This commit is contained in:
Awni Hannun
2024-09-17 12:06:14 -07:00
committed by CircleCI Docs
parent 27e07888b0
commit 6a6ffb598d
739 changed files with 28107 additions and 8524 deletions

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@@ -19,17 +19,19 @@ Let's write a custom kernel that computes ``exp`` elementwise:
kernel = mx.fast.metal_kernel(
name="myexp",
input_names=["inp"],
output_names=["out"],
source=source,
)
outputs = kernel(
inputs={"inp": a},
template={"T": mx.float32},
inputs=[a],
template=[("T", mx.float32)],
grid=(a.size, 1, 1),
threadgroup=(256, 1, 1),
output_shapes={"out": a.shape},
output_dtypes={"out": a.dtype},
output_shapes=[a.shape],
output_dtypes=[a.dtype],
)
return outputs["out"]
return outputs[0]
a = mx.random.normal(shape=(4, 16)).astype(mx.float16)
b = exp_elementwise(a)
@@ -40,15 +42,16 @@ Let's write a custom kernel that computes ``exp`` elementwise:
The full function signature will be generated using:
* The keys and shapes/dtypes of ``inputs``
* The shapes/dtypes of ``inputs``
In the above, ``a`` is an ``mx.array`` of type ``mx.float16`` and we pass it with the key ``inp``
so we will add ``const device float16_t* inp`` to the signature.
``inp_shape``, ``inp_strides`` and ``inp_ndim`` are also added for convenience.
* The keys and values of ``output_shapes`` and ``output_dtypes``
``inp_shape``, ``inp_strides`` and ``inp_ndim`` are also added for convenience if they are present
in ``source``.
* The list of ``output_dtypes``
In the above, ``out`` is an ``mx.array`` of type ``mx.float16``
so we add ``device float16_t* out``.
* Template parameters passed using ``template``
In the above, ``template={"T": mx.float32}`` adds a template of ``template <typename T>`` to the function
In the above, ``template=[("T", mx.float32)]`` adds a template of ``template <typename T>`` to the function
and instantiates the template with ``custom_kernel_myexp_float<float>``.
Template parameters can be ``mx.core.Dtype``, ``int`` or ``bool``.
* Metal attributes used in ``source`` such as ``[[thread_position_in_grid]]``
@@ -73,7 +76,7 @@ Putting this all together, the generated function signature for ``myexp`` is as
template [[host_name("custom_kernel_myexp_float")]] [[kernel]] decltype(custom_kernel_myexp_float<float>) custom_kernel_myexp_float<float>;
You can print the generated code for a ``mx.fast.metal_kernel`` by passing ``verbose=True`` when you call it.
Passing ``verbose=True`` to ``mx.fast.metal_kernel.__call__`` will print the generated code for debugging purposes.
Using Shape/Strides
-------------------
@@ -103,21 +106,316 @@ Let's convert ``myexp`` above to support arbitrarily strided arrays without rely
kernel = mx.fast.metal_kernel(
name="myexp_strided",
input_names=["inp"],
output_names=["out"],
source=source
)
outputs = kernel(
inputs={"inp": a},
template={"T": mx.float32},
inputs=[a],
template=[("T", mx.float32)],
grid=(a.size, 1, 1),
threadgroup=(256, 1, 1),
output_shapes={"out": a.shape},
output_dtypes={"out": a.dtype},
output_shapes=[a.shape],
output_dtypes=[a.dtype],
ensure_row_contiguous=False,
)
return outputs["out"]
return outputs[0]
a = mx.random.normal(shape=(4, 16)).astype(mx.float16)
# make non-contiguous
a = a[::2]
b = exp_elementwise(a)
assert mx.allclose(b, mx.exp(a))
Complex Example
-----------------------------
Let's implement a more complex example: ``grid_sample`` in ``"bilinear"`` mode.
