Kimi-K2.6 · original · l12_default_gpt
correct 28_BMM_InstanceNorm_Sum_ResidualAdd_Multiply.py
model
Kimi-K2.6
turns / max
5 / 10
tool calls
5
tokens (total)
0
wall clock
—
truncated
no
backend
cuda fp32
variant
original
runtime
2.71 μs
ref runtime
2.79 μs
speedup
1.03x
started
2026-05-02T17:48:57Z
timingkernelbench.timing
kernel runtime
2.71 μs
ref runtime
2.79 μs
speedup
1.03x
kernel mean / median / std
2.71 / — / 0.00 μs
ref mean / median / std
2.79 / — / 0.00 μs
numerical precisioneval_kernel_against_ref
max abs error
9.54e-07
mean abs error
1.35e-08
max rel error
0.90
mean rel error
1.78e-07
gpu memoryextended_metrics.measure_memory
kernel peak
673.06 MB
ref peak
673.07 MB
kernel / ref
1.00x
kernel launches / fusiontorch.profiler
kernel launches
7
ref launches
31
fusion ratio (ref / kernel)
4.43x
total cuda time
5601 μs
energyNVML (pynvml)
kernel mJ / run
1224.38
ref mJ / run
2643.60
ratio (ref / kernel)
2.16x
avg power
452.69 W
ref avg power
946.98 W
SOL (speed-of-light)nsight_hardware_counters
SOL score (0–1)
0.859
dram util %
85.9%
compute util %
84.3%
bottleneck
memory-bound
dominant pipe
FP32
arithmetic intensity
—
ridge point
20.00
roofline / occupancynsight_hardware_counters
dram bandwidth
2878.45 GB/s
dram util %
85.9%
fp32 tflops
—
fp32 util %
—
fp16 tflops
—
occupancy %
95.7%
bottleneck
memory-bound
dominant pipe %
84.3%
arithmetic intensity
—
ridge point
20.00
L1 hit %
—
L2 hit %
117.6%
ld sectors / req
20.00
st sectors / req
—
regs / thread
286
smem / block
36480 B
block size
384
peak bw
3350.00 GB/s
peak fp32 tflops
67.00
peak fp16 tflops
1979.00
warp stalls (top 5)nsight
long_scoreboard
9407.5%
mio_throttle
188.4%
short_scoreboard
175.8%
reference PyTorch source (the prompt the agent sees)
import torch
import torch.nn as nn

class Model(nn.Module):
    """
    Model that performs a batch matrix multiplication, instance normalization, summation, residual addition, and multiplication.
    """
    def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1):
        super(Model, self).__init__()
        self.bmm = nn.Linear(in_features, out_features)
        self.instance_norm = nn.InstanceNorm2d(out_features, eps=eps, momentum=momentum)

    def forward(self, x, y):
        """
        Args:
            x (torch.Tensor): Input tensor of shape (batch_size, in_features).
            y (torch.Tensor): Input tensor of shape (batch_size, out_features).

        Returns:
            torch.Tensor: Output tensor of shape (batch_size, out_features).
        """
        x = self.bmm(x)
        x = self.instance_norm(x.unsqueeze(1).unsqueeze(1)).squeeze(1).squeeze(1)
        x = x + y
        x = x * y
        return x

batch_size = 1024  # Increased batch size
in_features = 8192  # Increased input features
out_features = 8192  # Increased output features

def get_inputs():
    return [torch.rand(batch_size, in_features), torch.rand(batch_size, out_features)]

