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from typing import Optional, Tuple, Union
import torch
from einops import rearrange, repeat
import torch.nn.functional as F
import triton
import triton.language as tl
# @triton.autotune(
# configs=[
# triton.Config({"BLOCK_M": 2}),
# triton.Config({"BLOCK_M": 4}),
# triton.Config({"BLOCK_M": 8}),
# triton.Config({"BLOCK_M": 16}),
# ],
# key=["CACHE_KEY_SEQLEN", "BLOCK_K", "INTERLEAVED"],
# )
@triton.jit
def rotary_kernel(
OUT, # Pointers to matrices
X,
COS,
SIN,
CU_SEQLENS,
SEQLEN_OFFSETS, # this could be int or a pointer
# Matrix dimensions
seqlen,
nheads,
rotary_dim,
seqlen_ro,
CACHE_KEY_SEQLEN,
# strides
stride_out_batch,
stride_out_nheads,
stride_out_seqlen,
stride_out_headdim,
stride_x_batch,
stride_x_nheads,
stride_x_seqlen,
stride_x_headdim,
# Meta-parameters
BLOCK_K: tl.constexpr,
IS_SEQLEN_OFFSETS_TENSOR: tl.constexpr,
IS_VARLEN: tl.constexpr,
INTERLEAVED: tl.constexpr,
CONJUGATE: tl.constexpr,
BLOCK_M: tl.constexpr,
):
pid_m = tl.program_id(axis=0)
pid_batch = tl.program_id(axis=1)
pid_head = tl.program_id(axis=2)
rotary_dim_half = rotary_dim // 2
if not IS_VARLEN:
X = X + pid_batch * stride_x_batch + pid_head * stride_x_nheads
OUT = OUT + pid_batch * stride_out_batch + pid_head * stride_out_nheads
COS = COS + pid_batch * seqlen_ro * rotary_dim_half
SIN = SIN + pid_batch * seqlen_ro * rotary_dim_half
else:
start_idx = tl.load(CU_SEQLENS + pid_batch)
seqlen = tl.load(CU_SEQLENS + pid_batch + 1) - start_idx
X = X + start_idx * stride_x_seqlen + pid_head * stride_x_nheads
OUT = OUT + start_idx * stride_out_seqlen + pid_head * stride_out_nheads
if pid_m * BLOCK_M >= seqlen:
return
rm = pid_m * BLOCK_M + tl.arange(0, BLOCK_M)
if not IS_SEQLEN_OFFSETS_TENSOR:
rm_cs = rm + SEQLEN_OFFSETS
else:
rm_cs = rm + tl.load(SEQLEN_OFFSETS + pid_batch)
rk = tl.arange(0, BLOCK_K)
rk_half = tl.arange(0, BLOCK_K // 2)
if not INTERLEAVED:
# Load the 1st and 2nd halves of X, do calculation, then store to 1st and 2nd halves of OUT
X = X + (rm[:, None] * stride_x_seqlen + rk_half[None, :] * stride_x_headdim)
COS = COS + (rm_cs[:, None] * rotary_dim_half + rk_half[None, :])
SIN = SIN + (rm_cs[:, None] * rotary_dim_half + rk_half[None, :])
cos = tl.load(
COS, mask=(rm_cs[:, None] < seqlen_ro) & (rk_half[None, :] < rotary_dim_half), other=1.0
)
sin = tl.load(
SIN, mask=(rm_cs[:, None] < seqlen_ro) & (rk_half[None, :] < rotary_dim_half), other=0.0
)
x0 = tl.load(
X, mask=(rm[:, None] < seqlen) & (rk_half[None, :] < rotary_dim_half), other=0.0
)
x1 = tl.load(
X + rotary_dim_half * stride_x_headdim,
mask=(rm[:, None] < seqlen) & (rk_half[None, :] < rotary_dim_half),
other=0.0,
)
if CONJUGATE:
sin = -sin
o0 = x0 * cos - x1 * sin
o1 = x0 * sin + x1 * cos
# write back result
OUT = OUT + (rm[:, None] * stride_out_seqlen + rk_half[None, :] * stride_out_headdim)
tl.store(OUT, o0, mask=(rm[:, None] < seqlen) & (rk_half[None, :] < rotary_dim_half))
tl.store(
OUT + rotary_dim_half * stride_out_headdim,
o1,
mask=(rm[:, None] < seqlen) & (rk_half[None, :] < rotary_dim_half),
)
else:
# We don't want to load X[0, 2, 4, ...] and X[1, 3, 5, ...] separately since both are slow.
# Instead, we load x0 = X[0, 1, 2, 3, ...] and x1 = X[1, 0, 3, 2, ...].
# Loading x0 will be fast but x1 will be slow.
# Then we load cos = COS[0, 0, 1, 1, ...] and sin = SIN[0, 0, 1, 1, ...].
# Then we do the calculation and use tl.where to pick put the right outputs for the even
# and for the odd indices.
rk_swap = rk + ((rk + 1) % 2) * 2 - 1 # 1, 0, 3, 2, 5, 4, ...
