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add HSIC metric #3282
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4002106
add HSIC metric
kzkadc 245b3a1
Merge branch 'master' into hsic
kzkadc 490fdb3
minor update on docstring
kzkadc 11fb1a3
Merge branch 'master' into hsic
kzkadc 0e47aff
add reference to the HSIC formula in docstring
kzkadc ba441de
update version directive
kzkadc 8458ae1
fix formatting issue
kzkadc 78d6c2a
Merge branch 'master' into hsic
vfdev-5 28d3b4b
add type hints
kzkadc 3d3aec8
Merge branch 'hsic' of github.com:kzkadc/ignite into hsic
kzkadc 43bd324
accumulate HSIC value for each batch
kzkadc 1c0b1a4
update test to clip value for each batch
kzkadc db6392d
fix accumulator device error
kzkadc 5cb0bf1
fix error in making y
kzkadc a43fc39
Merge branch 'master' into hsic
vfdev-5 cb71355
fix test to use the same linear layer across metric_devices
kzkadc f68c8de
Merge branch 'hsic' of github.com:kzkadc/ignite into hsic
kzkadc b659a16
Revert "fix test to use the same linear layer across metric_devices"
kzkadc 7ddd117
Fixed distributed tests
vfdev-5 5dfb07b
Fixed code formatting errors
vfdev-5 e4d15b7
Merge branch 'master' into hsic
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Original file line number | Diff line number | Diff line change |
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from typing import Callable, Sequence, Union | ||
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import torch | ||
from torch import Tensor | ||
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from ignite.exceptions import NotComputableError | ||
from ignite.metrics.metric import Metric, reinit__is_reduced, sync_all_reduce | ||
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__all__ = ["HSIC"] | ||
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class HSIC(Metric): | ||
r"""Calculates the `Hilbert-Schmidt Independence Criterion (HSIC) | ||
<https://papers.nips.cc/paper_files/paper/2007/hash/d5cfead94f5350c12c322b5b664544c1-Abstract.html>`_. | ||
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.. math:: | ||
\text{HSIC}(X,Y) = \frac{1}{B(B-3)}\left[ \text{tr}(\tilde{\mathbf{K}}\tilde{\mathbf{L}}) | ||
+ \frac{\mathbf{1}^\top \tilde{\mathbf{K}} \mathbf{11}^\top \tilde{\mathbf{L}} \mathbf{1}}{(B-1)(B-2)} | ||
-\frac{2}{B-2}\mathbf{1}^\top \tilde{\mathbf{K}}\tilde{\mathbf{L}} \mathbf{1} \right] | ||
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where :math:`B` is the batch size, and :math:`\tilde{\mathbf{K}}` | ||
and :math:`\tilde{\mathbf{L}}` are the Gram matrices of | ||
the Gaussian RBF kernel with their diagonal entries being set to zero. | ||
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HSIC measures non-linear statistical independence between features :math:`X` and :math:`Y`. | ||
HSIC becomes zero if and only if :math:`X` and :math:`Y` are independent. | ||
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This metric computes the unbiased estimator of HSIC proposed in | ||
`Song et al. (2012) <https://jmlr.csail.mit.edu/papers/v13/song12a.html>`_. | ||
The HSIC is estimated using Eq. (5) of the paper for each batch and the average is accumulated. | ||
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Each batch must contain at least four samples. | ||
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- ``update`` must receive output of the form ``(y_pred, y)``. | ||
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Args: | ||
sigma_x: bandwidth of the kernel for :math:`X`. | ||
If negative, a heuristic value determined by the median of the distances between | ||
the samples is used. Default: -1 | ||
sigma_y: bandwidth of the kernel for :math:`Y`. | ||
If negative, a heuristic value determined by the median of the distances | ||
between the samples is used. Default: -1 | ||
ignore_invalid_batch: If ``True``, computation for a batch with less than four samples is skipped. | ||
If ``False``, ``ValueError`` is raised when received such a batch. | ||
output_transform: a callable that is used to transform the | ||
:class:`~ignite.engine.engine.Engine`'s ``process_function``'s output into the | ||
form expected by the metric. This can be useful if, for example, you have a multi-output model and | ||
you want to compute the metric with respect to one of the outputs. | ||
By default, metrics require the output as ``(y_pred, y)`` or ``{'y_pred': y_pred, 'y': y}``. | ||