def get_init_inputs():
    return [in_features, out_features]
turn 0 · 1 tool call(s) · 105.3s turn · 105.3s LLM · 45,725 chars (click to expand)
turn 0105.3s turn · 105.3s LLM · 0.0s tools
reasoning
We need to write a custom CUDA kernel for the forward of a model that does: 1. Linear(x) where x shape (batch_size, in_features), weight shape (out_features, in_features), bias shape (out_features). 2. InstanceNorm2d on the output, but note the weird unsqueeze(1).unsqueeze(1). The output of linear is (batch_size, out_features). Then unsqueeze to (batch_size, 1, 1, out_features). InstanceNorm2d with num_features=out_features operates over spatial dims (H=1, W=1) and computes per-channel mean/var across batch and spatial dims? Wait: nn.InstanceNorm2d normalizes across the batch and spatial dimensions for each channel. Input is (N, C, H, W). It computes mean and var over (N, H, W). So with H=1, W=1, it computes mean/var over batch size dimension, per channel. So effectively it's computing per-channel mean and variance across the batch (since spatial dims are 1). That is equivalent to batch normalization without tracking running stats? Actually instance norm per channel across each instance? Wait instance norm is per sample, per channel across spatial dims. But here spatial dims are 1, H=1, W=1. The standard instance norm computes mean and variance across H and W for each sample and channel independently. But the unsqueeze makes H=1, W=1. Thus mean = the value itself, variance = 0? Wait: InstanceNorm2d with affine=False or default affine=False? In reference they create nn.InstanceNorm2d(out_features, eps=eps, momentum=momentum). Default affine=False, track_running_stats=False? Actually nn.InstanceNorm2d default track_running_stats=False. Let's check PyTorch defaults: nn.InstanceNorm2d(num_features, eps=1e-5, momentum=0.1, affine=False, track_running_stats=False). So no affine parameters. It computes mean and var across (N, H, W) for each channel? Wait no: InstanceNorm2d computes mean and var across the spatial dimensions HxW for each sample and channel separately. But track_running_stats=False (default) means it doesn't use running stats. So for each channel c, for each sample n, compute mean over H,W. Since H=W=1, mean = x[n, c], var = 0. Then normalized = (x - mean) / sqrt(var + eps) = (x - x) / sqrt(eps) = 0. So the instance norm output would be all zeros? That seems suspicious. Let's verify. Wait, need to read PyTorch docs carefully. InstanceNorm2d: "Applies Instance Normalization over a 4D input (a mini-batch of 2D inputs with additional channel dimension) as described in the paper Instance Normalization: The Missing Ingredient for Fast Stylization. The input is expected to be of size (N, C, H, W). InstanceNorm2d computes the mean and standard-deviation using the dimensions N and H and W? Actually the docs: "The mean and standard-deviation are calculated per-dimension separately for each object in a mini-batch." But I need to check the exact dimensions. From PyTorch source: instance_norm calls batch_norm with a different definition. For InstanceNorm, the mean and variance are computed over the dimensions [2,3] (spatial) only, not over N. Wait, but there is also a parameter `use_input_stats` and `track_running_stats`. Let's look at the implementation. In PyTorch's functional.py: F.instance_norm(input, weight, bias, running_mean, running_var, use_input_stats, momentum, eps). It calls torch.batch_norm(input, weight, bias, running_mean, running_var, training, momentum, eps, torch.backends.cudnn.enabled) but with a view that groups the batch and channel dims? Actually no. Let's check. Looking at PyTorch code: For instance_norm, if input is 4D, they view it as (1, N*C, H, W) and then apply batch norm? Wait that's for group norm. I recall: For instance norm, the operation is equivalent to group norm with num_groups = num_channels. And group norm reshapes (N, C, H, W) to (N, num_groups, C//num_groups, H, W) and computes mean/var over (C//num_groups, H, W). Since num_groups = C, each group has 1 channel, so mean/var are computed over (1, H, W) per sample. So for each sample n and channel c, compute mean and var over the spatial dims HxW (which is just 1x1). So mean = x[n, c, 0, 0], var = 0. Then normalized = 0 / sqrt(eps) = 0. Indeed. But is that the intended semantics? The comment says "instance normalization", maybe they intended instance norm over the batch and spatial dims because unsqueeze makes it 4D? But instance norm with H=W=1 is trivial. Could the reference be intentionally trivial? Or maybe I misread: The `bmm` is nn.Linear, not batch matrix multiplication. They wrote `self.bmm = nn.Linear(in_features, out_features)`. Then forward: x = self.bmm(x). x shape (batch_size, out_features). Then x.unsqueeze(1).unsqueeze(1) shape (batch_size, 1, 1, out_features). nn.InstanceNorm2d(out_features) expects C = out_features. But note the tensor shape: (N, C, H, W) = (batch_size, out_features, 1, 1)? Wait: unsqueeze(1) adds a dim at index 1: (batch_size, 1, out_features). Then unsqueeze(1) again? Actually they call `.unsqueeze(1).unsqueeze(1)`. Let's trace: x is (B, out_features). x.unsqueeze(1) -> (B, 1, out_features). x.unsqueeze(1).unsqueeze(1) -> (B, 1, 1, out_features). But nn.InstanceNorm2d expects (N, C, H, W). So if input is (B, 1, 1, out_features), then C=1, not out_features. Wait, maybe they intended to unsqueeze(-1).unsqueeze(-1)? Because unsqueeze(1) twice inserts dims at position 1, resulting in shape (B, 1, 1, out_features). In PyTorch, nn.InstanceNorm2d(out_features) would complain because num_features=out_features but actual channels=1? Actually PyTorch would check that the number of channels matches `num_features`. If input has shape (N, C, H, W), it checks C == num_features. In this case C=1, num_features=out_features (8192). So it would raise an error unless out_features=1. So the reference as written would crash with the given dimensions. Did the user make a mistake? Let's re-read. ```python x = self.bmm(x) x = self.instance_norm(x.unsqueeze(1).unsqueeze(1)).squeeze(1).squeeze(1) ``` This is indeed wrong for out_features != 1. But maybe they meant `unsqueeze(-1).unsqueeze(-1)` to get (B, out_features, 1, 1)? That would make sense. The comment says "batch matrix multiplication, instance normalization, summation, residual addition, and multiplication." If x becomes (B, out_features, 1, 1), instance norm over spatial dims 1x1 yields all zeros? Still trivial. Wait, maybe they intended `nn.InstanceNorm1d`? If x is (B, out_features), then instance norm 1d with num_features=out_features expects (N, C, L) or (N, C). For InstanceNorm1d, input shape can be (N, C) or (N, C, L). If (N, C), it computes mean and var over N? Actually InstanceNorm1d on (N, C) computes per-channel mean and variance across the batch? Let's check. PyTorch InstanceNorm1d: "The input is expected to be of size (N, C, L) or (N, C). InstanceNorm1d computes the mean and standard-deviation using the dimensions N and L? Wait国家标准. Actually for InstanceNorm1d, if input is 2D (N, C), the mean and standard-deviation are computed over the batch dimension N for each channel C? No, that's BatchNorm1d. Let's check the docs. From PyTorch docs: For InstanceNorm1d: "The mean and standard-deviation are calculated per-dimension separately for each object in a mini-batch. γ and β are learnable parameter vectors of size C (if affine is True)." And: "Input: (N, C) or (N, C, L)". So for 2D input, it normalizes each channel across the batch? Let's verify with code mentally: If input is (N,C), and instance norm per object (i.e., per sample), then each sample has C features. But normalization per sample across C features would be like layer norm? Actually "per-dimension separately for each object" means for each object (sample), for each channel dimension? No, "per-dimension" means per channel. "separately for each object in a mini-batch" means for each sample, compute stats across some dimensions. For InstanceNorm1d on (N, C, L), stats are computed over L for each (N, C). For (N, C), what are the stats computed over? I think for 2D, it's equivalent to L=1, so stats are computed over nothing? Let's check PyTorch source. In F.instance_norm, the input is reshaped to (1, N*C, *). Actually instance_norm uses `view(1, N * C, ...)` and then calls batch_norm. Wait, that's group norm. Let's look up exact code. Actually, the implementation of instance_norm is: if input.dim() == 2 or input.dim() == 3: - For 3D (N, C, L): reshape to (1, N*C, L) and apply batch norm with batch size 1, num_features N*C? Not exactly. Let's recall: batch_norm on (N, C, H, W) computes stats over N, H, W. Group norm groups channels. Instance norm is group norm with num_groups = C. For 2D/3D data, it becomes more complex. In PyTorch, F.instance_norm handles 2D, 3D, 4D, 5D. I found in PyTorch source: `def instance_norm(input, running_mean, running_var, weight, bias, use_input_stats, momentum, eps):` ``` dim = input.dim() if dim == 2: # N, C -> N, C, 1 input = input.unsqueeze(2) # ... ``` Wait, let's search memory. I think in PyTorch's `functional.py`, instance_norm is implemented as: ```python def instance_norm(input, running_mean=None, running_var=None, weight=None, bias=None, use_input_stats=True, momentum=0.1, eps=1e-5): if not use_input_stats and (running_mean is None or running_var is None): raise ValueError('Expected running_mean and running_var to be not None when use_input_stats=False') return torch.batch_norm( input, weight, bias, running_mean, running_var, use_input_stats, momentum, eps, torch.backends.cudnn.enabled) ``` No, that's too simple. Actually `torch.batch_norm` expects stats over N dimension. For instance norm, they might reshape the input. Wait, I'm overcomplicating. Let's just think about what the reference actually does given the shapes. Since the reference as written would error with out_features=8192, there must be a mistake in my understanding of unsqueeze. Let's re-evaluate: x shape: (batch_size, out_features) = (1024, 8192). x.unsqueeze(1) -> shape (1024, 1, 8192). Then .unsqueeze(1) again -> shape (1024, 1, 1, 8192). nn.InstanceNorm2d(out_features=8192) expects input of shape (N, C, H, W) where C = 8192. But here C = 1. So it would error. So either the reference code is flawed, or the evaluation environment expects us to replicate the behavior of the flawed code? But the evaluation environment must run the reference to compare outputs. If the reference errors, the evaluation can't run. So perhaps my shape analysis is wrong: In PyTorch, `unsqueeze(1)` inserts a dimension at index 1. `unsqueeze(1)` again inserts a dimension at index 1 (shifting the previous one to index 2). So: Start: x: [B, F] after unsqueeze(1): [B, 1, F] after unsqueeze(1): [B, 1, 1, F] Yes, that is correct. So C=1, F=8192. That mismatches InstanceNorm2d(8192). Unless PyTorch's InstanceNorm2d accepts other shapes? No, it checks num_features against channel dimension. Wait, maybe they meant `unsqueeze(-1).unsqueeze(-1)`? If so, shape would be [B, F, 1, 1], which works with C=F=8192. And the squeeze(1).squeeze(1) would error because squeezing dim 1 (which is F) would not remove it if F>1. Actually squeeze(1) on [B, F, 1, 1] would leave [B, F, 1, 1] if F>1. Wait, squeeze(dim) only removes the dimension if its size is 1. Since F=8192, squeeze(1) does nothing. So they would need squeeze(-1).squeeze(-1) to get back to [B, F]. But they wrote squeeze(1).squeeze(1). That matches unsqueeze(1).unsqueeze(1) because those insert dims of size 1 at positions 1 and 2. Then squeeze(1) removes the first inserted dim, squeeze(1) again removes the second (now at position 1). So that part is consistent. The only inconsistency is the channel dimension. Unless... nn.InstanceNorm2d(out_features) applied to (B, 1, 1, out_features) does not error because PyTorch treats the input as (N, C, H, W) where C is the second dimension. If C=1, then it mismatches out_features. So it must error. Could the user have swapped in_features and out_features in the linear? In their init: `self.bmm = nn.Linear(in_features, out_features)`. So weight shape (out_features, in_features). x is (B, in_features). Output is (B, out_features). That is correct. Let's test with a small script mentally: `m = nn.InstanceNorm2d(3); x = torch.randn(2,1,1,3); m(x)` -> error: `Given normalized_shape=(3,), expected input with shape [*, 3], but got input of size[2, 1, 1, 3]`? Wait, InstanceNorm2d uses `torch.nn.functional.instance_norm`. Let's check the exact error. In PyTorch, `nn.InstanceNorm2d(3)` creates a layer that checks input shape on forward. The code for `_InstanceNorm` (base class) forward calls `F.instance_norm(...)`. But before that, `_check_input_dim` is called. For `_InstanceNorm`, `_check_input_dim` checks that `input.dim()` is one of expected dims. For `InstanceNorm2d`, it expects 4D input. It might also check that `input.size(1) == self.num_features`. Yes, in `nn.modules.batchnorm._NormBase.forward`, there is a check: `if input.size(1) != self.num_features: raise ValueError(...)`. Actually, the base class for instance norm checks this. So it would error. Wait, maybe they are using `nn.InstanceNorm2d(out_features, affine=False)` but not checking? No, the check exists. However, the user might have made a typo in the problem statement but the actual evaluation code might have corrected shapes, or perhaps the dims are different? Let's re-read the task description carefully. "Model that performs a batch matrix multiplication, instance normalization, summation, residual addition, and multiplication." Could `self.bmm` actually be something else? No, it's defined as `nn.Linear(in_features, out_features)`. But maybe they meant `bmm` as a placeholder. Given that the reference code as provided seems broken, but the evaluation must run it, perhaps PyTorch's `nn.InstanceNorm2d` with `track_running_stats=False` does not check channel count? No, it definitely does. Wait, there's another possibility: The input `x` after linear is (batch_size, out_features). Then `x.unsqueeze(1).unsqueeze(1)` yields (batch_size, 1, 1, out_features). Then `self.instance_norm` is `nn.InstanceNorm2d(1, eps=eps, momentum=momentum)`? But they passed `out_features` as num_features. Not 1. Unless `out_features` is 1? But they set `out_features = 8192`. Could this be a trick question where the reference is actually `nn.InstanceNorm2d(out_features, ...)` and the unsqueeze operations are on a tensor of shape (batch_size, out_features, 1, 1)? Maybe they wrote unsqueeze(1) when they meant unsqueeze(2).unsqueeze(2)? No. Let's search my memory: There are known problems from some coding challenge sites (like LeetCode, Kaggle, etc.) where they ask to optimize a PyTorch model. I recall a problem similar to this. Let's think. Maybe the instance norm is actually `nn.InstanceNorm2d(out_features)` applied to a tensor of shape (batch_size, out_features, 1, 1) but the code in the prompt has a typo. However, in the actual test harness, the reference might be correct. But we are asked to replace the forward computation of the PyTorch model below. The harness likely runs the provided `Model` class. If the provided class is broken, the harness might fail before even evaluating our kernel. The problem statement is what we have to replicate. We could try to replicate the code exactly, even if it seems broken, but then our kernel would need to produce the same outputs as the reference. If the reference crashes, what does the harness do? Probably the harness uses a corrected version or runs exactly this code. Wait, perhaps I misread: `self.instance_norm = nn.InstanceNorm2d(out_features, eps=eps, momentum=momentum)`. Then in forward: `x = self.instance_norm(x.unsqueeze(1).unsqueeze(1)).squeeze(1).squeeze(1)`. Actually, if x is (B, out_features), and you `unsqueeze(1)` -> (B, 1, out_features). Then `unsqueeze(1)` -> (B, 1, 1, out_features). In PyTorch, `nn.InstanceNorm2d` on a 4D tensor of shape (N, C, H, W) uses C = out_features? No, C = 1. But maybe the layer is actually `nn.InstanceNorm2d(1)`? But they passed `out_features`. Unless `out_features` is a variable that equals 1? No. Alternatively, could it be that `nn.InstanceNorm2d` treats the channel dim as the last dimension for some reason? No. Let's consider the possibility that the user meant `x.unsqueeze(-1).unsqueeze(-1)`. That would produce (B, out_features, 1, 1). Then `nn.InstanceNorm2d(out_features)` works. Then `.squeeze(1).squeeze(1)` would not remove anything because dim 1 is out_features (8192). But `.squeeze()` without arguments removes all dims of size 1, so `.squeeze()` would give (B, out_features). However they wrote `.squeeze(1).squeeze(1)`. If they used `unsqueeze(-1).unsqueeze(-1)`, then `squeeze(1)` does nothing (dim 1 size is 8192), `squeeze(1)` again does nothing. So output remains (B, out_features, 1, 1). That would be wrong. But if they used `squeeze(-1).squeeze(-1)`, that would work. So the squeezes also match the unsqueezes only if unsqueeze was done on dims 1 and 2. Wait, let's re-evaluate: If x is (B, out_features). unsqueeze(1) -> (B, 1, out_features). unsqueeze(2) -> (B, 1, 1, out_features). But they did unsqueeze(1) twice. So the inserted dims are at positions 1 and 2? Actually after first unsqueeze(1), shape is [B, 1, out_features]. Then unsqueeze(1) inserts at index 1 again, pushing the previous dim to index 2: shape [B, 1, 1, out_features]. So inserted dims are at positions 1 and 2. After instance norm, they do squeeze(1) which removes dim at index 1 (size 1). Then squeeze(1) which removes the new dim at index 1 (size 1). So back to [B, out_features]. So the code is self-consistent in insertion and removal, but inconsistent with InstanceNorm2d's expected channel count. Could it be that `nn.InstanceNorm2d` does NOT check channel count when `affine=False`? Let's check the PyTorch source. The `forward` method of `_InstanceNorm` (derived from `_NormBase`) calls `_check_input_dim` which is overridden in `InstanceNorm2d`. Let's check `_check_input_dim` for `InstanceNorm2d`. It likely checks `if input.dim() != 4: raise ValueError`. It might also not check the channel size. Actually, `_NormBase` has a `num_features` attribute, and its `forward` method does: ```python def forward(self, input: Tensor) -> Tensor: self._check_input_dim(input) # ... ``` Where does it check `input.size(1) == self.num_features`? That is typically in `BatchNorm`. For instance norm, maybe `_check_input_dim` only checks dimensions, not channel count. Let's check memory: In `nn.modules.instancenorm`, the class `InstanceNorm2d` inherits from `_InstanceNorm`. `_InstanceNorm` inherits from `_NormBase`. In `_NormBase.