Within the previous article of this collection, operation in all fields of laptop science: matrix multiplication. It’s closely utilized in neural networks to compute the activation of linear layers. Nevertheless, activations on their very own are tough to interpret, since their values and statistics (imply, variance, min-max amplitude) can range wildly from layer to layer. This is without doubt one of the the explanation why we use activation features, for instance the logistic perform (aka sigmoid) which initiatives any actual quantity within the [0; 1] vary.
The softmax perform, also called the normalised exponential perform, is a multi-dimensional generalisation of the sigmoid. It converts a vector of uncooked scores (logits) right into a likelihood distribution over M courses. We will interpret it as a weighted common that behaves as a clean perform and may be conveniently differentiated. It’s a essential element of dot-product consideration, language modeling, and multinomial logistic regression.
On this article, we’ll cowl:
- Implementing an environment friendly softmax kernel in Triton.
- Implementing the backward move (
autograd). - Optimisation: cache modifiers and auto-tuning.
If you happen to aren’t acquainted with Triton but, consult with the earlier articles!
Disclaimer: all of the illustrations and animations are made by the writer except specified in any other case.
Definition
The softmax is outlined as follows:
The normalisation ensures that the vector sums to 1, in order that it may be interpreted as a sound likelihood distribution.
Be aware that this formulation of the softmax is extremely delicate to numerical overflow. Recall that the utmost worth a typical float16 can characterize is 65 504, which is roughly exp(11). Which means that any enter worth larger than ~11 will end in exp(z_i) exceeding the representable vary, resulting in overflow.
A typical trick to mitigate this subject is to subtract the utmost worth of the enter vector from each aspect, such that the brand new most is 0 earlier than exponentiation and 1 after.

Naive Implementation
As you may see, computing the softmax includes two discount operations, a max and a sum. A naive algorithm require three separate passes over the enter vector. First to compute the utmost, then the sum, and eventually the normalised outputs.
Right here’s what a naive Numpy implementation appears to be like like:
A recurrent theme on this Triton collection is minimising high-latency world reminiscence entry. Our present Numpy implementation requires three separate reminiscence reads of the total enter vector, which is extremely inefficient.
On-line Softmax
Fortuitously, we will use a intelligent trick, often called the on-line softmax, to fuse the max and sum steps, lowering the variety of reminiscence reads to 2.
First, we outline the sum of exponentials recursively. Within the following set of equalities, m_i refers back to the most over x till the i-th index.

This equality permits us to compute the sum of exponentials iteratively utilizing the utmost worth thus far. We will leverage it to fuse the primary and second loop within the naive implementation and compute the utmost and sum of exponentials iteratively.
Our algorithm turns into:

That is simply translated to Numpy:
Now that we perceive the principle rules behind the softmax, we’ll implement it in Triton, beginning by the easy, single-block model and constructing as much as the web, multi-block formulation. In the long run, we would like our kernel to behave like a PyTorch module and be appropriate with autograd.
Sadly, from PyTorch’s standpoint, Triton kernels behave like black containers: the operations they carry out should not traced by autograd. This requires us to implement the backward move ourselves and explicitly specify how gradients ought to be computed. Let’s brush up on our beloved chain rule and derive the softmax gradient.
Gradient
For the reason that outputs of the softmax are strictly optimistic, we will use the logarithmic spinoff to make the derivation of the gradient simpler. Right here, we take the spinoff of the log of the output and apply the chain rule:

From there, we rearrange the phrases and observe these steps:

Now assume that we now have some upstream gradient, for instance generated by a loss perform L (e.g. a cross-entropy loss). We get the next expression of the gradient:

