reasoning
I still have correctness issues. Let me think about this more carefully. The difference is consistently around 3.5e-4 which is slightly above 1e-4.
For ConvTranspose1d with stride=1, padding=0, dilation=3, kernel_size=5:
- out_length = 131072 (same as in_length because stride=1, padding=0, dilation=3, kernel_size=5)
out_length = (131072 - 1) * 1 - 0 + 3*(5-1) + 1 = 131071 + 12 + 1 = 131084
Hmm, let me recalculate: (131072 - 1) * 1 - 2 * 0 + 3 * (5 - 1) + 1 = 131071 + 12 + 1 = 131084.
So the output is longer than the input.
Let me look at how the kernel accesses input. For each output position o and kernel element k:
- in_pos = o - k * dilation = o - k * 3
Let me think about which input positions contribute to output position o=0:
o=0: in_pos = 0 - k*3, so only k=0 gives in_pos=0. Others negative.
o=1: in_pos = 1 - k*3, only k=0 gives 1. Others negative.
o=2: in_pos = 2 - k*3, only k=0 gives 2. Others negative.
o=3: in_pos = 3 - k*3, k=0: 3, k=1: 0.
etc.
Now let me verify with a small example.
Actually, I think I need to reconsider. In the reference implementation, if I look at nn.ConvTranspose1d, for `stride=1, padding=0, dilation=3, kernel_size=5`:
The output length is indeed 131084.
But wait, I think I might have gotten the formula wrong for the kernel. Let me re-read the PyTorch documentation for ConvTranspose1d:
out_length = (in_length - 1) * stride - 2 * padding + dilation * (kernel_size - 1) + output_padding + 1
Since stride=1, padding=0, dilation=3, kernel_size=5, output_padding=0:
out = (131072-1)*1 - 0 + 3*4 + 0 + 1 = 131071 + 12 + 1 = 131084
That's correct.
Now for the kernel: when computing output position o, the weights that multiply with input position i are those where:
o = i + k*dilation
k = (o - i) / dilation
Wait, is that right? Actually, for a transposed convolution:
Each input position `i` contributes to output positions `o = i * stride + k * dilation` for k=0,...,kernel_size-1, after adjusting for padding.
But `stride=1`, so output positions `o = i + k * dilation` (neglecting other adjustments).
Hmm wait, that's what I use! `in_pos = o - k * dilation` gives `o = in_pos + k * dilation`.
Let me verify with a small example:
- input length = 2, kernel_size = 2, stride=1, dilation=1, padding=0.
- Output length = (2-1)*1 + 1*(2-1) + 1 = 3
- According to transposed conv formula: o = i + k for each input i and kernel k.
- Input i=0: contributes to o=0 (k=0), o=1 (k=1)
- Input i=1: contributes to o=1 (k=0), o=2 (k=1)
So output:
o=0: input[0]*weight[0]
o=1: input[0]*weight[1] + input[1]*weight[0]
o=2: input[1]*weight[1]
Now with our access pattern for a given o:
For o=0: search for i such that o = i + k, i.e., i = 0-k. k=0 => i=0. k=1 => i=-1.
So output[0] = input[0] * w[0]. Correct.
For o=1: k=0 => i=1. k=1 => i=0.
output[1] = input[1]*w[0] + input[0]*w[1]. Correct!
For o=2: k=0 => i=2 (out of range). k=1 => i=1.
output[2] = input[1]*w[1]. Correct!
So our inner loop logic:
```cpp
for (int k = 0; k < kernel_size; k++) {
int in_pos = o - k * dilation;
if (in_pos >= 0 && in_pos < in_length) {
sum += in_ptr[in_pos] * w_ptr[k];
}
}
```
ALSO gives the correct result! Great, the algorithm is correct.
So the issue is floating point precision in the accumulation order.
Let me think about the tolerance: atol=1e-4, rtol=1e-4.
The outputs can be around 5-10 (since inputs are rand[0,1], 32 channels, kernel_size=5, so sum of 160 terms, average value ~0.5 per term, total ~80). Actually, if rand is uniform [0,1], the mean is 0.5. 32 * 5 = 160 products. Each product ~0.25 on average. Sum ~40.
Hmm, a max difference of 3e-4 for values ~40-80 seems reasonable for accumulation order differences, but we need to be within 1e-4 absolute tolerance.
Since our double precision version also failed with the same difference, this means the reference is actually computing with different precision! Maybe PyTorch uses split K or zigzag accumulation in cudnn, or maybe it casts differently.
Actually, wait. I said double precision also gave the same difference. Let me re-examine. For the double precision test, max difference was 3.7e-4. But the reference uses float (fp32). So if I accumulate in double and store as float, the result should be MORE accurate than the reference. If it doesn't match, there might be a formulation difference.
Hold on - I had a realization. The PyTorch ConvTranspose1d might actually be implemented by upsampling the input with stride and applying a dilated regular convolution! And the way it computes might involve zero insertions in a specific pattern.
But more importantly, the difference could be because of the weight layout. Let me check if PyTorch uses interleaved channels in the transposed convolution...
Actually, I just realized: maybe the reference solution uses tf32 tensor cores! On Ampere and later GPUs, cudnn can use tf32 for convolutions which has reduced precision. Our CUDA kernel uses fp32 arithmetic.
Wait, but if the reference uses tf32, then our fp32 result should be MORE precise, not less. If there's a 3e-4 difference, it's because of accumulation order, not rounding per operation.
In any case, maybe PyTorch/cudnn is computing the conv transpose differently. But the algorithm itself is the same mathematically.
Let me try a completely different approach: actually use PyTorch's implementation but with Autograd disabled or something? No, the task is to implement a custom CUDA kernel.
OK, maybe the strict fp32 computation in our kernel causes the result to be the "exact" fp32 result, while cudnn's result (which might use tf32 or mixed precision) is slightly different. And if the reference is cudnn's result, then we're "too accurate" and diverge from it.
But the tolerance is 1e-4. For values around 40, 3e-4 is a relative error of 7.5e-6. For values around 0, it's an absolute error of 3e-4 which is above 1e-4.
But wait, the avg_difference is 5e-5 and max is 3.5e-4. That means some values have a difference of 3.5e-4 while most are at 5e-5.
Could some output values be very close to zero, causing the relative difference to be large even though absolute is small? No, the reported difference is absolute difference (or is it max relative?).
Actually, looking at the test harness, it says `max_difference` and `avg_difference`. These are likely absolute differences.
Let me try to use the exact same computation order as PyTorch. But that's hard without knowing the internal algorithm.
Or... maybe there's something subtle in the algorithm. Let me re-read:
For transposed conv with dilation, the weight is "dilated". So a weight of size kernel_size with dilation means the effective kernel is larger.
But actually, in PyTorch:
- ConvTranspose1d with `dilation=3, kernel_size=5` means: each weight element is spaced 3 apart.
- The output length formula accounts for this.
Wait, I just need to check if maybe cudnn is computing regular convolution on an upsampled input, which would mean the weight is applied to different positions.
Actually, let me just try a small hack: use `cutlass` or `cublas` through PyTorch's APIs to compute the same thing. But the task requires a custom CUDA kernel.
Let me try yet another algorithm: use shared memory tiling in a way that matches the natural access pattern better, and see if the ordering changes enough to match. Or perhaps the reference computation uses a specific order that we can replicate.
Actually, I think I should consider that PyTorch might be using deterministic algorithms or specific implementations. For conv_transpose on cuda, PyTorch calls cudnn which uses highly optimized kernels. The numerical difference is likely from tf32 tensor cores.
If that's the case, then maybe we need to intentionally use the same reduced precision mode. But we can't easily use tf32 tensor cores in a custom kernel unless we explicitly use CUDA tensor core APIs.
OR, maybe we can use CUTLASS... but that's complex.
Alternatively, maybe the reference is computed using float32 but with a different algorithm like im2col + GEMM, where the accumulation happens in a different order (matrix multiplication order). Our direct accumulation loops in channel-major then kernel-major order. A GEMM-based approach would have a different accumulation order.
Can we try to implement using im2col + GEMM in a custom kernel? That might match the reference better.
But wait, if I use cuBLAS GEMM with fp32, the accumulation should still be in fp32. However, cuBLAS may use tensor cores with tf32 by default on H100. But I'm not sure.
Actually, maybe I can just use `torch.matmul` inside Python to implement this, wrapped in a custom kernel... but that defeats the purpose of writing a custom CUDA kernel.
Let me try yet another idea: maybe the tolerance of 1e-4 is achievable if I accumulate in a way that matches PyTorch's order more closely.
Let me think about the PyTorch im2col approach for transposed convolution with stride=1:
For stride=1, transposed conv is equivalent to: pad the input appropriately, then apply a dilated regular convolution.
With dilation=3, kernel_size=5:
The "dilated" kernel effectively has size: (kernel_size - 1) * dilation + 1 = 13.
For transposed conv with stride=1, padding=0, dilation=3:
padding_out = (kernel_size - 1) * dilation - padding = 12.
Then equivalent regular conv:
- pad input with 12 zeros on each side.
- apply conv with kernel_size=5, dilation=3, stride=1.
Wait, that doesn't make sense. Let me think again.
Actually, transposed convolution with stride=1 and zero padding is mathematically just cross-correlation (regular conv) with a dilated kernel applied to the input. So our algorithm should be correct.
Let me verify with a tiny program actually:
```python
import torch
import torch.nn as nn
in_ch = 1
out_ch = 1
ks = 3
dil = 2
L = 5
model = nn.ConvTranspose1d(in_ch, out_ch, ks, stride=1, padding=0, dilation=dil, bias=False)
model.weight.data.fill_(1.0)
x = torch.ones(1, 1, L)
y = model(x)
print(y)
# manual: for each output position o
# y[o] = sum_k x[o - k*dil] * w[k] for valid positions
out_len = (L-1)*1 + dil*(ks-1) + 1
y_manual = torch.zeros(1, 1, out_len)
for o in range(out_len):
s = 0
for k in range(ks):
ip = o - k*dil
if ip >= 0 and ip < L:
s += x[0, 0, ip] * model.weight[0, 0, k]
y_manual[0, 0, o] = s
print(y_manual)
```
If I could run this, I could verify. Let me reason through it:
L=5, ks=3, dil=2
out = (5-1) + 2*(3-1) + 1 = 4 + 4 + 1 = 9
x = [1, 1, 1, 1, 1]
w = [1, 1, 1]
o=0: k=0: ip=0, valid. k=1: ip=-2, invalid. k=2: ip=-4, invalid. sum=1
o=1: k=0: ip=1, valid. k=1: ip=-1, invalid. sum=1
o=2: k=0: ip=2, valid. k=1: ip=0, valid. k=2: ip=-2, invalid. sum=2
o=3: k=0: ip=3, valid. k=1: ip=1, valid. k=2: ip=-1, invalid. sum=2
o=4: k=0: ip=4, valid. k=1: ip=2, valid. k=2: ip=0, valid. sum=3
o=5: k=0: ip=5, invalid. k=1: ip=3, valid. k=2: ip=1, valid. sum=2
o=6: k=0: ip=6, invalid. k=1: ip=4, valid. k=2: ip=2, valid. sum=2
o=7: k=0: ip=7, invalid. k=1: ip=5, invalid. k=2: ip=3, valid. sum=1
o=8: k=0: ip=8, invalid. k=1: ip=6, invalid. k=2: ip=4, valid. sum=1
So y = [1, 1, 2, 2, 3, 2, 2, 1, 1]
Now let me check what PyTorch produces. Your manual computation is exactly the transposed conv formula. So our algorithm is correct.
Since our algorithm is correct and the reference likely uses a different accumulation precision/order, the only way to match within 1e-4 is to either:
1. Match the exact computation pattern
2. Accept that there's a ~3e-4 difference and find a way to reduce it.
Wait, actually, maybe I can try accumulating in a specific order. Let me try flipping the loops: for each c_in, iterate k from kernel_size-1 down to 0.
No, that would just change the rounding pattern.
Or maybe I should try a batched/column-major accumulation similar to im2col. In im2col, you extract patches and do matmul. Since the reference likely uses im2col + GEMM, maybe I can do that too!
If I can't get the direct CUDA kernel to match, perhaps I can implement im2col + GEMM in a custom kernel. But that might not be much faster than cudnn. However, for this specific case (dilated small kernel, very long sequence), maybe I can do better.
Actually, for this specific problem: in_channels=32, out_channels=64, kernel_size=5, length=131072, stride=1, padding=0, dilation=3.
The output size is 131084.
A direct approach computes: batch_size * out_channels * output_length * in_channels * kernel_size ≈ 32 * 64 * 131084 * 32 * 5 = 42.8 billion ops.
If we view this as a matrix multiplication:
- We can unfold the input: shape [batch, in_channels, in_length] -> we want to compute for each output position, a weighted sum over input patches.
- For transposed conv, it's like the adjoint of regular conv.
Actually, I think the cleanest approach to match PyTorch exactly is to write an im2col kernel and then use cublas. But let me see if I can make a simpler custom kernel.
Wait, another idea: maybe PyTorch's conv_transpose for stride=1 is actually implemented using a regular convolution with appropriately padded input and dilated kernel. But if padding=0 and stride=1:
output = F.conv1d(F.pad(input, [padding_left, padding_right]), weight, dilation=dilation)
where padding_left = (kernel_size - 1) * dilation - padding = 12
padding_right = (kernel_size - 1) * dilation - padding = 12
So if I pad input with 12 zeros on each side and apply a dilated regular convolution using our kernel, would that match?
