cartesian coordinates in xyz.dat file and reference data in y.dat file. Gaussian kernel will be used and hyperparameters σ and λ will be optimized.

createMLmodel

In order to create an ML model and save it to a file on a disk, use option createMLmodel:

mlatom createMLmodel [other options]

For both estAccMLmodel and createMLmodel additional input option Yfile should be used (see Section Input).

Example:

mlatom createMLmodel Yfile=y.dat XYZfile=xyz.dat MLmodelOut=mlmod.unf kernel=Gaussian sigma=opt lambda=opt

This command will request creating an ML model for molecules provided in Cartesian coordinates in xyz.dat file and reference data in y.dat file and save it to mlmod.unf file. Gaussian kernel will be used and hyperparameters σ and λ will be optimized.

useMLmodel

Loading existing ML model from a file and performing ML calculations with this model can be done with option useMLmodel:

mlatom useMLmodel [other options]

For useMLmodel additional input option MLmodelIn should be used (see Section Input).

Example:

mlatom useMLmodel MLmodelIn=mlmod.unf XYZfile=xyz.dat YestFile=yest.dat

This command will request making predictions with an ML model read from mlmod.unf file for molecules provided in Cartesian coordinates in xyz.dat file and save predicted values in yest.dat file. Program will output summary of the loaded model, such as used kernel and values of hyperparameters used to create it.

deltaLearn

All above ML operations can be also performed within Δ-ML approach requested by deltaLearn. The baseline values should be provided using Yb option. The target values for training should be provided with Yt option. The Δ-ML can be saved to file specified with YestT, while the corrections themselves to file specified with YestFile.

selfCorrect

Self-correction can be requested by option selfCorrect. Currently it works only with four layers and file with reference values should be named y.dat.

learningCurve

Another ML operation, the task learning curve can automatically train models and estimate their accuracy, then give a summary file in comma separated values (CSV) format. Use learningCurve option to perform this task. The options for this task, just as those for estAccMLmodel, except for the Ntrain which is replaced by lcNtrains and a extra option lcNrepeats. As their names show, the choice of traning set sizes and number of repeats are defined in these two new options.

Example:

mlatom learningCurve Yfile=y.dat XYZfile=xyz.dat kernel=Gaussian sigma=opt lambda=opt lcNtrains=100,250,500,1000,2500,5000,10000 lcNrepeats=64,32,16,8,4,2,1

With this command training set sizes lited in lcNtrains will be tested repeatedly for 64, 32, 16, 8, 4, 2, 1 time(s), respectively. All data generated (including csv reports) will be stored in the folder learningCurve under current directory.

crossSection

MLatom can accelerate the calculation of cross-section with Nuclear Ensemble Approach: paper link>>>

Newton-X and Gaussian should be available.

Requirements for ML-NEA

To run ML-NEA calculations of absorption cross sections, you also need to define some environment:

  1. Install Newton-X (NX)
  2. use export NX=/path/to/Newton-X to define the $NX
  3. install matplotlib with the command python3 -m pip install matplotlib
  4. Have Gaussian installed.

usage: MLatom.py cross-section [optional arguments] 

optional arguments:

  • Nexcitations=N number of excited states to calculate.
    (default=3)
  • nQMpoints=N user-defined number of QM calculations for training ML. (default=0, number of QM calculations will be determined iteratively)
  • plotQCNEA requests plotting QC-NEA cross section
  • deltaQCNEA=float define the broadening parameter of QC-NEA cross section
  • plotQCSPC requests plotting cross section obtained via single point convolution

advanced arguments (not recommended to modify):

  • nMaxPoints=N maximum number of QC calculations in the iterative
    procedure. (default=10000)
  • MLpoints=N number of ML calculations.
    (default=50000)

environment variables

  • $NX Newton-X environment
  • Environment for calculations with Gaussian program package. details>>>

In bash, you can for example use the following command (provide the correct path to Newton-X bin directory):
export NX=/home/users/bxxue/NX/bin

required files:

  1. mandatory file
    1. gaussian_optfreq.com input file for Gaussian opt and freq calculations Alternatively, files eq.xyz (XYZ file with equilibrium, optimized, geometry) and nea_geoms.xyz (file with all geometries in nuclear ensemble) can be provided.
    2. gaussian_ef.com template file for calculating excitation energies and oscillator strengths with Gaussian. 
  2. optional file
    1. cross-section_ref.dat reference cross section file calculated in format similar to that of Newton-X (1st column: DE/eV; 2nd column: lambda/nm; 3rd column: sigma/A^2)
    2. eq.xyz file with optimized geometry (has to be used together with nea_geoms.xyz)
    3. nea_geoms.xyz file with all geometries in nuclear ensemble (has to be used together with eq.xyz)
    4. E1.dat  E2.dat ... and f1.dat  f2.dat ... files that stores the exciting energy and oscillator strength per line which correspond to nea_geoms.xyz.