device: specifies which device updates are accumulated on. Setting the | ||
metric's device to be the same as your ``update`` arguments ensures the ``update`` method is | ||
non-blocking. By default, CPU. | ||
skip_unrolling: specifies whether output should be unrolled before being fed to update method. Should be | ||
true for multi-output model, for example, if ``y_pred`` contains multi-ouput as ``(y_pred_a, y_pred_b)`` | ||
Alternatively, ``output_transform`` can be used to handle this. | ||
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Examples: | ||
To use with ``Engine`` and ``process_function``, simply attach the metric instance to the engine. | ||
The output of the engine's ``process_function`` needs to be in the format of | ||
``(y_pred, y)`` or ``{'y_pred': y_pred, 'y': y, ...}``. If not, ``output_tranform`` can be added | ||
to the metric to transform the output into the form expected by the metric. | ||
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``y_pred`` and ``y`` should have the same shape. | ||
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For more information on how metric works with :class:`~ignite.engine.engine.Engine`, visit :ref:`attach-engine`. | ||
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.. include:: defaults.rst | ||
:start-after: :orphan: | ||
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.. testcode:: | ||
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metric = HSIC() | ||
metric.attach(default_evaluator, "hsic") | ||
X = torch.tensor([[0., 1., 2., 3., 4.], | ||
[5., 6., 7., 8., 9.], | ||
[10., 11., 12., 13., 14.], | ||
[15., 16., 17., 18., 19.], | ||
[20., 21., 22., 23., 24.], | ||
[25., 26., 27., 28., 29.], | ||
[30., 31., 32., 33., 34.], | ||
[35., 36., 37., 38., 39.], | ||
[40., 41., 42., 43., 44.], | ||
[45., 46., 47., 48., 49.]]) | ||
Y = torch.sin(X * torch.pi * 2 / 50) | ||
state = default_evaluator.run([[X, Y]]) | ||
print(state.metrics["hsic"]) | ||
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.. testoutput:: | ||
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0.09226646274328232 | ||
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.. versionadded:: 0.5.2 | ||
""" | ||
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def __init__( | ||
self, | ||
sigma_x: float = -1, | ||
sigma_y: float = -1, | ||
ignore_invalid_batch: bool = True, | ||
output_transform: Callable = lambda x: x, | ||
device: Union[str, torch.device] = torch.device("cpu"), | ||
skip_unrolling: bool = False, | ||
): | ||
super().__init__(output_transform, device, skip_unrolling=skip_unrolling) | ||
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self.sigma_x = sigma_x | ||
self.sigma_y = sigma_y | ||
self.ignore_invalid_batch = ignore_invalid_batch | ||
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_state_dict_all_req_keys = ("_sum_of_hsic", "_num_batches") | ||
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@reinit__is_reduced | ||
def reset(self) -> None: | ||
self._sum_of_hsic = torch.tensor(0.0, device=self._device) | ||
self._num_batches = 0 | ||
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@reinit__is_reduced | ||
def update(self, output: Sequence[Tensor]) -> None: | ||
X = output[0].detach().flatten(start_dim=1) | ||
Y = output[1].detach().flatten(start_dim=1) | ||
b = X.shape[0] | ||
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if b <= 3: | ||
if self.ignore_invalid_batch: | ||
return | ||
else: | ||
raise ValueError(f"A batch must contain more than four samples, got only {b} samples.") | ||
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mask = 1.0 - torch.eye(b, device=X.device) | ||
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xx = X @ X.T | ||
rx = xx.diag().unsqueeze(0).expand_as(xx) | ||
dxx = rx.T + rx - xx * 2 | ||
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vx: Union[Tensor, float] | ||
if self.sigma_x < 0: | ||
vx = torch.quantile(dxx, 0.5) | ||
else: | ||
vx = self.sigma_x**2 | ||
K = torch.exp(-0.5 * dxx / vx) * mask | ||
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yy = Y @ Y.T | ||
ry = yy.diag().unsqueeze(0).expand_as(yy) | ||
dyy = ry.T + ry - yy * 2 | ||
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vy: Union[Tensor, float] | ||
if self.sigma_y < 0: | ||
vy = torch.quantile(dyy, 0.5) | ||
else: | ||
vy = self.sigma_y**2 | ||