We'll start with the following MLX implementation using standard ops:
.. code-block:: python
def grid_sample_ref(x, grid):
N, H_in, W_in, _ = x.shape
ix = ((grid[..., 0] + 1) * W_in - 1) / 2
iy = ((grid[..., 1] + 1) * H_in - 1) / 2
ix_nw = mx.floor(ix).astype(mx.int32)
iy_nw = mx.floor(iy).astype(mx.int32)
ix_ne = ix_nw + 1
iy_ne = iy_nw
ix_sw = ix_nw
iy_sw = iy_nw + 1
ix_se = ix_nw + 1
iy_se = iy_nw + 1
nw = (ix_se - ix) * (iy_se - iy)
ne = (ix - ix_sw) * (iy_sw - iy)
sw = (ix_ne - ix) * (iy - iy_ne)
se = (ix - ix_nw) * (iy - iy_nw)
I_nw = x[mx.arange(N)[:, None, None], iy_nw, ix_nw, :]
I_ne = x[mx.arange(N)[:, None, None], iy_ne, ix_ne, :]
I_sw = x[mx.arange(N)[:, None, None], iy_sw, ix_sw, :]
I_se = x[mx.arange(N)[:, None, None], iy_se, ix_se, :]
mask_nw = (iy_nw >= 0) & (iy_nw <= H_in - 1) & (ix_nw >= 0) & (ix_nw <= W_in - 1)
mask_ne = (iy_ne >= 0) & (iy_ne <= H_in - 1) & (ix_ne >= 0) & (ix_ne <= W_in - 1)
mask_sw = (iy_sw >= 0) & (iy_sw <= H_in - 1) & (ix_sw >= 0) & (ix_sw <= W_in - 1)
mask_se = (iy_se >= 0) & (iy_se <= H_in - 1) & (ix_se >= 0) & (ix_se <= W_in - 1)
I_nw *= mask_nw[..., None]
I_ne *= mask_ne[..., None]
I_sw *= mask_sw[..., None]
I_se *= mask_se[..., None]
output = nw[..., None] * I_nw + ne[..., None] * I_ne + sw[..., None] * I_sw + se[..., None] * I_se
return output
Now let's use ``mx.custom_function`` together with ``mx.fast.metal_kernel``
to write a fast GPU kernel for both the forward and backward passes.
First we'll implement the forward pass as a fused kernel:
.. code-block:: python
@mx.custom_function
def grid_sample(x, grid):
assert x.ndim == 4, "`x` must be 4D."
assert grid.ndim == 4, "`grid` must be 4D."
B, _, _, C = x.shape
_, gN, gM, D = grid.shape
out_shape = (B, gN, gM, C)
assert D == 2, "Last dim of `grid` must be size 2."
source = """
uint elem = thread_position_in_grid.x;
int H = x_shape[1];
int W = x_shape[2];
int C = x_shape[3];
int gH = grid_shape[1];
int gW = grid_shape[2];
int w_stride = C;
int h_stride = W * w_stride;
int b_stride = H * h_stride;
uint grid_idx = elem / C * 2;
float ix = ((grid[grid_idx] + 1) * W - 1) / 2;
float iy = ((grid[grid_idx + 1] + 1) * H - 1) / 2;
int ix_nw = floor(ix);
int iy_nw = floor(iy);
int ix_ne = ix_nw + 1;
int iy_ne = iy_nw;
int ix_sw = ix_nw;
int iy_sw = iy_nw + 1;
int ix_se = ix_nw + 1;
int iy_se = iy_nw + 1;
T nw = (ix_se - ix) * (iy_se - iy);
T ne = (ix - ix_sw) * (iy_sw - iy);
T sw = (ix_ne - ix) * (iy - iy_ne);
T se = (ix - ix_nw) * (iy - iy_nw);
int batch_idx = elem / C / gH / gW * b_stride;
int channel_idx = elem % C;
int base_idx = batch_idx + channel_idx;
T I_nw = x[base_idx + iy_nw * h_stride + ix_nw * w_stride];
T I_ne = x[base_idx + iy_ne * h_stride + ix_ne * w_stride];
T I_sw = x[base_idx + iy_sw * h_stride + ix_sw * w_stride];
T I_se = x[base_idx + iy_se * h_stride + ix_se * w_stride];
I_nw = iy_nw >= 0 && iy_nw <= H - 1 && ix_nw >= 0 && ix_nw <= W - 1 ? I_nw : 0;
I_ne = iy_ne >= 0 && iy_ne <= H - 1 && ix_ne >= 0 && ix_ne <= W - 1 ? I_ne : 0;
I_sw = iy_sw >= 0 && iy_sw <= H - 1 && ix_sw >= 0 && ix_sw <= W - 1 ? I_sw : 0;
I_se = iy_se >= 0 && iy_se <= H - 1 && ix_se >= 0 && ix_se <= W - 1 ? I_se : 0;
out[elem] = nw * I_nw + ne * I_ne + sw * I_sw + se * I_se;
"""
kernel = mx.fast.metal_kernel(
name="grid_sample",
input_names=["x", "grid"],
output_names=["out"],
source=source,
)
outputs = kernel(
inputs=[x, grid],
template=[("T", x.dtype)],
output_shapes=[out_shape],
output_dtypes=[x.dtype],
grid=(np.prod(out_shape), 1, 1),
threadgroup=(256, 1, 1),
)
return outputs[0]
For a reasonably sized input such as:
.. code-block:: python
x.shape = (8, 1024, 1024, 64)
grid.shape = (8, 256, 256, 2)
On an M1 Max, we see a big performance improvement:
``55.7ms -> 6.7ms => 8x speed up``
Grid Sample VJP
---------------
Since we decorated ``grid_sample`` with ``mx.custom_function``, we can now define
its custom vjp transform so MLX can differentiate it.