__init__`, `self.num_features = num_features` is stored. But does `_InstanceNorm` check channel count? I'm not 100% sure. In `BatchNorm`, `_check_input_dim` checks channel count because batch norm uses `num_features` to define running_mean shape. But `InstanceNorm` by default does not have running stats. However, even if `track_running_stats=False`, `num_features` is still stored. Let's check `nn.InstanceNorm2d` source. I can approximate: In PyTorch source `torch/nn/modules/instancenorm.py`: ```python class InstanceNorm2d(_InstanceNorm): def _check_input_dim(self, input): if input.dim() != 4: raise ValueError('expected 4D input (got {}D input)'.format(input.dim())) ``` It might NOT check `input.size(1) == self.num_features`. Because instance norm doesn't need `num_features` for its computation (unless affine=True or track_running_stats=True). Actually, if `affine=False` and `track_running_stats=False`, `num_features` is completely unused. The running_mean and running_var are None. Weight and bias are None. So it doesn't matter what `num_features` is. The `num_features` argument is just there for API consistency. So `nn.InstanceNorm2d(8192)` applied to input of shape (B, 1, 1, 8192) might work! Wait, but what does it compute? The instance norm normalizes per channel (dim 1). Since C=1, it computes mean and var across (N, H, W) for that single channel. So the entire tensor is considered as one channel. It computes one mean and one var across all elements (batch * 1 * 1 = batch), then normalizes each element by subtracting that global mean and dividing by global std. That is, it does a global normalization over the entire batch, not per-feature. But wait, instance norm computes stats per channel, not batch. Let's verify with PyTorch docs: For InstanceNorm2d on input (N,C,H,W), it computes mean and var over (N, H, W) for each channel c. Actually, there is confusion between instance norm and batch norm. Wait, let's get this straight once and for all. Instance Normalization (Ulyanov et al.) normalizes each sample independently across channels and spatial dimensions? No. Instance norm normalizes each channel for each sample independently, i.e., for each sample n and channel c, compute mean over HxW. So stats are per (n, c). The formula is: y_{n,c,h,w} = (x_{n,c,h,w} - mean_{n,c}) / sqrt(var_{n,c} + eps) where mean_{n,c} = 1/(HW) sum_{h,w} x_{n,c,h,w}. Thus for each sample and each channel, it normalizes across spatial dims. Group norm normalizes per sample, per group of channels across spatial dims. For group norm with num_groups = C, it becomes instance norm. This matches what I said. However, there is also `LayerNorm` which normalizes per sample across all channels and spatial dims. But PyTorch's `InstanceNorm2d` with `track_running_stats=False` and `affine=False` does exactly the above: per (N, C) statistics over H, W. Wait, is there any variant where instance norm computes stats over (N, H, W) per channel? That would be batch norm without running stats (i.e., batch norm in training mode). But batch norm uses running stats and affine by default. Some people confuse instance norm with "batch norm per channel across batch and spatial". Let's check the PyTorch source for `instance_norm`. In `aten/src/ATen/native/Normalization.cpp`, there is a function `instance_norm`. It takes input, weight, bias, running_mean, running_var, use_input_stats, momentum, eps. The implementation might call `batch_norm` with a reshaped input. Let's recall. Actually, I think the confusion arises because PyTorch's `instance_norm` is implemented by calling `batch_norm` on a reshaped tensor. For a 4D input (N, C, H, W), to compute per-(N,C) stats over H and W, you can reshape to (1, N*C, H, W) and apply batch norm (which computes stats over batch and spatial dims). Wait, if you reshape to (1, N*C, H, W) and apply batch norm, it would compute stats over the batch dimension (size 1) and spatial dims (H, W), giving per-(N*C) stats, which is per sample per channel across spatial dims. Yes! That is the trick. So for input (N, C, H, W): - Reshape to (1, N*C, H, W) - Apply batch norm (with batch size 1). Batch norm computes mean and var over N_batch (which is 1) and H, W, resulting in per-channel stats for the reshaped input, which correspond to per-(N,C) stats in the original. - Then reshape back. Thus instance norm is implemented using batch norm on a reshaped tensor. Given that, for input (B, 1, 1, F): - Reshape to (1, B*1, 1, F) = (1, B, 1, F) - Batch norm computes stats over N=1, H=1, W=F for each channel c in {1..B}. Wait, the reshaped tensor has channels = B. For each channel b (0..B-1), BN computes mean over N=1, H=1, W=F, i.e., mean over the F elements of sample b. So it normalizes each sample's features across the feature dimension! That is, for each sample b, compute mean and var over the out_features dimension (since W=F). That is exactly layer normalization per sample! But note: BN on (1, B, 1, F) computes per-channel stats. Channel dimension is B (number of samples). Spatial dims are H=1, W=F. BN computes mean over N (batch size of BN) = 1 and H=1 and W=F. So for each original sample b, it computes mean across the F features. That is, per-sample feature normalization. This is often called "layer normalization" in some contexts? Actually layer norm normalizes per sample across all features (and spatial/channels). But here it's per sample across the last dimension (F). Since H=1, it's across F. Wait, let's check the reshape: original input (N, C, H, W) = (B, 1, 1, F). Reshape to (1, N*C, H, W) = (1, B, 1, F). Batch norm on (1, B, 1, F) with num_features = B. BN computes mean over N=1, H=1, W=F for each channel b. So for channel b, mean = average of sample b's F features. Var = variance of sample b's F features. Then normalizes each feature of sample b by that sample's mean and var. So output (after BN) is (1, B, 1, F). Reshape back to (B, 1, 1, F). Then squeeze -> (B, F). Thus the overall effect is: for each sample in the batch, compute mean and variance across the `out_features` dimension, and normalize the linear output per-sample across features. That is NOT instance norm in the usual sense (which would be per-channel per-sample across spatial dims). But because of the weird unsqueeze arrangement, it does per-sample normalization across the feature vector. Wait, is that correct? Let's verify with a tiny script. I can't run code here, but I can reason. Actually, for `nn.InstanceNorm2d(num_features)`, the running_mean and running_var are shaped (num_features,) if track_running_stats=True. But default is False. The internal implementation of `instance_norm` in PyTorch's C++ does not use the `num_features` argument for anything else if there are no parameters. But does it reshape (N, C, H, W) to (1, N*C, H, W)? The C++ code for `instance_norm` is likely: ```cpp std::tuple<Tensor, Tensor, Tensor> instance_norm( const Tensor& input, const Tensor& weight, const Tensor& bias, const Tensor& running_mean, const Tensor& running_var, bool use_input_stats, double momentum, double eps) { // ... auto input_reshaped = input.unsqueeze(0).view({1, input.size(0) * input.size(1), input.size(2), input.size(3)}); auto out = at::batch_norm(input_reshaped, weight_, bias_, running_mean_, running_var_, use_input_stats, momentum, eps, cudnn_enabled); return out.view(input.sizes()); } ``` Wait, `input.unsqueeze(0)` makes it (1, N, C, H, W). Then view to (1, N*C, H, W). Yes. So for input (B, 1, 1, F): - unsqueeze(0): (1, B, 1, 1, F) - view(1, B*1, 1, F): (1, B, 1, F). - batch_norm: N=1, C=B, H=1, W=F. - BN computes mean/var over N=1, H=1, W=F per channel. So per original sample. - Reshape back to (B, 1, 1, F). So the effect is per-sample normalization across the feature dimension. But wait, does BN compute over N, H, W? Yes, batch norm computes stats over dimensions N, H, W. It does NOT compute over C. So for reshaped input (1, B, 1, F), BN computes stats for each channel (of which there are B) over N=1, H=1, W=F. So it's exactly per-channel stats over W=F. Since H=1, no effect. Thus the instance norm layer in this specific shape configuration computes, for each sample i, the mean μ_i and variance σ_i^2 across the `out_features` dimension, and then normalizes x[i, j] as (x[i,j] - μ_i) / sqrt(σ_i^2 + eps). Then after instance norm, there is a residual addition: x = x + y, and x = x * y. y is a tensor of shape (batch_size, out_features), same as x after norm. So the full forward is: 1. x = Linear(x0) + b (x0 shape (B, in_features), weight W shape (out_features, in_features)) 2. For each sample i=0..B-1: μ_i = mean_j x[i, j] σ_i^2 = var_j x[i, j] (population var or unbiased? need to check PyTorch) x[i, j] = (x[i, j] - μ_i) / sqrt(σ_i^2 + eps) 3. x = x + y 4. x = x * y We need to implement this as a single fused CUDA kernel to be faster than PyTorch reference. Now, we need to know the exact variance computation: PyTorch uses biased or unbiased variance in instance norm? In batch norm, the running variance uses unbiased? Actually, batch norm computes the biased variance (dividing by N*H*W) for the normalization, and the unbiased variance (dividing by N*H*W - 1) is used for something else? Wait, in PyTorch's batch_norm, the `running_var` is updated using a biased or unbiased estimator? Let's check. In PyTorch's batch norm implementation, during training, it computes: - `mean` = sum / (N * H * W) - `var` = sum((x - mean)^2) / (N * H * W) [population variance] But when updating running_var, it uses `momentum * var + (1 - momentum) * running_var`. Wait, actually the running stats in batch norm use biased variance. Let's verify. In PyTorch's `torch/nn/functional.py`, `batch_norm` calls `_batch_norm_impl_index` which goes to ATen. In ATen's `batch_norm_cpu` or `batch_norm_cuda`, the variance computed for normalization is the unbiased or biased one? From the docs: At training time, batch norm uses the mean and variance of the current batch (population variance, i.e., divided by N). The running variance is updated with `running_var = momentum * var + (1 - momentum) * running_var`, where var is the population variance. Wait, let's check. Actually, some sources say PyTorch's BatchNorm uses biased variance (Bessel's correction not applied) for the batch statistics in training. It computes `var = mean(x^2) - mean(x)^2` or `sum((x-mean)^2)/N`. For the running variance, it uses the same. I think it's population variance (divided by N). Let's verify with a simple mental test: If input is [0, 0], batch size 2, feature size 1. Batch norm training: mean = 0, var = 0 (since both same). If unbiased, var = 0 too (divided by 1). So both give 0. For [0, 2], mean=1, var = ((0-1)^2 + (2-1)^2)/2 = 1. Unbiased = 2/1 = 2. Does PyTorch give 1 or 2 for the epsilon denominator? Let's see. I know that `torch.nn.BatchNorm1d` on training mode with input [0,2] (2 samples, 1 feature) yields normalized output [-1, 1] if var=1, or [-0.7071, 0.7071] if var=2. I recall that batch norm yields [-1, 1] in that case. So var=1 (population). Yes, PyTorch uses population variance (N) for normalization, not unbiased (N-1). However, there is a nuance: In batch norm, the variance used for normalization is computed as `var = sum((x-mean)^2) / (N*H*W)`. So it's population. But wait, for instance norm, does it also use population variance? Since it's implemented via batch_norm on reshaped input, yes, it uses the same variance calculation: `var = sum((x-mean)^2) / (N*H*W)`. Here N (batch size of the BN) is 1, H=1, W=F. So denominator = F. So it computes population variance across features: `var_i = sum_j (x[i,j] - μ_i)^2 / F`. But there is a subtlety: The instance norm layer might have `momentum` and `eps`. The `momentum` is irrelevant since `use_input_stats=True` and `track_running_stats=False` (default). The `eps` is used for numerical stability in the sqrt. So our kernel should compute: For each sample i in [0, B): μ_i = (1/F) * sum_j x[i,j] var_i = (1/F) * sum_j (x[i,j] - μ_i)^2 inv_std_i = 1 / sqrt(var_i + eps) For each feature j: out_norm[i,j] = (x[i,j] - μ_i) * inv_std_i Then: tmp[i,j] = out_norm[i,j] + y[i,j] out[i,j] = tmp[i,j] * y[i,j] x before norm is `x0 @ W^T + b`. We need to handle large sizes: batch_size = 1024, in_features = 8192, out_features = 8192. The PyTorch reference likely does: - Linear: x @ W.T + b. This is a large GEMM: (1024, 8192) x (8192, 8192). Wait, W shape is (out_features, in_features) = (8192, 8192). So GEMM is (1024 x 8192) * (8192 x 8192)? Actually linear computes x (B, in) @ W^T (in, out) -> (B, out). So M=1024, N=8192, K=8192. This is a large GEMM: 1024 * 8192 * 8192 * 2 FLOPs ~ 137 GFLOPs. This dominates. - InstanceNorm2d on (1024, 1, 1, 8192) using batch norm on reshaped (1, 1024, 1, 8192). This is kind of a row-wise reduction over 8192 elements for 1024 rows. This is memory bound but small compared to GEMM. - Elementwise add and mul: memory bound. So the main optimization opportunity is to fuse the linear, instance norm, add, and mul into a single kernel? But the linear is a huge GEMM. Fusing the rest with the GEMM output is possible if we write a custom matrix multiplication kernel that writes directly to the normalized output. However, writing a fast GEMM for 1024x8192x8192 from scratch in CUDA is extremely difficult to beat cuBLAS. But maybe we can call `torch.matmul` or `F.linear` and then fuse the norm+add+mul into a custom kernel that operates on the output, saving memory bandwidth. That would be a reasonable approach: keep cuBLAS for the GEMM, and then do a single fused kernel for the rest. The PyTorch reference does separate ops: linear -> instance norm (which might use several kernels) -> add -> mul. By fusing the post-processing, we can reduce memory round trips. Alternatively, we could try to call `torch.nn.functional.linear` and then write a kernel that does row-wise layer norm + add + mul. That should give a good speedup because the memory bandwidth after GEMM is significant. But wait, the reference uses `nn.InstanceNorm2d`. In PyTorch, applying instance norm to (B,1,1,F) via `nn.InstanceNorm2d` might go through generic C++ code that is not particularly optimized, especially for this weird shape. It might involve multiple kernel launches: compute mean, compute var, normalize. Then squeeze and unsqueeze are views but might also cause copies? Actually squeeze is a view. But the instance norm itself might be slow because it's not a typical shape. So a fused kernel for the rest after linear is definitely beneficial. But can we fuse the bias addition into the normalization kernel as well? Yes. The linear produces output (B, out). We can launch a kernel over (B, out) elements that reads the linear output, computes per-row mean and var, normalizes, adds y, multiplies by y. But to compute mean and var, we need to read the entire row. In a naive element-wise kernel, each thread processes one element and would need to compute row mean by some cooperative reduction. A better approach is to have each block process one row (or multiple rows) and perform a reduction within the block. Since out_features = 8192, we can have a block of e.g., 256 or 1024 threads. But 8192 is large. We can do a two-stage reduction or use warp shuffle. Alternatively, we can call the linear with `matmul`, write output to a temporary buffer, then launch a per-row reduction kernel, store mean and inv_std in shared memory, then compute the final output. To avoid reading x twice (once for reduction, once for normalization), we could store the row in shared memory? 8192 floats per row is 32 KB. With a block processing one row, we could load the entire row into shared memory. But shared memory per SM is limited (e.g., 100KB). 32 KB is fine. Then each block of 256 threads loads 8192 floats: each thread loads 32 floats, stores in shared memory. Then compute mean via reduction. Then compute var via reduction on differences. Then compute normalized values, add y, multiply by y, and write out. But we also need to read y. And we need the bias from linear. Actually, we can compute x = input @ W^T + b. That is done by cuBLAS. So we have a buffer `gemm_out` of shape (B, out). Then we launch the fused kernel reading `gemm_out` and `y`. But maybe we can avoid writing `gemm_out` to global memory and then reading it back by using CUTLASS or something. But writing a custom GEMM is overkill and likely slower. However, we can use the fact that PyTorch's linear might support CUBLASLT epilogue fusion? But we are writing a custom kernel via `load_inline`. We cannot easily call CUBLASLT fused epilogues from Python unless we use torch's built-in linear. We can call `torch.nn.functional.linear` which uses cuBLAS under the hood. Then we launch our custom kernel. Will this be faster than the reference? The reference does linear (fast cuBLAS), then instance norm (which might be a sequence of reductions and elementwise ops), then add, then mul. Our approach does linear (same), then one fused kernel that does row-wise mean/var/normalize/add/mul. This saves several global memory passes. The speedup might be modest but should be sufficient. However, there is another potential issue: The reference uses `nn.InstanceNorm2d` which with `track_running_stats=False` and `affine=False` might actually be implemented via the "instance_norm" native function. Let's check how many kernels it launches. For the shape (B, 1, 1, F), it might dispatch to `batch_norm`. `batch_norm` on CUDA might launch a fast kernel. Let's see. Since it's `track_running_stats=False`, it might not be too bad. But still, it likely reads the data multiple times. To be safe and maximize speedup, we should fuse everything after linear into a single kernel. Let's design the fused kernel. We have: - `x`: output of linear, shape (B, F) - `y`: input, shape (B, F) - `eps`: float For each row i (0 <= i < B): mean = sum_j x[i,j] / F var = sum_j (x[i,j] - mean)^2 / F inv_std = rsqrtf(var + eps) for each j: out[i,j] = ((x[i,j] - mean) * inv_std + y[i,j]) * y[i,j] Wait, is the variance formula exactly sum((x-mean)^2)/F? Let's double-check PyTorch's instance norm implementation. As I reasoned, instance norm is implemented by reshaping and calling batch_norm. Batch norm computes `var` as `E[(X - mean)^2]` (population variance). Let's confirm by looking at PyTorch source or docs. From PyTorch docs for BatchNorm2d: " The mean and standard-deviation are calculated per-dimension over the mini-batches ... during training ... the very same statistics are used for normalization. ... By default, during training this layer keeps running estimates of its computed mean and variance, which are then used for normalization during evaluation. The running estimates are kept with a default momentum of 0.1. ... The standard-deviation is calculated via the biased estimator, equivalent to torch.var(input, unbiased=False)." Wait, does it say "biased estimator"? Let me check. Actually, I think the docs say: "The standard-deviation is calculated via the biased estimator, equivalent to torch.var(input, unbiased=False)." I'm not entirely sure if they explicitly mention "biased". But I believe batch norm uses population variance (unbiased=False). In PyTorch, the `running_var` is computed with unbiased=False? Let's check: In PyTorch's `batch_norm` backward, the variance used is `save_var`. In the implementation, `save_var` is computed as `1/(N*H*W) * sum((x-mean)^2)`. Yes, it's biased. But let's verify with a known fact: If you have a batch of size 1, BatchNorm will compute var = 0 (since all values are same as mean), and then output is all zeros divided by sqrt(eps). That uses population var (since N=1, unbiased would be dividing by 0, which is undefined). So they must use population. Thus instance norm on reshaped (1, B, 1, F) will compute for each channel (which is each original sample): - mean = sum over N=1, H=1, W=F of the values, divided by F. - var = sum over N=1, H=1, W=F of (value - mean)^2, divided by F. So yes, denominator is F. One subtlety: In some implementations, `eps` is added inside the sqrt: `inv_std = 1 / sqrt(var + eps)`. That is standard. Another subtlety: Is `momentum` used? Since `track_running_stats=False` (default for InstanceNorm2d), `momentum` is irrelevant. The reference sets `momentum=0.1`, but it's not used. So our kernel should implement exactly that. Now, we need to write a CUDA kernel that performs this. Kernel design: Option A: One thread block per row (sample). Each block has `THREADS` threads (e.g., 256). We need to reduce 8192 floats. We can use shared memory for the row. Each thread loads `F / THREADS` floats. For F=8192, if THREADS=256, each thread loads 32 floats. If we use float4, each thread loads 8 float4s. But we also need to read `y` for the final computation. And we need to write `out`. Since F=8192 = 256 * 32, it's nicely divisible. Algorithm for one block per row: ```cuda __global__ void fused_kernel(const float* __restrict__ x, const float* __restrict__ y, float* __restrict__ out, int B, int F, float eps) { int row = blockIdx.x; if (row >= B) return; const float* row_x = x + row * F; const float* row_y = y + row * F; float* row_out = out + row * F; __shared__ float s_mean; __shared__ float s_invstd; // Step 1: each thread computes partial sum float sum = 0.0f; for (int j = threadIdx.x; j < F; j += blockDim.x) { sum += row_x[j]; } // Warp reduction then block reduction __shared__ float sdata[256]; sdata[threadIdx.x] = sum; __syncthreads(); for (int s = blockDim.x/2; s > 0; s >>= 1) { if (threadIdx.x < s) sdata[threadIdx.x] += sdata[threadIdx.x + s]; __syncthreads(); } if (threadIdx.x == 0) { s_mean = sdata[0] / F; } __syncthreads(); // Step 2: compute partial sum of squared diff float sum_sq = 0.0f; float mean = s_mean; for (int j = threadIdx.x; j < F; j += blockDim.x) { float diff = row_x[j] - mean; sum_sq += diff * diff; } sdata[threadIdx.x] = sum_sq; __syncthreads(); for (int s = blockDim.x/2; s > 0; s >>= 1) { if (threadIdx.x < s) sdata[threadIdx.x] += sdata[threadIdx.x + s]; __syncthreads(); } if (threadIdx.x == 0) { float var = sdata[0] / F; s_invstd = rsqrtf(var + eps); } __syncthreads(); // Step 3: compute output float invstd = s_invstd; for (int j = threadIdx.x; j < F; j += blockDim.x) { float val = (row_x[j] - mean) * invstd; float yval = row_y[j]; row_out[j] = (val + yval) * yval; } } ``` This is simple. However, reading `row_x` three times (for sum, sum_sq, and final output) costs memory bandwidth. But since we can't store 8192 floats per row in shared memory for all three passes (well, we can store 8192 floats ~32KB, which is okay), we could load the row into shared memory once, then do reductions and final computation from shared memory. That would reduce global memory reads of x to just one pass. But note that we also need to read y. Since y is only read once, it's fine. If we store x in shared memory: ```cuda __shared__ float s_x[8192]; // size F ``` But F might not be known at compile time. We can declare dynamically sized shared memory, or we can pass as template parameter if it's fixed. In this problem, F=out_features=8192 is fixed. But to make it general for the constructor arguments, we should handle arbitrary F. However, the problem says constructor arguments are `in_features, out_features, eps, momentum`. The test harness may instantiate with these arguments. It might use the default sizes or different ones. We should handle arbitrary out_features. But dynamic shared memory size is passed at kernel launch: `kernel<<<grid, block, shared_mem_size>>>`. In `load_inline`, we can write the shared memory array as `extern __shared__ float s_mem[];`. Or we can allocate a fixed maximum if we know the max. Since the problem doesn't specify constraints, using dynamic shared memory is better. Wait, but in the reference, out_features is a constructor argument. It could be any value. The test harness might create `ModelNew(in_features, out_features)`. So we need a kernel that works for arbitrary F. Using shared memory for the entire row might be problematic if F is large (e.g., > 48k floats = 192KB, exceeding shared memory). But the test will likely use the default values (8192). To be safe, we could not store the entire row in shared memory, but stream through it. However, using shared memory for the row is fine for F up to ~8192 (32KB). For 16384, it's 64KB, still okay on modern GPUs (max shared memory per block is 96KB or 164KB depending on architecture). We don't know the target GPU. Let's get GPU specs.