output files:

  1. cross-section/cross-section_ml-nea.dat: cross-section spectra calculated with ML-NEA method
  2. cross-section/cross-section_qc-nea.dat: cross-section spectra calculated with QC-NEA method
  3. cross-section/cross-section_spc.dat: cross-section spectra calculated with single-point-convolution
  4. cross-section/plot.png: the plotting that contains cross-section calculated with different kinds of method.

Data Set Tasks

XYZ2X

Converting XYZ coordinates into an input vector (molecular descriptor) for ML

You can use XYZ2X option to convert XYZ coordinates of a series of molecules provided in file requested by option XYZfile=[filename] to the molecular descriptor (input) vectors for ML calculations saved in file requested by option XfileOut=[filename] in estAccMLmodel with other options.

Example:

mlatom XYZ2X XYZfile=xyz.dat XfileOut=x.dat

Given a data set of molecules either in XYZ format or in molecular descriptor form, you can sample their subsets (e.g. the training and test sets), by using sample option:

mlatom sample [other options]

Basically, one can use this option to generate indices of the training, test, sub-training, and validation sets without performing ML calculations. Thus, other options used for Model Validation and Hyperparameter Tuning are applicable.

analyze

This task requires reference data and estimated data to give a statistical report.

For reference data at least one of these arguments below is required:
Yfile=S YgradXYZfile=S 

And for estimated data, correspondingly:
YestFile=S YgradXYZestFile=S

Example:

MLatom.py analyze Yfile=en.dat YestFile=enest.dat

sample

You can specify a type of sampling into the training and other sets using option sampling=[type of sampling]. Available types of sampling are: none, random, user-defined, structure-based, farthest-point.

  • random: default. Simple random sampling
  • user-defined: requests MLatom to read indices for the training, test, and, if necessary, for the subtraining and validation sets from files defined by options iTrainIn, iTestIn, iSubtrainIn, iValidateIn. Corresponding options Ntrain, Ntest, Nsubtrain, and Nvalidate can be used as well. Cross-validation parts can be read in from files with names starting with prefixes specified by options iCVtestPrefIn and iCVoptPrefIn.
  • structure-based: performs structure-based sampling. Only works with  molDescriptor=RE.
  • farthest-point: farthest-point traversal iterative procedure, which starts from two points farthest apart
  • none: simply splitting the data set into the training, test, and, if necessary, training set into the subtraining and validation sets (in this order) without changing the order of indices

Structure-based Sampling from Sliced Data

Options for sorting geometries by the Euclidean distance of their corresponding ML input vector to the input vector of the equilibrium geometry and slicing the ordered data set into requested number of regions of the same size:

  • slice: slice data set
    • nslices=[number of slices] [default = 3]
    • XfileIn=[file with input vectors X]
    • eqXfileIn=[file S with input vector for the equilibrium]

This options create files xordered.dat (input vectors sorted by distance), indices_ordered.dat (indices of ordered data set wrt the original data set), and distances_ordered.dat (list of Euclidean distances of ordered data points to the equilibrium). They also create directories slice1, slice2 etc. Each of them contains three files: x.dat, slice_indices.dat, and slice_distances.dat that are slices of the corresponding files of the entire data set.

Options to perform structure-based sampling to sample the desired number of data from each slice:

  • sampleFromSlices: sample from each slice
    • nslices=[number of slices] [default = 3]
    • Ntrain=[total integer number N of training points from all slices]

This command creates itrain.dat files with training set indices in each slice[1-...] directory. Note: it is possible to modify sliceData.py script to submit the jobs in parallel to the queue.

To merge sampled indices from all slices into indices files for the training, test, sub-training, and validation sets using the same order of data points as in original data set:

  • mergeSlices: merges indices from slices [see sliceData help]
    • nslices=[number of slices] [default = 3]
    • Ntrain=[total integer number N of training points from all slices]

This command creates four files with indices: itrain.dat (with 4480 points for training), isubtrain.dat (with 80% of training points also chosen using structure-based sampling), itest.dat, and ivalidate.dat.