rk_repeat = tl.arange(0, BLOCK_K) // 2
X0 = X + (rm[:, None] * stride_x_seqlen + rk[None, :] * stride_x_headdim)
X1 = X + (rm[:, None] * stride_x_seqlen + rk_swap[None, :] * stride_x_headdim)
COS = COS + (rm_cs[:, None] * rotary_dim_half + rk_repeat[None, :])
SIN = SIN + (rm_cs[:, None] * rotary_dim_half + rk_repeat[None, :])
cos = tl.load(
COS,
mask=(rm_cs[:, None] < seqlen_ro) & (rk_repeat[None, :] < rotary_dim_half),
other=1.0,
).to(tl.float32)
sin = tl.load(
SIN,
mask=(rm_cs[:, None] < seqlen_ro) & (rk_repeat[None, :] < rotary_dim_half),
other=0.0,
).to(tl.float32)
x0 = tl.load(X0, mask=(rm[:, None] < seqlen) & (rk[None, :] < rotary_dim), other=0.0).to(
tl.float32
)
x1 = tl.load(
X1, mask=(rm[:, None] < seqlen) & (rk_swap[None, :] < rotary_dim), other=0.0
).to(tl.float32)
if CONJUGATE:
sin = -sin
x0_cos = x0 * cos
x1_sin = x1 * sin
out = tl.where(rk[None, :] % 2 == 0, x0_cos - x1_sin, x0_cos + x1_sin)
OUT = OUT + (rm[:, None] * stride_out_seqlen + rk[None, :] * stride_out_headdim)
tl.store(OUT, out, mask=(rm[:, None] < seqlen) & (rk[None, :] < rotary_dim))
def apply_rotary(
x: torch.Tensor,
cos: torch.Tensor,
sin: torch.Tensor,
seqlen_offsets: Union[int, torch.Tensor] = 0,
cu_seqlens: Optional[torch.Tensor] = None,
max_seqlen: Optional[int] = None,
interleaved=False,
inplace=False,
conjugate=False,
) -> torch.Tensor:
"""
Arguments:
x: (batch, seqlen, nheads, headdim) if cu_seqlens is None
else (total_seqlen, nheads, headdim).
cos: (seqlen_ro, rotary_dim / 2)
sin: (seqlen_ro, rotary_dim / 2)
seqlen_offsets: integer or integer tensor of size (batch,)
cu_seqlens: (batch + 1,) or None
max_seqlen: int
Returns:
y: (batch, seqlen, nheads, headdim)
"""
batch, nheads, seqlen, headdim = x.shape
batch_ro, seqlen_ro, rotary_dim = cos.shape
assert batch == batch_ro
assert sin.shape == cos.shape
rotary_dim *= 2
assert rotary_dim <= headdim, "rotary_dim must be <= headdim"
assert headdim <= 256, "Only support headdim <= 256"
assert seqlen_ro >= seqlen, "seqlen_ro must be >= seqlen"
assert (
cos.dtype == sin.dtype
), f"cos and sin must have the same dtype, got {cos.dtype} and {sin.dtype}"
assert (
x.dtype == cos.dtype
), f"Input and cos/sin must have the same dtype, got {x.dtype} and {cos.dtype}"
cos, sin = cos.contiguous(), sin.contiguous()
if isinstance(seqlen_offsets, torch.Tensor):
assert seqlen_offsets.shape == (batch,)
assert seqlen_offsets.dtype in [torch.int32, torch.int64]
seqlen_offsets = seqlen_offsets.contiguous()
else:
assert seqlen_offsets + seqlen <= seqlen_ro
output = torch.empty_like(x) if not inplace else x
if rotary_dim < headdim and not inplace:
output[..., rotary_dim:].copy_(x[..., rotary_dim:])
BLOCK_K = (
32
if rotary_dim <= 32
else (64 if rotary_dim <= 64 else (128 if rotary_dim <= 128 else 256))
)
grid = lambda META: (triton.cdiv(seqlen, META["BLOCK_M"]), batch, nheads) # noqa
BLOCK_M = 4 if interleaved else (8 if rotary_dim <= 64 else 4)