call → get_gpu_specs
callget_gpu_specs {}
result ← get_gpu_specs (ok)
okget_gpu_specs GPU specs for NVIDIA H100 80GB HBM3: total memory (runtime): 79.1 GB spec entry: H100 GPU Architecture: Hopper GPU Memory: 80GB Memory Bandwidth: 3.35 TB/s FP64 TFLOPS: 34 FP64 Tensor Core TFLOPS: 67 FP32 TFLOPS: 67 TF32 Tensor Core TFLOPS: 989 with sparsity BFLOAT16 Tensore Core TFLOPS: 1979 with sparsity FP16 Tensor Core TFLOPS: 1979 with sparsity FP8 Tensor Core TFLOPS: 3958 with sparsity INT8 Tensor Core TOPS: 3958 with sparsity Register File Size: 64K 32-bit registers per SM Maximum number of registers per thread: 255 Maximum number of thread blocks per SM: 32 Shared memory capacity per SM: 228 KB Maximum shared memory per thread block: 227 KB
turn 1 · 1 tool call(s) · 145.9s turn · 145.9s LLM · 68,552 chars (click to expand)
turn 1145.9s turn · 145.9s LLM · 0.0s tools
reasoning
Let me analyze the reference model: ```python class Model(nn.Module): def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1): super(Model, self).__init__() self.bmm = nn.Linear(in_features, out_features) self.instance_norm = nn.InstanceNorm2d(out_features, eps=eps, momentum=momentum) def forward(self, x, y): x = self.bmm(x) # (batch_size, out_features) x = self.instance_norm(x.unsqueeze(1).unsqueeze(1)).squeeze(1).squeeze(1) x = x + y x = x * y return x ``` Wait, there's something odd here. `self.bmm` is actually `nn.Linear`, not `nn.BMM`. Let me re-read... The `bmm` member is `nn.Linear(in_features, out_features)`. So it's a linear layer (matrix multiplication + bias). Then `instance_norm` on `x.unsqueeze(1).unsqueeze(1)`: - x starts as (batch_size, out_features) - unsqueeze twice gives (batch_size, 1, 1, out_features) - InstanceNorm2d with out_features channels, so it normalizes over (H, W) = (1, 1) - Wait, InstanceNorm2d normalizes over the spatial dimensions for each channel independently. With H=1, W=1, the mean is just the single value itself, and variance is 0... hmm. Wait, let me think more carefully. The input to InstanceNorm2d is (N, C, H, W). - N = batch_size (but instance norm treats each sample independently) - C = out_features - H = 1 - W = 1 For InstanceNorm, it computes mean and variance over H*W for each (N, C). Since H=W=1, each channel has only 1 value. - mean = that single value - var = 0 (or very small, clamped by eps) - normalized = (x - mean) / sqrt(var + eps) = 0 / sqrt(0 + eps) = 0 - Then gamma * normalized + beta = beta (the affine parameters) Wait, but the model has default `affine=True` in InstanceNorm2d. So output for each channel would be beta (learnable parameter). But during training with default momentum, the running stats would be updated. But wait... for inference (eval mode), it uses running stats. But the problem shows no eval() call, so it might be training mode. Actually, let me re-check. The reference implementation uses `self.instance_norm(x.unsqueeze(1).unsqueeze(1))`. Note the `.squeeze(1).squeeze(1)` afterwards. Wait, I need to be more careful. InstanceNorm2d on (N, C, H, W) = (batch_size, out_features, 1, 1). - In training mode: for each (n, c), compute mean over H*W = 1 element. var over 1 element = 0 (but biased/unbiased). - Actually for 1 element, unbiased sample variance is NaN or 0 depending on implementation. PyTorch typically uses biased variance for normalization. For a single element, var = 0. - So normalized = (x - x) / sqrt(eps) = 0 - Output = gamma * 0 + beta = beta - In eval mode: use running_mean and running_var. Unless these have been trained, they are 0 and 1. - So normalized = (x - 0) / sqrt(1 + eps) ≈ x - Output = gamma * x + beta Hmm, but this is a single forward pass, presumably in training mode (since model defaults to training). Let me think about what actually happens... Actually, I should consider how PyTorch's InstanceNorm2d behaves with spatial size 1x1. Looking at PyTorch source or documentation: - For affine=True (default), there are learnable parameters weight and bias of shape (C,) - The mean and var are computed across H, W for each N, C independently - For H=W=1: mean = the single value, var = 0 (since there's no variation) - But actually in PyTorch, for very small sample sizes or when unbiased is used, there might be edge cases. Wait, InstanceNorm2d doesn't support `track_running_stats` parameter? Let me check. Actually, InstanceNorm2d does NOT track running stats by default (`track_running_stats=False`). So during both training and eval, it computes batch statistics per instance. Actually in training mode with track_running_stats=False: it computes mean/var for each instance on the fly and doesn't update running stats. For H=W=1, mean = value, var = 0. So output = (value - value) / sqrt(0 + eps) * gamma + beta = 0 * gamma + beta = beta. Wait, but gamma and beta are initialized to ones and zeros by default! So the instance norm would output all zeros! Let me verify this mental model. For a (1024, 8192, 1, 1) tensor: - Each spatial location in each channel has exactly 1 value. - InstanceNorm normalizes across spatial dims per instance (n) and channel (c). - mean = that single value - var = 0 - out = (x - mean) / sqrt(var + eps) * gamma + beta = 0 + 0 = 0 But wait! Is `momentum` even used when `track_running_stats=False`? Let me check... Yes, momentum is used if track_running_stats=True. But InstanceNorm2d defaults to track_running_stats=False. Hmm, let me look at the actual PyTorch documentation... Actually, `nn.InstanceNorm2d` defaults: `eps=1e-5, momentum=0.1, affine=False, track_running_stats=False`. Wait, the constructor in the reference calls `nn.InstanceNorm2d(out_features, eps=eps, momentum=momentum)` without specifying `affine` or `track_running_stats`. So defaults are `affine=False` and `track_running_stats=False`. With `affine=False`: no gamma and beta parameters. With track_running_stats=False: don't track running stats. So for (N, C, 1, 1): - mean = x itself - var = 0 - output = (x - x) / sqrt(0 + eps) = 0 So the instance norm ALWAYS outputs zeros for 1x1 spatial size with affine=False! After instance norm: x = 0 (all zeros) Then x = x + y = 0 + y = y Then x = x * y = y * y = y^2 Wait, this seems too simple. Let me double check by actually considering if there might be some other behavior. If I'm right, the entire forward pass reduces to: 1. self.bmm(x) -- but result is thrown away because instance norm zeroes everything 2. instance_norm produces all zeros 3. x + y = y 4. x * y = y^2 But that would mean `self.bmm` parameters are completely irrelevant! That seems very odd for a benchmark. Let me reconsider. Hmm, wait. Let me re-read the model. In PyTorch's InstanceNorm, it computes variance for H*W=1. Let me check if unbiased variance estimator is used... No, PyTorch uses biased variance for normalization in batch norm and instance norm. But for 1 element, the variance is 0. The output is definitely 0. Actually, let me test this more carefully with PyTorch. Maybe I should try to understand the exact shape: x is (batch_size, out_features) x.unsqueeze(1) -> (batch_size, 1, out_features) x.unsqueeze(1).unsqueeze(1) -> Hmm wait, x.unsqueeze(1) makes it (B, 1, out_features). Then .unsqueeze(1) on THAT makes it (B, 1, 1, out_features). But InstanceNorm2d expects (N, C, H, W). So if it's (B, 1, 1, out_features) and C=1, that normalizes 1 feature with H=1, W=out_features... wait! OH! I see my mistake. Let me re-read: `x = self.bmm(x)` -> shape (batch_size, out_features) `x.unsqueeze(1)` -> (batch_size, 1, out_features) `x.unsqueeze(1).unsqueeze(1)` -> NO, the code says `x.unsqueeze(1).unsqueeze(1)` Wait, `(x.unsqueeze(1)).unsqueeze(1)`: - x: (batch_size, out_features) - x.unsqueeze(1): (batch_size, 1, out_features) - x.unsqueeze(1).unsqueeze(1): (batch_size, 1, 1, out_features) Yes, that's what I said. But InstanceNorm2d with out_features means C = out_features. But the tensor is (batch_size, 1, 1, out_features), so it only has 1 channel! Oh wait, I see the confusion. `unsqueeze(1)` adds a dimension at position 1. For x of shape (B, out_features): - unsqueeze(1) gives (B, 1, out_features) - unsqueeze(1) again gives (B, 1, 1, out_features) -- but that makes the channels dimension = 1, not out_features! So the tensor passed to InstanceNorm2d is (B, 1, 1, out_features), and C=1. This normalizes 1 channel over H=1, W=out_features spatial dimensions! For each (n, c=1), the instance norm computes mean/var over W=out_features elements (with H=1). So it normalizes across the feature dimension! Then after instance norm and squeeze operations, it becomes (B, out_features) again. So the operation is: 1. Linear transform: x @ W^T + b 2. For each batch element, normalize across the out_features dimension - mean = mean of the out_features values - var = variance of the out_features values - output = (value - mean) / sqrt(var + eps) 3. Add y 4. Mul y BUT wait, does InstanceNorm2d normalize across H and W dimensions? Yes! For input (N, C, H, W), it normalizes each (n, c) over H*W elements. So for (B, 1, 1, out_features), each batch element n=0..B-1 has C=1 channel. For that one channel, it computes mean and var over H=1, W=out_features, i.e., over the out_features values. Then it normalizes each value. With affine=False (default), there's no learnable scaling or shifting. So the full forward is: 1. z = x @ W^T + b, where W, b are linear layer parameters 2. For each batch element i: mu[i] = mean(z[i, :]) sigma2[i] = var(z[i, :]) z_norm[i, j] = (z[i, j] - mu[i]) / sqrt(sigma2[i] + eps) 3. out = (z_norm + y) * y = z_norm * y + y^2 So the instance norm is NOT zeroing things out! It's a proper normalization across the feature dimension. Actually, this is effectively LayerNorm but without learnable parameters... Let me verify: - LayerNorm on (B, out_features) normalizes across the last dimension for each batch element - InstanceNorm2d on (B, 1, 1, out_features) normalizes across spatial (H, W) for each batch element and channel - For (B, 1, 1, out_features), the H*W spatial dims are 1*out_features = out_features elements, per (n, c) = per batch element and the single channel - So yes, this is equivalent to LayerNorm without affine parameters So I need to implement: linear + layer_norm + add + mul Now, since the input dimensions are large (batch_size=1024, in_features=8192, out_features=8192), the linear layer will dominate computationally: - Linear operations: 1024 * 8192 * 8192 ≈ 68.7 billion multiply-adds - At 67 TFLOPS FP32 on H100, this would take ~1ms ideally Let me think about optimization. Since this is a very large GEMM, we should probably use cuBLAS for the linear layer, then fuse the rest in a custom kernel. Wait, but can we fuse instance norm, add, and mul with the linear layer output? Yes, we can write a custom kernel that takes the linear output tensor, computes instance norm statistics per row, normalizes, then does add and mul with y. Actually, even better: can we write a fused kernel that does everything after the GEMM? Let me think. Block 1: Linear layer (GEMM) - use cuBLAS/matmul Block 2: Take z = (B, out_features), y = (B, out_features) Compute per-row mean and var of z Compute normalized z Compute (z_norm + y) * y store result This is standard. For large B=1024 and out_features=8192, we can write an efficient kernel for Block 2. Let me estimate memory bandwidth: - Input z: 1024 * 8192 * 4 bytes ≈ 33.5 MB - Input y: 1024 * 8192 * 4 bytes ≈ 33.5 MB - Output: 33.5 MB - Total memory traffic (if naive): ~100 MB - At 3.35 TB/s: ~30 microseconds So Block 2 is very fast. The linear layer is the bottleneck. Can we fuse the linear layer with the post-processing? We'd need to write our own GEMM+fusion, which is much harder. For such large matrices, cuBLAS is highly optimized and will get close to peak performance. Alternative idea: since the linear layer parameters are fixed at model creation, we could potentially precompute something... but no, the input x changes per forward pass. So the strategy is: 1. Keep the linear layer as a standard nn.Linear (or direct matmul) 2. Write a fused CUDA kernel for instance_norm + add + mul on the output But we need to beat the reference which does: - GEMM (cuBLAS) - unsqueeze/squeeze (no-op on memory) - InstanceNorm2d (custom kernel or implementation) - add + mul (elementwise kernel) The reference is already mostly fused? Let me think. In PyTorch, InstanceNorm2d on this specific case might use a custom kernel. But add and mul are separate kernels. So there are probably: 1. GEMM kernel 2. Instance norm kernel 3. Elementwise add kernel 4. Elementwise mul kernel We can fuse steps 2-4 into one custom kernel, which would give us: 1. GEMM kernel 2. Fused post-process kernel This saves memory round-trips between steps 2-4 and potentially between 1-2 if we can avoid writing z to memory and reading it back. But for such large dimensions, the GEMM output z must be materialized anyway (or we can use the GEMM output directly...) Actually, let me think about whether we can write this as a CUTLASS-like fused GEMM+epilogue. But the instance norm involves a reduction across the row, which makes the epilogue more complex. It's probably easier to: 1. Do GEMM -> write z to global memory 2. Launch kernel that: loads z and y, computes row stats, applies normalization, add, mul, writes result. Actually, wait. We could potentially compute z and y, then do everything in one kernel. But for large GEMM, the GPU will already be highly occupied, and adding a fused kernel afterward is straightforward. For the fused kernel, I need to write a custom CUDA kernel that: 1. Loads a row of z (the GEMM output) 2. Computes mean and variance of that row 3. Normalizes each element 4. Does (normalized + y) * y 5. Writes result For B = 1024, out_features = 8192, each row is 8192 elements of fp32 = 32 KB. This fits nicely in shared memory if we want to use it, but we actually need a two-pass algorithm (first pass compute mean/var, second pass compute output). Actually for numerical stability, we can use Welford's online algorithm in a single pass, but then we'd need to store the row or load it twice. For 8192 elements per row and 1024 rows, loading each row twice might be OK. Let's think about occupancy. Each thread block could process one or more rows. If each thread processes 8 elements (for coalesced access), then for 8192 elements we need 1024 threads per row. But that's a lot - 1024 threads per block * floating point operations... with 1024 rows total, this would only launch 1 block if 1 block = 1 row? No wait, 1024 threads per block, each processing 8 elements = 8192 elements per block. We'd launch 1024 blocks, each with 1024 threads. That's a lot of threads - about 1M threads total, which is fine for an H100. But each block would need to do a reduction across 1024 threads to compute mean and var, then apply to all elements. With __shared_memory__ for the reduction. Alternative: each block processes multiple rows with fewer threads per row. For example, 256 threads per block, each thread processes 32 elements. Each block handles multiple rows... but parallel reductions get more complex. Actually, since out_features = 8192, if we use 256 threads per block and each thread handles 32 elements (256 * 32 = 8192), then each block can process 1 row efficiently. Launching 1024 blocks total. Each block would accumulate in shared memory. But wait, 256 threads * 32 elements per thread = 8192 elements per row. Each thread loads 32 consecutive elements? That might not be perfectly coalesced if the row is contiguous and each thread accesses its own chunk. Actually if thread i accesses elements [i*32 : (i+1)*32], these are contiguous within each thread's chunk and across threads they form contiguous blocks, which should be coalesced. For the mean and variance computation, each thread can compute local mean and variance (or sum and sum of squares), then do a block-level reduction. Actually, for 256 threads per block, shared memory size: 256 * sizeof(float) * 2 (for sum and sum_sq) = 2KB, very small. Total blocks = 1024. Occupancy: with 256 threads/block and up to 2048 threads/SM on H100, we get 8 blocks/SM max (limited by thread count). With 132 SMs, total capacity is 132 * 8 = 1056 blocks, and we need 1024 blocks, so almost perfect occupancy. Wait, let me check H100 SM count. The get_gpu_specs output shows "SM count" but I don't see it explicitly. H100 has 132 or 144 SMs depending on the SKU. With 1024 blocks and 8 blocks per SM, we'd need 128 SMs. Should be fine. Let me reconsider the thread configuration. 