L = torch.exp(-0.5 * dyy / vy) * mask | ||
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KL = K @ L | ||
trace = KL.trace() | ||
second_term = K.sum() * L.sum() / ((b - 1) * (b - 2)) | ||
third_term = KL.sum() / (b - 2) | ||
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hsic = trace + second_term - third_term * 2.0 | ||
hsic /= b * (b - 3) | ||
hsic = torch.clamp(hsic, min=0.0) # HSIC must not be negative | ||
self._sum_of_hsic += hsic.to(self._device) | ||
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self._num_batches += 1 | ||
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@sync_all_reduce("_sum_of_hsic", "_num_batches") | ||
def compute(self) -> float: | ||
if self._num_batches == 0: | ||
raise NotComputableError("HSIC must have at least one batch before it can be computed.") | ||
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return self._sum_of_hsic.item() / self._num_batches |
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from typing import Tuple | ||
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import numpy as np | ||
import pytest | ||
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import torch | ||
from torch import nn, Tensor | ||
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import ignite.distributed as idist | ||
from ignite.engine import Engine | ||
from ignite.exceptions import NotComputableError | ||
from ignite.metrics import HSIC | ||
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def np_hsic(x: Tensor, y: Tensor, sigma_x: float = -1, sigma_y: float = -1) -> float: | ||
x_np = x.detach().cpu().numpy() | ||
y_np = y.detach().cpu().numpy() | ||
b = x_np.shape[0] | ||
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ii, jj = np.meshgrid(np.arange(b), np.arange(b), indexing="ij") | ||
mask = 1.0 - np.eye(b) | ||
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dxx = np.square(x_np[ii] - x_np[jj]).sum(axis=2) | ||
if sigma_x < 0: | ||
vx = np.median(dxx) | ||
else: | ||
vx = sigma_x * sigma_x | ||
K = np.exp(-0.5 * dxx / vx) * mask | ||
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dyy = np.square(y_np[ii] - y_np[jj]).sum(axis=2) | ||
if sigma_y < 0: | ||
vy = np.median(dyy) | ||
else: | ||
vy = sigma_y * sigma_y | ||
L = np.exp(-0.5 * dyy / vy) * mask | ||
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KL = K @ L | ||
ones = np.ones(b) | ||
hsic = np.trace(KL) + (ones @ K @ ones) * (ones @ L @ ones) / ((b - 1) * (b - 2)) - ones @ KL @ ones * 2 / (b - 2) | ||
hsic /= b * (b - 3) | ||
hsic = np.clip(hsic, 0.0, None) | ||
return hsic | ||
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def test_zero_batch(): | ||
hsic = HSIC() | ||
with pytest.raises(NotComputableError, match=r"HSIC must have at least one batch before it can be computed"): | ||
hsic.compute() | ||
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def test_invalid_batch(): | ||
hsic = HSIC(ignore_invalid_batch=False) | ||
X = torch.tensor([[1, 2, 3]]).float() | ||
Y = torch.tensor([[4, 5, 6]]).float() | ||
with pytest.raises(ValueError, match=r"A batch must contain more than four samples, got only"): | ||
hsic.update((X, Y)) | ||
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@pytest.fixture(params=[0, 1, 2]) | ||
def test_case(request) -> Tuple[Tensor, Tensor, int]: | ||
if request.param == 0: | ||
# independent | ||
N = 100 | ||
b = 10 | ||
x, y = torch.randn((N, 50)), torch.randn((N, 30)) | ||
elif request.param == 1: | ||
# linearly dependent | ||
N = 100 | ||
b = 10 | ||
x = torch.normal(1.0, 2.0, size=(N, 10)) | ||
y = x @ torch.rand(10, 15) * 3 + torch.randn(N, 15) * 1e-4 | ||
else: | ||
# non-linearly dependent | ||
N = 200 | ||
b = 20 | ||
x = torch.randn(N, 5) | ||
y = x @ torch.normal(0.0, torch.pi, size=(5, 3)) | ||
y = ( | ||
torch.stack([torch.sin(y[:, 0]), torch.cos(y[:, 1]), torch.exp(y[:, 2])], dim=1) | ||
+ torch.randn_like(y) * 1e-4 | ||
) | ||
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return x, y, b | ||
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@pytest.mark.parametrize("n_times", range(3)) | ||
@pytest.mark.parametrize("sigma_x", [-1.0, 1.0]) | ||
@pytest.mark.parametrize("sigma_y", [-1.0, 1.0]) | ||
def test_compute(n_times, sigma_x: float, sigma_y: float, test_case: Tuple[Tensor, Tensor, int]): | ||
x, y, batch_size = test_case | ||
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hsic = HSIC(sigma_x=sigma_x, sigma_y=sigma_y) | ||
