Torch utilities for training neural networks in gravitational wave physics applications.
You can install ml4gw
with pip:
pip install ml4gw
To build with a specific version of PyTorch/CUDA, please see the PyTorch installation instructions here to see how to specify the desired torch version and --extra-index-url
flag. For example, to install with torch 1.12 and CUDA 11.6 support, you would run
pip install ml4gw torch==1.12.0 --extra-index-url=https://download.pytorch.org/whl/cu116
ml4gw
is also fully compatible with use in Poetry, with your pyproject.toml
set up like
[tool.poetry.dependencies]
python = "^3.8" # python versions 3.8-3.11 are supported
ml4gw = "^0.3.0"
To build against a specific PyTorch/CUDA combination, consult the PyTorch installation documentation above and specify the extra-index-url
via the tool.poetry.source
table in your pyproject.toml
. For example, to build against CUDA 11.6, you would do something like:
[tool.poetry.dependencies]
python = "^3.8"
ml4gw = "^0.3.0"
torch = {version = "^1.12", source = "torch"}
[[tool.poetry.source]]
name = "torch"
url = "https://download.pytorch.org/whl/cu116"
secondary = true
default = false
Note: if you are building against CUDA 11.6 or 11.7, make sure that you are using python 3.8, 3.9, or 3.10. Python 3.11 is incompatible with torchaudio
0.13, and the following torchaudio
version is incompatible with CUDA 11.7 and earlier.
This library provided utilities for both data iteration and transformation via dataloaders defined in ml4gw/dataloading
and transform layers exposed in ml4gw/transforms
. Lower level functions and utilies are defined at the top level of the library and in the utils
library.
For example, to train a simple autoencoder using a cost function in frequency space, you might do something like:
import numpy as np
import torch
from ml4gw.dataloading import InMemoryDataset
from ml4gw.transforms import SpectralDensity
SAMPLE_RATE = 2048
NUM_IFOS = 2
DATA_LENGTH = 128
KERNEL_LENGTH = 4
DEVICE = "cuda" # or "cpu", wherever you want to run
BATCH_SIZE = 32
LEARNING_RATE = 1e-3
NUM_EPOCHS = 10
dummy_data = np.random.randn(NUM_IFOS, DATA_LENGTH * SAMPLE_RATE)
# this will create a dataloader that iterates through your
# timeseries data sampling 4s long windows of data randomly
# and non-coincidentally: i.e. the background from each IFO
# will be sampled independently
dataset = InMemoryDataset(
dummy_data,
kernel_size=KERNEL_LENGTH * SAMPLE_RATE,
batch_size=BATCH_SIZE,
batches_per_epoch=50,
coincident=False,
shuffle=True,
device=DEVICE # this will move your dataset to GPU up-front if "cuda"
)
nn = torch.nn.Sequential(
torch.nn.Conv1d(
in_channels=2,
out_channels=8,
kernel_size=7
),
torch.nn.ConvTranspose1d(
in_channels=8,
out_channels=2,
kernel_size=7
)
).to(DEVICE)
optimizer = torch.optim.Adam(nn.parameters(), lr=LEARNING_RATE)
spectral_density = SpectralDensity(SAMPLE_RATE, fftlength=2).to(DEVICE)
def loss_function(X, y):
"""
MSE in frequency domain. Obviously this doesn't
give you much on its own, but you can imagine doing
something like masking to just the bins you care about.
"""
X = spectral_density(X)
y = spectral_density(y)
return ((X - y)**2).mean()
for i in range(NUM_EPOCHS):
epoch_loss = 0
for X in dataset:
optimizer.zero_grad(set_to_none=True)
assert X.shape == (32, NUM_IFOS, KERNEL_LENGTH * SAMPLE_RATE)
y = nn(X)
loss = loss_function(X, y)
loss.backward()
optimizer.step()
epoch_loss += loss.item()
epoch_loss /= len(dataset)
print(f"Epoch {i + 1}/{NUM_EPOCHS} Loss: {epoch_loss:0.3e}")
As this library is still very much a work in progress, we anticipate that novel use cases will encounter errors stemming from a lack of robustness. We encourage users who encounter these difficulties to file issues on GitHub, and we'll be happy to offer support to extend our coverage to new or improved functionality. We also strongly encourage ML users in the GW physics space to try their hand at working on these issues and joining on as collaborators! For more information about how to get involved, feel free to reach out to [email protected] . By bringing in new users with new use cases, we hope to develop this library into a truly general-purpose tool which makes DL more accessible for gravitational wave physicists everywhere.
We are grateful for the support of the U.S. National Science Foundation (NSF) Harnessing the Data Revolution (HDR) Institute for Accelerating AI Algorithms for Data Driven Discovery (A3D3) under Cooperative Agreement No. PHY-2117997.