1024 blocks of 256 threads each: - Each thread handles 32 elements - We need two passes: first compute row sums (sum and sum_sq), second compute normalized + fused add/mul Actually, if we have 256 threads per block: - Each thread accumulates 32 elements into local_sum and local_sum_sq - Block reduction on local_sum and local_sum_sq using shared memory - Then each thread processes its 32 elements again (or we could load them again) to compute output The issue is we need to load z twice. But that's fine for memory bandwidth. Actually, we can optimize further. With 1024 threads per block and each thread handling 8 elements: - 1024 threads * 8 = 8192 elements - Each thread: local_sum = sum of 8 elements, local_sum_sq = sum of squares - Warp shuffle reduction for warps, then shared memory for cross-warp - After computing mean and var, each thread processes its 8 elements This might be more efficient since warps can use shuffle instructions. Let me think about register pressure and occupancy. With 1024 threads per block, we need at least 1024 blocks for 1024 rows. But with 1024 threads per block, we might only fit 2 blocks per SM (2048 threads / 1024 = 2), so about 2-3 blocks per SM. With ~132 SMs, that's 264-396 concurrent blocks, out of 1024 total. That means roughly 1/3 occupancy, which might be lower than ideal. Let me check: 1024 blocks total, can run ~300 concurrently. Each block takes time T. Total time = 1024/300 * T ≈ 3.4T. With 256 threads per block (4x more blocks per SM), we'd get 8 blocks per SM = ~1056 concurrent blocks for 1024 total blocks. So all blocks can run concurrently, time = T. So 256 threads per block is probably better for occupancy. Let me go with that. Each thread handles 32 elements. Do a two-pass approach: - Pass 1 (coalesced load): compute local_sum and local_sum_sq for 32 elements - Warp shuffle reduction within each warp - Shared memory reduction across warps - One thread computes mean and inv_std = 1/sqrt(var + eps) - Broadcast mean and inv_std to all threads (store in shared memory) - Pass 2 (coalesced load): for each element, compute (z - mean) * inv_std, then (norm + y) * y, store result Wait, can we load z and y in the same pass to compute sum? Yes, we need y anyway. But for sum and sum_sq, we only need z. For pass 2, we need both z and y. If z is stored in registers from pass 1, we don't need to reload it. But 32 floats per thread = 128 bytes = 32 registers just for z. Plus y = 32 registers. Plus local_sum, local_sum_sq, etc. That's about 70 registers per thread. With 256 threads per block, 70 * 256 = ~17920 registers per block. H100 has 64K registers per SM, so with 8 blocks per SM, that's 8 * 17920 = 143360 registers, which exceeds 64K! So we'd only fit ~3-4 blocks per SM if we keep everything in registers. Alternatively, we can reload z in pass 2. Then we only need to store sum and sum_sq (2 floats per thread = 512 floats per block = 2KB in shared memory). Each thread in pass 1 just accumulates sum and sum_sq without storing all z values. Pass 2 reloads z and loads y, computes output. This uses fewer registers. Let me calculate register usage without keeping z/y: - local_sum: 1 float - local_sum_sq: 1 float - loop variables, indices: a few - Total maybe 10-15 registers per thread - Per block: 15 * 256 = 3840 registers - Per SM with 8 blocks: ~30K registers, well under 64K limit This is much better! So the two-pass with reload approach is better for occupancy. Let me draft the kernel: ```cuda #include <torch/extension.h> #include <cuda_runtime.h> #include <math.h> __global__ void fused_kernel(const float* __restrict__ z, const float* __restrict__ y, float* __restrict__ out, int batch_size, int out_features, float eps) { int row = blockIdx.x; if (row >= batch_size) return; const float* z_row = z + row * out_features; const float* y_row = y + row * out_features; float* out_row = out + row * out_features; int tid = threadIdx.x; int num_threads = blockDim.x; float local_sum = 0.0f; float local_sum_sq = 0.0f; // Pass 1: compute sum and sum of squares for (int i = tid; i < out_features; i += num_threads) { float val = z_row[i]; local_sum += val; local_sum_sq += val * val; } // Block reduction using shared memory __shared__ float shared_sum[256]; __shared__ float shared_sum_sq[256]; __shared__ float mean; __shared__ float inv_std; shared_sum[tid] = local_sum; shared_sum_sq[tid] = local_sum_sq; __syncthreads(); // Tree reduction for (int stride = num_threads / 2; stride > 0; stride /= 2) { if (tid < stride) { shared_sum[tid] += shared_sum[tid + stride]; shared_sum_sq[tid] += shared_sum_sq[tid + stride]; } __syncthreads(); } if (tid == 0) { mean = shared_sum[0] / out_features; float variance = shared_sum_sq[0] / out_features - mean * mean; inv_std = rsqrtf(variance + eps); } __syncthreads(); // Pass 2: compute normalized + add + mul for (int i = tid; i < out_features; i += num_threads) { float z_val = z_row[i]; float y_val = y_row[i]; float norm = (z_val - mean) * inv_std; out_row[i] = (norm + y_val) * y_val; } } ``` Wait, I need to be careful. The variance computation uses population variance (denominator N), not sample variance (N-1). Does PyTorch use population or sample variance for InstanceNorm? In PyTorch, InstanceNorm uses the same variance computation as BatchNorm. For BatchNorm during training, it uses population variance (with biased estimator, i.e., denominator N). Actually, let me double check... PyTorch's batch_norm uses `var = mean(x^2) - mean(x)^2` with population denominator (N). For instance norm, it's the same. Actually, I should verify this. In training mode, batch norm computes running statistics with `momentum * batch_stat + (1 - momentum) * running_stat`. The batch variance is computed with N as the denominator (population variance). Let me check... From PyTorch docs for BatchNorm: "The standard-deviation is calculated via the biased estimator, equivalent to torch.var(input, unbiased=False)"... or is it? Actually, looking at PyTorch internals, during training, BatchNorm computes the mean and variance over the batch and spatial dimensions. The variance has B*H*W as the denominator. For InstanceNorm2d with (N, C, H, W), it computes mean and var per instance (n) and channel (c) over H*W elements. With our case (B, 1, 1, out_features), it computes per (n, c=1) over 1*out_features = out_features elements, using population variance (denominator = out_features). So my formula `variance = E[x^2] - (E[x])^2 = sum_sq / N - mean^2` with `N = out_features` is correct. But wait, there's a potential numerical issue. `E[x^2] - mean^2` can be negative due to floating point error. PyTorch applies `max(var, 0)` or clips it. I should make sure to guard against this. Using `fmaxf(variance, 0.0f) + eps` would be safer. Let me update: `inv_std = rsqrtf(fmaxf(variance, 0.0f) + eps);` Now, let me think about whether we can fuse the GEMM with this. If we launch a separate GEMM kernel and then this kernel, we're doing: 1. Read x, read W, write z 2. Read z, read y, write out For step 1: x is 1024*8192*4 = 33.5MB, W is 8192*8192*4 = 268MB, output z is 33.5MB. Total memory read: ~335MB, write: 33.5MB. Compute: 1024*8192*8192*2 FLOPs = 137G FLOPs. At 67 TFLOPS: ~2ms. At 3.35 TB/s memory bandwidth: memory-bound portion... Actually for large GEMM like 1024x8192x8192, cuBLAS should achieve good utilization. Let me not worry about fusing GEMM for now. Wait, actually, I can try to be clever. Since the linear layer is large, and the post-processing is bandwidth-bound, there might be enough compute headroom to fuse them if we write a custom GEMM... but that's an enormous amount of work and probably won't beat cuBLAS for such large, square-ish shapes. Let me think about the thread configuration again. With out_features = 8192, and blockDim.x = 256, each thread processes 32 elements with a stride loop. For coalesced access, if thread 0 accesses 0, 256, 512, ..., and thread 1 accesses 1, 257, 513, ..., these are NOT contiguous and strided access! That's bad for coalescing. Actually, if thread i accesses elements i, i+256, i+512, ... these are strided across the row. For a 1D array, strided access is coalesced if the stride is a multiple of 32 bytes (8 floats) and threads in a warp access consecutive cache lines. But with stride 256 floats = 1024 bytes, each thread accesses a different cache line, which might not be fully coalesced. Wait, in a warp of 32 threads, thread i accesses address `base + i * stride`. For stride 256, thread 0 accesses base, thread 1 accesses base+256, etc. That's 32 different cache lines. Each load of 4 bytes from a different cache line. This is terrible coalescing! Better approach: each thread accesses contiguous elements. For example, thread i accesses elements starting from `i * elements_per_thread` to `(i+1) * elements_per_thread - 1`. With 256 threads and 8192 elements per row, each thread handles 32 contiguous elements: thread 0 handles 0-31, thread 1 handles 32-63, etc. For coalescing within a warp (threads 0-31): thread 0 accesses element 0, thread 1 accesses element 32, thread 2 accesses element 64, etc. Wait, that's still strided by 32 elements = 128 bytes. For 32 threads, consecutive threads access memory 128 bytes apart. That's still not perfectly coalesced. For the best coalescing, consecutive threads in a warp should access consecutive elements. So if we have 32 threads in a warp and each thread accesses 1 element, we get perfect coalescing. But then we need more iterations (8192 / 32 = 256 iterations for a warp to process a row). With 256 threads per block and 32 warps per block: if each warp processes a contiguous chunk, like warp 0 processes elements 0-255, warp 1 processes 256-511, etc. Then within a warp, thread i accesses element warp_start + i. That's perfect coalescing! So the layout should be: - The row is divided into chunks of `blockDim.x` elements - Thread `tid` processes elements `chunk_start + tid` across all chunks - Because `tid` varies from 0 to 255, and consecutive threads access consecutive elements within a chunk Wait no, if each thread processes one element per chunk and there are multiple chunks... Let me be more careful. out_features = 8192, blockDim.x = 256. Number of chunks = 8192 / 256 = 32 chunks. For chunk c (from 0 to 31): thread tid processes element c * 256 + tid. So thread 0 processes: 0, 256, 512, ..., 7936 Thread 1 processes: 1, 257, 513, ..., 7937 ... Thread 255 processes: 255, 511, ..., 8191 In a warp (e.g., threads 0-31): For chunk 0: threads access 0, 1, 2, ..., 31 -> perfectly coalesced! For chunk 1: threads access 256, 257, ..., 287 -> perfectly coalesced! ... For chunk 31: threads access 7936, ..., 7967 -> perfectly coalesced! BUT within a single instruction, each thread in the warp loads from different memory addresses. For coalescing, the memory controller group contiguous accesses from a warp into cache lines. Since threads 0-31 in a warp access 0-31 in chunk 0, this is one or two 128-byte cache lines (assuming 128B line). Load per thread is 4 bytes, so 32 threads * 4 = 128 bytes = exactly one cache line. Perfect! However, each thread now accesses 32 elements (1 per chunk), and consecutive elements for a single thread are 256 apart (256 * 4B = 1KB apart). That's fine for instruction-level parallelism but each thread's accesses are not contiguous. Actually, since each warp processes one chunk at a time ( implicit in the current formulation if we loop by chunk), we need each thread to load element `base + tid` for chunk 0, then `base + 256 + tid` for chunk 1, etc. Wait, my earlier formulation was wrong. Let me write it clearly: ```cuda for (int idx = tid; idx < out_features; idx += blockDim.x) { float val = z_row[idx]; ... } ``` Here, for a warp of 32 threads: thread 0 loads idx=0, thread 1 loads idx=256, thread 2 loads idx=512, etc. That IS strided access within a warp and is bad for coalescing! The correct formulation for coalesced access is: ```cuda for (int i = tid; i < out_features; i += blockDim.x) { ``` Let me reconsider. In a warp: - Threads 0..31: i = 0, 1, 2, ..., 31? No, i goes from tid to out_features, step = blockDim.x = 256. - First iteration: thread 0 loads z_row[0], thread 1 loads z_row[1], ..., thread 31 loads z_row[31]. Yes! Consecutive threads load consecutive elements. - Second iteration: thread 0 loads z_row[256], thread 1 loads z_row[257], etc. Oh! I made an error. When `idx = tid`, and `tid` ranges from 0 to 31 in a warp, then indices are 0, 1, ..., 31 in the first iteration. That's perfect coalescing! My previous analysis was wrong because I was thinking `idx = tid * stride` but it's `idx = tid` with `stride = blockDim.x = 256`. Wait, but in the second iteration, `idx = tid + blockDim.x = tid + 256`. So thread 0 loads z_row[256], thread 1 loads z_row[257], etc. Still perfect! So the loop `for (int idx = tid; idx < out_features; idx += blockDim.x)` gives perfect coalescing. I was confusing myself earlier. Now let me think about the implementation: ```cuda __global__ void fused_postprocess(const float* __restrict__ z, const float* __restrict__ y, float* __restrict__ out, int batch_size, int out_features, float eps) { int row = blockIdx.x; if (row >= batch_size) return; int tid = threadIdx.x; int stride = blockDim.x; const float* z_row = z + row * out_features; const float* y_row = y + row * out_features; float* out_row = out + row * out_features; float sum = 0.0f; float sum_sq = 0.0f; // First pass: compute sum and sum_sq for (int i = tid; i < out_features; i += stride) { float val = z_row[i]; sum += val; sum_sq += val * val; } // Warp-level reduction for (int offset = warpSize / 2; offset > 0; offset /= 2) { sum += __shfl_down_sync(0xffffffff, sum, offset); sum_sq += __shfl_down_sync(0xffffffff, sum_sq, offset); } __shared__ float warp_sums[32]; __shared__ float warp_sum_sqs[32]; __shared__ float s_mean; __shared__ float s_inv_std; int warp_id = tid / warpSize; if (tid % warpSize == 0) { warp_sums[warp_id] = sum; warp_sum_sqs[warp_id] = sum_sq; } __syncthreads(); // Reduce across warps if (warp_id == 0) { float block_sum = (tid < (stride + warpSize - 1) / warpSize) ? warp_sums[tid] : 0.0f; float block_sum_sq = (tid < (stride + warpSize - 1) / warpSize) ? warp_sum_sqs[tid] : 0.0f; for (int offset = warpSize / 2; offset > 0; offset /= 2) { block_sum += __shfl_down_sync(0xffffffff, block_sum, offset); block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset); } if (tid == 0) { float mean = block_sum / out_features; float variance = block_sum_sq / out_features - mean * mean; s_mean = mean; s_inv_std = rsqrtf(fmaxf(variance, 0.0f) + eps); } } __syncthreads(); // Second pass: compute output for (int i = tid; i < out_features; i += stride) { float z_val = z_row[i]; float y_val = y_row[i]; float norm = (z_val - s_mean) * s_inv_std; out_row[i] = (norm + y_val) * y_val; } } ``` With blockDim.x = 256, we have 8 warps per block (256 / 32 = 8). The shared memory sizes warp_sums[8] and warp_sum_sqs[8] - I hardcoded 32 for simplicity but only use 8 elements. Wait, since blockDim.x might vary, let me not hardcode 32. Actually on H100, max 32 warps per block with 1024 threads. Let me just make shared memory size 32. Actually, with blockDim.x = 256, we have 8 warps, but shared memory array of size 32 is fine. The condition in the cross-warp reduction checks `tid < num_warps`. I'll compute num_warps = (stride + 31) / 32. Hmm, there's a potential issue. For the cross-warp reduction, only warp 0 threads participate. But `__shfl_down_sync` operates on all threads in the warp. We need to make sure all threads in warp 1-7 don't interfere. Since we do this only in warp 0, other warps are fine. I should also think about whether we can use vectorized loads. For fp32 with out_features = 8192, we can use float4 loads. Each float4 loads 4 consecutive floats = 128 bits. With 8192 / 4 = 2048 float4 elements. If we process float4 in the kernel: ```cuda for (int i = tid; i < out_features / 4; i += stride) { float4 z4 = reinterpret_cast<const float4*>(z_row)[i]; // unpack z4.x, z4.y, z4.z, z4.w } ``` For coalescing: 256 threads each loading float4 = 1024 floats per iteration. With 8 iterations (8192/1024), consecutive threads load consecutive float4s, each 16 bytes. A warp loads 32 * 16 = 512 consecutive bytes. That's 4 cache lines of 128B each. Not ideal for float4 (which is exactly a cache line). Actually, if we use half as many threads or process 8 floats per thread... Let me not overcomplicate this. Standard scalar loads might be fine, and the compiler will often generate vectorized loads automatically when it sees aligned memory accesses in a loop. For the instance norm operation with 8192 floats per row and 1024 rows, total elements = 8,388,608. At 3.35 TB/s, reading z + y and writing out = 3 * 8,388,608 * 4 bytes ≈ 100MB. Time = 100MB / 3.35TB/s ≈ 30 microseconds. This is negligible compared to the GEMM time. But let me think: the reference implementation probably uses PyTorch's built-in InstanceNorm2d, which on this specific shape might be slow because it's not a common case. And there are separate add and mul kernels. By fusing everything, we eliminate kernel launch overhead (~5-10 microseconds per kernel) and extra memory round-trips. Actually, for PyTorch's instance_norm on this shape, let me think about what it does. The input is (B, 1, 1, out_features). PyTorch might reshape it to (B, out_features) and call some 1D normalization. Or it might dispatch to cudnn or native kernels. Either way, our fused kernel should be competitive or faster. Now, what about the linear layer in our ModelNew? We can simply keep the nn.Linear module and call it. But that requires storing self.bmm parameters. Actually, we could use torch.matmul directly with the weight and bias from a Linear layer. Wait, in the reference, self.bmm is nn.Linear. During initialization, it creates weight and bias. In ModelNew, we can also create a nn.Linear layer in __init__ and use it in forward. That's the simplest and will call cuBLAS, which is optimal for large GEMM. But actually, the evaluation might compare against the reference creating a new Model. Since we need to produce numerically equivalent output, using the same nn.Linear should be fine. Hmm, but to be safe, let me think if we need to worry about the exact GEMM implementation. Both will use cuBLAS through ATen, so the numerical results should be identical (or at least within tolerance). Let me draft the complete ModelNew: ```python import torch import torch.nn as nn from torch.utils.cpp_extension import load_inline # Compile the CUDA kernel at module load time cuda_source = """ #include <torch/extension.h> #include <cuda_runtime.h> __global__ void fused_postprocess_kernel(const float* __restrict__ z, const float* __restrict__ y, float* __restrict__ out, int batch_size, int out_features, float eps) { int row = blockIdx.x; if (row >= batch_size) return; int tid = threadIdx.x; int num_threads = blockDim.x; int lane_id = tid & 31; int warp_id = tid >> 5; const float* z_row = z + (int64_t)row * out_features; const float* y_row = y + (int64_t)row * out_features; float* out_row = out + (int64_t)row * out_features; float local_sum = 0.0f; float local_sum_sq = 0.0f; // First pass: accumulate statistics for (int i = tid; i < out_features; i += num_threads) { float val = z_row[i]; local_sum += val; local_sum_sq += val * val; } // Warp reduction #pragma unroll for (int offset = 16; offset > 0; offset /= 2) { local_sum += __shfl_down_sync(0xffffffff, local_sum, offset); local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset); } __shared__ float warp_sum[32]; __shared__ float warp_sum_sq[32]; __shared__ float s_mean; __shared__ float s_inv_std; if (lane_id == 0) { warp_sum[warp_id] = local_sum; warp_sum_sq[warp_id] = local_sum_sq; } __syncthreads(); // Cross-warp reduction (only warp 0) if (warp_id == 0) { float block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0f; float block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0f; #pragma unroll for (int offset = 16; offset > 0; offset /= 2) { block_sum += __shfl_down_sync(0xffffffff, block_sum, offset); block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset); } if (lane_id == 0) { float mean = block_sum / out_features; float variance = block_sum_sq / out_features - mean * mean; s_mean = mean; s_inv_std = rsqrtf(fmaxf(variance, 0.0f) + eps); } } __syncthreads(); // Second pass: compute fused output for (int i = tid; i < out_features; i += num_threads) { float z_val = z_row[i]; float y_val = y_row[i]; float norm = (z_val - s_mean) * s_inv_std; out_row[i] = (norm + y_val) * y_val; } } torch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) { int batch_size = z.size(0); int out_features = z.size(1); auto out = torch::empty_like(z); const int threads = 256; const int blocks = batch_size; fused_postprocess_kernel<<<blocks, threads>>>( z.data_ptr<float>(), y.data_ptr<float>(), out.data_ptr<float>(), batch_size, out_features, eps ); return out; } """ cpp_source = """ torch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps); """ fused_postprocess = load_inline( name="fused_postprocess", cpp_sources=cpp_source, cuda_sources=cuda_source, functions=["fused_postprocess"], extra_cuda_cflags=["-O3"], verbose=False, ) class ModelNew(nn.Module): def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1): super().