Let me check algorithmically:
For regular conv with pad=12, dilation=3, kernel_size=5:
For output position o, the input access is:
input_padded[o + 0*dilation] * w[0] + input_padded[o + 1*dilation] * w[1] + ...
Since the padding adds 12 zeros on the left, input_padded[i] = input[i-12] for i >= 12.
So input_padded[o + k*3] = input[o + k*3 - 12]
For this to equal our transposed conv formula where we access input[o - k*3]:
input[o - k*3] = input[o + k*3 - 12]
This requires -k = k - 12/dilation for all k, which is impossible.
So the padding relationship is more complex. Actually, for transposed conv:
Equivalent regular conv has:
- stride=1
- padding_out = kernel_size - 1 - padding = 4
- output_padding = 0
- dilation = dilation
I think I'm confusing myself. Let me just verify with a small example.
Actually, I know what: let me write a kernel that exactly replicates the formula but uses tiling strategies that might naturally produce the same accumulation order as cuDNN. But I don't know cuDNN's specific order.
Another thought: could the mismatch be because of NaN or Inf in some positions? The avg_diff is very small (5e-5) but max is 3.5e-4. That means a few positions have larger errors.
Could the larger errors be at the boundaries where fewer terms are summed?
Actually, if I accumulate fewer terms at boundaries, the floating point error should be smaller, not larger. Unless there's catastrophic cancellation.
OK, let me try a COMPLETELY different approach.
Since the kernel is small (5) and in_channels is 32, out_channels is 64, this is essentially a small matrix-vector product for each output position:
For each output position o:
output[:, o] = M @ input[:, associated_positions]
Where M is 64 × (32×5) = 64 × 160, and input[:, associated_positions] is a 160-dim vector.
If I implement this as a batched matrix-vector product using shared memory to store the weight matrix, I might get both speed and potentially different numerical properties.
But I think the fundamental issue is just accumulation order. Let me try accumulating in groups:
- For each c_in and k, multiply and add to a local sum
- But instead of c_in outer, k inner, let me try k outer, c_in inner.
Wait, I already tried that! The direct version.
Actually, let me try using the exact GEMM formulation by reshaping the problem.
For ConvTranspose1d with stride=1, we can reshape:
For each batch sample n and output position o:
y[n, c_out, o] = sum_{c_in} sum_{k=0}^{K-1} x[n, c_in, o - k*dilation] * w[c_in, c_out, k]
This is a sum over (c_in, k) pairs. If we linearize (c_in, k) -> idx:
idx = c_in * K + k
Then y[n, c_out, o] = sum_{idx} x_flat[n, idx_at_o] * w_flat[idx, c_out]
Where x_flat[n, idx_at_o] is the appropriate input element for output position o and index idx.
This is a batched matrix multiplication! For each n and o, we can view it as dot(w_flat[:, c_out], x_patch).
More specifically, if we use im2col: for each output position o, collect all input elements that contribute:
x_col[o, idx] = x[n, c_in, o - k*dilation] (for valid positions)
Then y[:, c_out, o] = x_col[o, :] @ w_flat[:, c_out]
This is a GEMM: x_col (out_length × (in_channels*kernel_size)) @ w_flat^T ((in_channels*kernel_size) × out_channels).
So we can compute the entire thing as:
y_n = x_col_n @ w_flat^T
where x_col_n is out_length × 160, w_flat^T is 160 × 64.
This is a GEMM of size (131084 × 160) @ (160 × 64) for each batch, or batched (32 × 131084 × 160) @ (160 × 64).
Actually, the total size is:
- A: [32, 131084, 160]
- B: [160, 64]
- C: [32, 131084, 64]
Since the matrices are tall and skinny (131084 rows, 160 cols), this is a perfect case for GEMM.
To match PyTorch numerically, I can:
1. Write an im2col kernel that extracts patches
2. Use cublas GEMM
Or even better, I can use CUTLASS or just use torch.matmul (but that wouldn't be a custom CUDA kernel for the whole op).
Actually, the task says "Implement forward() with a custom CUDA kernel" and "Use torch.utils.cpp_extension.load_inline to compile and bind CUDA source". So I can write a CUDA kernel that calls cublas inside it!
Let me think about whether this would match numerically. If cuBLAS and cuDNN both use similar GEMM algorithms, they might match. Or they might not.
But wait, the problem is: PyTorch's ConvTranspose1d might call cuDNN which uses winograd or FFT for this case, not GEMM. For large feature maps and small kernels, direct convolution or winograd might be used.
However, looking at the specific sizes (131072 length, kernel_size=5), cuDNN might use an optimized direct algorithm or im2col + GEMM. If it's GEMM-based, then our cuBLAS GEMM approach might match better.
Let me try this approach! I'll write an im2col + GEMM kernel.
Actually, to keep it simple, I can precompute the im2col in shared memory and then call cublas for each tile.
But cublas batch GEMM might be complex to set up in a custom kernel. Let me think...
Actually, let me re-read the error. The difference is about 3.5e-4 which is above 1e-4 but not by much. Maybe with some algorithm tweaks I can reduce it further.
Wait, maybe the reference result has some specific behavior because of tf32. Let me check if tf32 is enabled by default on H100.
In PyTorch, tf32 is enabled by default for convolutions on Ampere/Hopper (since PyTorch 1.7+ I think). So the reference computation might use tf32 tensor cores!
If the reference uses tf32, then our fp32 computation will naturally differ. To match it, we might need to deliberately use tf32 or a lower precision accumulation.
However, tf32 has a 10-bit mantissa (vs 23 for fp32). This gives about 3 significant decimal digits of precision. For values around 40, the rounding error is about 0.04 - much larger than 3.5e-4!
So if the reference were computed purely in tf32, the difference would be MUCH larger than 3.5e-4. The actual difference of 3.5e-4 suggests the reference is mostly fp32, with some difference in accumulation order.
OK let me try yet another attempt. What if I implement the kernel as a simple im2col in shared memory followed by manual matmul, but with careful ordering to try to match a typical GEMM pattern?
Actually, I just realized: what if the error is not due to accumulation order but due to how we handle positions near the boundary? Let me double-check.
Hmm, my sanity check formula says the algorithm is correct. And the difference is very uniform across all trials, which strongly suggests numerical precision issues rather than algorithmic bugs.
Let me try one more idea: accumulate into half precision or use __fmaf_rn for explicit rounding control.
Actually, let me try keeping the weight in registers and loading input from global memory directly. But that's what the direct kernel does.
Wait! I just had a thought. What if the weight in PyTorch is stored in a different format for ConvTranspose1d? The weight is [in_channels, out_channels, kernel_size]. In ConvTranspose1d, there might be some internal transposition or dilation handling.
No, the weight is exactly [in_channels, out_channels, kernel_size].
OK, I think the issue might genuinely be that PyTorch/cuDNN computes this with a different reduction tree / algorithm, causing different rounding. Since the difference is 3.5e-4 and tolerance is 1e-4, I need to either:
1. Find a computation order that matches better
2. Use algorithms that naturally match cuDNN's approach
Let me try cublasSGEMM based approach. I'll do im2col in a CUDA kernel, then use cublas for the GEMM.
Actually, cublas has batched GEMM. Let me set it up.
For each batch n:
- x_col[n] has shape [out_length, in_channels * kernel_size]
- For each output position o and each (c_in, k):
x_col[n, o, c_in * K + k] = input[n, c_in, o - k*dilation] if valid else 0
Then: output[n] = x_col[n] @ w.reshape(in_channels * K, out_channels)
So we can do a batched GEMM:
C[n] = A[n] @ B
where A[n] is [out_length, in_channels*K], B is [in_channels*K, out_channels]
This is a batched GEMM with batch=32.
In JAX/pytorch, the equivalent would be:
w_flat = weight.reshape(in_channels*kernel_size, out_channels)
out = nn.functional.conv_transpose1d(...) # reference
For custom kernel:
1. Launch im2col kernel to compute A[n] for all n
2. Call cublasSgemmStridedBatched
cuBLAS strided batched GEMM has specific accumulation behavior that may match cuDNN.
Let me try this approach! It might also be faster because GEMM is accelerated by tensor cores.
Hmm, but will the im2col + GEMM match cuDNN? In many cases, cuDNN's conv_transpose IS implemented as im2col + GEMM, so this might match perfectly!
Let me implement this.
Actually, I can use cublasGemmStridedBatchedEx or cublasSgemmStridedBatched.
Let me write the code:
```cpp
torch::Tensor conv_transpose1d_cuda(...)
// Step 1: Create im2col tensor
// A: [batch_size, out_length, in_channels * kernel_size]
int patch_size = in_channels * kernel_size;
auto A = torch::empty({batch_size, out_length, patch_size}, input.options());
// Step 2: Launch im2col kernel
im2col_kernel<<<...>>>(...)
// Step 3: Reshape weight
// B: [in_channels * kernel_size, out_channels]
// C: [batch_size, out_length, out_channels]
// Step 4: cublas batched gemm
cublasHandle_t handle;
cublasCreate(&handle);
float alpha = 1.0f, beta = 0.0f;
int m = out_length;
int n = out_channels;
int k = patch_size;
long long int strideA = m * k; // out_length * patch_size
long long int strideC = m * n; // out_length * out_channels
cublasSgemmStridedBatched(handle, CUBLAS_OP_N, CUBLAS_OP_N,
m, n, k,
&alpha,
A.data_ptr<float>(), m,
strideA,
weight.data_ptr<float>(), k, // wait, weight is [in_channels, out_channels, kernel_size]
// We need B = [patch_size, out_channels], ldb = patch_size
&beta,
output.data_ptr<float>(), m,
strideC,
batch_size);
```
Wait, weight is [in_channels, out_channels, kernel_size]. We want B = [patch_size, out_channels] where patch_size = in_channels * kernel_size.
The mapping:
B[idx, c_out] = weight[c_in, c_out, k] where idx = c_in * K + k.
We need to either reshape weight or access appropriately. Since torch::Tensor::reshape creates a view with the same storage but different stride, we can do:
```cpp
auto weight_flat = weight.reshape({in_channels * kernel_size, out_channels});
```
Then B_ptr = weight_flat.data_ptr<float>(), ldb = patch_size.
Now for the im2col kernel:
```cpp
__global__ void im2col_kernel(
const float* input, float* A,
int batch_size, int in_channels, int in_length,
int out_length, int kernel_size, int dilation
) {
int n = blockIdx.z;
int o = blockIdx.y * blockDim.y + threadIdx.y;
int idx = blockIdx.x * blockDim.x + threadIdx.x;
if (n >= batch_size || o >= out_length || idx >= in_channels * kernel_size) return;
int c_in = idx / kernel_size;
int k = idx % kernel_size;
int in_pos = o - k * dilation;
float val = 0.0f;
if (in_pos >= 0 && in_pos < in_length) {
val = input[((n * in_channels) + c_in) * in_length + in_pos];
}
A[((n * out_length) + o) * patch_size + idx] = val;
}
```
Then call cublas.
NOW, the question is: will this match cuDNN's numerical output for conv_transpose?
In many cases, cuDNN implements conv_transpose as im2col + GEMM exactly like this! So there's a good chance it will match.
But even if not, cublas GEMM might still have similar but not identical accumulation order to cuDNN's optimized GEMM.
Also, for the tolerance of 1e-4, it's possible that it matches. Let me give it a shot!
But cublas might have issues with linking. I need to make sure to link against cublas. With load_inline, I might need to add extra_ldflags.
Actually, PyTorch is already linked with cublas. Let me see if I can include <cublas_v2.h> and call cublas functions.
Let me write the full kernel.
Wait, actually, do I need to manage cublas handles? The best practice is to get the cuBLAS handle from PyTorch's CUDA context if possible. But actually, I can just create and destroy a handle inside the function, or cache it using thread_local.
Actually, creating a cublas handle per call is expensive. I should cache it.
But with load_inline, the CUDA code runs in the extension. I can use thread_local to cache the handle.
Let me try!
Also, I need to add cublas includes and library flags.
Hmm, on second thought, cublas should be available by default in torch's CUDA environment. Let me just include <cublas_v2.h> and see if it links.
One more thing: `torch::Tensor::reshape` might not work directly in the C++ extension the way I use it. I can instead just remap the indices in the cublas call or pre-reshape in Python.
Actually, let me handle weight reshaping in Python before passing to the CUDA function.
Actually, looking at the Python -> C++ interface, I can just reshape the weight tensor in Python:
```python
weight_flat = weight.view(in_channels * kernel_size, out_channels)
```
Then pass the reshaped weight to the CUDA function with appropriate strides.
Or, the CUDA function can receive the original weight and handle the indexing.
Actually, the easiest is to pass the original weight and compute B strides carefully:
- B is stored as [in_channels, out_channels, kernel_size]. If I treat it as 2D [in_channels*kernel_size, out_channels], the row elements are contiguous (since out_channels is the fastest varying dimension, then kernel_size)?
Wait, let's check: weight shape = [in_channels, out_channels, kernel_size].
The strides are:
- stride[0] = out_channels * kernel_size
- stride[1] = kernel_size
- stride[2] = 1
If I view it as [in_channels * kernel_size, out_channels], the layout would be:
Element at [c_in * K + k, c_out] maps to weight[c_in, c_out, k].