ML Algorithm

KRR

You can use the following options for performing kernel ridge regression calculations:

  • lambda=R: sets regularization parameter λ to a floating-point number R. Default value is 0.0. You can request optimization of this parameter with lambda=opt, see below for more options related to hyperparameter tuning.
  • kernel=[type of kernel]: requests using one of the available types of kernel, which are self-explaining.
    • kernel=Gaussian (set by default).
    • kernel=Laplacian
    • kernel=exponential
    • kernel=Matern

Kernel width σ is a parameter, which can be also changed by the user using the following option:

  • sigma=R: sets σ to a floating-point number R. You can request optimization of this parameter with sigma=opt, see below for more options related to hyperparameter tuning. Default values are different for different kernels:
    • sigma=100.0 for the Gaussian and Matérn kernels
    • sigma=800.0 for the Laplacian and exponential kernels

In case of Matérn kernel, there is an additional integer parameter n, which is set by default to 2, and can be changed to an integer number N using option nn=N.

Permutation of atomic indices (especially of the same element) should not change predictions made by ML model. This can be achieved by using permutationally invariant kernel (preferred) or sorting indices of atoms in some unique way (described below in Section Molecular Descriptors). Calculations with permutationally invariant kernel can be requested by using optionpermInvKerneland:

  • by providing file with molecular geometries in XYZ format and specifying atoms to permute using options permInvNuclei=[atomic indices separated by '-'] molDescrType=permuted.
  • by providing file with input vectors and specifying number of permutations using option Nperm=[number of permutations]. Each line of input vector file must contain input vectors with molecular descriptors concatenated for all atomic permutation of a single geometry.

Molecular Descriptors

molDescriptor=[molecular descriptor]: requests using one of the available molecular descriptors:

  • molDescriptor=CM: requests using the Coulomb matrix
  • molDescriptor=RE: requests using the RE descriptor (normalized inverted internuclear distances; default). It is a vector {req/r}, where r is an internuclear distance in a current molecule and req is an internuclear distance in the equilibrium (or other reference) structure. Equilibrium structure should be provided in a file named ‘eq.xyz’ in XYZ format.

Variants of these descriptors can be requested by option molDescrType=[type]:

  • molDescrType=unsorted: uses the same order of atoms as in input file with XYZ coordinates of molecules. Default for molDescriptor=RE.
  • molDescrType=sorted : sorts atoms and ensures permutation invariance on input vector level (especially useful for sorting; when possible, permutationally invariant kernel should be prefered for ML calculations):
    • sorts Coulomb matrix by norms of its rows formolDescriptor=CM (default for Coulomb matrix).
    • sorts atoms by the sum of their nuclear repulsions to all other atoms for molDescriptor=RE. Atoms to sort can be specified by option permInvNuclei=[atomic indices separated by '-']. If option permInvNucleiis not used, all atoms are sorted.
  • molDescrType=permuted : generate multiple XYZ structures of a single geometry by permuting atoms specified with option permInvNuclei=[atomic indices separated by '-'], convert each of them to molecular descriptor, and concatenate the latter into a single input vector. This option is necessary to run calculations with permutationally invariant kernel.

KREG model

The KREG model is the default ML model of MLatom. It is KRR ML algorithm with the Gaussian kernel function and RE molecular descriptor.

Model Validation

ML model can be validated (generalization error can be estimated) in several ways:

  • on a hold-out test set not used for training. Both training and test sets can be sampled in one of the ways described above. Number of points in the sub-training and validation sets is set by options Ntrain=Rand Ntest=R, respectively. If R is an integer larger or equal to 1, this number of points is sampled from the data set. If R is a floating-point number less than 1.0, it is used to define a fraction of the data set points to sample. By default, 80% of the data set points are used as the training set and remaining 20% as the test set;
  • by performing N-fold cross-validation. User can request this procedure using option CVtest and define the number of folds N by using option NcvTestFolds=N. By default, 5-fold cross-validation is used. If N is equal to the number of data points, leave-one-out cross-validation is performed. Only random or no sampling can be used for cross-validation.
  • by performing leave-one-out cross-validation. User can request this procedure using option LOOtest. Only random or no sampling can be used.

Hyperparameter Tuning

Gaussian, Laplacian, exponential, and Matérn kernels have σ and λ tunable hyperparameters. Their optimization can be requested with options sigma=opt and lambda=opt, respectively.