__init__() self.bmm = nn.Linear(in_features, out_features) self.eps = eps def forward(self, x, y): z = self.bmm(x) return fused_postprocess.fused_postprocess(z, y, self.eps) ``` Wait, I need to compile this and test. Let me also think about whether there are any numerical issues. One concern: my variance computation uses `sum_sq / N - mean * mean`. This can numerically give slightly negative results, hence the `fmaxf(variance, 0.0f)`. PyTorch likely does something similar. Another concern: the reduction order matters for floating point accuracy. Since I'm reducing within warps using shuffle, and then across warps, the order is NOT the same as PyTorch's implementation. This might cause discrepancies larger than 1e-4. For better numerical reproducibility, I should try to match PyTorch's approach. But what order does PyTorch use? For instance norm on a large vector, PyTorch probably uses some tree-based reduction or uses cuDNN's optimized implementation. The exact order is hard to match. Given the tolerance is 1e-4 for fp32, independent reduction order shouldn't matter too much for random data, but let me think if there's a way to make it more robust. Actually, I could use Welford's online algorithm for better numerical stability, but since the data are normalized anyway, it's probably not a huge issue. Let me think about the reference implementation more carefully. PyTorch's InstanceNorm2d on a tensor of shape (N, C, H, W) with track_running_stats=False computes: 1. Reshape or view so that we compute mean and var over some dimensions 2. For (B, 1, 1, out_features), PyTorch calls into a native kernel Actually, rather than trying to match the exact reduction order, let me just make sure I use double precision or Kahan summation for better accuracy. For increased accuracy in the first pass sum and sum_sq, I can use float accumulation but loop in a specific order. The tree reduction within warps is deterministic for a given block configuration. PyTorch's reduction order might be different, but for random fp32 data, the difference should be within 1e-4. Actually, let me check if there might be a larger issue. For a vector of 8192 elements, each element is ~O(1) and the sum is ~O(8192). Adding 8192 numbers of similar magnitude... tree reduction vs sequential reduction shouldn't differ by more than O(N * eps) ≈ 8192 * 1e-7 ≈ 8e-4 in relative error? That could be on the borderline. Actually absolute error: each addition can have rounding error of ~1e-7. Accumulating 8192 of them could have absolute error of ~1e-3 to 1e-4. For normalized values (subtracting mean, dividing by std ~1), the error could be similar. Wait, but we need to compute var = E[x^2] - mean^2. If mean has 1e-3 absolute error and E[x^2] has 1e-3 absolute error, then var could have error on the order of 1e-3, and inv_std could have error propagated. This might cause output differences larger than 1e-4. To improve accuracy, I can use double precision for the intermediate mean and var computations, while still loading data as float. This is a common optimization: ```cuda double local_sum = 0.0; double local_sum_sq = 0.0; ``` Then the reduction also uses double. At the end, convert to float for the normalization step. This adds some overhead but improves numerical accuracy significantly. Actually, since we only need mean and inv_std (two double values per block spread via shared memory), the overhead is minimal. Let me use double precision for the accumulation. But wait, do I need to match PyTorch exactly? PyTorch might also use float or float accumulator depending on the backend. For most PyTorch operations on CUDA, fp32 inputs are accumulated in fp32. Using fp64 might actually give BETTER accuracy than PyTorch, but could cause issues if the tolerance is tight and PyTorch's result has more error... Actually, for the tolerance test, the absolute tolerance is 1e-4. If PyTorch computes with fp32 accumulation and gets an error of say 5e-5 in some elements, and I compute with fp64 and get 1e-6, both are within 1e-4 of the true result. The difference between them might be ~5e-5, which is still within 1e-4. So using double precision accumulation should be safe and might actually help ensure we pass the tolerance test. Let me update the kernel to use double for accumulation: ```cuda double local_sum = 0.0; double local_sum_sq = 0.0; for (int i = tid; i < out_features; i += num_threads) { float val = z_row[i]; local_sum += (double)val; local_sum_sq += (double)val * (double)val; } // Warp shuffle for double for (int offset = warpSize / 2; offset > 0; offset /= 2) { local_sum += __shfl_down_sync(0xffffffff, local_sum, offset); local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset); } ``` Wait, __shfl_down_sync doesn't support double directly? Actually it does, it's a template and works for any 32-bit or smaller type. For double (64-bit), I think it might work on newer architectures but I'm not 100% sure. Let me split into two floats: ```cuda float local_sum_hi = __shfl_down_sync(mask, __double2hiint(local_sum), offset); float local_sum_lo = __shfl_down_sync(mask, __double2loint(local_sum), offset); local_sum += __hiloint2double(local_sum_hi, local_sum_lo); ``` Or I can just reduce to shared memory from each warp, using atomicAdd or a second shared memory reduction. Actually, a simpler approach: After each warp computes its fp64 sum (reduced from fp32 inputs), store to shared memory. Then use atomicAdd to shared memory? No, atomicAdd on shared memory for double is slow. Actually, for fp64 shuffle on Volta+ (H100), I believe __shfl_down_sync works with double. Let me verify... On SM70+, I think __shfl_down_sync works with any type that fits in a register. Double fits in one 64-bit register. So it should work. Wait, I should just test and see. If there's a compile error, I'll fix it. Actually, looking at CUDA documentation, `__shfl_down_sync` accepts any 32-bit or 64-bit type. Double should work. Actually wait, let me reconsider. Even with fp64 accumulation, the difference in reduction ORDER between my kernel and PyTorch might still be noticeable. The sequential loop order within each thread is the same (stride by blockDim.x), but my warp-level and block-level reductions differ from a pure sequential sum. For random data, this is almost always within 1e-4 for 8192 elements. Let me not overthink it. If it fails, I'll debug and adjust. One more thing: I should align the thread count to 256 or maybe 512. With out_features = 8192: - 128 threads: each handles 64 elements, 8 warps - 256 threads: each handles 32 elements, 8 warps - 512 threads: each handles 16 elements, 16 warps With 512 threads per block, we'd only get 4 blocks per SM (2048/512 = 4). Total concurrent blocks: ~528, still plenty for 1024 blocks (roughly 2 waves). I'll go with 256 for now. Let me also consider float4 vectorization. For the second pass where we do the math and write output, using float4 could be beneficial: ```cuda for (int i = tid; i < out_features / 4; i += num_threads) { float4 z4 = reinterpret_cast<const float4*>(z_row)[i]; float4 y4 = reinterpret_cast<const float4*>(y_row)[i]; float4 out4; out4.x = ((z4.x - s_mean) * s_inv_std + y4.x) * y4.x; out4.y = ((z4.y - s_mean) * s_inv_std + y4.y) * y4.y; out4.z = ((z4.z - s_mean) * s_inv_std + y4.z) * y4.z; out4.w = ((z4.w - s_mean) * s_inv_std + y4.w) * y4.w; reinterpret_cast<float4*>(out_row)[i] = out4; } ``` This assumes the memory is aligned for float4. PyTorch tensors of size (1024, 8192) should be aligned to at least 256 bytes. But we should check if `z_row`, `y_row`, and `out_row` are aligned. The base tensor pointer should be aligned to 512 bytes or more. Each row starts at `base + row * out_features * sizeof(float)`. With out_features = 8192, row_stride = 8192 * 4 = 32768 bytes, which is a multiple of 128 bytes. So rows are aligned. But for access to z_row[i] where i = tid, with float4 indexing, we'd access 4 * tid. For tid = 0, address = z_row. For tid = 1, address = z_row + 4. That's not aligned for float4! We need tid to index float4 elements, not scalar elements. Wait, if we change the loop to `for (int i = tid; i < out_features / 4; i += num_threads)`, then thread 0 reads float4 at offset 0, thread 1 reads at offset 1 float4 (16 bytes), etc. Within a warp, threads read 0, 16, 32, 48, ..., 496 bytes (for 32 threads). That's 32 cache lines for 32 float4s of 512 bytes total. Actually, consecutive threads read consecutive float4s (16 bytes each). A warp reads 32 * 16 = 512 consecutive bytes. That's 4 cache lines of 128 bytes each. Not perfectly coalesced in a single instruction, but the memory controller can merge nearby requests. Hmm, actually for float4 loads, each thread issues a 128-bit (16-byte) load. Consecutive threads loading consecutive 16-byte chunks gives 512 bytes of contiguous memory per warp, which is exactly 4 L2 cache sectors. The memory controller should handle this fine - it's perfectly coalesced in the sense that all accesses are to contiguous memory. Actually, in NVIDIA terminology, perfect coalescing for a warp is when the warp accesses a contiguous memory range where each thread accesses 4 bytes (128 bytes total for 32 threads). For float4 (16 bytes per thread), a warp accesses 512 bytes, which might require multiple transactions but is still fully coalesced. Let me check: the L1 cache line is 128 bytes, so each thread's float4 spans exactly one L1 cache line (16B < 128B). A warp accessing consecutive float4s accesses 32 cache lines (not all distinct, but 32 cache lines in the sense of 16B sectors). Actually, 512 bytes / 128 bytes per cache line = 4 cache lines. The memory controller will issue 4 transactions of 128 bytes each to cover the warp's 512-byte contiguous access. Wait, that doesn't sound right. Each thread issues a single 16-byte load instruction. The L1 cache can handle multiple threads' loads in a single transaction if they're within the same cache line. With 128B lines and 16B loads, 8 threads per cache line. So 32 threads = 4 cache lines. The hardware can do up to 4 or 8 sector requests per warp. For 4 cache lines, that's 4 sector requests. This is perfectly coalesced. So float4 should definitely help. Let me see if I can use it for both passes. For the first pass (sum and sum_sq): ```cuda for (int i = tid; i < out_features / 4; i += num_threads) { float4 z4 = reinterpret_cast<const float4*>(z_row)[i]; local_sum += z4.x + z4.y + z4.z + z4.w; local_sum_sq += z4.x * z4.x + z4.y * z4.y + z4.z * z4.z + z4.w * z4.w; } ``` Then we need to handle any remainder. With 8192 / 4 = 2048, perfectly divisible by 4. No remainder. For the second pass: ```cuda for (int i = tid; i < out_features / 4; i += num_threads) { float4 z4 = reinterpret_cast<const float4*>(z_row)[i]; float4 y4 = reinterpret_cast<const float4*>(y_row)[i]; float4 out4; out4.x = ((z4.x - s_mean) * s_inv_std + y4.x) * y4.x; ... reinterpret_cast<float4*>(out_row)[i] = out4; } ``` This would be significantly more efficient in terms of instruction count and memory throughput. Let me verify alignment requirements. `z_row` points to `z + row * 8192`. If `z` is aligned to 512 bytes, then `z_row` for any `row` is aligned to at least 512 bytes since 8192 * 4 = 32768 is a multiple of 512. So float4 access is safe and aligned. Let me update the kernel with float4 vectorization. I need to be careful with the `reinterpret_cast` to ensure proper aliasing. ```cuda __global__ void fused_kernel(...) { // ... const float4* z4_row = reinterpret_cast<const float4*>(z_row); const float4* y4_row = reinterpret_cast<const float4*>(y_row); float4* out4_row = reinterpret_cast<float4*>(out_row); double local_sum = 0.0; double local_sum_sq = 0.0; int num_vec = out_features / 4; for (int i = tid; i < num_vec; i += num_threads) { float4 z4 = z4_row[i]; local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w; local_sum_sq += (double)z4.x * z4.x + (double)z4.y * z4.y + (double)z4.z * z4.z + (double)z4.w * z4.w; } // ... same reduction ... float mean = s_mean; float inv_std = s_inv_std; for (int i = tid; i < num_vec; i += num_threads) { float4 z4 = z4_row[i]; float4 y4 = y4_row[i]; float4 o4; o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x; o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y; o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z; o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w; out4_row[i] = o4; } } ``` Now for the reduction of doubles with warp shuffle. On H100 (SM90), let me make sure `__shfl_down_sync` works with double. I believe it does, but to be safe, I can also use float and accept lower accuracy, or do a two-step reduction via shared memory. Actually, let me first try without double and see if it passes correctness. If not, I'll add double. Wait, but I should think about one more thing: what if `out_features` is not divisible by 4? In the actual problem, it is 8192, which is divisible by 4. But `ModelNew` should work for any valid `out_features`. A robust kernel would handle the remainder with scalar operations. Actually, the problem states specific dimensions, and the model should handle the same constructor arguments. The test might use different shapes. Let me make the kernel generic. I'll add a remainder loop: ```cuda // Vectorized main loop for (int i = tid; i < num_vec; i += num_threads) { ... } // Scalar remainder for (int i = tid + num_vec * 4; i < out_features; i += num_threads) { ... } ``` Similarly for the output pass. Let me write the full kernel code and compile it. Actually wait, I'm mixing up the task. Let me make sure I understand: I need to define `ModelNew` which implements the exact same behavior as `Model`. The instance norm is applied to `x.unsqueeze(1).unsqueeze(1)` where x after bmm is (batch_size, out_features). So unsqueezed it's (batch_size, 1, 1, out_features). InstanceNorm2d with default affine=False and track_running_stats=False normalizes over H and W. For our custom implementation, we need to handle this exactly. Let me write the code and test. I'll use float4 for efficiency and handle remainders. One more consideration: does PyTorch's instance norm use Bessel's correction (N-1 denominator)? Let me check... For BatchNorm and InstanceNorm in PyTorch, the variance during training uses the population variance (N denominator), not the unbiased sample variance. So `var = sum_sq / N - mean^2` with N = number of elements over which normalization happens. For (B, 1, 1, out_features), N = 1 * out_features = out_features per (batch, channel) pair. Since C=1 and we normalize over H*W = out_features, yes, N = out_features. Actually, wait. InstanceNorm2d computes the mean over H and W for each (N, C). The variance formula with `unbiased=False` gives denominator H*W. So for each sample n and channel c, we compute mean and var over h=0, w=0..out_features-1. The denominator is out_features. My formula is correct. Now let me draft the complete code: ```python import torch import torch.nn as nn from torch.utils.cpp_extension import load_inline cuda_source = """ #include <torch/extension.h> #include <cuda_runtime.h> __global__ void fused_postprocess_kernel(const float* __restrict__ z, const float* __restrict__ y, float* __restrict__ out, int batch_size, int out_features, float eps) { int row = blockIdx.x; if (row >= batch_size) return; int tid = threadIdx.x; int num_threads = blockDim.x; int lane_id = tid & 31; int warp_id = tid >> 5; const float* z_row = z + (int64_t)row * out_features; const float* y_row = y + (int64_t)row * out_features; float* out_row = out + (int64_t)row * out_features; double local_sum = 0.0; double local_sum_sq = 0.0; int num_vec = out_features / 4; const float4* z4_row = reinterpret_cast<const float4*>(z_row); // Vectorized first pass for (int i = tid; i < num_vec; i += num_threads) { float4 z4 = z4_row[i]; local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w; local_sum_sq += (double)z4.x * (double)z4.x + (double)z4.y * (double)z4.y + (double)z4.z * (double)z4.z + (double)z4.w * (double)z4.w; } // Scalar remainder for (int i = tid + num_vec * 4; i < out_features; i += num_threads) { double val = (double)z_row[i]; local_sum += val; local_sum_sq += val * val; } // Warp reduction for double #pragma unroll for (int offset = 16; offset > 0; offset /= 2) { local_sum += __shfl_down_sync(0xffffffff, local_sum, offset); local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset); } __shared__ double warp_sum[32]; __shared__ double warp_sum_sq[32]; __shared__ float s_mean; __shared__ float s_inv_std; if (lane_id == 0) { warp_sum[warp_id] = local_sum; warp_sum_sq[warp_id] = local_sum_sq; } __syncthreads(); // Cross-warp reduction if (warp_id == 0) { double block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0; double block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0; #pragma unroll for (int offset = 16; offset > 0; offset /= 2) { block_sum += __shfl_down_sync(0xffffffff, block_sum, offset); block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset); } if (lane_id == 0) { float mean = (float)(block_sum / (double)out_features); double variance = block_sum_sq / (double)out_features - (double)mean * (double)mean; if (variance < 0.0) variance = 0.0; float inv_std = rsqrtf((float)variance + eps); s_mean = mean; s_inv_std = inv_std; } } __syncthreads(); float mean = s_mean; float inv_std = s_inv_std; // Vectorized second pass const float4* y4_row = reinterpret_cast<const float4*>(y_row); float4* out4_row = reinterpret_cast<float4*>(out_row); for (int i = tid; i < num_vec; i += num_threads) { float4 z4 = z4_row[i]; float4 y4 = y4_row[i]; float4 o4; o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x; o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y; o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z; o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w; out4_row[i] = o4; } // Scalar remainder for (int i = tid + num_vec * 4; i < out_features; i += num_threads) { float z_val = z_row[i]; float y_val = y_row[i]; float norm = (z_val - mean) * inv_std; out_row[i] = (norm + y_val) * y_val; } } torch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) { int batch_size = z.size(0); int out_features = z.size(1); auto out = torch::empty_like(z); int threads = 256; if (out_features <= 128) threads = 64; else if (out_features <= 512) threads = 128; int blocks = batch_size; fused_postprocess_kernel<<<blocks, threads>>>( z.data_ptr<float>(), y.data_ptr<float>(), out.data_ptr<float>(), batch_size, out_features, eps ); return out; } """ cpp_source = """ torch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps); """ fused_postprocess = load_inline( name="fused_postprocess", cpp_sources=cpp_source, cuda_sources=cuda_source, functions=["fused_postprocess"], extra_cuda_cflags=["-O3", "--use_fast_math"], ) class ModelNew(nn.Module): def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1): super().__init__() self.bmm = nn.Linear(in_features, out_features) self.eps = eps # momentum is not used since track_running_stats=False in reference # but we keep it for API compatibility def forward(self, x, y): z = self.bmm(x) return fused_postprocess.fused_postprocess(z, y, self.eps) ``` Wait, I'm being careful about the __shfl_down_sync with double. Let me check... On H100, I'm pretty sure it works. One lingering concern: does `nn.InstanceNorm2d` with the default `affine=False` and `track_running_stats=False` use the N denominator for variance? Yes. Another concern: does the reference compute `running_mean` or `running_var` even when `track_running_stats=False`? No, when False, it doesn't track them. Another concern: in training mode, does InstanceNorm2d update anything? With track_running_stats=False and affine=False, no parameters are updated. So it's purely a function of the input. Now, for the linear layer, could there be a difference between using `self.bmm(x)` and doing `torch.matmul(x, self.bmm.weight.t()) + self.bmm.bias`? They should be the same at the kernel level. Alright, let me write out the complete code and compile it to check for syntax errors. I'll make sure no pybind11 module block is included. Actually, wait. I realize there might be an issue with `momentum` in the reference vs. our implementation. In the reference, `momentum` is passed to InstanceNorm2d but since `track_running_stats=False`, it's ignored. So we don't need to do anything with it. Also, I noticed that the reference uses `nn.Linear` but names it `self.bmm`. That's fine, it's just a name. Let me compile and test.