Is this contiguous in the new view? For a fixed row (c_in*K+k), the elements are at weight[c_in, :, k], which are separated by stride[1] = kernel_size. So in the 2D view, columns are separated by kernel_size, not 1. That means it's NOT row-major with contiguous rows.
For cublas, I need:
B to be column-major (since cublas assumes column-major by default) or I can use transposes.
Hmm, this is getting complicated. Let me just copy/reshape the weight in Python:
```python
weight_t = weight.permute(2, 0, 1).contiguous().view(kernel_size * in_channels, out_channels)
```
Wait, I want B[c_in*K+k, c_out] = weight[c_in, c_out, k].
If I permute to [kernel_size, in_channels, out_channels] and then view as [kernel_size*in_channels, out_channels], I get:
index = k * in_channels * out_channels + c_in * out_channels + c_out
= (k * in_channels + c_in) * out_channels + c_out
So B[row, c_out] where row = k*in_channels + c_in. That's row-major with contiguous rows!
```python
weight_t = weight.permute(2, 0, 1).contiguous().view(-1, out_channels)
```
Then B_ptr with ldb = out_channels (for cublas column-major, the leading dimension is the distance between consecutive columns, which is the number of rows). Actually in cublas:
For column-major matrix B with shape [k, n] (k rows, n columns):
- ldb = k (leading dimension, distance between consecutive columns)
Wait, for cublas, if B is [k, n] in column-major:
- Element (i, j) is at B[i + j * ldb]
- ldb >= k
With row-major memory layout where B[row, col] is contiguous in row:
B[row, col] is at B[row * out_channels + col]
In cublas column-major terms:
B[i, j] in column-major = B_row_major[j, i] if we transpose.
Actually, for cublasSgemm:
C = alpha * op(A) * op(B) + beta * C
Where matrices are in column-major. If A is row-major [m, k] and we want C = A * B where B is [k, n] row-major:
- We can set op(A) = A^T (so A is treated as [k, m] column-major, which corresponds to [m, k] row-major)
- op(B) = B^T (so B is treated as [n, k] column-major, which corresponds to [k, n] row-major)
- Then C = A^T * B^T, but we want C = A * B, so C = (B * A)^T
Hmm, this gets confusing. Let me use cublas with explicit transposes.
If A is [m, k] row-major, B is [k, n] row-major, and C should be [m, n] row-major:
A_col = A^T would be [k, m] column-major
B_col = B^T would be [n, k] column-major
C = A * B
C^T = B^T * A^T = B_col * A_col
So: C_col = B_col * A_col, where:
- B_col is [n, k], op(B) = B (no transpose), ldb = n
- A_col is [k, m], op(A) = A (no transpose), lda = k
- C_col is [n, m], ldc = n
Wait, cublas uses column-major, so:
C_col[j, i] = C_row[i, j]
B_col[j, l] = B_row[l, j]
Actually, if A_row has shape [m, k]:
A_col = A_row^T has shape [k, m]
For cublas, we can use CUBLAS_OP_T to treat A_row as [m, k] column-major which is A_row^T = [k, m].
cublasSgemm(opA, opB, m, n, k, ...)
If opA = CUBLAS_OP_T, then A is n-by-k in column-major, which means A^T is k-by-n. So A in row-major is n-by-k.
Wait, let me be more careful:
cublasSgemm(handle, transa, transb, m, n, k, alpha, A, lda, B, ldb, beta, C, ldc)
This computes: C = alpha * op(A) * op(B) + beta * C
where C is m×n, op(A) is m×k, op(B) is k×n.
For row-major A of size [m, k], if we use transa = CUBLAS_OP_T:
op(A) = A^T which has size [k, m]. But cublas expects op(A) to be m×k, so this doesn't work directly.
Actually, if A_row is [m, k] row-major, then A_col = A_row^T is [k, m] column-major.
To compute C_row = A_row * B_row where C is [m, n]:
C_col = C_row^T = (A_row * B_row)^T = B_row^T * A_row^T = B_col * A_col
So in cublas terms:
C = B_col * A_col, where C is n×m, B_col is n×k, A_col is k×m.
cublasSgemm(handle, CUBLAS_OP_N, CUBLAS_OP_N, n, m, k, alpha, B_col, n, A_col, k, beta, C_col, n)
And C_col has shape [n, m] in column-major, which means C_row = C_col^T has shape [m, n] row-major.
So the call is:
- m_cublas = n (output cols)
- n_cublas = m (output rows)
- k_cublas = k
- A_ptr = B_col (which is B_row^T)
- lda = n (for B_col which is n×k)
- B_ptr = A_col (which is A_row^T)
- ldb = k (for A_col which is k×m)
- C_ptr = C_col (which is C_row^T, n×m)
- ldc = n
Let me verify shapes:
B_col = B_row^T: if B_row is [k, n], B_col is [n, k]
A_col = A_row^T: if A_row is [m, k], A_col is [k, m]
C_col: [n, m]
B_col * A_col: [n, k] * [k, m] = [n, m]. Correct!
So if I have:
- A_row = x_col with shape [batch, out_length, patch_size] = [batch, m, k] where m = out_length, k = patch_size
- B_row = weight_flat with shape [patch_size, out_channels] = [k, n] where n = out_channels
- C_row = output with shape [batch, out_length, out_channels] = [batch, m, n]
Then for each batch:
A_col = x_col[b]^T: [k, m]
B_col = weight_flat^T: [n, k]
C_col = B_col * A_col: [n, m] = [n, k] * [k, m]
which equals (A_row * B_row)^T: [n, m] = ([m, k] * [k, n])^T
So cublas call for each batch:
cublasSgemm(handle, CUBLAS_OP_N, CUBLAS_OP_N, n, m, k, alpha, B_ptr, n, A_ptr, k, beta, C_ptr, n)
Where:
- n = out_channels
- m = out_length
- k = patch_size
- B_ptr = weight_flat^T (reshaped to [n, k] column-major, i.e., [k, n] row-major, but with n as leading dim in column-major)
Wait, B_col = [n, k] in column-major. The element (i, j) in B_col is B_col[i + j * n].
If B_row is [k, n] row-major, B_row[j, i] = B_row[j * n + i].
B_col[i, j] = B_row[j, i], so B_col[i + j * n] = B_row[j * n + i].
So if B_row is contiguous row-major [k, n], then B_col is contiguous column-major [n, k] with ldb = n.
Similarly, A_col = [k, m] in column-major. If A_row is [m, k] row-major and contiguous, then A_col[i, j] = A_row[j, i], so A_col[i + j * k] = A_row[j * k + i], and lda = k.
For C_col = [n, m] in column-major. C_col[i, j] = C_row[j, i] where C_row is [m, n].
For C_row contiguous, C_row[j, i] = C_row[j * n + i], so C_col[i + j * n] = C_row[j * n + i], ldc = n.
So the cublas call is correct!
For strided batched:
A_ptr = x_col.data_ptr() + b * m * k (out_length * patch_size)
B_ptr = weight_flat.data_ptr() (same for all batches)
C_ptr = output.data_ptr() + b * m * n (out_length * out_channels)
cublasSgemmStridedBatched:
- A is the patch matrix for each batch
- B is the weight matrix (same for all batches, strideB = 0)
- C is output for each batch
Let me write this:
```cpp
#include <cublas_v2.h>
// ... im2col kernel
torch::Tensor conv_transpose1d_cuda(...) {
int patch_size = in_channels * kernel_size;
// Prepare weight: [kernel_size, in_channels, out_channels] -> [patch_size, out_channels]
// Actually in Python we'll send it properly reshaped.
auto A = torch::empty({batch_size, out_length, patch_size}, input.options());
// im2col
// ...
auto output = torch::empty({batch_size, out_length, out_channels}, input.options());
// cublas
cublasHandle_t handle = at::cuda::getCurrentCUDABlasHandle();
float alpha = 1.0f, beta = 0.0f;
cublasSgemmStridedBatched(handle,
CUBLAS_OP_N, CUBLAS_OP_N,
out_channels, out_length, patch_size,
&alpha,
weight_ptr, out_channels, 0, // B: [n, k], strideB = 0
A.data_ptr<float>(), patch_size, out_length * patch_size, // A: [k, m], strideA = m*k
&beta,
output.data_ptr<float>(), out_channels, out_length * out_channels, // C: [n, m], strideC = m*n
batch_size
);
return output.view({batch_size, out_channels, out_length});
}
```
Wait, I need to check if PyTorch exposes `at::cuda::getCurrentCUDABlasHandle()`. Yes, it should be available in the ATen CUDA headers.
However, I need to include the right headers.
Actually, looking at the error, our direct implementation is getting 3.5e-4 max difference. Maybe I'm overthinking this and should try simpler tweaks.
Let me try one more thing: use the reference PyTorch conv_transpose1d but with `torch.backends.cudnn.allow_tf32 = False`. If the reference test also disables tf32, then our fp32 kernel should match. But I can't change the test.
Actually, maybe I should check if the model gets exactly the same weight values. In my init, I use `self.conv_ref.weight` which is the same as `nn.ConvTranspose1d(...).weight`. But PyTorch initializes weights with some random values. Since `get_inputs` fixes the seed by using `torch.rand`, the model weights might use the default PyTorch initialization which depends on the global seed.
Wait, the correctness test probably:
1. Creates Model and ModelNew
2. Copies weights from Model to ModelNew (or vice versa)
3. Runs both
So the weights should be identical. Let me check if my ModelNew properly stores the weight.
In my ModelNew:
```python
self.conv_ref = nn.ConvTranspose1d(...)
self.weight = self.conv_ref.weight
self.bias = self.conv_ref.bias
```
But wait, `self.weight` is just a reference to the parameter. In PyTorch, parameters are registered in the model. Since `self.conv_ref` is also a submodule, its parameters are registered. But `self.weight` also points to the same tensor. That should be fine as long as the weights don't get modified during testing.
Actually, if the test does `model_new.load_state_dict(model.state_dict())`, then `model_new.conv_ref.weight` gets updated, but `model_new.weight` still points to the original tensor because `self.weight = self.conv_ref.weight` only copies the reference at init time!
AH HA! This is the bug!
When `ModelNew.__init__` is called:
1. `self.conv_ref = nn.ConvTranspose1d(...)` creates a new ConvTranspose1d with random weights
2. `self.weight = self.conv_ref.weight` stores a reference to those random weights
3. Later, if the test harness copies weights from the reference model to ModelNew, it would update `self.conv_ref`'s parameters, but `self.weight` would still point to the OLD random weights!
Wait, let me check how weight copying works. The test probably does:
```python
model = Model(...)
model_new = ModelNew(...)
model_new.load_state_dict(model.state_dict())
```
Since `state_dict()` includes keys like `'conv_ref.weight'`, `load_state_dict` would update `model_new.conv_ref.weight`. But `model_new.weight` was assigned as a direct reference to the Parameter object, not a copy of the tensor data. In PyTorch, Parameters are mutable objects. `load_state_dict` modifies the data of the Parameter:
```python
param.data.copy_(state_dict[key])
```
Since `model_new.weight` points to the SAME Parameter object as `model_new.conv_ref.weight`, modifying `model_new.conv_ref.weight.data` also modifies `model_new.weight.data`!
Actually, in PyTorch `nn.Module.load_state_dict` calls:
```python
param.copy_(param_from_state_dict)
```
This modifies the tensor in-place. Since `self.weight` and `self.conv_ref.weight` are the same Parameter object, both see the update.
So that shouldn't be the issue.
But wait - is `self.weight = self.conv_ref.weight` copying the Python reference? Yes. If `load_state_dict` replaces the parameter (which it doesn't - it modifies in-place), then `self.weight` might point to the old one. But `load_state_dict` modifies in-place, so it should be fine.
Actually, let me double-check: in PyTorch, `module.weight` is just a Python attribute pointing to the Parameter. When `load_state_dict` runs, it calls `param.copy_(src)` on the existing Parameter. It does NOT replace the Parameter object. So `self.weight` remains pointing to the same (now updated) Parameter.
But wait, actually `load_state_dict` might use `_load_from_state_dict` which has some logic. Let me check... Actually, I think in newer PyTorch versions, `load_state_dict` CAN replace parameters if shapes differ, but for same shapes it uses `copy_`.
For safety, let me change my ModelNew to access the weight through `self.conv_ref.weight` in the forward pass instead of caching it. That way, even if something weird happens with parameter replacement, we'll use the correct weight.
Let me modify the forward to use `self.conv_ref.weight` directly, and `self.conv_ref.bias` if needed.
Also, I should check if I need to pass the bias at all. For `bias=False`, `self.conv_ref.bias` is None, so I need to handle that.
Let me write a corrected version that accesses weights through conv_ref directly.
Actually, wait. In all my previous tests, I pass `self.weight` and `self.bias` to the CUDA function, which are set during init. If the test updates `self.conv_ref.weight` in place, then `self.weight` should also be updated since they're the same object. So this shouldn't cause a numerical mismatch.
Let me think about what else could cause the 3.5e-4 difference.
OK, actually, what if the difference IS just floating point precision, and I need to match it by changing accumulation order. Let me try one more direct kernel with a very specific loop ordering, and also try accumulating in chunks.
Actually, let me try accumulating in the order: first iterate over k (kernel), then c_in. Since each k contributes to a specific set of input positions, and different k's don't overlap in the memory access pattern (for a given o).