MLatom can tune hyperparameters either to minimize mean absolute error or to minimize root-mean-square error as defined by option using either option minimizeError=MAE or minimizeError=RMSE (default), respectively. Hyperparameters can be tuned to minimize

  • the error of the ML model trained on the sub-training set in a hold-out validation set. Both sub-training and validation sets can be sampled from the training set in one of the ways described above. Number of points in the sub-training and validation sets is set by options Nsubtrain=Rand Nvalidate=R, respectively. If R is an integer larger or equal to 1, this number of points is sampled from the training set. If R is a floating-point number less than 1.0, it is used to define a fraction of the training set points to sample. By default, 80% of the training set points are used as the sub-training set and remaining 20% as the validation set;
  • N-fold cross-validation error. User can request this procedure using option CVopt and define the number of folds N by using option NcvOptFolds=N. By default, 5-fold cross-validation is used. If N is equal to the number of data points, leave-one-out cross-validation is performed. Only random or no sampling can be used for cross-validation.
  • leave-one-out cross-validation error. User can request this procedure using option LOOopt. Only random or no sampling can be used.

MLatom searches optimal parameters on a logarithmic grid. After best parameters found in the first iteration, MLatom can perform more iterations of a logarithmic grid search. Number of iterations is controlled by lgOptDepth=N keyword with N=3 by default. User can adjust number of grid points, starting and finishing points on the grid by using the following options for

  • λ hyperparameter:
    • NlgLambda=N defines the number of points on the logarithmic grid (base 2). By default 6 points are used.
    • lgLambdaL=R Lowest value of log2 λ for a logarithmic grid optimization of lambda. Default value is -35.0.
    • lgLambdaH=R Highest value of log2 λ for a logarithmic grid optimization of lambda. Default value is -6.0.
  • σ hyperparameter:
    • NlgSigma=N defines the number of points on the logarithmic grid (base 2). By default 6 points are used.
    • lgSigmaL=R Lowest value of log2 λ for a logarithmic grid optimization of lambda. Default value is 2.0 for the Gaussian and Matérn kernels, 5.0 for the Laplacian and exponential kernels.
    • lgSigmaH=R Highest value of log2 λ for a logarithmic grid optimization of lambda. Default value is 9.0 for the Gaussian and Matérn kernels, 12.0 for the Laplacian and exponential kernels.

Another approach for hyperparameter tuning in MLatom is using the hyperopt interface (https://github.com/hyperopt/hyperopt). hyperopt is a package that provide general solution of the optimization problem. To trigger this approach in MLatom, all you need is just substituding numeric vaule(s) you want to optimize with function-like hyperopt.xxx(), which has several options available for the triple x:

  • hyperopt.uniform(lb,ub): linear search space from lower bound lb, and upper bound ub.
  • hyperopt.loguniform(lb,ub): logarithmic search space, base 2.
  • hyperopt.qunifrom(lb,ub,q): discrete linear space, rounded by q.

The maximum number of attemps is defined by option hyperopt.max_evals=N, and the type of optimization loss is determined by hyperopt.losstype=S, where S can be geomean(default) or weighted. If the latter is chosen, the weight for gradients can be defined by hyperopt.w_grad.

To enable hyperopt, please run pip install hyperopt to install hyperopt.

First Derivatives

MLatom can be also used to calculate first derivatives given a file with an existing ML model. In order to request such calculations, simply add to the options used with useMLmodel option additional output option YgradEstFile=[name of a file to save gradients in] or YgradXYZestFile=[name of a file to save XYZ gradients in].

Example:

mlatom useMLmodel MLmodelIn=mlmod.unf XYZfile=xyz.dat YgradXYZestFile=ygradest.dat

This command will request making predictions with an ML model read from mlmod.unf file for molecules provided in Cartesian coordinates in xyz.dat file and save predicted gradients in ygradest.dat file.

Interfaces to third-party programs

MLatom  aslo provides interfaces to some third-party software. 

To use third-party software, MLprog should be set to a third-party software.