The simplification of the left time period in (9) is because of the truth that δ_ij will solely be equal to 1 for the i-th aspect, collapsing the sum over j to a single time period.
Triton Implementation
Single Block Softmax
Now that we labored via the derivation of the gradient, we will write the ahead and backward softmax kernels. First, let’s deal with the PyTorch wrapper to know how the one block implementation works at a excessive degree. Given a 2D enter tensor, the ahead and backward kernels are going to course of all rows in parallel.
For simplicity, we’ll outline the BLOCK_SIZE to be massive sufficient to deal with all columns without delay. Particularly, we’ll set it as the subsequent energy of two superior to the variety of columns, as required by Triton.
Then, we’ll outline our `grid` to be the variety of rows (it may doubtlessly additionally deal with a batch dimension).
The PyTorch wrapper for our SoftmaxSingleBlock is a category inheriting from torch.autograd.Perform that implements ahead and backward. Each strategies take a ctx argument, which we’ll use to cache the softmax outputs throughout the ahead move and reuse them throughout the backward move.
Each kernels are fairly easy, we begin by loading the row inputs utilizing the identical syntax as in my earlier vector addition article. Discover that BLOCK_SIZE and num_warps are computed utilizing a calculate_settings perform. This perform comes from the Unsloth library and was reused in different kernel libraries corresponding to LigerKernel (which the kernels on this article are loosely based mostly on), it offers heuristics to tune each variables:
def calculate_settings(n: int) -> tuple[int, int]:
MAX_FUSED_SIZE = 65536 # most grid dimension on Nvidia GPUs
BLOCK_SIZE = next_power_of_2(n)
if BLOCK_SIZE > MAX_FUSED_SIZE:
# we take away this assertion on this article
elevate RuntimeError(
f"Can't launch Triton kernel since n = {n} exceeds "
f"the utmost CUDA blocksize = {MAX_FUSED_SIZE}."
)
num_warps = 4
if BLOCK_SIZE >= 32768:
num_warps = 32
elif BLOCK_SIZE >= 8192:
num_warps = 16
elif BLOCK_SIZE >= 2048:
num_warps = 8
return BLOCK_SIZE, num_warps
Then, we implement the common softmax for the ahead move and equation (10) for the backward move. The one novelty right here in comparison with earlier articles is using cache modifiers, which inform the compiler how you can cache and evict information. For now, we’ll solely deal with three cache modifiers:
.ca(Cache in any respect ranges): Tells the compiler to load the information in each L1 and L2 cache, suggesting that it could be reused quickly. This modifier ought to be used when the information is sufficiently small to suit into L1 (~128–192KB per SM on an A100) and can probably be accessed repeatedly..cs(Streaming): Deal with information as streaming, it will likely be used as soon as after which discarded to release house in L1..wb(Write-back): Regular cached write, the information will stay within the cache hierarchy, good if the output could also be reused.
Within the following kernels, we’ll use the .ca modifier for hundreds since we carry out a number of operations on the loaded information. For storing, we’ll use .cs within the ahead move, because the outputs received’t be instantly reused and .wb within the backward move since within the context of autograd (i.e. the chain rule), gradient outputs will probably be consumed by downstream kernels.
Multi-Block Softmax
Now, let’s check out the web formulation of the softmax. On this part, we implement a multi-block variant of the earlier kernel. This model will use BLOCK_SIZE < n_cols, in different phrases, we’ll solely load a tile with BLOCK_SIZE parts at a time, just like how we dealt with tiled GEMM within the last tutorial. Now you would possibly ask “how can we choose the block measurement?”.
It is a nice event to introduce Triton’s autotune utility. Supplied with a listing of configuration, autotune will carry out a grid-search to find out and cache the perfect configuration for a selected enter form. This course of is repeated each time a brand new enter form is handed to the kernel.
Right here, we carry out a grid search over the block measurement and variety of warps utilizing the next utility perform:
from itertools import product
# --- Multi Block Tuning ---
BLOCK_SIZES = [256, 512, 1024, 2048, 4096, 8192]
NUM_WARPS = [2, 4, 8, 16]
def get_autotune_config(
block_sizes: record[int], num_warps: record[int]
) -> record[triton.Config]:
return [
triton.Config(kwargs={"BLOCK_SIZE": bs}, num_warps=nw)
for (bs, nw) in list(product(block_sizes, num_warps))
]
We will now embellish our multi-block kernels with autotune and move the record of configs, key=”n_cols” signifies that the optimum config depends on the variety of columns of the enter.