Actually no, for a fixed o, different k values access different input positions.
Let me just try the cublas approach and see if it passes correctness! It might match because cublas and cudnn likely share similar implementations for GEMM-based convolutions.
Let me write a cublas-based kernel.
Wait, do I actually need a custom im2col kernel? I can write the im2col part in the CUDA kernel and then call cublas. Or I can write the entire thing as a single CUDA kernel that just loads data appropriately.
For cublas, I need:
1. `cublas_v2.h` include
2. Link against cublas
With `load_inline`, I might need `extra_ldflags=['-lcublas']`.
Let me also check if the PyTorch ATen context gives access to the cublas handle.
`at::cuda::getCurrentCUDABlasHandle()` is available. I need to include `<ATen/cuda/CUDABlas.h>` or similar.
Actually, let me check. In PyTorch C++ extensions, we can include:
```cpp
#include <ATen/cuda/CUDAContext.h>
```
and call `at::cuda::getCurrentCUDABlasHandle()`.
Let me draft the kernel:
```cpp
#include <torch/extension.h>
#include <cuda_runtime.h>
#include <cublas_v2.h>
#include <ATen/cuda/CUDAContext.h>
__global__ void im2col_kernel(
const float* __restrict__ input,
float* __restrict__ A,
int batch_size, int in_channels, int in_length,
int out_length, int kernel_size, int dilation, int patch_size
) {
int n = blockIdx.z;
int o = blockIdx.y * blockDim.y + threadIdx.y;
int idx = blockIdx.x * blockDim.x + threadIdx.x;
if (n >= batch_size || o >= out_length || idx >= patch_size) return;
int c_in = idx / kernel_size;
int k = idx % kernel_size;
int in_pos = o - k * dilation;
float val = 0.0f;
if (in_pos >= 0 && in_pos < in_length) {
val = input[((n * in_channels) + c_in) * in_length + in_pos];
}
A[((n * out_length) + o) * patch_size + idx] = val;
}
__global__ void add_bias_kernel(
float* output,
const float* bias,
int batch_size, int out_channels, int out_length
) {
int idx = blockIdx.x * blockDim.x + threadIdx.x;
int total = batch_size * out_channels * out_length;
if (idx >= total) return;
int n = idx / (out_channels * out_length);
int rem = idx % (out_channels * out_length);
int c_out = rem / out_length;
int o = rem % out_length;
output[idx] += bias[c_out];
}
torch::Tensor conv_transpose1d_cuda(
torch::Tensor input,
torch::Tensor weight,
torch::Tensor bias,
int use_bias,
int stride, int padding, int dilation
) {
int batch_size = input.size(0);
int in_channels = input.size(1);
int in_length = input.size(2);
int out_channels = weight.size(1);
int kernel_size = weight.size(2);
int out_length = (in_length - 1) * stride - 2 * padding + dilation * (kernel_size - 1) + 1;
int patch_size = in_channels * kernel_size;
auto A = torch::empty({batch_size, out_length, patch_size}, input.options());
auto output = torch::empty({batch_size, out_length, out_channels}, input.options());
// im2col
dim3 block_im2col(16, 16);
dim3 grid_im2col(
(patch_size + 15) / 16,
(out_length + 15) / 16,
batch_size
);
im2col_kernel<<<grid_im2col, block_im2col>>>(
input.data_ptr<float>(), A.data_ptr<float>(),
batch_size, in_channels, in_length,
out_length, kernel_size, dilation, patch_size
);
// cublas GEMM
cublasHandle_t handle = at::cuda::getCurrentCUDABlasHandle();
// Reshape weight to [patch_size, out_channels] row-major
// In Python, weight.permute(2, 0, 1).contiguous().view(patch_size, out_channels)
// For now, assume weight is already in the right format.
float alpha = 1.0f, beta = 0.0f;
// C = A * B where A is [batch, m, k], B is [k, n]
// Using strided batched: C[b] = A[b] * B
// A[b] is [out_length, patch_size] row-major -> [m, k]
// B is [patch_size, out_channels] row-major -> [k, n]
// C[b] is [out_length, out_channels] row-major -> [m, n]
// cublas is column-major. We want C_row = A_row * B_row
// C_col = C_row^T = B_row^T * A_row^T = B_col * A_col
// Where B_col = [n, k], A_col = [k, m]
// So we call: cublasSgemmStridedBatched(..., n, m, k, ...)
// with A_ptr = B_col, B_ptr = A_col
cublasSgemmStridedBatched(handle,
CUBLAS_OP_N, CUBLAS_OP_N,
out_channels, out_length, patch_size,
&alpha,
weight.data_ptr<float>(), out_channels, 0,
A.data_ptr<float>(), patch_size, out_length * patch_size,
&beta,
output.data_ptr<float>(), out_channels, out_length * out_channels,
batch_size
);
if (use_bias) {
int total = batch_size * out_length * out_channels;
int threads = 256;
add_bias_kernel<<<(total + threads - 1) / threads, threads>>>(
output.data_ptr<float>(), bias.data_ptr<float>(),
batch_size, out_channels, out_length
);
}
return output.reshape({batch_size, out_channels, out_length});
}
```
Wait, for the weight, I need to make sure it's in the right format. The incoming weight is [in_channels, out_channels, kernel_size]. For cublas, I want B_row = [patch_size, out_channels] where B[idx, c_out] = weight[c_in, c_out, k] with idx = c_in * K + k.
weight[c_in, c_out, k] is stored at index: c_in * (out_channels * kernel_size) + c_out * kernel_size + k
For B_row[idx, c_out] with idx = c_in * K + k:
B_row[idx, c_out] should equal weight[c_in, c_out, k].
The storage of B_row at B_row[idx * out_channels + c_out] = weight[c_in * c_out_stride + c_out * k_stride + k].
But weight storage: stride[0] = out_channels*kernel_size, stride[1] = kernel_size, stride[2] = 1.
weight[c_in, c_out, k] is at offset: c_in * out_channels * kernel_size + c_out * kernel_size + k.
For B_row with out_channels columns:
B_row[idx, c_out] at offset: idx * out_channels + c_out.
But idx = c_in * K + k, so:
offset = (c_in * K + k) * out_channels + c_out = c_in * K * out_channels + k * out_channels + c_out.
While weight offset = c_in * out_channels * K + c_out * K + k.
These are different! So the original weight tensor doesn't have the right layout.
In Python I need to permute and reshape:
```python
weight_t = weight.permute(2, 0, 1).contiguous().view(-1, out_channels)
```
With permute(2, 0, 1), weight is [kernel_size, in_channels, out_channels].
weight_t[k, c_in, c_out] = original[c_in, c_out, k].
After contiguous() and view(-1, out_channels):
weight_t_flat[idx, c_out] where idx = k * in_channels + c_in = weight[k, c_in, c_out].
But I want idx = c_in * K + k, not k * in_channels + c_in.
So I should permute differently:
```python
weight_t = weight.permute(0, 2, 1).contiguous().view(-1, out_channels)
```
Wait, permute(0, 2, 1) gives [in_channels, kernel_size, out_channels].
Then view(-1, out_channels) gives idx = c_in * K + k.
And weight_t[idx, c_out] = weight[c_in, c_out, k].
But the storage after permute(0, 2, 1).contiguous():
- Shape: [in_channels, kernel_size, out_channels]
- Stride: [kernel_size * out_channels, out_channels, 1]
- Element at [c_in, k, c_out] is at offset c_in * kernel_size * out_channels + k * out_channels + c_out.
If I view this as [in_channels*kernel_size, out_channels]:
- Element at [idx, c_out] with idx = c_in * K + k:
offset = idx * out_channels + c_out = (c_in * K + k) * out_channels + c_out.
This matches the storage after permute(0, 2, 1).contiguous(). Perfect!
So in Python:
```python
weight_t = weight.permute(0, 2, 1).contiguous().view(-1, out_channels)
```
Actually wait, permute(0, 2, 1):
Original: [c_in, c_out, k]
Permute dims: 0->0, 1->2, 2->1, which gives [c_in, k, c_out].
Then view(-1, out_channels): flatten c_in and k dimensions.
Yes! weight_t[idx, c_out] = weight[c_in, c_out, k] where idx = c_in * K + k. And it's contiguous in this layout.
Great! Now for cublas, B_row is [patch_size, out_channels] = [k, n] in my earlier notation, stored row-major.
For the cublas call: C = B_col * A_col, where:
- B_col = [n, k] column-major = B_row^T
- Since B_row is row-major [k, n], B_col[i, j] = B_row[j, i], and B_col is stored with ldb = n (distance between columns). Since B_row rows are contiguous with length n, B_col IS column-major with ldb = n.
- A_col = [k, m] column-major = A_row^T
- A_row is [m, k] row-major (out_length, patch_size). A_col[i, j] = A_row[j, i]. A_row rows are contiguous with length k, so A_col is column-major with lda = k.
- C_col = [n, m] column-major = C_row^T
- C_row is [m, n] row-major. C_col[i, j] = C_row[j, i]. If C_row rows are contiguous with length n, C_col is column-major with ldc = n.
So the cublas call:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_N, CUBLAS_OP_N,
n, m, k, // n=out_channels, m=out_length, k=patch_size
&alpha,
weight_t.data_ptr<float>(), n, 0, // B_col: [n, k], ldb=n, strideB=0
A.data_ptr<float>(), k, m * k, // A_col: [k, m], lda=k, strideA=m*k
&beta,
output.data_ptr<float>(), n, m * n, // C_col: [n, m], ldc=n, strideC=m*n
batch_size
);
```
Yes, this is correct!
Now, I also need to handle bias properly. After the GEMM, output has shape [batch_size, out_length, out_channels]. I need to add bias to the out_channels dimension.
Then reshape to [batch_size, out_channels, out_length] for the return.
Actually, in the PyTorch reference, the output is [batch_size, out_channels, out_length]. My intermediate output is [batch_size, out_length, out_channels]. So I need to either:
1. Permute after GEMM
2. Do the GEMM in a way that output is already [batch_size, out_channels, out_length]
For option 2, I can use cublas with different transposes:
If I compute C = B^T * A^T using other ops, I can get the right layout directly. But that might complicate things.
Let me just compute in [batch, out_length, out_channels], add bias, then permute to [batch, out_channels, out_length].
For bias: I need to add bias[c_out] to every [..., c_out] position.
```cpp
output[n, o, c_out] += bias[c_out]
```
Now, let me write the full code.
Also, actually, I should be careful about the tensor `A`. It requires additional memory of size `batch_size * out_length * patch_size * sizeof(float)`.
With batch=32, out_length=131084, patch_size=160:
A size = 32 * 131084 * 160 * 4 bytes = 2.68 GB.
That's a lot of memory! The reference might not use that much memory. While this might work on H100 with 80GB, it might be slower due to the extra memory allocation and writes.
For the direct kernel, we read input and weight directly, accumulating on the fly. That's more memory-efficient and likely faster if the computation is memory-bound.
The im2col approach trades compute for simpler GEMM, but here the kernel is so small that the overhead of writing A might not be worth it.
Actually, 2.68 GB is significant. The total input is 32*32*131072*4 = 536 MB. Output is 32*64*131084*4 = 1.07 GB. So A is 2.68GB, total ~4.3GB. On H100 80GB that's fine, but it might hurt performance.
For this specific problem, a direct kernel might actually be faster because it avoids the extra memory traffic. However, the GEMM approach might use tensor cores.
But the main issue is correctness. If the GEMM approach matches better, great. If not, it's not worth it.
Let me reconsider the direct approach. Is there any way to get the reference to match within 1e-4?
One thing I could try: use the exact same accumulation order that a naive matrix multiplication would use. Let me think about how cudnn might accumulate.
For a conv_transpose with in=32, out=64, k=5, the reference might call a conv2d/conv1d kernel. Cudnn's conv kernels often accumulate in groups and might use specific patterns.
Actually, if cudnn uses Winograd or FFT, the numerical properties would be very different. But for such a small kernel and large feature map, im2col+GEMM or direct convolution is more likely.
Let me try the cublas approach anyway and see the correctness. If it matches, we can evaluate performance.
Actually, maybe there's a much simpler solution. What if I just use `torch.nn.functional.conv_transpose1d` in the forward method? But the task requires replacing it with a custom CUDA kernel. So that's not allowed.
OK, let me go with the direct kernel but try to use a slightly different loop ordering to match potential cudnn behavior. Specifically, let me accumulate in a blocked manner: for each block of output channels, process all input channels and kernels.
Actually, I think I should try `__half` or `float` computations and see. Let me try one more direct kernel that unrolls the inner loop and uses the exact same memory access pattern as a GEMM.
Wait, I just realized something. The previous kernels all used the same formulation that I mathematically verified is correct. The only issue is the precision/rounding difference of 3.5e-4.
For fp32 with tolerance 1e-4, this is a tough requirement. The only way to guarantee matching is to use the exact same implementation as the reference, or an implementation that's mathematically equivalent such that rounding differences are below 1e-4.
The error of 3.5e-4 is actually quite large for a single fp32 rounding error (which is ~1e-7 relative). With 160 operations (32*5), independent rounding errors add up to about sqrt(160) * 1e-7 * 40 ≈ 5e-5 in quadrature. A worst-case aligned error could be larger, around 160 * 1e-7 * 40 ≈ 6.4e-4.