Currently implemented programs and the default choises when MLmodelType and MLprog is difined:

  Supported ML model types and default programs:
 
  +-------------+----------------+ 
  | MLmodelType | default MLprog | 
  +-------------+----------------+ 
  | KREG        | MLatomF        | 
  +-------------+----------------+ 
  | sGDML       | sGDML          | 
  +-------------+----------- ----+ 
  | GAP-SOAP    | GAP            | 
  +-------------+----------------+ 
  | PhysNet     | PhysNet        | 
  +-------------+----------------+ 
  | DeepPot-SE  | DeePMD-kit     | 
  +-------------+----------------+ 
  | ANI         | TorchANI       | 
  +-------------+----------------+ 
 
 Supported interfaces with default and tested ML model types:
 
  +------------+----------------------+
  | MLprog     | MLmodelType          |
  +------------+----------------------+
  | MLatomF    | KREG [default]       |
  |            | see                  |
  |            | MLatom.py KRR help   |
  +------------+----------------------+
  | sGDML      | sGDML [default]      |
  |            | GDML                 |
  +------------+----------------------+
  | GAP        | GAP-SOAP             |
  +------------+----------------------+
  | PhysNet    | PhysNet              |
  +------------+----------------------+
  | DeePMD-kit | DeepPot-SE [default] |
  |            | DPMD                 |
  +------------+----------------------+
  | TorchANI   | ANI [default]        |
  +------------+----------------------+

DeePMD-kit

Installation

1. download installer for DeePMD-kit from GitHub https://github.com/deepmodeling/deepmd-kit/releases (tested v1.2.2)

2. run installer

3. add environmetal variable $DeePMDkit that point to the where dp binary is located (bin/ in your installation directory)

e.g. export DeePMDkit=/export/home/fcge/deepmd-kit-1.2/bin

usage

Set MLprog=DeePMD-kitto enable the interface.

options

Expressions like deepmd.xxx.xxx=X specify arguments for DeePMD, follows the structure of DeePMD’s json input file.

For example:   

deepmd.training.stop_batch=N is an equivalent of

  {                    
    ...                
    "training": {      
      ...              
      "stop_batch": N  
      ...              
    }                  
    ...                
  }                     in DeePMD-kit’s json input.
 

In addition, option deepmd.input=S intakes a input json file S as a template. Final input file will be generated base on it with deepmd.xxx.xxx=X options (if any). Check default template file bin/interfaces/DeePMDkit/template.json for defualt values

GAP and QUIP

Installation

1. compile QUIP and GAP from source

1.1 install prerequisites

sudo apt-get install gcc gfortran python python-pip libblas-dev liblapack-dev (for system uses apt, do equivalent for your OS)
pip install numpy ase f90wrap

1.2 get source code of QUIP and GAP

git clone --recursive https://github.com/libAtoms/QUIP.git

Get source code of GAP from http://www.libatoms.org/gap/gap_download.html (form-filling required).
Then put source code in QUIP/src/.

1.3 compile

cd QUIP
export QUIP_ARCH=linux_x86_64_gfortran_openmp # enable multi-threading, use 'export QUIP_ARCH=linux_x86_64_gfortran' if no OpenMP thus no MT capability
export QUIPPY_INSTALL_OPTS=--user # omit for a system-wide installation
make config 

Enter Y for gap or edit build/linux_x86_64_gfortran/Makefile.inc  with HAVE_GAP=1, then:
make

Built binaries are in QUIP/build/linux_x86_64_gfortran/quip and QUIP/build/linux_x86_64_gfortran/gap_fit.

2. add environmetal variable $quip and $gap_fit for quip and gap_fit

e.g. export quip='/export/home/fcge/GAP-SOAP/QUIP/build/linux_x86_64_gfortran_openmp/quip'
export gap_fit='/export/home/fcge/GAP-SOAP/QUIP/build/linux_x86_64_gfortran_openmp/gap_fit'

visit https://libatoms.github.io/GAP/index.html for more info.

usage

Set MLprog=GAPto enable the interface.

options

gapfit.xxx=x xxx could be any option for gap_fit (e.g. default_sigma).
Note that there’s no need to set at_file and gp_file.
gapfit.gap.xxx=x xxx could be any option for gap.

Arguments with their default values:
 
gapfit.default_sigma={0.0005,0.001,0,0} hyperparameter sigmas for energies, forces, virals and hessians
gapfit.e0_method=average method for determining e0  
gapfit.gap.type=soap descriptor type
gapfit.gap.l_max=6 max number of angular basis functions  
gapfit.gap.n_max=6 max number of radial basis functions   
gapfit.gap.atom_sigma=0.5 hyperparameter for Gaussain smearing of atom density
gapfit.gap.zeta=4 hyperparameter for kernel sensitivity  
gapfit.gap.cutoff=6.0 cutoff radius of local environment     
gapfit.gap.cutoff_transition_width=0.5 cutoff transition width              
gapfit.gap.delta=1 hyperparameter delta for kernel scaling