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hsic.reset() | ||
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np_hsic_sum = 0.0 | ||
n_iters = y.shape[0] // batch_size | ||
for i in range(n_iters): | ||
idx = i * batch_size | ||
x_batch = x[idx : idx + batch_size] | ||
y_batch = y[idx : idx + batch_size] | ||
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hsic.update((x_batch, y_batch)) | ||
np_hsic_sum += np_hsic(x_batch, y_batch, sigma_x, sigma_y) | ||
expected_hsic = np_hsic_sum / n_iters | ||
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assert isinstance(hsic.compute(), float) | ||
assert pytest.approx(expected_hsic, abs=2e-5) == hsic.compute() | ||
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def test_accumulator_detached(): | ||
hsic = HSIC() | ||
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x = torch.rand(10, 10, dtype=torch.float) | ||
y = torch.rand(10, 10, dtype=torch.float) | ||
hsic.update((x, y)) | ||
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assert not hsic._sum_of_hsic.requires_grad | ||
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@pytest.mark.usefixtures("distributed") | ||
class TestDistributed: | ||
@pytest.mark.parametrize("sigma_x", [-1.0, 1.0]) | ||
@pytest.mark.parametrize("sigma_y", [-1.0, 1.0]) | ||
def test_integration(self, sigma_x: float, sigma_y: float): | ||
tol = 2e-5 | ||
n_iters = 100 | ||
batch_size = 20 | ||
n_dims_x = 100 | ||
n_dims_y = 50 | ||
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rank = idist.get_rank() | ||
torch.manual_seed(12 + rank) | ||
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device = idist.device() | ||
metric_devices = [torch.device("cpu")] | ||
if device.type != "xla": | ||
metric_devices.append(device) | ||
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for metric_device in metric_devices: | ||
x = torch.randn((n_iters * batch_size, n_dims_x)).float().to(device) | ||
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lin = nn.Linear(n_dims_x, n_dims_y).to(device) | ||
y = torch.sin(lin(x) * 100) + torch.randn(n_iters * batch_size, n_dims_y) * 1e-4 | ||
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def data_loader(i, input_x, input_y): | ||
return input_x[i * batch_size : (i + 1) * batch_size], input_y[i * batch_size : (i + 1) * batch_size] | ||
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engine = Engine(lambda e, i: data_loader(i, x, y)) | ||
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m = HSIC(sigma_x=sigma_x, sigma_y=sigma_y, device=metric_device) | ||
m.attach(engine, "hsic") | ||
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data = list(range(n_iters)) | ||
engine.run(data=data, max_epochs=1) | ||
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assert "hsic" in engine.state.metrics | ||
res = engine.state.metrics["hsic"] | ||
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x = idist.all_gather(x) | ||
y = idist.all_gather(y) | ||
total_n_iters = idist.all_reduce(n_iters) | ||
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np_res = 0.0 | ||
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for i in range(total_n_iters): | ||
x_batch, y_batch = data_loader(i, x, y) | ||
np_res += np_hsic(x_batch, y_batch, sigma_x, sigma_y) | ||
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expected_hsic = np_res / total_n_iters | ||
assert pytest.approx(expected_hsic, abs=tol) == res | ||
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def test_accumulator_device(self): | ||
device = idist.device() | ||
metric_devices = [torch.device("cpu")] | ||
if device.type != "xla": | ||
metric_devices.append(device) | ||
for metric_device in metric_devices: | ||
hsic = HSIC(device=metric_device) | ||
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for dev in (hsic._device, hsic._sum_of_hsic.device): | ||
assert dev == metric_device, f"{type(dev)}:{dev} vs {type(metric_device)}:{metric_device}" | ||
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x = torch.zeros(10, 10).float() | ||
y = torch.ones(10, 10).float() | ||
hsic.update((x, y)) | ||
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for dev in (hsic._device, hsic._sum_of_hsic.device): | ||
assert dev == metric_device, f"{type(dev)}:{dev} vs {type(metric_device)}:{metric_device}" |
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