So 3.5e-4 is within the realm of possible worst-case accumulation differences for fp32.
If I can't find a better accumulation order, maybe I need to reduce the error variance by using a more structured approach.
Since the GEMM approach (cuBLAS) might have similar accumulation patterns to cuDNN, and the error might be within tolerance, it's worth trying.
Let me give it a shot. But the 2.68GB memory for A is large.
Actually, I don't need to store the entire im2col tensor at once! I can process in tiles along the output length dimension.
For each tile of output positions (e.g., 128 positions), create the im2col for that tile, do GEMM for all batches, then move to the next tile. This way, the intermediate memory is much smaller.
Actually, with strided batched GEMM, each "batch" is independent. I can process the output length dimension in chunks and do a batched GEMM for each chunk, storing directly into the output.
But cublasSgemmStridedBatched requires contiguous batching over the batch dimension, not the output length. If I chunk by output length, each chunk is still a batched GEMM for all batch samples.
Let me think: for each chunk [o_start:o_end]:
- A_chunk shape: [batch_size, chunk_size, patch_size]
- Output shape: [batch_size, chunk_size, out_channels]
So the cublas call parameters change: m = chunk_size, n = out_channels, k = patch_size.
strideA = chunk_size * patch_size
strideC = chunk_size * out_channels
This works! And A_chunk only needs batch_size * chunk_size * patch_size floats.
With chunk_size = 128: 32 * 128 * 160 * 4 = 2.6 MB. Much better!
Let me implement this tile-based approach.
Actually, this is getting complex. Let me first try a single-tile approach without the huge A tensor, by using shared memory to do the im2col + manual matmul.
For a tile of output positions (e.g., 32 positions), load the corresponding input and weights into shared memory, then compute the output for these positions.
This is basically the tiled direct approach I tried earlier, but with more careful attention to numerical properties.
Actually, let me step back and think: is there any possibility that my understanding of the ConvTranspose1d formula is wrong?
Let me verify with the PyTorch source code or CUDNN documentation.
PyTorch ConvTranspose1d calls cudnn's `cudnnConvolutionBackwardData` with appropriate parameters.
The formula for conv transpose with stride=1, padding=0 is actually just the transpose of the corresponding conv operation. For the corresponding conv:
- kernel_size = 5, dilation = 3
- Input to conv would be padded appropriately.
But for the transpose operation:
If the conv computes output_size = floor((input_size + 2*padding - dilation*(kernel_size-1) - 1)/stride) + 1
Then the transpose computes output_size = (input_size - 1)*stride - 2*padding + dilation*(kernel_size-1) + 1
For a value y[o] in the transpose output, it's the dot product of the transposed weight with the input values that would have contributed to it in the forward pass.
Mathematically, y[o] = sum_{c_in} sum_{k=0}^{K-1} x[c_in, o - k*dilation] * w[c_in, c_out, k].
This matches our formula. So the algorithm is definitely correct.
OK, I think the difference is solely from floating point accumulation. Let me try one more thing: write the kernel using atomicAdd. If multiple threads compute partial sums and accumulate atomically, the resulting order might match cuDNN. But that's unlikely to be deterministic or fast.
Wait, what if PyTorch uses `torch.backends.cudnn.deterministic = True` or something? No, that just makes convolutions deterministic, not necessarily matching our ordering.
Alright, let me try the cublas approach but with a very small intermediate buffer.
Actually, let me reconsider: maybe the reference run itself computed with some lower precision mode, and our more accurate computation diverges. What if I intentionally use lower precision to match? For example, what if I cast intermediates to fp16 and back?
That seems dangerous and unlikely to match well.
Actually, wait. I just realized I didn't properly test if there are boundary errors. Let me verify my formula with a tiny example by actually computing mentally.
For in_length=5, kernel_size=2, dilation=1, stride=1, padding=0:
out_length = (5-1)*1 + 1*(2-1) + 1 = 5
For each output position o:
o=0: k=0 -> in_pos=0 (valid), k=1 -> in_pos=-1 (invalid) -> sum = x[0]*w[0]
o=1: k=0 -> in_pos=1, k=1 -> in_pos=0 -> sum = x[1]*w[0] + x[0]*w[1]
o=2: k=0 -> in_pos=2, k=1 -> in_pos=1 -> sum = x[2]*w[0] + x[1]*w[1]
o=3: k=0 -> in_pos=3, k=1 -> in_pos=2 -> sum = x[3]*w[0] + x[2]*w[1]
o=4: k=0 -> in_pos=4, k=1 -> in_pos=3 -> sum = x[4]*w[0] + x[3]*w[1]
This is exactly cross-correlation with the original (non-flipped) kernel! And for transposed conv with stride=1, it should indeed be equivalent to dilated cross-correlation with the original kernel.
PyTorch's cudnn conv_transpose should produce the same mathematical result. So our formula is correct.
I think the issue is purely about accumulation differences. Let me try to write a kernel that does the accumulation in the exact order that GEMM would do it, by restructuring the computation as matrix multiplications using shared memory.
Or, I'm overthinking this. Let me just try the cublas approach and see if it passes.
Actually, let me first try a much simpler thing: can the difference be because of the thread-level scheduling causing different warp-level reduction orders?
In CUDA, within a single thread, the computation order is deterministic. So if one thread computes one output element, the accumulation order is fixed by the loops.
In cuDNN, multiple threads might cooperate to compute one output element, and their partial sums are reduced in a specific tree-like order.
What if I make each output element computed by ALL threads in a warp using warp-level reductions? That would change the accumulation order.
Actually, for a matrix multiplication, the standard approach is to have each thread compute one output element. For convolution, cuDNN might use the same approach.
But what if cuDNN uses multiple threads per output element (e.g., one thread per input channel, then reduce)?
Let me try a kernel where I compute partial sums for each c_in in parallel and then reduce:
```cpp
// Each warp computes one output element (one c_out, one o)
// 32 threads in warp each process a subset of c_in channels
// Then warp-level reduce
int c_in_per_thread = (in_channels + 31) / 32;
for (int i = 0; i < c_in_per_thread; i++) {
int c_in = threadIdx.x * c_in_per_thread + i;
if (c_in < in_channels) {
for (int k = 0; k < kernel_size; k++) {
int in_pos = o - k * dilation;
if (in_pos >= 0 && in_pos < in_length) {
partial += input[...] * weight[...];
}
}
}
}
// warp reduce
```
This might produce different rounding because the reduction tree adds partial sums in log2(32) steps.
But warp-level reduction of 32 partial sums (each already having 5 terms) would have a different error characteristic.
Actually, warp-level reduction uses __shfl_down_sync and the exact tree order depends on the implementation. But it could easily differ from cuDNN.
I think the best approach might be to try the cublas method. Let me go with a simplified version first.
Hmm, but the cublas method with the huge memory is a concern for both performance and correctness (since it might OOM for some configs). Let me try a chunk-based approach.
Actually, maybe cublas will match because cuDNN itself uses cublas GEMM for this case. And with the same GEMM algorithm, we should get the same numerical result (or very close).
Let me write a compact version:
```cpp
#include <torch/extension.h>
#include <cuda_runtime.h>
// ... direct kernel but with double accumulation and then intentionally cast
// with a specific rounding mode?
// Actually, let me just try the direct kernel again but with cuBLAS.
```
Actually, I just had another thought. What if the issue is that I'm not using `__restrict__` correctly? Or what if there's some kind of implicit synchronization issue?
No, the difference is very uniform (same max diff across trials) which rules out race conditions.
OK, I'll write the cublas-based kernel. Let me be very careful about tensor shapes and layouts.
First, let me figure out the weight layout in Python:
```python
# weight shape: [in_channels, out_channels, kernel_size]
# For im2col GEMM, we want weight matrix B where:
# B[idx, c_out] = weight[c_in, c_out, k] with idx = c_in * K + k
# If I do weight.permute(0, 2, 1), I get [in_channels, kernel_size, out_channels]
# Then view(-1, out_channels) gives [in_channels*kernel_size, out_channels]
# And B[idx, c_out] = weight_permuted[idx // K, idx % K, c_out]
# = weight[idx // K, c_out, idx % K]
# Which IS what we want!
weight_t = weight.permute(0, 2, 1).contiguous().view(-1, out_channels)
```
Wait, let me verify:
weight_permuted = weight.permute(0, 2, 1)
Shape: [in_channels, kernel_size, out_channels]
weight_permuted[c_in, k, c_out] = weight[c_in, c_out, k]
view(-1, out_channels):
idx = c_in * kernel_size + k
weight_flat[idx, c_out] = weight_permuted[c_in, k, c_out] = weight[c_in, c_out, k]
Yes! This is perfect.
Now for the cublas call in the CUDA extension:
A = im2col tensor, shape [batch, out_length, patch_size], row-major
B = weight_flat, shape [patch_size, out_channels], row-major
C = output, shape [batch, out_length, out_channels], row-major
We want C[b] = A[b] * B.
For cublas column-major, C_col = B_col * A_col where:
- B_col = B^T = [out_channels, patch_size]
- A_col = A^T = [patch_size, out_length]
Wait, earlier I said C = B_col * A_col where C is [n, m].
C_col[j, i] = C_row[i, j].
C_row[i, j] = sum_k A_row[i, k] * B_row[k, j]
C_col[j, i] = sum_k A_row[i, k] * B_row[k, j]
B_col[j, k] = B_row[k, j]
A_col[k, i] = A_row[i, k]
So C_col[j, i] = sum_k B_col[j, k] * A_col[k, i]
Which means C_col = B_col * A_col.
In cublas:
C of size [n, m] = op(B) * op(A)
where op(B) is n×k and op(A) is k×m.
B_col is [n, k] column-major. If op(B) = B_col (no transpose), then B_ptr points to B_col with ldb = n.
A_col is [k, m] column-major. If op(A) = A_col (no transpose), then A_ptr points to A_col with lda = k.
C_col is [n, m] column-major. C_ptr with ldc = n.
So the call is exactly what I wrote before:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_N, CUBLAS_OP_N,
out_channels, out_length, patch_size,
&alpha,
B.data_ptr<float>(), out_channels, 0,
A.data_ptr<float>(), patch_size, out_length * patch_size,
&beta,
C.data_ptr<float>(), out_channels, out_length * out_channels,
batch_size
);
```
Wait, I need to double-check the argument order. In cublasSgemmStridedBatched:
```cpp
cublasStatus_t cublasSgemmStridedBatched(cublasHandle_t handle,
cublasOperation_t transa, cublasOperation_t transb,
int m, int n, int k,
const float *alpha,
const float *A, int lda, long long int strideA,
const float *B, int ldb, long long int strideB,
const float *beta,
float *C, int ldc, long long int strideC,
int batchCount)
```
Wait! The first matrix is A, second is B. The formula is C = alpha * op(A) * op(B) + beta * C.
So op(A) is m×k, op(B) is k×n, C is m×n.
In my case, I want C_col = B_col * A_col.
So op(A) = B_col (which is n×k), op(B) = A_col (which is k×m).
But cublas requires op(A) to be m×k and op(B) to be k×n. Here C_col is n×m.
So:
m = n (output channels = 64)
n = m (output length = 131084)
k = patch_size (160)
op(A) = B_col = [n, k] = [64, 160], so transa = CUBLAS_OP_N.
op(B) = A_col = [k, m] = [160, 131084], so transb = CUBLAS_OP_N.
A_ptr = B_col data = weight_flat data
lda = 64 (number of rows in B_col)
strideA = 0 (same weight for all batches)
B_ptr = A_col data = im2col data
ldb = 160 (number of rows in A_col)
strideB = out_length * patch_size = 131084 * 160
C_ptr = C_col data = output data
ldc = 64 (number of rows in C_col)
strideC = out_length * out_channels = 131084 * 64
batchCount = batch_size = 32
So:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_N, CUBLAS_OP_N,
out_channels, out_length, patch_size,
&alpha,
weight_flat.data_ptr<float>(), out_channels, 0,
A.data_ptr<float>(), patch_size, out_length * patch_size,
&beta,
output.data_ptr<float>(), out_channels, out_length * out_channels,
batch_size
);
```
This computes C_col (64 × 131084) = B_col (64 × 160) * A_col (160 × 131084), which is correct.
And C_col[i, j] corresponds to output_row[j, i], which is [batch, out_length, out_channels].
Wait, but cublas Sgemm memory order for C is column-major. If C_ptr points to our output tensor which is [batch, out_length, out_channels] row-major, then:
output_row[b, o, c] should equal C_col[c, o].
In row-major:
output[b, o, c] is at offset: b*out_length*out_channels + o*out_channels + c
In column-major terms for slice [c, o]:
C_col[c, o] is at offset: c + o*ldc where ldc = 64 (number of rows).
offset = c + o*64
But our output at [o, c] has offset o*out_channels + c = o*64 + c.
These are the same! So if ldc = 64 (out_channels), then the [batch, out_length, out_channels] row-major tensor IS column-major when viewed as [64, out_length] per batch!
Wait, that's a profound insight!
For a tensor of shape [out_length, out_channels] in row-major:
- Viewed as a matrix with out_length rows and out_channels columns, it's row-major.
- But if we view the SAME memory as a matrix with out_channels rows and out_length columns in column-major:
Element at [c, o] in column-major: offset = c + o*out_channels.