The implementation of those kernels is conceptually very near the web softmax we lined earlier than, the principle variations is that we iterate over tiles (not over single parts like in Numpy), which requires some changes. As an example, we add a sum over the tile within the d replace and the backward kernel now requires two iterations as nicely.
Be aware: the PyTorch wrapper is strictly the identical besides we delete the road the place BLOCK_SIZE and num_warps are declared (since they’re picked by autotune).
Testing and Benchmarking
We will now execute a ahead and backward move with each kernels and guarantee they match the PyTorch baselines:
def validate_kernel(kernel_fn: callable) -> None:
machine = "cuda:0" if torch.cuda.is_available() else "cpu"
torch.random.manual_seed(0)
# Generate inputs
x = torch.randn((256, 512), machine=machine) # triton enter
x.requires_grad = True
xt = deepcopy(x) # torch enter
triton_output = kernel_fn(x)
torch_output = torch.softmax(xt, dim=1)
torch.testing.assert_close(triton_output, torch_output) # check fwd kernel
# Setup pretend labels
y = torch.zeros_like(x)
inds = (torch.arange(0, y.form[0]), torch.randint(0, 3, (y.form[0],)))
y[inds] = 1
# Outline loss and run backward move
loss_fn = torch.nn.CrossEntropyLoss()
loss = loss_fn(torch_output, y)
loss.backward()
# Save gradient tensor for later
torch_xgrad = xt.grad.detach().clone()
triton_loss = loss_fn(triton_output, y)
triton_loss.backward()
torch.testing.assert_close(x.grad, torch_xgrad) # check grad outputs
validate_kernel(softmax_sb)
validate_kernel(softmax_mb)
Lastly, we benchmark our implementation in opposition to the PyTorch baseline utilizing the next snippet:
# --- Supply: Triton softmax tutorial ---
@triton.testing.perf_report(
triton.testing.Benchmark(
x_names=["N"], # argument names to make use of as an x-axis for the plot
x_vals=[
128 * i for i in range(2, 100)
], # completely different attainable values for `x_name`
line_arg="supplier", # argument title whose worth corresponds to a unique line within the plot
line_vals=[
"triton_single_block",
"triton_multi_block",
"torch",
], # attainable values for `line_arg``
line_names=[
"Triton_single_block",
"Triton_multi_block",
"Torch",
], # label title for the strains
kinds=[("blue", "-"), ("green", "-"), ("red", "-")],
ylabel="GB/s", # label title for the y-axis
plot_name="softmax-performance", # title for the plot. Used additionally as a file title for saving the plot.
args={"M": 4096}, # values for perform arguments not in `x_names` and `y_name`
)
)
def benchmark(M, N, supplier):
x = torch.randn(M, N, machine=DEVICE, dtype=torch.float32)
stream = getattr(torch, DEVICE.kind).Stream()
getattr(torch, DEVICE.kind).set_stream(stream)
if supplier == "torch":
ms = triton.testing.do_bench(lambda: torch.softmax(x, axis=-1))
if supplier == "triton_single_block":
torch.cuda.synchronize()
ms = triton.testing.do_bench(lambda: softmax_sb(x))
torch.cuda.synchronize()
if supplier == "triton_multi_block":
torch.cuda.synchronize()
ms = triton.testing.do_bench(lambda: softmax_mb(x))
torch.cuda.synchronize()
gbps = lambda ms: 2 * x.numel() * x.element_size() * 1e-9 / (ms * 1e-3)
return gbps(ms)
benchmark.run(show_plots=True, print_data=True)
Excellent news! Our single-block kernel persistently outperforms the PyTorch baseline whereas the multi-block variant falls off for inputs with greater than 6k columns:

Contemplating bigger inputs, we will make a number of observations:
- The multi-block kernel finally stabilises round 900GB/s of throughput, surpassing the PyTorch baseline for inputs with greater than 30k columns.
- Curiously, it looks as if the multi-block variant will dominate for inputs with greater than 60k columns.
- Though we exceed the utmost block measurement with the single-block variant, the kernel nonetheless runs easily for some purpose. Certainly, Triton routinely manages the block measurement below the hood.
Whenn_colsis bigger than the {hardware} restrict, Triton will break down the enter and iterate over it. Nevertheless, this appears to be slower than the multi-block method.
To go additional, we may mix each approaches in a single kernel that explicitly selects the optimum kernel based mostly on the enter measurement. This fashion, we’d profit from the excessive efficiency of the single-block kernel for small inputs and the upper throughput of the multi-block variant for inputs with greater than 60k columns.

This concludes the third episode of this Triton collection, thanks once more to your help!
Within the subsequent article, we’ll leverage the web softmax formulation within the context of Flash Consideration.
Till subsequent time! 👋
