chapter_linear-networks/softmax-regression-concise_origin.md
:label:sec_softmax_concise
Just as high-level APIs of deep learning frameworks
made it much easier
to implement linear regression in :numref:sec_linear_concise,
we will find it similarly (or possibly more)
convenient for implementing classification models. Let us stick with the Fashion-MNIST dataset
and keep the batch size at 256 as in :numref:sec_softmax_scratch.
from d2l import mxnet as d2l
from mxnet import gluon, init, npx
from mxnet.gluon import nn
npx.set_np()
#@tab pytorch
from d2l import torch as d2l
import torch
from torch import nn
#@tab tensorflow
from d2l import tensorflow as d2l
import tensorflow as tf
#@tab all
batch_size = 256
train_iter, test_iter = d2l.load_data_fashion_mnist(batch_size)
As mentioned in :numref:sec_softmax,
the output layer of softmax regression
is a fully-connected layer.
Therefore, to implement our model,
we just need to add one fully-connected layer
with 10 outputs to our Sequential.
Again, here, the Sequential is not really necessary,
but we might as well form the habit since it will be ubiquitous
when implementing deep models.
Again, we initialize the weights at random
with zero mean and standard deviation 0.01.
net = nn.Sequential()
net.add(nn.Dense(10))
net.initialize(init.Normal(sigma=0.01))
#@tab pytorch
# PyTorch does not implicitly reshape the inputs. Thus we define a layer to
# reshape the inputs in our network
class Reshape(torch.nn.Module):
def forward(self, x):
return x.view(-1,784)
net = nn.Sequential(Reshape(), nn.Linear(784, 10))
def init_weights(m):
if type(m) == nn.Linear:
torch.nn.init.normal_(m.weight, std=0.01)
net.apply(init_weights)
#@tab tensorflow
net = tf.keras.models.Sequential()
net.add(tf.keras.layers.Flatten(input_shape=(28, 28)))
weight_initializer = tf.keras.initializers.RandomNormal(mean=0.0, stddev=0.01)
net.add(tf.keras.layers.Dense(10, kernel_initializer=weight_initializer))
:label:subsec_softmax-implementation-revisited
In the previous example of :numref:sec_softmax_scratch,
we calculated our model's output
and then ran this output through the cross-entropy loss.
Mathematically, that is a perfectly reasonable thing to do.
However, from a computational perspective,
exponentiation can be a source of numerical stability issues.
Recall that the softmax function calculates
$\hat y_j = \frac{\exp(o_j)}{\sum_k \exp(o_k)}$,
where $\hat y_j$ is the $j^\mathrm{th}$ element of
the predicted probability distribution $\hat{\mathbf{y}}$
and $o_j$ is the $j^\mathrm{th}$ element of the logits
$\mathbf{o}$.
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 (i.e., overflow).
This would make the denominator (and/or numerator) inf (infinity)
and we wind up encountering either 0, inf, or nan (not a number) for $\hat y_j$.
In these situations we do not get a well-defined
return value for cross entropy.
One trick to get around this is to first subtract $\max(o_k)$
from all $o_k$ before proceeding with the softmax calculation.
You can verify that this shifting of each $o_k$ by constant factor
does not change the return value of softmax.
After the subtraction and normalization step,
it might be possible that some $o_j$ have large negative values
and thus that the corresponding $\exp(o_j)$ will take values close to zero.
These might be rounded to zero due to finite precision (i.e., underflow),
making $\hat y_j$ zero and giving us -inf for $\log(\hat y_j)$.
A few steps down the road in backpropagation,
we might find ourselves faced with a screenful
of the dreaded nan 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 these two operators softmax and cross entropy together, we can escape the numerical stability issues that might otherwise plague us during backpropagation. As shown in the equation below, we avoid calculating $\exp(o_j)$ and can use instead $o_j$ directly due to the canceling in $\log(\exp(\cdot))$.
$$ \begin{aligned} \log{(\hat y_j)} & = \log\left( \frac{\exp(o_j)}{\sum_k \exp(o_k)}\right) \ & = \log{(\exp(o_j))}-\log{\left( \sum_k \exp(o_k) \right)} \ & = o_j -\log{\left( \sum_k \exp(o_k) \right)}. \end{aligned} $$
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 will 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".
loss = gluon.loss.SoftmaxCrossEntropyLoss()
#@tab pytorch
loss = nn.CrossEntropyLoss()
#@tab tensorflow
loss = tf.keras.losses.SparseCategoricalCrossentropy(from_logits=True)
Here, we use minibatch stochastic gradient descent with a learning rate of 0.1 as the optimization algorithm. Note that this is the same as we applied in the linear regression example and it illustrates the general applicability of the optimizers.
trainer = gluon.Trainer(net.collect_params(), 'sgd', {'learning_rate': 0.1})
#@tab pytorch
trainer = torch.optim.SGD(net.parameters(), lr=0.1)
#@tab tensorflow
trainer = tf.keras.optimizers.SGD(learning_rate=.1)
Next we call the training function defined in :numref:sec_softmax_scratch to train the model.
#@tab all
num_epochs = 10
d2l.train_ch3(net, train_iter, test_iter, loss, num_epochs, trainer)
As before, this algorithm converges to a solution that achieves a decent accuracy, albeit this time with fewer lines of code than before.
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