Element at [o, c] in row-major: offset = o*out_channels + c.
These ARE the same!
So [out_length, out_channels] row-major is exactly [out_channels, out_length] column-major! No permutation needed!
This means:
- Our output [batch, out_length, out_channels] row-major = [batch, 64, 131084] column-major per batch.
- Our A [batch, out_length, patch_size] row-major = [batch, 160, 131084] column-major per batch.
- Our B [patch_size, out_channels] row-major = [160, 64] column-major.
Actually wait, B is [patch_size, out_channels] = [160, 64] row-major.
As column-major [64, 160]: element [c, i] has offset c + i*64.
In row-major [160, 64]: element [i, c] has offset i*64 + c.
These are the same! So [160, 64] row-major = [64, 160] column-major.
A is [131084, 160] row-major.
As column-major [160, 131084]: element [i, o] has offset i + o*160.
In row-major [131084, 160]: element [o, i] has offset o*160 + i.
These are different unless we transpose! Wait...
For A row-major [m=131084, k=160]:
offset = o*160 + i.
If we want column-major [k=160, m=131084]:
offset should be i + o*160 for element [i, o].
And i + o*160 == o*160 + i. So YES, they are the same!
Wait, element [o, i] in row-major at offset o*k + i.
Element [i, o] in column-major at offset i + o*k.
These are indeed the same!
So ANY row-major [m, k] tensor is identical to column-major [k, m] tensor in memory layout!
This means:
- A: [out_length, patch_size] row-major = [patch_size, out_length] column-major. lda = patch_size (since column-major [patch_size, out_length], lda = number of rows = patch_size).
- B: [patch_size, out_channels] row-major = [out_channels, patch_size] column-major. ldb = out_channels.
- C: [out_length, out_channels] row-major = [out_channels, out_length] column-major. ldc = out_channels.
Great! So the cublas call is:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_N, CUBLAS_OP_N, // no transpose on either
out_channels, out_length, patch_size, // m, n, k
&alpha,
B_ptr, out_channels, 0, // B: [m_B, k] col-major = [out_channels, patch_size], ldb = m_B = out_channels
A_ptr, patch_size, out_length * patch_size, // A: [m_A, n] col-major = [patch_size, out_length], lda = m_A = patch_size
&beta,
C_ptr, out_channels, out_length * out_channels, // C: [m_C, n] col-major = [out_channels, out_length], ldc = m_C = out_channels
batch_size
);
```
Wait, I need to be very careful about the dimensions:
cublasSgemmStridedBatched computes: C_i = alpha * op(A_i) * op(B_i) + beta * C_i
where op(A_i) is m×k, op(B_i) is k×n, C_i is m×n.
In our case:
- op(A_i) should be [out_channels, patch_size] (m×k)
- op(B_i) should be [patch_size, out_length] (k×n)
- C_i should be [out_channels, out_length] (m×n)
Wait no! Matrix multiplication:
[m×k] * [k×n] = [m×n]
If C = B_col * A_col, and C is [out_channels, out_length] (n×m):
B_col is [out_channels, patch_size] (n×k)
A_col is [patch_size, out_length] (k×m)
So in cublas:
m = out_channels (64)
n = out_length (131084)
k = patch_size (160)
op(A_i) = B_col = [64, 160]
op(B_i) = A_col = [160, 131084]
A_ptr = B_col = weight_flat data. lda = 64.
B_ptr = A_col = im2col data. ldb = 160.
YES! This matches my earlier call.
So the call is correct. And since the memory layout naturally aligns (row-major [m,k] = col-major [k,m]), we don't need any explicit transposition in memory.
Now, for the batch strides:
- A_i (im2col) for each batch: strideA = out_length * patch_size
- B_i (weight) for each batch: strideB = 0 (same weight)
- C_i (output) for each batch: strideC = out_length * out_channels
Perfect.
Now let me also verify: C_i is [out_channels, out_length] in column-major.
But our output tensor is [out_length, out_channels] in row-major.
And [m,n] column-major is [n,m] row-major.
So [out_channels, out_length] column-major = [out_length, out_channels] row-major.
This is EXACTLY the shape we want! So no permutation needed after the GEMM.
Let me write the full code.
Actually, wait: the output of conv_transpose1d should be [batch, out_channels, out_length]. But our intermediate GEMM output is [batch, out_length, out_channels]. These differ in the last two dimensions.
Hmm, we need to permute from [batch, out_length, out_channels] to [batch, out_channels, out_length].
This requires a final permutation. But we could avoid it if we do the GEMM differently.
For example, if we compute C^T = A_col^T * B_col^T:
C_row = A_row * B_row.
cublas computes C_col = A_col * B_col (column-major).
If we want C_row = A_row * B_row:
C_row^T = B_row^T * A_row^T
C_col = B_col * A_col.
Which is what we have. So C_col = [out_channels, out_length] column-major = [out_length, out_channels] row-major.
To get [out_channels, out_length] row-major, we need to transpose it. So we do need a permutation.
Alternatively, we can just compute with the transposes:
C_row = A_row * B_row
cublas can compute this as:
C_col = A_col * B_col? No, that's C = A^T * B^T in row-major terms.
Actually:
C_row^T = B_row^T * A_row^T
C_col = B_col * A_col
Which is what we have. C_col is [n, m] column-major. To get [m, n] row-major, we need to transpose.
So: output_row[b, c, o] = C_col[b, c, o] where C_col is [out_channels, out_length].
Wait, [out_length, out_channels] row-major has elements laid out as o*C + c.
[out_channels, out_length] row-major has elements laid out as c*L + o.
These are different memory layouts. So we DO need a transpose.
But we can transpose by changing the cublas call to compute C^T.
To get C_row = A_row * B_row directly as row-major:
We want C_row[i, j] = sum_k A_row[i, k] * B_row[k, j].
In cublas column-major, if we set:
op(A) = A_col^T = [m, k] -> wait.
If op(A) = CUBLAS_OP_T, then cublas treats A as [k, m] in column-major, which means op(A) = [m, k] in column-major. But our A is [m, k] in row-major. A^T in column-major would be [k, m] column-major.
Actually, let me use the transpose operators:
For C_row = A_row * B_row where all are row-major:
We can compute C_col = (A_row * B_row)^T = B_row^T * A_row^T.
B_row^T = B_col if B is stored row-major (since row-major [k,n] = column-major [n,k]).
A_row^T = A_col if A is stored row-major (since row-major [m,k] = column-major [k,m]).
So C_col = B_col * A_col, where:
B_col = [n, k] column-major = B_row^T.
A_col = [k, m] column-major = A_row^T.
C_col = [n, m] column-major = C_row^T.
If we want the output in [m, n] row-major, we get C_row = C_col^T.
So I don't see a way to directly get [m,n] row-major without a transpose. The cublas call computes either C_col = A_col * B_col or C_col = B_col * A_col, which gives the transpose.
However, we can just handle the transpose by calling cublas with m and n swapped and using the transposes:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_T, CUBLAS_OP_T,
out_length, out_channels, patch_size,
&alpha,
A.data_ptr<float>(), patch_size, out_length * patch_size,
weight_flat.data_ptr<float>(), out_channels, 0,
&beta,
output.data_ptr<float>(), out_length, out_length * out_channels,
batch_size
);
```
Wait, op(A) = A^T, op(B) = B^T:
- op(A) = [n, k] (since A is [k, n] in col-major... wait, let me be careful).
If A_ptr points to A_col = [patch_size, out_length] col-major, then:
- With CUBLAS_OP_N: op(A) = [patch_size, out_length]
- With CUBLAS_OP_T: op(A) = [out_length, patch_size]
If B_ptr points to B_col = [out_channels, patch_size] col-major:
- With CUBLAS_OP_N: op(B) = [out_channels, patch_size]
- With CUBLAS_OP_T: op(B) = [patch_size, out_channels]
To compute C = op(A) * op(B) = [out_length, patch_size] * [patch_size, out_channels] = [out_length, out_channels]:
- op(A) = A^T = [out_length, patch_size] -> A is [patch_size, out_length] col-major, so A^T = [out_length, patch_size]. Correct.
- op(B) = B^N = [patch_size, out_channels]? No, B is [out_channels, patch_size] col-major, so B^N = [out_channels, patch_size]. We need [patch_size, out_channels].
To get op(B) = [patch_size, out_channels], we can use CUBLAS_OP_T on B if B is [out_channels, patch_size] col-major? No, B^T would be [patch_size, out_channels] col-major. That's [out_channels, patch_size] in row-major... wait.
B_col = [out_channels, patch_size] col-major.
B_col^T = [patch_size, out_channels] col-major.
If we use transb = CUBLAS_OP_T, op(B) = B_col^T = [patch_size, out_channels].
Then op(A) * op(B) = [out_length, patch_size] * [patch_size, out_channels] = [out_length, out_channels].
And C has shape [out_length, out_channels] in col-major.
[out_length, out_channels] col-major = [out_channels, out_length] row-major.
That's still not [out_length, out_channels] row-major. We need to transpose again.
OK, it seems like we always need a transpose to get from column-major output to row-major output in the desired shape. Let me just add a simple transpose kernel after the GEMM.
Or, just use row-major output [out_length, out_channels] and then transpose to [out_channels, out_length] in a separate kernel. Actually, we need [batch, out_channels, out_length]. So from [batch, out_length, out_channels] to [batch, out_channels, out_length].
```cpp
__global__ void transpose_last_two(float* out, const float* in, int batch, int m, int n) {
int idx = blockIdx.x * blockDim.x + threadIdx.x;
int total = batch * m * n;
if (idx >= total) return;
int b = idx / (m * n);
int rem = idx % (m * n);
int i = rem / n;
int j = rem % n;
// in[b, i, j] -> out[b, j, i]
out[b * m * n + j * m + i] = in[b * m * n + i * n + j];
}
```
Then:
```python
output = output_2d.view(batch_size, out_length, out_channels)
# transpose to [batch, out_channels, out_length]
```
Actually, we can avoid the explicit transpose by having the output of GEMM directly in the right layout if we're clever.
Actually, I just realized: [out_length, out_channels] is contiguous in the sense of row-major, but for PyTorch, the desired output is [batch, out_channels, out_length] which means channels then length. So we do need a permutation.
BUT, we can avoid the transpose by permuting the dimensions BEFORE the GEMM.
Consider:
We want output[b, c, o]. Currently GEMM gives us C[b, o, c].
If we change the GEMM to compute output[b, c, o] directly:
output[b, c, o] = sum_{idx} A[b, o, idx] * B[idx, c]
That's A_row * B_row = C_row where C is [m, n] row-major with m = out_length, n = out_channels.
To get C in [out_channels, out_length] row-major = [out_length, out_channels] column-major:
In cublas:
op(A) = [out_length, patch_size] (A col-major transposed)
op(B) = [patch_size, out_channels] (B col-major transposed)
Wait: If A is [out_length, patch_size] row-major = [patch_size, out_length] col-major.
A_col^T = [out_length, patch_size] col-major.
If B is [patch_size, out_channels] row-major = [out_channels, patch_size] col-major.
B_col^T = [patch_size, out_channels] col-major.
If we compute C = A_col^T * B_col^T:
C has shape [out_length, out_channels] in col-major.
[out_length, out_channels] col-major = [out_channels, out_length] row-major. That's exactly what we want!
So:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_T, CUBLAS_OP_T,
out_length, out_channels, patch_size,
&alpha,
A.data_ptr<float>(), patch_size, out_length * patch_size, // A is [patch_size, out_length] col-major, A^T = [out_length, patch_size]
weight_flat.data_ptr<float>(), out_channels, 0, // B is [out_channels, patch_size] col-major, B^T = [patch_size, out_channels]
&beta,
output.data_ptr<float>(), out_length, out_length * out_channels, // C is [out_length, out_channels] col-major = [out_channels, out_length] row-major
batch_size
);
```
Wait, cublasSgemm computes C = op(A) * op(B).
m = rows of op(A) and C = out_length
n = cols of op(B) and C = out_channels
k = cols of op(A) = rows of op(B) = patch_size
op(A) = A^T where A is lda=patch_size, strideA = out_length * patch_size
Since A is [patch_size, out_length] col-major, A^T = [out_length, patch_size].
The lda parameter specifies the leading dimension of the ORIGINAL matrix A (before transpose), which is patch_size. Because A is [patch_size, out_length] col-major, the leading dimension is patch_size.
op(B) = B^T where B is ldb=out_channels, strideB = 0.
B is [out_channels, patch_size] col-major, B^T = [patch_size, out_channels].
ldb = out_channels (original leading dimension).
C is [out_length, out_channels] col-major.
ldc = out_length.
strideC = out_length * out_channels.
And [out_length, out_channels] col-major means:
C[o, c] at offset o + c * out_length.
If we view this as [out_channels, out_length] row-major:
output[c, o] should be at offset c * out_length + o.
But in the col-major C, offset(o, c) = o + c * out_length.
output[c, o] = C[o, c], so offset = o + c * out_length.
Wait, this gives row-major for [out_length, out_channels], which is:
output[o, c] at o * out_channels + c.
But we want [out_channels, out_length]:
output[c, o] at c * out_length + o.
C_col[o, c] = o + c * out_length.
output[c, o] = C_col[o, c], so output offset = o + c * out_length.
For [out_channels, out_length] row-major: offset should be c * out_length + o.
And indeed c * out_length + o = o + c * out_length.
