Concise Implementation of Softmax Regression

Just as high-level deep learning frameworks made it easier to implement linear regression (see “linear concise”), they are similarly convenient here.

from d2l import torch as d2l
import torch
from torch import nn
from torch.nn import functional as F

Defining the Model

As in “linear concise”, we construct our fully connected layer using the built-in layer. The built-in __call__ method then invokes forward whenever we need to apply the network to some input.

:begin_tab:mxnet Even though the input X is a fourth-order tensor, the built-in Dense layer will automatically convert X into a second-order tensor by keeping the dimensionality along the first axis unchanged. :end_tab:

:begin_tab:pytorch We use a Flatten layer to convert the fourth-order tensor X to second order by keeping the dimensionality along the first axis unchanged.

:end_tab:

:begin_tab:tensorflow We use a Flatten layer to convert the fourth-order tensor X by keeping the dimension along the first axis unchanged. :end_tab:

:begin_tab:jax Flax allows users to write the network class in a more compact way using @nn.compact dectorator. With @nn.compact, one can simply write all network logic inside a single “forward pass” method, without needing to define the standard setup method in the dataclass. :end_tab:

class SoftmaxRegression(d2l.Classifier):  #@save
    """The softmax regression model."""
    def __init__(self, num_outputs, lr):
        super().__init__()
        self.save_hyperparameters()
        self.net = nn.Sequential(nn.Flatten(),
                                 nn.LazyLinear(num_outputs))

    def forward(self, X):
        return self.net(X)

Softmax Revisited

In “softmax scratch” we calculated our model's output and applied the cross-entropy loss. While this is perfectly reasonable mathematically, it is risky computationally, because of numerical underflow and overflow in the exponentiation.

Recall that the softmax function computes probabilities via $\hat y_j = \frac{\exp(o_j)}{\sum_k \exp(o_k)}$ . If some of the $o_k$ are very large, i.e., very positive, then $\exp(o_k)$ might be larger than the largest number we can have for certain data types. This is called overflow. Likewise, if every argument is a very large negative number, we will get underflow. For instance, single precision floating point numbers approximately cover the range of $10^{-38}$ to $10^{38}$ . As such, if the largest term in $\mathbf{o}$ lies outside the interval $[-90, 90]$ , the result will not be stable. A way round this problem is to subtract $\bar{o} \stackrel{\textrm{def}}{=} \max_k o_k$ from all entries:

\hat y_j = \frac{\exp o_j}{\sum_k \exp o_k} = \frac{\exp(o_j - \bar{o}) \exp \bar{o}}{\sum_k \exp (o_k - \bar{o}) \exp \bar{o}} = \frac{\exp(o_j - \bar{o})}{\sum_k \exp (o_k - \bar{o})}.

By construction we know that $o_j - \bar{o} \leq 0$ for all $j$ . As such, for a $q$ -class classification problem, the denominator is contained in the interval $[1, q]$ . Moreover, the numerator never exceeds $1$ , thus preventing numerical overflow. Numerical underflow only occurs when $\exp(o_j - \bar{o})$ numerically evaluates as $0$ . Nonetheless, a few steps down the road we might find ourselves in trouble when we want to compute $\log \hat{y}_j$ as $\log 0$ . In particular, in backpropagation, we might find ourselves faced with a screenful of the dreaded NaN (Not a Number) results.

Fortunately, we are saved by the fact that even though we are computing exponential functions, we ultimately intend to take their log (when calculating the cross-entropy loss). By combining softmax and cross-entropy, we can escape the numerical stability issues altogether. We have:

\log \hat{y}_j = \log \frac{\exp(o_j - \bar{o})}{\sum_k \exp (o_k - \bar{o})} = o_j - \bar{o} - \log \sum_k \exp (o_k - \bar{o}).

This avoids both overflow and underflow. We will want to keep the conventional softmax function handy in case we ever want to evaluate the output probabilities by our model. But instead of passing softmax probabilities into our new loss function, we just [pass the logits and compute the softmax and its log all at once inside the cross-entropy loss function,] which does smart things like the "LogSumExp trick".

@d2l.add_to_class(d2l.Classifier)  #@save
def loss(self, Y_hat, Y, averaged=True):
    Y_hat = d2l.reshape(Y_hat, (-1, Y_hat.shape[-1]))
    Y = d2l.reshape(Y, (-1,))
    if tab.selected('mxnet'):
        fn = gluon.loss.SoftmaxCrossEntropyLoss()
        l = fn(Y_hat, Y)
        return l.mean() if averaged else l
    if tab.selected('pytorch'):
        return F.cross_entropy(
            Y_hat, Y, reduction='mean' if averaged else 'none')
    if tab.selected('tensorflow'):
        fn = tf.keras.losses.SparseCategoricalCrossentropy(from_logits=True)
        return fn(Y, Y_hat)

Training

Next we train our model. We use Fashion-MNIST images, flattened to 784-dimensional feature vectors.

data = d2l.FashionMNIST(batch_size=256)
model = SoftmaxRegression(num_outputs=10, lr=0.1)
trainer = d2l.Trainer(max_epochs=10)
trainer.fit(model, data)

As before, this algorithm converges to a solution that is reasonably accurate, albeit this time with fewer lines of code than before.

Summary

High-level APIs are very convenient at hiding from their user potentially dangerous aspects, such as numerical stability. Moreover, they allow users to design models concisely with very few lines of code. This is both a blessing and a curse. The obvious benefit is that it makes things highly accessible, even to engineers who never took a single class of statistics in their life (in fact, they are part of the target audience of the book). But hiding the sharp edges also comes with a price: a disincentive to add new and different components on your own, since there is little muscle memory for doing it. Moreover, it makes it more difficult to fix things whenever the protective padding of a framework fails to cover all the corner cases entirely. Again, this is due to lack of familiarity.

As such, we strongly urge you to review both the bare bones and the elegant versions of many of the implementations that follow. While we emphasize ease of understanding, the implementations are nonetheless usually quite performant (convolutions are the big exception here). It is our intention to allow you to build on these when you invent something new that no framework can give you.

Exercises

Deep learning uses many different number formats, including FP64 double precision (used extremely rarely), FP32 single precision, BFLOAT16 (good for compressed representations), FP16 (very unstable), TF32 (a new format from NVIDIA), and INT8. Compute the smallest and largest argument of the exponential function for which the result does not lead to numerical underflow or overflow.
INT8 is a very limited format consisting of nonzero numbers from $1$ to $255$ . How could you extend its dynamic range without using more bits? Do standard multiplication and addition still work?
Increase the number of epochs for training. Why might the validation accuracy decrease after a while? How could we fix this?
What happens as you increase the learning rate? Compare the loss curves for several learning rates. Which one works better? When?

:begin_tab:mxnet

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:begin_tab:pytorch

:end_tab:

:begin_tab:tensorflow

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:begin_tab:jax

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