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Learning irreducible representations of noncommutative Lie groups, applied to constructing equivariant neural networks

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learning_irreps

Learning irreducible representations of noncommutative Lie groups, applied to constructing group equivariant neural networks.

4D "Lorentz harmonics", analogues of the "spherical harmonic" functions

The tensor product of two 4D irreps of $\text{SO}(3,1)$ decomposes as the direct sum of a 1D representation (known in physics as the "spacetime interval"), 9D irrep, and 2 isomorphic 3D irreps. I.e., $4 \otimes 4 = 1 \oplus 3 \oplus 3 \oplus 9$.

Let $u = (u_1, ..., u_9)$ denote the 9D irrep decomposed from the tensor product $v \otimes v$ where $v = (t,x,y,z)$ is a spacetime 4-vector. The animated figure above depicts the 9 components of $u$ as a function of the components of $v$. Since $v$ is 4D, we choose to make it animated, with each frame plotting v within fixed-time slices of $\mathbb{R}^4$.

Introduction

This document is a guide for reproducing the results presented in our submission by using the source code included in the file learning_irreps.zip.

Please see the main submission for all theoretical background and definitions.

We intend to publish the included source code on GitHub after the review process is complete.

Dependencies

Please ensure wget is installed and available.

Please create a Python 3.7 environment. We suggest using pip to manage dependencies.

Run the script install_deps.sh. This will use pip to install all needed dependencies. The requirements.txt file is incomplete due to our use of one package that is hosted as a github repository. Please see install_deps.sh for details.

We use the PyTorch deep learning library \cite{pytorch}.

Shortcut Script

The script

reproduce_paper.sh

will automatically run through the tasks outlined in this document. These tasks are described individually in the following sections.

Learning Irreducible Representations (GroupReps)

This experiment may be reproduced by running:

python learn_spacetime_reps.py

This takes about 10 minutes on a 1.4 GHz Dual-Core Intel Core i7 CPU\footnote{We recommend using CPU for learning the GroupReps as 64 bit floating point arithmetic is used. Once the GroupReps are learned to high precision they may be used to build equivariant networks of lower (e.g. 32 bit) precision.}.

This uses random initialization points so the total time required may fluctuate, but in practice it rarely takes longer than 15 minutes.

After the GroupReps are learned they are stored in the numpy data file irreps.npy. You are of course free to inspect the contents manually verify that the matrices satisfy the appropriate commutation relations. However we suggest instead using our utilities to plot the tensor product structure and loss vs. iteration:

python make_plots.py grouprep_learning

This will produce seven files total inside the plots/ directory. The first three files have names learning_$Nd_representations_$ALGEBRA_NAME.pdf in which $N is the dimension of the GroupRep and $ALGEBRA_NAME is one of $\text{SO}(3), \text{SO}(2,1),$ or $\text{SO}(3,1)$. These correspond to the plots in Figure 3 of the main submission.

The remaining four plots are at paths tensor_product_decomposition_svd_$REP_$ALGEBRA_NAME.pdf in which $ALGEBRA_NAME is as above and $REP is the identity of the GroupRep. Primed GroupReps are those learned by gradient descent, while unprimed GroupReps come from formulas, as explained in the submission.

Generating MNIST-Live Datasets

The program mnist_live/make_data.py makes datasets. The command line arguments are somewhat self-explanatory. Please run the following commands to generate the datasets we used to train Poincar'e-equivariant neural networks:

python mnist_live/make_data.py \
    --included-classes='[0,9]' \
    --ndim 2 \
    --plane xy \
    --fname mnist_live__xy_plane_2D.npy

python mnist_live/make_data.py \
    --included-classes='[0,9]' \
    --ndim 3 \
    --plane xy \
    --fname mnist_live__xy_plane_3D.npy

Training Poincar'e-equivariant Neural Networks

The program spacetime_nn.py can train neural networks which are equivariant to the groups $\text{SO}(2,1)$ and $\text{SO}(3,1)$ using GroupReps obtained from formulas or learned through gradient descent (the latter are referred to in the code as "gd" reps). Please run the following command

python spacetime_nn.py \
    --additional-args-json='{"group": "SO(2,1)", "data_file": "mnist_live__xy_plane_2D.npy", "train_size": 4096, "dev_size": 124, "rep_source": "tensor_power_gd"}' \
    --model-kwargs-json='{"num_channels":3,"num_layers":3}' \
    --skip-equivariance-test \
    --checkpoint='checkpoint_SO21_xy_plane.tar' \
    --epochs 2 --batch-size 16 \
    --checkpoint-on-batch=20 \
    --plot-to='training_plot_SO21_xy_plane.pdf'


python spacetime_nn.py \
    --additional-args-json='{"group": "SO(3,1)", "data_file": "mnist_live__xy_plane_3D.npy", "train_size": 4096, "dev_size": 124, "rep_source": "tensor_power_gd"}' \
    --model-kwargs-json='{"num_channels":3,"num_layers":3}' \
    --skip-equivariance-test \
    --checkpoint='checkpoint_SO31_xy_plane.tar' \
    --epochs 2 --batch-size 16 \
    --checkpoint-on-batch=20 \
    --plot-to='training_plot_SO31_xy_plane.pdf'

As a first step in setting up the equivariant networks, this program will solve for the Clebsch-Gordan coefficients as described in our paper. This may take some time due to our use of a randomized algorithm to compute the coefficients. Error messages of the form "Encountered error with CG coeffs..." may safely be ignored, as the algorithm will automatically retry until succeeding. Once the coefficients are obtained they will be saved with the model checkpoints for future use.

The models will checkpoint to checkpoint_SO21_xy_plane.tar and checkpoint_SO31_xy_plane.tar as set in the command line arguments.

To plot the training performance etc., please run

python make_plots.py nn_history

The plotted neural network training history is in plots/checkpoint_$NETWORK.pdf where $NETWORK indicates the model type. This is how we produce the plots for Figure 5 of the submission. This will also print the total accuracy on the held-out test set. We obtain accuracies of $0.81195$ and $0.827171$ for the $\text{SO}(2,1)$- and $\text{SO}(3,1)$- equivariant networks, respectively.

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