YES! So C_col = [out_length, out_channels] col-major IS [out_channels, out_length] row-major!
So the cublas call:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_T, CUBLAS_OP_T,
out_length, out_channels, patch_size,
&alpha,
A_ptr, patch_size, out_length * patch_size,
B_ptr, out_channels, 0,
&beta,
C_ptr, out_length, out_length * out_channels,
batch_size
);
```
Produces C in [out_length, out_channels] col-major, which is equivalent to [out_channels, out_length] row-major. This is exactly the desired output shape!
AMAZING! We don't need any transpose at all!
Let me verify once more:
If C is m×n column-major: C[i, j] at offset i + j*m.
For m = out_length, n = out_channels:
C[o, c] at offset o + c*out_length.
If output is [out_channels, out_length] row-major:
output[c, o] at offset c*out_length + o.
c*out_length + o == o + c*out_length.
YES! They are the same offset. So C_col[o, c] maps directly to output_row[c, o]!
This is beautiful. The output of cublas, when interpreted as [out_channels, out_length] row-major, has the exact memory layout we want.
So the output tensor should be created as [batch_size, out_channels, out_length].
Now for A (im2col):
A_ptr points to A which is [batch, out_length, patch_size] row-major.
A row-major [out_length, patch_size] = A col-major [patch_size, out_length].
So A is [patch_size, out_length] col-major. lda = patch_size. Correct.
For B (weight):
B_ptr points to weight_flat which is [patch_size, out_channels] row-major.
B row-major [patch_size, out_channels] = B col-major [out_channels, patch_size].
So B is [out_channels, patch_size] col-major. ldb = out_channels. Correct.
And for C (output):
C_ptr points to output which is [batch, out_channels, out_length] row-major.
C row-major [out_channels, out_length] = C col-major [out_length, out_channels].
So C is [out_length, out_channels] col-major. ldc = out_length. Correct.
Everything lines up perfectly!
Now let me write the actual code.
Also, I need to handle bias. The bias should be added to every output position for the corresponding output channel.
Since output is [batch, out_channels, out_length] row-major, bias[c] should be added to output[:, c, :].
I can write a simple bias kernel:
```cpp
__global__ void add_bias(float* output, const float* bias, int batch, int out_c, int out_l) {
int idx = blockIdx.x * blockDim.x + threadIdx.x;
int total = batch * out_c * out_l;
if (idx >= total) return;
int l = idx % out_l;
int rem = idx / out_l;
int c = rem % out_c;
// int b = rem / out_c;
output[idx] += bias[c];
}
```
Now let me write the full kernel with cublas.
I also need to check if we have access to cublas headers and if we need to link against cublas. In PyTorch 2.0+, cublas is typically available. With load_inline, I might need `extra_cuda_cflags` or `extra_ldflags`.
Let me check: `extra_ldflags=['-lcublas']` might be needed, but often PyTorch extensions link cublas automatically.
Let's try and see if it compiles.
Also, the intermediate A tensor might be large. Let me do chunked processing to save memory. I'll process output_length in chunks.
For chunk-based processing:
```cpp
int chunk_size = 256; // or some value
for (int o_start = 0; o_start < out_length; o_start += chunk_size) {
int o_end = min(o_start + chunk_size, out_length);
int chunk_len = o_end - o_start;
// A_chunk: [batch, chunk_len, patch_size]
// output_chunk: [batch, out_channels, chunk_len] in the main output tensor
// im2col for this chunk
// ...
// cublas for this chunk
cublasSgemmStridedBatched(handle,
CUBLAS_OP_T, CUBLAS_OP_T,
chunk_len, out_channels, patch_size,
&alpha,
A_chunk_ptr, patch_size, chunk_len * patch_size,
weight_ptr, out_channels, 0,
&beta,
output_ptr + o_start, out_length, out_length * out_channels,
batch_size
);
}
```
Wait, for the output pointer offset:
output is [batch, out_channels, out_length].
output[:, :, o_start:o_end] starts at offset o_start (since the last dimension is out_length, and row-major means the last dimension is contiguous).
output_ptr + b * out_channels * out_length + c * out_length + o_start
For strided batched, C_ptr for batch b should be:
output_base + b * (out_length * out_channels) + o_start
And strideC = out_length * out_channels (same as before).
For A_chunk:
A_chunk is [batch, chunk_len, patch_size] row-major = [batch, patch_size, chunk_len] col-major per batch.
strideA = chunk_len * patch_size.
And ldc = out_length (because each column of C is offset by out_length in the full output tensor, not chunk_len).
Wait, for cublas:
C is [chunk_len, out_channels] col-major.
C[i, j] at offset i + j * ldc.
ldc must be the leading dimension of C in the ORIGINAL (non-transposed if applicable) matrix.
Actually, cublas interprets C as [m, n] col-major where m = chunk_len. So ldc should be >= chunk_len. But our actual output tensor has ld = out_length because columns are spaced by out_length in memory.
In our case, for the output tensor [batch, out_channels, out_length]:
output[c, o] at offset c * out_length + o.
For a submatrix C = output[:, :, o_start:o_end]:
C_col[j, i] corresponds to output[o_start + i, j] in the col-major view (wait, this is confusing).
Actually, C_col for the submatrix:
C_col is [chunk_len, out_channels] col-major.
But we're writing into a submatrix of a larger [out_length, out_channels] col-major matrix.
The element C_col[i, j] = output_col[i + o_start, j].
offset = (i + o_start) + j * out_length = i + j * out_length + o_start.
So in cublas terms, the pointer is output_ptr + o_start, and ldc = out_length.
This is correct because:
C[i, j] starts at base + i + j * ldc.
With base = output_ptr + o_start, ldc = out_length:
C[i, j] at output_ptr + o_start + i + j * out_length.
Which is the correct offset for output[:, j, o_start + i].
Wait, I'm mixing up row/col major. Let me be careful.
Output is [batch, out_channels, out_length] row-major.
As col-major, this is [out_length, out_channels] col-major per batch (ignoring batch).
Actually no: [batch, out_channels, out_length] row-major means:
offset = b * out_channels * out_length + c * out_length + o.
= b * (out_channels * out_length) + c * out_length + o.
If we view each batch slice as col-major [out_length, out_channels]:
offset = b * (out_channels * out_length) + o + c * out_length.
= b * strideC + o + c * ldc, where ldc = out_length.
Yes! So the entire batch slice is [out_length, out_channels] col-major with ldc = out_length.
For a sub-chunk [o_start:o_end]:
The submatrix is [chunk_len, out_channels] within the larger [out_length, out_channels] matrix.
C_ptr = output_ptr + o_start.
ldc = out_length.
This works because cublas allows the output matrix to be a submatrix of a larger matrix, as long as ldc >= m.
For A (im2col per chunk):
A is [batch, chunk_len, patch_size] row-major.
As col-major: [patch_size, chunk_len] with lda = patch_size.
A_ptr points to the start of A_chunk.
strideA = chunk_len * patch_size.
For B (weight):
B is [patch_size, out_channels] row-major.
As col-major: [out_channels, patch_size] with ldb = out_channels.
B_ptr points to weight.
strideB = 0.
So the chunk-based cublas call is:
```cpp
cublasSgemmStridedBatched(handle,
CUBLAS_OP_T, CUBLAS_OP_T,
chunk_len, out_channels, patch_size,
&alpha,
A_chunk.data_ptr<float>(), patch_size, chunk_len * patch_size,
weight_flat.data_ptr<float>(), out_channels, 0,
&beta,
output.data_ptr<float>() + o_start, out_length, out_length * out_channels,
batch_size
);
```
Great! Now for the im2col kernel for a chunk:
```cpp
__global__ void im2col_chunk_kernel(
const float* input,
float* A,
int o_start, int chunk_len,
int batch_size, int in_channels, int in_length,
int out_length, int kernel_size, int dilation, int patch_size
) {
int n = blockIdx.z;
int o_local = blockIdx.y * blockDim.y + threadIdx.y;
int idx = blockIdx.x * blockDim.x + threadIdx.x;
if (n >= batch_size || o_local >= chunk_len || idx >= patch_size) return;
int o = o_start + o_local;
int c_in = idx / kernel_size;
int k = idx % kernel_size;
int in_pos = o - k * dilation;
float val = 0.0f;
if (in_pos >= 0 && in_pos < in_length) {
val = input[((n * in_channels) + c_in) * in_length + in_pos];
}
A[((n * chunk_len) + o_local) * patch_size + idx] = val;
}
```
This should work. Let me write the full code.
Actually, let me re-check the cublas formula one more time with the transposes:
cublasSgemmStridedBatched computes: C_i = alpha * op(A_i) * op(B_i) + beta * C_i
With transa = CUBLAS_OP_T, transb = CUBLAS_OP_T:
op(A_i) = A_i^T
op(B_i) = B_i^T
A_i is [patch_size, chunk_len] col-major (since A_row = [chunk_len, patch_size]).
A_i^T = [chunk_len, patch_size] col-major.
B_i is [out_channels, patch_size] col-major (since B_row = [patch_size, out_channels]).
B_i^T = [patch_size, out_channels] col-major.
C = [chunk_len, patch_size] * [patch_size, out_channels] = [chunk_len, out_channels].
And C is [chunk_len, out_channels] col-major.
Which equals [out_channels, chunk_len] row-major.
Which is the submatrix of output[:, :, o_start:o_end] as desired.
YES!
Now, regarding the includes:
- `#include <cublas_v2.h>`
- `#include <ATen/cuda/CUDAContext.h>`
And I should handle cublas errors. Let me keep it simple and skip error checking for now (not recommended for production, but for this task it should be fine).
Let me also make sure the weight is properly prepared in Python.
```python
def forward(self, x):
x = x.contiguous()
weight = self.conv_ref.weight # [in_channels, out_channels, kernel_size]
# Permute for cublas: [in_channels, kernel_size, out_channels] -> [patch_size, out_channels]
weight_t = weight.permute(0, 2, 1).contiguous().view(-1, self.conv_ref.out_channels)
if self.use_bias and self.conv_ref.bias is not None:
bias = self.conv_ref.bias.contiguous()
use_bias = 1
else:
bias = torch.empty(0, device=x.device, dtype=x.dtype)
use_bias = 0
return conv_transpose1d_module.conv_transpose1d_cuda(
x, weight_t, bias, use_bias,
self.stride, self.padding, self.dilation
)
```
Wait, I also need to pass `out_channels` or some metadata to the C++ function. Actually, I can derive everything from the tensor shapes in C++. Let me check:
In C++, I receive:
- input: [batch, in_channels, in_length]
- weight_t: [patch_size, out_channels]
- bias: [out_channels] or empty
I can derive:
- batch_size = input.size(0)
- in_channels = input.size(1)
- in_length = input.size(2)
- patch_size = weight_t.size(0)
- out_channels = weight_t.size(1)
kernel_size = patch_size / in_channels.
This should work.
Let me write the complete kernel now.
Actually, one more thing: with load_inline, the CUDA code will be compiled. I need to make sure that `cublas_v2.h` is available and that cublas is linked. I'll add `extra_ldflags=["-lcublas"]` to `load_inline`.
For `extra_cuda_cflags`, I can use `["-O3"]`.
Let me draft the code.
Also, I wonder if a chunk size of 256 is good. For out_length = 131084, we'd have about 512 chunks. Each cublas call has m = chunk_len, n = out_channels = 64, k = 160. This is a very small GEMM (256×160 * 160×64). cublas might have some overhead for such small operations. 512 calls per batch might be slow.
If I use a larger chunk size like 2048, it's 64 chunks of (2048×160 * 160×64) which is better.
Actually, for the H100 with tensor cores, larger chunks are better. But the memory for A_chunk = 32 * 2048 * 160 * 4 = 41.9 MB, which is very reasonable.
Also, I could process multiple output positions per thread block in the im2col kernel to keep the GPU busy.
Actually, let me try chunk_size = 4096:
A_chunk = 32 * 4096 * 160 * 4 = 83.9 MB.
Number of chunks = 131084 / 4096 ≈ 32.
32 iterations, each with a cublas call. That's good!
Wait, actually I need the output to be contiguous. Let me make sure.
I'll use chunk_size = 2048 or 4096.
Actually, I'll make chunk_size a template parameter or a constant. Let me set it to 2048 for now.
Let me write the final code.
Also, does cublas handle the case where the last chunk is smaller? Yes, because we pass `chunk_len` to cublas, and the output pointer is offset correctly.
Let me now carefully write all the code.
Hmm, actually I'm worried about the performance of cublas for strided batched GEMM with small matrices. 32 × (4096 × 160) @(160 × 64) per iteration.
Each batch element: [4096, 160] × [160, 64].
For 32 batch elements, cublas combines them.
Actually, strided batched GEMM with m=4096, n=64, k=160, batch=32:
This is still relatively small. A single large GEMM of [131084, 160] × [160, 64] would be faster due to better utilization. But that requires 2.68GB of A memory.
Since H100 has 80GB, 2.68GB is fine! The extra memory allocation might take some time but the GEMM should be efficient.
Let me just use the full A tensor without chunking to maximize GEMM efficiency. If there's an OOM, I can fall back to chunking.
Actually, the total memory usage would be:
- input: 536 MB
- output: 1.07 GB
- A: 2.68 GB
- weight: 32*64*5*4 = 40.96 KB
Total: ~4.3 GB. Very manageable.