# Need this, otherwise Triton tries to launch from cuda:0 and we get
# ValueError: Pointer argument (at 0) cannot be accessed from Triton (cpu tensor?)
with torch.cuda.device(x.device.index):
rotary_kernel[grid](
output, # data ptrs
x,
cos,
sin,
cu_seqlens,
seqlen_offsets,
seqlen, # shapes
nheads,
rotary_dim,
seqlen_ro,
seqlen // 128, # key for triton cache (limit number of compilations)
output.stride(0), # batch_strides
output.stride(-3), # nheads_stride
output.stride(-2), # seqlen_stride
output.stride(-1), # headdim_stride
x.stride(0), # batch_strides
x.stride(-3), # nheads stride
x.stride(-2), # seqlen stride
x.stride(-1), # headdim stride
BLOCK_K,
isinstance(seqlen_offsets, torch.Tensor),
False,
interleaved,
conjugate,
BLOCK_M,
)
return output
class ApplyRotaryEmb(torch.autograd.Function):
@staticmethod
def forward(
ctx,
x,
cos,
sin,
interleaved=False,
inplace=False,
seqlen_offsets: Union[int, torch.Tensor] = 0,
cu_seqlens: Optional[torch.Tensor] = None,
max_seqlen: Optional[int] = None,
):
out = apply_rotary(
x,
cos,
sin,
seqlen_offsets=seqlen_offsets,
cu_seqlens=cu_seqlens,
max_seqlen=max_seqlen,
interleaved=interleaved,
inplace=inplace,
)
if isinstance(seqlen_offsets, int):
ctx.save_for_backward(cos, sin, cu_seqlens) # Can't save int with save_for_backward
ctx.seqlen_offsets = seqlen_offsets
else:
ctx.save_for_backward(cos, sin, cu_seqlens, seqlen_offsets)
ctx.seqlen_offsets = None
ctx.interleaved = interleaved
ctx.inplace = inplace
ctx.max_seqlen = max_seqlen
return out if not inplace else x
@staticmethod
def backward(ctx, do):
seqlen_offsets = ctx.seqlen_offsets
if seqlen_offsets is None:
cos, sin, cu_seqlens, seqlen_offsets = ctx.saved_tensors
else:
cos, sin, cu_seqlens = ctx.saved_tensors
# TD [2023-09-02]: For some reason Triton (2.0.0.post1) errors with
# "[CUDA]: invalid device context", and cloning makes it work. Idk why. Triton 2.1.0 works.
if not ctx.interleaved and not ctx.inplace:
do = do.clone()
dx = apply_rotary(
do,
cos,
sin,
seqlen_offsets=seqlen_offsets,
cu_seqlens=cu_seqlens,
max_seqlen=ctx.max_seqlen,
interleaved=ctx.interleaved,
inplace=ctx.inplace,
conjugate=True,
)
return dx, None, None, None, None, None, None, None
def apply_rotary_emb(
x,
cos,
sin,
interleaved=False,
inplace=False,
seqlen_offsets: Union[int, torch.Tensor] = 0,
cu_seqlens: Optional[torch.Tensor] = None,
max_seqlen: Optional[int] = None,
):
"""
Arguments:
x: (batch_size, seqlen, nheads, headdim) if cu_seqlens is None
else (total_seqlen, nheads, headdim)
cos, sin: (seqlen_rotary, rotary_dim / 2)
interleaved: if True, rotate pairs of even and odd dimensions (GPT-J style) instead
of 1st half and 2nd half (GPT-NeoX style).
inplace: if True, apply rotary embedding in-place.
seqlen_offsets: (batch_size,) or int. Each sequence in x is shifted by this amount.
Most commonly used in inference when we have KV cache.
cu_seqlens: (batch + 1,) or None
max_seqlen: int
Return:
out: (batch_size, seqlen, nheads, headdim) if cu_seqlens is None
else (total_seqlen, nheads, headdim)
rotary_dim must be <= headdim
Apply rotary embedding to the first rotary_dim of x.
"""
return ApplyRotaryEmb.apply(
x, cos, sin, interleaved, inplace, seqlen_offsets, cu_seqlens, max_seqlen
)
# For backward compatibility
apply_rotary_emb_func = apply_rotary_emb
class FastRotaryEmbedding(torch.nn.Module):
"""
The rotary position embeddings from RoFormer_ (Su et. al).
A crucial insight from the method is that the query and keys are
transformed by rotation matrices which depend on the relative positions.
Other implementations are available in the Rotary Transformer repo_ and in
GPT-NeoX_, GPT-NeoX was an inspiration
.. _RoFormer: https://arxiv.org/abs/2104.09864
.. _repo: https://github.com/ZhuiyiTechnology/roformer
.. _GPT-NeoX: https://github.com/EleutherAI/gpt-neox
If scale_base is not None, this implements XPos (Sun et al., https://arxiv.org/abs/2212.10554).