TorchANI

Installation

1. install Numpy and nightly version of PyTorch

pip install numpy
pip install --pre torch torchvision -f \ https://download.pytorch.org/whl/nightly/cu100/torch_nightly.html

2. install TorchANI

pip install torchani

Visit https://aiqm.github.io/torchani/ for more info.

usage

Set MLprog=TorchANIto enable the interface.

options

Arguments with their default values:

ani.batch_size=8 batch size                           
ani.max_epochs=10000000 max epochs                           
ani.early_stopping_learning_rate=0.00001 learning rate that triggers early-stopping                      
ani.force_coefficient=0.1                   weight for force                     
ani.Rcr=5.2                                 radial cutoff radius                 
ani.Rca=3.5                                 angular cutoff radius                
ani.EtaR=1.6                                radial smoothness in radial part     
ani.ShfR=0.9,1.16875,1.4375,1.70625,1.975,2.24375,2.5125,2.78125,3.05,3.31875,3.5875,3.85625,4.125,4.9375,4.6625,4.93125 radial shifts in radial part         
ani.Zeta=32 angular smoothness                   
ani.ShfZ=0.19634954,0.58904862,0.9817477,1.3744468,                             
1.7671459,2.1598449,2.552544,2.9452431 angular shifts                       
ani.EtaA=8 radial smoothness in angular part    
ani.ShfA=0.9,1.55,2.2,2.85 radial shifts in angular part        
ani.Neuron_l1=160 number of neurons in layer 1         
ani.Neuron_l2=128 number of neurons in layer 2         
ani.Neuron_l3=96 number of neurons in layer 3         
ani.AF1='CELU' acitivation function for layer 1     
ani.AF2='CELU' acitivation function for layer 2     
ani.AF3='CELU' acitivation function for layer 3     

PhysNet

Installation

1. clone form PhysNet‘s GitHub page

git clone https://github.com/MMunibas/PhysNet.git

2. install TensorFlow:

pip install tensorflow

3. if you useTensorFlow v2, you need to execute the command below in PhysNet’s directory to make the scripts compatible with TFv2.

for i in `find . -name '*.py'`; do sed -i -e 's/import tensorflow as tf/import tensorflow.compat.v1 as tf\ntf.disable_v2_behavior()/g' -e 's/import tensorflow as tf/import tensorflow.compat.v1 as tf\ntf.disable_v2_behavior()/g' $i; done

4. add environmetal variable $PhysNet to the directory

e.g. export PhysNet=/export/home/fcge/PhysNet/

usage

Set MLprog=PhysNet to enable the interface.

options

Arguments with their default values:

physnet.num_features=128 number of input features             
physnet.num_basis=64 number of radial basis functions     
physnet.num_blocks=5 number of stacked modular building blocks                     
physnet.num_residual_atomic=2 number of residual blocks for atom-wise refinements 
physnet.num_residual_interaction=3 number of residual blocks for refinements of proto-message        
physnet.num_residual_output=1 number of residual blocks in output blocks                       
physnet.cutoff=10.0 cutoff radius for interactions in the neural network 
physnet.seed=42 random seed
physnet.learning_rate=0.0008 starting learning rate                physnet.decay_steps=10000000 decay steps                          
physnet.decay_rate=0.1 decay rate for learning rate         
physnet.batch_size=12 training batch size                  
physnet.valid_batch_size=2 validation batch size                
physnet.force_weight=52.91772105638412 weight for force                   
physnet.summary_interval=5 interval for summary                 
physnet.validation_interval=5 interval for validation              
physnet.save_interval=10 interval for model saving            

sGDML

Installation

1. install sGDML

pip install sgdml

2. add the path of sGDML binary to environmetal variable $sGDML

e.g. export sGDML=/export/home/fcge/.linuxbrew/bin/sgdml

Visit http://quantum-machine.org/gdml/doc/ for more info

usage

Set MLprog=sGDMLto enable the interface.

options

Arguments with their default values:

sgdml.gdml=False use GDML instead of sGDML                     
sgdml.cprsn=False compress kernel matrix along symmetric degrees of freedom
sgdml.no_E=False not to predict energies 
sgdml.E_cstr=False include the energy constraints in the kernel  
sgdml.s=<s1>[,<s2>[,...]] or <start>:[<step>:]<stop> set hyperparameter sigma, see sgdml create -h for details.

Support

If you want to collaborate, have some suggestions for improving the program, or want to report a bug, please write to me.