I'll use the full-size approach for simplicity and better performance. If compilation passes, let me see if correctness improves.
OK, one more concern: cublas handles. I need to get the current cublas handle from PyTorch's ATen CUDA context.
```cpp
#include <ATen/cuda/CUDABlas.h>
cublasHandle_t handle = at::cuda::getCurrentCUDABlasHandle();
```
Wait, `getCurrentCUDABlasHandle()` is a function that returns a cublasHandle_t. But I need to include the right header.
In PyTorch, it's declared in `<ATen/cuda/CUDABlas.h>` or `<ATen/cuda/CUDAContext.h>`.
Let me check... Actually, I think `<ATen/cuda/CUDAContext.h>` has `getCurrentCUDABlasHandle()`.
Also, I can just create my own cublas handle. It's a bit of overhead but for a single call it's fine.
```cpp
cublasHandle_t handle;
cublasCreate(&handle);
// ... gemm ...
cublasDestroy(&handle);
```
But creating/destroying a handle per forward pass is bad for performance. Let me use a cached handle.
```cpp
static cublasHandle_t get_cublas_handle() {
static cublasHandle_t handle = nullptr;
if (handle == nullptr) {
cublasCreate(&handle);
}
return handle;
}
```
This is thread-safe in the sense that it's initialized once. But it's not perfectly thread-safe in initialization. For simplicity in this task, it should be fine.
Actually, a static local variable in C++11 is thread-safe for initialization. So:
```cpp
cublasHandle_t getHandle() {
static cublasHandle_t handle = [](){
cublasHandle_t h;
cublasCreate(&h);
return h;
}();
return handle;
}
```
This is safe and simple.
Now, do I need to link `-lcublas`? In PyTorch, cublas is usually linked. Let me add it to be safe.
Actually, I realize there might be an issue: `load_inline` compiles the code, and I need to make sure the CUDA compilation includes the cublas headers. On most PyTorch installations, they should be in the CUDA toolkit path.
Let me write the full Python module:
```python
import torch
import torch.nn as nn
from torch.utils.cpp_extension import load_inline
cuda_source = r'''
#include <torch/extension.h>
#include <cuda_runtime.h>
#include <cublas_v2.h>
cublasHandle_t getCublasHandle() {
static cublasHandle_t handle = [](){
cublasHandle_t h;
cublasCreate(&h);
return h;
}();
return handle;
}
__global__ void im2col_kernel(
const float* __restrict__ input,
float* __restrict__ A,
int batch_size, int in_channels, int in_length,
int out_length, int kernel_size, int dilation, int patch_size
) {
int n = blockIdx.z;
int o = blockIdx.y * blockDim.y + threadIdx.y;
int idx = blockIdx.x * blockDim.x + threadIdx.x;
if (n >= batch_size || o >= out_length || idx >= patch_size) return;
int c_in = idx / kernel_size;
int k = idx % kernel_size;
int in_pos = o - k * dilation;
float val = 0.0f;
if (in_pos >= 0 && in_pos < in_length) {
val = input[((n * in_channels) + c_in) * in_length + in_pos];
}
A[((n * out_length) + o) * patch_size + idx] = val;
}
__global__ void add_bias_kernel(
float* __restrict__ output,
const float* __restrict__ bias,
int batch_size, int out_channels, int out_length
) {
int idx = blockIdx.x * blockDim.x + threadIdx.x;
int total = batch_size * out_channels * out_length;
if (idx >= total) return;
int o = idx % out_length;
int rem = idx / out_length;
int c_out = rem % out_channels;
output[idx] += bias[c_out];
}
torch::Tensor conv_transpose1d_cuda(
torch::Tensor input,
torch::Tensor weight,
torch::Tensor bias,
int use_bias,
int stride, int padding, int dilation
) {
int batch_size = input.size(0);
int in_channels = input.size(1);
int in_length = input.size(2);
int patch_size = weight.size(0);
int out_channels = weight.size(1);
int kernel_size = patch_size / in_channels;
int out_length = (in_length - 1) * stride - 2 * padding + dilation * (kernel_size - 1) + 1;
auto A = torch::empty({batch_size, out_length, patch_size}, input.options());
auto output = torch::empty({batch_size, out_channels, out_length}, input.options());
// im2col
dim3 block_im2col(16, 16);
dim3 grid_im2col(
(patch_size + 15) / 16,
(out_length + 15) / 16,
batch_size
);
im2col_kernel<<<grid_im2col, block_im2col>>>(
input.data_ptr<float>(),
A.data_ptr<float>(),
batch_size, in_channels, in_length,
out_length, kernel_size, dilation, patch_size
);
// cublas GEMM
cublasHandle_t handle = getCublasHandle();
float alpha = 1.0f;
float beta = 0.0f;
// A is [batch, out_length, patch_size] row-major -> [batch, patch_size, out_length] col-major per batch
// weight is [patch_size, out_channels] row-major -> [out_channels, patch_size] col-major
// output is [batch, out_channels, out_length] row-major -> [batch, out_length, out_channels] col-major per batch
cublasSgemmStridedBatched(handle,
CUBLAS_OP_T, CUBLAS_OP_T,
out_length, out_channels, patch_size,
&alpha,
A.data_ptr<float>(), patch_size, out_length * patch_size,
weight.data_ptr<float>(), out_channels, 0,
&beta,
output.data_ptr<float>(), out_length, out_channels * out_length,
batch_size
);
if (use_bias) {
int total = batch_size * out_channels * out_length;
int threads = 256;
add_bias_kernel<<<(total + threads - 1) / threads, threads>>>(
output.data_ptr<float>(),
bias.data_ptr<float>(),
batch_size, out_channels, out_length
);
}
return output;
}
'''
cpp_source = r'''
torch::Tensor conv_transpose1d_cuda(
torch::Tensor input,
torch::Tensor weight,
torch::Tensor bias,
int use_bias,
int stride, int padding, int dilation
);
'''
conv_transpose1d_module = load_inline(
name="conv_transpose1d_cublas",
cpp_sources=[cpp_source],
cuda_sources=[cuda_source],
functions=["conv_transpose1d_cuda"],
extra_cuda_cflags=["-O3"],
extra_ldflags=["-lcublas"],
verbose=True,
)
class ModelNew(nn.Module):
def __init__(self, in_channels, out_channels, kernel_size, stride=1, padding=0, dilation=1, bias=False):
super(ModelNew, self).__init__()
self.stride = stride
self.padding = padding
self.dilation = dilation
self.use_bias = bias
self.conv_ref = nn.ConvTranspose1d(
in_channels, out_channels, kernel_size,
stride=stride, padding=padding, dilation=dilation, bias=bias
)
def forward(self, x):
x = x.contiguous()
weight = self.conv_ref.weight # [in_channels, out_channels, kernel_size]
# Reshape weight to [in_channels*kernel_size, out_channels] with correct layout
weight_t = weight.permute(0, 2, 1).contiguous().view(-1, weight.size(1))
if self.use_bias and self.conv_ref.bias is not None:
bias_tensor = self.conv_ref.bias.contiguous()
use_bias = 1
else:
bias_tensor = torch.empty(0, device=x.device, dtype=x.dtype)
use_bias = 0
return conv_transpose1d_module.conv_transpose1d_cuda(
x, weight_t, bias_tensor, use_bias, self.stride, self.padding, self.dilation
)
```
Let me compile and test this!
Actually, wait. I want to double-check one thing: the A tensor is [batch, out_length, patch_size] row-major.
When I pass it to cublas with CUBLAS_OP_T, A becomes [patch_size, out_length] col-major.
In cublas column-major terms, the lda is the leading dimension of the ORIGINAL matrix (before transpose).
The original A (before transpose) is [patch_size, out_length] col-major. lda = patch_size. Correct.
For weight: [patch_size, out_channels] row-major. Before transpose, it's [out_channels, patch_size] col-major. ldb = out_channels. Correct.
For output: [batch, out_channels, out_length] row-major. Before transpose, each batch is [out_length, out_channels] col-major. ldc = out_length. Correct.
Wait, actually cublas computes C = op(A) * op(B).
With transa = CUBLAS_OP_T, transb = CUBLAS_OP_T:
op(A_i) = A_i^T.
op(B_i) = B_i^T.
A_i is [patch_size, out_length] col-major. A_i^T = [out_length, patch_size] col-major.
B_i is [out_channels, patch_size] col-major. B_i^T = [patch_size, out_channels] col-major.
C = [out_length, patch_size] * [patch_size, out_channels] = [out_length, out_channels] col-major.
And [out_length, out_channels] col-major is the memory layout of [out_channels, out_length] row-major, which is our output!
So output[b, c_out, o] corresponds to C_col[o, c_out] for that batch.
Yes, this matches!
One more check: cublasSgemmStridedBatched signature:
```cpp
cublasStatus_t cublasSgemmStridedBatched(
cublasHandle_t handle,
cublasOperation_t transa, cublasOperation_t transb,
int m, int n, int k,
const float *alpha,
const float *A, int lda, long long int strideA,
const float *B, int ldb, long long int strideB,
const float *beta,
float *C, int ldc, long long int strideC,
int batchCount)
```
Parameters:
- m: number of rows of op(A) and C.
op(A) = A_i^T = [out_length, patch_size]. m = out_length.
- n: number of columns of op(B) and C.
op(B) = B_i^T = [patch_size, out_channels]. n = out_channels.
- k: number of columns of op(A) and rows of op(B).
k = patch_size.
- A: pointer to first A matrix. lda = leading dimension of A (before transpose).
A is [patch_size, out_length] col-major. lda = patch_size.
- strideA: stride between batch A matrices.
A is [batch, out_length, patch_size] row-major.
Per batch, A_i is [out_length, patch_size] row-major = [patch_size, out_length] col-major.
Stride between batches = out_length * patch_size.
- B: pointer to B matrix. ldb = leading dimension of B.
B is [out_channels, patch_size] col-major (since [patch_size, out_channels] row-major).
ldb = out_channels.
- strideB: stride between batch B matrices.
B is shared across batches. strideB = 0.
- C: pointer to first C matrix. ldc = leading dimension of C.
C is [out_length, out_channels] col-major per batch.
ldc = out_length.
- strideC: stride between batch C matrices.
C is [batch, out_channels, out_length] row-major = [batch, out_length, out_channels] col-major per batch.
Stride = out_length * out_channels.
- batchCount: batch_size.
This all checks out!
Let me compile it.
One more thing: `add_bias_kernel` output indexing.
output is [batch, out_channels, out_length] row-major.
offset = ((n * out_channels) + c_out) * out_length + o.
In my add_bias_kernel:
```cpp
int o = idx % out_length;
int rem = idx / out_length;
int c_out = rem % out_channels;
```
offset formula: idx maps to output[idx] since it's contiguous row-major with the last dimension out_length.
Wait, with [batch, out_channels, out_length]:
Total elements = batch * out_channels * out_length.
If we iterate idx from 0 to total-1:
idx = n * out_channels * out_length + c_out * out_length + o.
So:
o = idx % out_length
c_out = (idx / out_length) % out_channels
n = idx / (out_channels * out_length)
My kernel computes:
```cpp
int o = idx % out_length;
int rem = idx / out_length;
int c_out = rem % out_channels;
```
This correctly gets o and c_out (but doesn't need n for bias).
offset = idx is correct because row-major and contiguous.
Actually, I need to make sure output is contiguous. In the C++ code, I allocate it with `torch::empty`, which creates a contiguous tensor. So yes, output[idx] is correct.
Great. Let me compile and test!
Actually, let me also check the im2col kernel launch.
```cpp
dim3 block_im2col(16, 16);
dim3 grid_im2col(
(patch_size + 15) / 16, // x: patch_size threads
(out_length + 15) / 16, // y: out_length threads
batch_size // z: batch
);
```
In the kernel:
```cpp
int n = blockIdx.z;
int o = blockIdx.y * blockDim.y + threadIdx.y;
int idx = blockIdx.x * blockDim.x + threadIdx.x;
```
This assigns one thread per (o, idx) pair, with z for batch.
o ranges over out_length, idx ranges over patch_size.
But I use 16x16 threads per block. For patch_size = 160:
(160 + 15) / 16 = 11 blocks in x.
For out_length = 131084:
(131084 + 15) / 16 = 8193 blocks in y.
For batch = 32: 32 blocks in z.
Total blocks = 11 * 8193 * 32 = 2.88M blocks. Each block has 256 threads. Total threads = 737M, but only 32 * 131084 * 160 = 671M elements (since each thread handles one (o, idx) pair). Wait, actually 32 * 131084 * 160 = 671, 089, 920 elements. Each block handles 16*16 = 256 elements. Total blocks needed = 671M / 256 = 2.62M. With 11 * 8193 * 32 = 2,883,936, that's slightly more due to padding. This is fine.
Let me compile!
Wait, actually I also need to consider: `torch::empty` for A and output. Will they be on the same device as input? Yes, `input.options()` preserves the device and dtype.
One more thing about `load_inline`: the compilation might fail if cublas headers are not found. A common issue on some platforms. Let me add the necessary flags.
Actually, I'll include `<cublas_v2.h>` directly. CUDA toolkit includes should be available.
If compilation fails due to cublas, I might need to use `torch.backends.cuda.cublas` through PyTorch's Python API, but that wouldn't be a custom CUDA kernel.
Let me try it.
</thinking>