call → compile_kernel
callcompile_kernel { "kernel_code": "\nimport torch\nimport torch.nn as nn\nfrom torch.utils.cpp_extension import load_inline\n\ncuda_source = \"\"\"\n#include <torch/extension.h>\n#include <cuda_runtime.h>\n\n__global__ void fused_postprocess_kernel(const float* __restrict__ z,\n const float* __restrict__ y,\n float* __restrict__ out,\n int batch_size,\n int out_features,\n float eps) {\n int row = blockIdx.x;\n if (row >= batch_size) return;\n \n int tid = threadIdx.x;\n int num_threads = blockDim.x;\n int lane_id = tid & 31;\n int warp_id = tid >> 5;\n \n const float* z_row = z + (int64_t)row * out_features;\n const float* y_row = y + (int64_t)row * out_features;\n float* out_row = out + (int64_t)row * out_features;\n \n double local_sum = 0.0;\n double local_sum_sq = 0.0;\n \n int num_vec = out_features / 4;\n const float4* z4_row = reinterpret_cast<const float4*>(z_row);\n \n // Vectorized first pass\n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w;\n local_sum_sq += (double)z4.x * (double)z4.x \n + (double)z4.y * (double)z4.y \n + (double)z4.z * (double)z4.z \n + (double)z4.w * (double)z4.w;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n double val = (double)z_row[i];\n local_sum += val;\n local_sum_sq += val * val;\n }\n \n // Warp reduction for double\n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n local_sum += __shfl_down_sync(0xffffffff, local_sum, offset);\n local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset);\n }\n \n __shared__ double warp_sum[32];\n __shared__ double warp_sum_sq[32];\n __shared__ float s_mean;\n __shared__ float s_inv_std;\n \n if (lane_id == 0) {\n warp_sum[warp_id] = local_sum;\n warp_sum_sq[warp_id] = local_sum_sq;\n }\n __syncthreads();\n \n // Cross-warp reduction\n if (warp_id == 0) {\n double block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0;\n double block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0;\n \n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n block_sum += __shfl_down_sync(0xffffffff, block_sum, offset);\n block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset);\n }\n \n if (lane_id == 0) {\n float mean = (float)(block_sum / (double)out_features);\n double variance = block_sum_sq / (double)out_features - (double)mean * (double)mean;\n if (variance < 0.0) variance = 0.0;\n float inv_std = rsqrtf((float)variance + eps);\n s_mean = mean;\n s_inv_std = inv_std;\n }\n }\n __syncthreads();\n \n float mean = s_mean;\n float inv_std = s_inv_std;\n \n // Vectorized second pass\n const float4* y4_row = reinterpret_cast<const float4*>(y_row);\n float4* out4_row = reinterpret_cast<float4*>(out_row);\n \n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n float4 y4 = y4_row[i];\n float4 o4;\n o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x;\n o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y;\n o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z;\n o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w;\n out4_row[i] = o4;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n float z_val = z_row[i];\n float y_val = y_row[i];\n float norm = (z_val - mean) * inv_std;\n out_row[i] = (norm + y_val) * y_val;\n }\n}\n\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) {\n int batch_size = z.size(0);\n int out_features = z.size(1);\n \n auto out = torch::empty_like(z);\n \n int threads = 256;\n if (out_features <= 128) threads = 64;\n else if (out_features <= 512) threads = 128;\n \n int blocks = batch_size;\n \n fused_postprocess_kernel<<<blocks, threads>>>(\n z.data_ptr<float>(),\n y.data_ptr<float>(),\n out.data_ptr<float>(),\n batch_size,\n out_features,\n eps\n );\n \n return out;\n}\n\"\"\"\n\ncpp_source = \"\"\"\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps);\n\"\"\"\n\nfused_postprocess = load_inline(\n name=\"fused_postprocess\",\n cpp_sources=cpp_source,\n cuda_sources=cuda_source,\n functions=[\"fused_postprocess\"],\n extra_cuda_cflags=[\"-O3\", \"--use_fast_math\"],\n)\n\nclass ModelNew(nn.Module):\n def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1):\n super().__init__()\n self.bmm = nn.Linear(in_features, out_features)\n self.eps = eps\n \n def forward(self, x, y):\n z = self.bmm(x)\n return fused_postprocess.fused_postprocess(z, y, self.eps)\n" }
result ← compile_kernel (ok)
okcompile_kernel compile_kernel PASSED: kernel compiled without errors.
turn 2 · 1 tool call(s) · 5.6s turn · 5.6s LLM · 6,421 chars (click to expand)
turn 25.6s turn · 5.6s LLM · 0.0s tools
reasoning
Good, it compiled. Now let me check correctness.
call → run_correctness
callrun_correctness { "kernel_code": "\nimport torch\nimport torch.nn as nn\nfrom torch.utils.cpp_extension import load_inline\n\ncuda_source = \"\"\"\n#include <torch/extension.h>\n#include <cuda_runtime.h>\n\n__global__ void fused_postprocess_kernel(const float* __restrict__ z,\n const float* __restrict__ y,\n float* __restrict__ out,\n int batch_size,\n int out_features,\n float eps) {\n int row = blockIdx.x;\n if (row >= batch_size) return;\n \n int tid = threadIdx.x;\n int num_threads = blockDim.x;\n int lane_id = tid & 31;\n int warp_id = tid >> 5;\n \n const float* z_row = z + (int64_t)row * out_features;\n const float* y_row = y + (int64_t)row * out_features;\n float* out_row = out + (int64_t)row * out_features;\n \n double local_sum = 0.0;\n double local_sum_sq = 0.0;\n \n int num_vec = out_features / 4;\n const float4* z4_row = reinterpret_cast<const float4*>(z_row);\n \n // Vectorized first pass\n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w;\n local_sum_sq += (double)z4.x * (double)z4.x \n + (double)z4.y * (double)z4.y \n + (double)z4.z * (double)z4.z \n + (double)z4.w * (double)z4.w;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n double val = (double)z_row[i];\n local_sum += val;\n local_sum_sq += val * val;\n }\n \n // Warp reduction for double\n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n local_sum += __shfl_down_sync(0xffffffff, local_sum, offset);\n local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset);\n }\n \n __shared__ double warp_sum[32];\n __shared__ double warp_sum_sq[32];\n __shared__ float s_mean;\n __shared__ float s_inv_std;\n \n if (lane_id == 0) {\n warp_sum[warp_id] = local_sum;\n warp_sum_sq[warp_id] = local_sum_sq;\n }\n __syncthreads();\n \n // Cross-warp reduction\n if (warp_id == 0) {\n double block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0;\n double block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0;\n \n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n block_sum += __shfl_down_sync(0xffffffff, block_sum, offset);\n block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset);\n }\n \n if (lane_id == 0) {\n float mean = (float)(block_sum / (double)out_features);\n double variance = block_sum_sq / (double)out_features - (double)mean * (double)mean;\n if (variance < 0.0) variance = 0.0;\n float inv_std = rsqrtf((float)variance + eps);\n s_mean = mean;\n s_inv_std = inv_std;\n }\n }\n __syncthreads();\n \n float mean = s_mean;\n float inv_std = s_inv_std;\n \n // Vectorized second pass\n const float4* y4_row = reinterpret_cast<const float4*>(y_row);\n float4* out4_row = reinterpret_cast<float4*>(out_row);\n \n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n float4 y4 = y4_row[i];\n float4 o4;\n o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x;\n o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y;\n o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z;\n o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w;\n out4_row[i] = o4;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n float z_val = z_row[i];\n float y_val = y_row[i];\n float norm = (z_val - mean) * inv_std;\n out_row[i] = (norm + y_val) * y_val;\n }\n}\n\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) {\n int batch_size = z.size(0);\n int out_features = z.size(1);\n \n auto out = torch::empty_like(z);\n \n int threads = 256;\n if (out_features <= 128) threads = 64;\n else if (out_features <= 512) threads = 128;\n \n int blocks = batch_size;\n \n fused_postprocess_kernel<<<blocks, threads>>>(\n z.data_ptr<float>(),\n y.data_ptr<float>(),\n out.data_ptr<float>(),\n batch_size,\n out_features,\n eps\n );\n \n return out;\n}\n\"\"\"\n\ncpp_source = \"\"\"\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps);\n\"\"\"\n\nfused_postprocess = load_inline(\n name=\"fused_postprocess\",\n cpp_sources=cpp_source,\n cuda_sources=cuda_source,\n functions=[\"fused_postprocess\"],\n extra_cuda_cflags=[\"-O3\", \"--use_fast_math\"],\n)\n\nclass ModelNew(nn.Module):\n def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1):\n super().__init__()\n self.bmm = nn.Linear(in_features, out_features)\n self.eps = eps\n \n def forward(self, x, y):\n z = self.bmm(x)\n return fused_postprocess.fused_postprocess(z, y, self.eps)\n" }
result ← run_correctness (ok)
okrun_correctness run_correctness PASSED: (5 / 5) trials all matched the reference. Numerical precision: max_abs_err=9.54e-07 mean_abs_err=1.35e-08 max_rel_err=8.98e-01
turn 3 · 1 tool call(s) · 7.1s turn · 7.1s LLM · 6,357 chars (click to expand)
turn 37.1s turn · 7.1s LLM · 0.0s tools
reasoning
The kernel compiles and is numerically correct. Let me run the static check and then submit.
call → static_check
callstatic_check { "kernel_code": "\nimport torch\nimport torch.nn as nn\nfrom torch.utils.cpp_extension import load_inline\n\ncuda_source = \"\"\"\n#include <torch/extension.h>\n#include <cuda_runtime.h>\n\n__global__ void fused_postprocess_kernel(const float* __restrict__ z,\n const float* __restrict__ y,\n float* __restrict__ out,\n int batch_size,\n int out_features,\n float eps) {\n int row = blockIdx.x;\n if (row >= batch_size) return;\n \n int tid = threadIdx.x;\n int num_threads = blockDim.x;\n int lane_id = tid & 31;\n int warp_id = tid >> 5;\n \n const float* z_row = z + (int64_t)row * out_features;\n const float* y_row = y + (int64_t)row * out_features;\n float* out_row = out + (int64_t)row * out_features;\n \n double local_sum = 0.0;\n double local_sum_sq = 0.0;\n \n int num_vec = out_features / 4;\n const float4* z4_row = reinterpret_cast<const float4*>(z_row);\n \n // Vectorized first pass\n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w;\n local_sum_sq += (double)z4.x * (double)z4.x \n + (double)z4.y * (double)z4.y \n + (double)z4.z * (double)z4.z \n + (double)z4.w * (double)z4.w;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n double val = (double)z_row[i];\n local_sum += val;\n local_sum_sq += val * val;\n }\n \n // Warp reduction for double\n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n local_sum += __shfl_down_sync(0xffffffff, local_sum, offset);\n local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset);\n }\n \n __shared__ double warp_sum[32];\n __shared__ double warp_sum_sq[32];\n __shared__ float s_mean;\n __shared__ float s_inv_std;\n \n if (lane_id == 0) {\n warp_sum[warp_id] = local_sum;\n warp_sum_sq[warp_id] = local_sum_sq;\n }\n __syncthreads();\n \n // Cross-warp reduction\n if (warp_id == 0) {\n double block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0;\n double block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0;\n \n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n block_sum += __shfl_down_sync(0xffffffff, block_sum, offset);\n block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset);\n }\n \n if (lane_id == 0) {\n float mean = (float)(block_sum / (double)out_features);\n double variance = block_sum_sq / (double)out_features - (double)mean * (double)mean;\n if (variance < 0.0) variance = 0.0;\n float inv_std = rsqrtf((float)variance + eps);\n s_mean = mean;\n s_inv_std = inv_std;\n }\n }\n __syncthreads();\n \n float mean = s_mean;\n float inv_std = s_inv_std;\n \n // Vectorized second pass\n const float4* y4_row = reinterpret_cast<const float4*>(y_row);\n float4* out4_row = reinterpret_cast<float4*>(out_row);\n \n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n float4 y4 = y4_row[i];\n float4 o4;\n o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x;\n o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y;\n o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z;\n o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w;\n out4_row[i] = o4;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n float z_val = z_row[i];\n float y_val = y_row[i];\n float norm = (z_val - mean) * inv_std;\n out_row[i] = (norm + y_val) * y_val;\n }\n}\n\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) {\n int batch_size = z.size(0);\n int out_features = z.size(1);\n \n auto out = torch::empty_like(z);\n \n int threads = 256;\n if (out_features <= 128) threads = 64;\n else if (out_features <= 512) threads = 128;\n \n int blocks = batch_size;\n \n fused_postprocess_kernel<<<blocks, threads>>>(\n z.data_ptr<float>(),\n y.data_ptr<float>(),\n out.data_ptr<float>(),\n batch_size,\n out_features,\n eps\n );\n \n return out;\n}\n\"\"\"\n\ncpp_source = \"\"\"\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps);\n\"\"\"\n\nfused_postprocess = load_inline(\n name=\"fused_postprocess\",\n cpp_sources=cpp_source,\n cuda_sources=cuda_source,\n functions=[\"fused_postprocess\"],\n extra_cuda_cflags=[\"-O3\", \"--use_fast_math\"],\n)\n\nclass ModelNew(nn.Module):\n def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1):\n super().__init__()\n self.bmm = nn.Linear(in_features, out_features)\n self.eps = eps\n \n def forward(self, x, y):\n z = self.bmm(x)\n return fused_postprocess.fused_postprocess(z, y, self.eps)\n" }
result ← static_check (ok)
okstatic_check static_check PASSED: no violations or warnings detected.
turn 4 · FINAL · 1 tool call(s) · 15.2s turn · 15.2s LLM · 7,506 chars (click to expand)
turn 415.2s turn · 15.2s LLM · 0.0s tools · FINAL
reasoning
The kernel compiled successfully, passes correctness, and has no static check violations. Let me now submit this kernel. To summarize what I optimized: 1. The nn.Linear is compute-bound on a large matrix of size 1024x8192, so I kept it as-is, letting cuBLAS handle it optimally 2. The post-linear operations (instance norm, residual add, element-wise multiply) are memory-bound, so I fused them into a single kernel that: - Computes mean and variance over each row (instance norm across last dim) - Computes normalized output, adds residual, and multiplies with residual - All in one pass per row, reducing memory bandwidth by 4x - Uses float4 vectorized loads/stores for better memory throughput - Uses double precision for reduction to avoid numerical errors This should be significantly faster than the reference which does multiple separate memory passes.
call → submit_kernel
callsubmit_kernel { "kernel_code": "\nimport torch\nimport torch.nn as nn\nfrom torch.utils.cpp_extension import load_inline\n\ncuda_source = \"\"\"\n#include <torch/extension.h>\n#include <cuda_runtime.h>\n\n__global__ void fused_postprocess_kernel(const float* __restrict__ z,\n const float* __restrict__ y,\n float* __restrict__ out,\n int batch_size,\n int out_features,\n float eps) {\n int row = blockIdx.x;\n if (row >= batch_size) return;\n \n int tid = threadIdx.x;\n int num_threads = blockDim.x;\n int lane_id = tid & 31;\n int warp_id = tid >> 5;\n \n const float* z_row = z + (int64_t)row * out_features;\n const float* y_row = y + (int64_t)row * out_features;\n float* out_row = out + (int64_t)row * out_features;\n \n double local_sum = 0.0;\n double local_sum_sq = 0.0;\n \n int num_vec = out_features / 4;\n const float4* z4_row = reinterpret_cast<const float4*>(z_row);\n \n // Vectorized first pass\n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w;\n local_sum_sq += (double)z4.x * (double)z4.x \n + (double)z4.y * (double)z4.y \n + (double)z4.z * (double)z4.z \n + (double)z4.w * (double)z4.w;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n double val = (double)z_row[i];\n local_sum += val;\n local_sum_sq += val * val;\n }\n \n // Warp reduction for double\n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n local_sum += __shfl_down_sync(0xffffffff, local_sum, offset);\n local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset);\n }\n \n __shared__ double warp_sum[32];\n __shared__ double warp_sum_sq[32];\n __shared__ float s_mean;\n __shared__ float s_inv_std;\n \n if (lane_id == 0) {\n warp_sum[warp_id] = local_sum;\n warp_sum_sq[warp_id] = local_sum_sq;\n }\n __syncthreads();\n \n // Cross-warp reduction\n if (warp_id == 0) {\n double block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0;\n double block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0;\n \n #pragma unroll\n for (int offset = 16; offset > 0; offset /= 2) {\n block_sum += __shfl_down_sync(0xffffffff, block_sum, offset);\n block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset);\n }\n \n if (lane_id == 0) {\n float mean = (float)(block_sum / (double)out_features);\n double variance = block_sum_sq / (double)out_features - (double)mean * (double)mean;\n if (variance < 0.0) variance = 0.0;\n float inv_std = rsqrtf((float)variance + eps);\n s_mean = mean;\n s_inv_std = inv_std;\n }\n }\n __syncthreads();\n \n float mean = s_mean;\n float inv_std = s_inv_std;\n \n // Vectorized second pass\n const float4* y4_row = reinterpret_cast<const float4*>(y_row);\n float4* out4_row = reinterpret_cast<float4*>(out_row);\n \n for (int i = tid; i < num_vec; i += num_threads) {\n float4 z4 = z4_row[i];\n float4 y4 = y4_row[i];\n float4 o4;\n o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x;\n o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y;\n o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z;\n o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w;\n out4_row[i] = o4;\n }\n \n // Scalar remainder\n for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {\n float z_val = z_row[i];\n float y_val = y_row[i];\n float norm = (z_val - mean) * inv_std;\n out_row[i] = (norm + y_val) * y_val;\n }\n}\n\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) {\n int batch_size = z.size(0);\n int out_features = z.size(1);\n \n auto out = torch::empty_like(z);\n \n int threads = 256;\n if (out_features <= 128) threads = 64;\n else if (out_features <= 512) threads = 128;\n \n int blocks = batch_size;\n \n fused_postprocess_kernel<<<blocks, threads>>>(\n z.data_ptr<float>(),\n y.data_ptr<float>(),\n out.data_ptr<float>(),\n batch_size,\n out_features,\n eps\n );\n \n return out;\n}\n\"\"\"\n\ncpp_source = \"\"\"\ntorch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps);\n\"\"\"\n\nfused_postprocess = load_inline(\n name=\"fused_postprocess\",\n cpp_sources=cpp_source,\n cuda_sources=cuda_source,\n functions=[\"fused_postprocess\"],\n extra_cuda_cflags=[\"-O3\", \"--use_fast_math\"],\n)\n\nclass ModelNew(nn.Module):\n def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1):\n super().__init__()\n self.bmm = nn.Linear(in_features, out_features)\n self.eps = eps\n \n def forward(self, x, y):\n z = self.bmm(x)\n return fused_postprocess.fused_postprocess(z, y, self.eps)\n" }
result ← submit_kernel (ok)
oksubmit_kernel submit_kernel PASSED: (5 / 5) correctness trials all passed. Kernel runtime: 2.71 μs Runtime stats: mean=2.71μs median=?μs std=0.00μs Numerical precision: max_abs_err=9.54e-07 mean_abs_err=1.35e-08 max_rel_err=8.98e-01 Memory: 673.06 MB peak (ref: 673.07 MB, ratio: 1.0x) Kernel launches: 7 (ref: 31, fusion ratio: 4.4286) Energy: 1224.38 mJ/run (ref: 2643.6 mJ, ratio: 2.1591x) SOL score: 0.8592
final submitted kernel (164 lines, 5,241 chars) — full source, untruncated
import torch
import torch.nn as nn
from torch.utils.cpp_extension import load_inline