A recommended value for scale_base is 512: https://github.com/HazyResearch/flash-attention/issues/96
Reference: https://github.com/sunyt32/torchscale/blob/main/torchscale/component/xpos_relative_position.py
"""
def __init__(
self,
dim: int,
base=10000,
interleaved=False,
scale_base=None,
pos_idx_in_fp32=True,
device=None,
):
"""
interleaved: if True, rotate pairs of even and odd dimensions (GPT-J style) instead
of 1st half and 2nd half (GPT-NeoX style).
pos_idx_in_fp32: if True, the position indices [0.0, ..., seqlen - 1] are in fp32,
otherwise they might be in lower precision.
This option was added because previously (before 2023-07-02), when we construct
the position indices, we use the dtype of self.inv_freq. In most cases this would
be fp32, but if the model is trained in pure bf16 (not mixed precision), then
self.inv_freq would be bf16, and the position indices are also in bf16.
Because of the limited precision of bf16 (e.g. 1995.0 is rounded to 2000.0), the
embeddings for some positions will coincide.
To maintain compatibility with models previously trained in pure bf16,
we add this option.
"""
super().__init__()
self.dim = dim
self.base = base
self.pos_idx_in_fp32 = pos_idx_in_fp32
# Generate and save the inverse frequency buffer (non trainable)
inv_freq = self._compute_inv_freq(device)
self.register_buffer("inv_freq", inv_freq)
self.interleaved = interleaved
self.scale_base = scale_base
scale = (
(torch.arange(0, dim, 2, device=device, dtype=torch.float32) + 0.4 * dim) / (1.4 * dim)
if scale_base is not None
else None
)
self.register_buffer("scale", scale, persistent=False)
self._seq_len_cached = 0
self._cos_cached = None
self._sin_cached = None
self._cos_k_cached = None
self._sin_k_cached = None
self.cos = None
self.sin = None
def _compute_inv_freq(self, device=None):
return 1.0 / (
self.base
** (torch.arange(0, self.dim, 2, device=device) / self.dim)
# ** (torch.arange(0, self.dim, 2, device=device).float() / self.dim)
)
def _update_cos_sin_cache(self, seqlen, position_id, device=None, dtype=None):
if (
seqlen > self._seq_len_cached
):
self._seq_len_cached = seqlen
# We want fp32 here, not self.inv_freq.dtype, since the model could be loaded in bf16
# And the output of arange can be quite large, so bf16 would lose a lot of precision.
# However, for compatibility reason, we add an option to use the dtype of self.inv_freq.
if self.pos_idx_in_fp32:
t = torch.arange(seqlen, device=device, dtype=torch.float32)
# We want fp32 here as well since inv_freq will be multiplied with t, and the output
# will be large. Having it in bf16 will lose a lot of precision and cause the
# cos & sin output to change significantly.
# We want to recompute self.inv_freq if it was not loaded in fp32
if self.inv_freq.dtype != torch.float32:
inv_freq = self._compute_inv_freq(device=device)
else:
inv_freq = self.inv_freq
else:
t = torch.arange(seqlen, device=device, dtype=self.inv_freq.dtype)
inv_freq = self.inv_freq
freqs = torch.einsum("i,j->ij", t, inv_freq)
if self.scale is None:
self._cos_cached = torch.cos(freqs).to(dtype)
self._sin_cached = torch.sin(freqs).to(dtype)
else:
power = (
torch.arange(seqlen, dtype=self.scale.dtype, device=self.scale.device)
- seqlen // 2
) / self.scale_base
scale = self.scale.to(device=power.device) ** rearrange(power, "s -> s 1")
# We want the multiplication by scale to happen in fp32
self._cos_cached = (torch.cos(freqs) * scale).to(dtype)
self._sin_cached = (torch.sin(freqs) * scale).to(dtype)
self._cos_k_cached = (torch.cos(freqs) / scale).to(dtype)
self._sin_k_cached = (torch.sin(freqs) / scale).to(dtype)
def forward(
self,
q: torch.Tensor,
k: torch.Tensor,
position_ids: torch.Tensor,
max_seqlen,
) -> Tuple[torch.Tensor, torch.Tensor]:
"""
q: (batch, nheads, seqlen, headdim)
k: (batch, nheads, seqlen, headdim)
position_id: (batch, seqlen)
max_seqlen: int
layer_id: int
only if layer_id == 0, then update cons and sin
Apply rotary embedding *inplace* to q k.
"""
self._update_cos_sin_cache(max_seqlen, position_ids, device=q.device, dtype=q.dtype)
cos, sin = F.embedding(position_ids, self._cos_cached), F.embedding(position_ids, self._sin_cached)
q = apply_rotary_emb_func(
q,
cos,
sin,
interleaved=self.interleaved,
inplace=True
)
k = apply_rotary_emb_func(
k,
cos,
sin,
interleaved=self.interleaved,
inplace=True
)
return q, k
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