cuda_source = """
#include <torch/extension.h>
#include <cuda_runtime.h>

__global__ void fused_postprocess_kernel(const float* __restrict__ z,
                                         const float* __restrict__ y,
                                         float* __restrict__ out,
                                         int batch_size,
                                         int out_features,
                                         float eps) {
    int row = blockIdx.x;
    if (row >= batch_size) return;
    
    int tid = threadIdx.x;
    int num_threads = blockDim.x;
    int lane_id = tid & 31;
    int warp_id = tid >> 5;
    
    const float* z_row = z + (int64_t)row * out_features;
    const float* y_row = y + (int64_t)row * out_features;
    float* out_row = out + (int64_t)row * out_features;
    
    double local_sum = 0.0;
    double local_sum_sq = 0.0;
    
    int num_vec = out_features / 4;
    const float4* z4_row = reinterpret_cast<const float4*>(z_row);
    
    // Vectorized first pass
    for (int i = tid; i < num_vec; i += num_threads) {
        float4 z4 = z4_row[i];
        local_sum += (double)z4.x + (double)z4.y + (double)z4.z + (double)z4.w;
        local_sum_sq += (double)z4.x * (double)z4.x 
                      + (double)z4.y * (double)z4.y 
                      + (double)z4.z * (double)z4.z 
                      + (double)z4.w * (double)z4.w;
    }
    
    // Scalar remainder
    for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {
        double val = (double)z_row[i];
        local_sum += val;
        local_sum_sq += val * val;
    }
    
    // Warp reduction for double
    #pragma unroll
    for (int offset = 16; offset > 0; offset /= 2) {
        local_sum += __shfl_down_sync(0xffffffff, local_sum, offset);
        local_sum_sq += __shfl_down_sync(0xffffffff, local_sum_sq, offset);
    }
    
    __shared__ double warp_sum[32];
    __shared__ double warp_sum_sq[32];
    __shared__ float s_mean;
    __shared__ float s_inv_std;
    
    if (lane_id == 0) {
        warp_sum[warp_id] = local_sum;
        warp_sum_sq[warp_id] = local_sum_sq;
    }
    __syncthreads();
    
    // Cross-warp reduction
    if (warp_id == 0) {
        double block_sum = (lane_id < (num_threads >> 5)) ? warp_sum[lane_id] : 0.0;
        double block_sum_sq = (lane_id < (num_threads >> 5)) ? warp_sum_sq[lane_id] : 0.0;
        
        #pragma unroll
        for (int offset = 16; offset > 0; offset /= 2) {
            block_sum += __shfl_down_sync(0xffffffff, block_sum, offset);
            block_sum_sq += __shfl_down_sync(0xffffffff, block_sum_sq, offset);
        }
        
        if (lane_id == 0) {
            float mean = (float)(block_sum / (double)out_features);
            double variance = block_sum_sq / (double)out_features - (double)mean * (double)mean;
            if (variance < 0.0) variance = 0.0;
            float inv_std = rsqrtf((float)variance + eps);
            s_mean = mean;
            s_inv_std = inv_std;
        }
    }
    __syncthreads();
    
    float mean = s_mean;
    float inv_std = s_inv_std;
    
    // Vectorized second pass
    const float4* y4_row = reinterpret_cast<const float4*>(y_row);
    float4* out4_row = reinterpret_cast<float4*>(out_row);
    
    for (int i = tid; i < num_vec; i += num_threads) {
        float4 z4 = z4_row[i];
        float4 y4 = y4_row[i];
        float4 o4;
        o4.x = ((z4.x - mean) * inv_std + y4.x) * y4.x;
        o4.y = ((z4.y - mean) * inv_std + y4.y) * y4.y;
        o4.z = ((z4.z - mean) * inv_std + y4.z) * y4.z;
        o4.w = ((z4.w - mean) * inv_std + y4.w) * y4.w;
        out4_row[i] = o4;
    }
    
    // Scalar remainder
    for (int i = tid + num_vec * 4; i < out_features; i += num_threads) {
        float z_val = z_row[i];
        float y_val = y_row[i];
        float norm = (z_val - mean) * inv_std;
        out_row[i] = (norm + y_val) * y_val;
    }
}

torch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps) {
    int batch_size = z.size(0);
    int out_features = z.size(1);
    
    auto out = torch::empty_like(z);
    
    int threads = 256;
    if (out_features <= 128) threads = 64;
    else if (out_features <= 512) threads = 128;
    
    int blocks = batch_size;
    
    fused_postprocess_kernel<<<blocks, threads>>>(
        z.data_ptr<float>(),
        y.data_ptr<float>(),
        out.data_ptr<float>(),
        batch_size,
        out_features,
        eps
    );
    
    return out;
}
"""

cpp_source = """
torch::Tensor fused_postprocess(torch::Tensor z, torch::Tensor y, float eps);
"""

fused_postprocess = load_inline(
    name="fused_postprocess",
    cpp_sources=cpp_source,
    cuda_sources=cuda_source,
    functions=["fused_postprocess"],
    extra_cuda_cflags=["-O3", "--use_fast_math"],
)

class ModelNew(nn.Module):
    def __init__(self, in_features, out_features, eps=1e-5, momentum=0.1):
        super().__init__()
        self.bmm = nn.Linear(in_features, out_features)
        self.eps = eps
        
    def forward(self, x, y):
        z = self.bmm(x)
        return fused_postprocess.fused_postprocess(z, y, self.eps)