The backwards pass requires atomically updating ``x_grad``/``grid_grad`` and so
requires a few extra ``mx.fast.metal_kernel`` features:
* ``init_value=0``
Initialize all of the kernel's outputs to this value before it runs. This allows us to update only part of the output arrays with the kernel.
* ``atomic_outputs=True``
Designate all of the kernel outputs as ``atomic`` in the function signature.
This means we can use Metal's ``atomic`` features to simultaneously update the ``x_grad`` and ``grid_grad`` arrays from multiple threadgroups.
See section 6.15 of the `Metal Shading Language Specification <https://developer.apple.com/metal/Metal-Shading-Language-Specification.pdf>`_ for more details.
We can then implement the backwards pass as follows:
.. code-block:: python
@grid_sample.vjp
def grid_sample_vjp(primals, cotangent, _):
x, grid = primals
B, _, _, C = x.shape
_, gN, gM, D = grid.shape
assert D == 2, "Last dim of `grid` must be size 2."
source = """
uint elem = thread_position_in_grid.x;
int H = x_shape[1];
int W = x_shape[2];
int C = x_shape[3];
// Pad C to the nearest larger simdgroup size multiple
int C_padded = ceildiv(C, threads_per_simdgroup) * threads_per_simdgroup;
int gH = grid_shape[1];
int gW = grid_shape[2];
int w_stride = C;
int h_stride = W * w_stride;
int b_stride = H * h_stride;
uint grid_idx = elem / C_padded * 2;
float ix = ((grid[grid_idx] + 1) * W - 1) / 2;
float iy = ((grid[grid_idx + 1] + 1) * H - 1) / 2;
int ix_nw = floor(ix);
int iy_nw = floor(iy);
int ix_ne = ix_nw + 1;
int iy_ne = iy_nw;
int ix_sw = ix_nw;
int iy_sw = iy_nw + 1;
int ix_se = ix_nw + 1;
int iy_se = iy_nw + 1;
T nw = (ix_se - ix) * (iy_se - iy);
T ne = (ix - ix_sw) * (iy_sw - iy);
T sw = (ix_ne - ix) * (iy - iy_ne);
T se = (ix - ix_nw) * (iy - iy_nw);
int batch_idx = elem / C_padded / gH / gW * b_stride;
int channel_idx = elem % C_padded;
int base_idx = batch_idx + channel_idx;
T gix = T(0);
T giy = T(0);
if (channel_idx < C) {
int cot_index = elem / C_padded * C + channel_idx;
T cot = cotangent[cot_index];
if (iy_nw >= 0 && iy_nw <= H - 1 && ix_nw >= 0 && ix_nw <= W - 1) {
int offset = base_idx + iy_nw * h_stride + ix_nw * w_stride;
atomic_fetch_add_explicit(&x_grad[offset], nw * cot, memory_order_relaxed);
T I_nw = x[offset];
gix -= I_nw * (iy_se - iy) * cot;
giy -= I_nw * (ix_se - ix) * cot;
}
if (iy_ne >= 0 && iy_ne <= H - 1 && ix_ne >= 0 && ix_ne <= W - 1) {
int offset = base_idx + iy_ne * h_stride + ix_ne * w_stride;
atomic_fetch_add_explicit(&x_grad[offset], ne * cot, memory_order_relaxed);
T I_ne = x[offset];
gix += I_ne * (iy_sw - iy) * cot;
giy -= I_ne * (ix - ix_sw) * cot;
}
if (iy_sw >= 0 && iy_sw <= H - 1 && ix_sw >= 0 && ix_sw <= W - 1) {
int offset = base_idx + iy_sw * h_stride + ix_sw * w_stride;
atomic_fetch_add_explicit(&x_grad[offset], sw * cot, memory_order_relaxed);
T I_sw = x[offset];
gix -= I_sw * (iy - iy_ne) * cot;
giy += I_sw * (ix_ne - ix) * cot;
}
if (iy_se >= 0 && iy_se <= H - 1 && ix_se >= 0 && ix_se <= W - 1) {
int offset = base_idx + iy_se * h_stride + ix_se * w_stride;
atomic_fetch_add_explicit(&x_grad[offset], se * cot, memory_order_relaxed);
T I_se = x[offset];
gix += I_se * (iy - iy_nw) * cot;
giy += I_se * (ix - ix_nw) * cot;
}
}
T gix_mult = W / 2;
T giy_mult = H / 2;
// Reduce across each simdgroup first.
// This is much faster than relying purely on atomics.
gix = simd_sum(gix);
giy = simd_sum(giy);
if (thread_index_in_simdgroup == 0) {
atomic_fetch_add_explicit(&grid_grad[grid_idx], gix * gix_mult, memory_order_relaxed);
atomic_fetch_add_explicit(&grid_grad[grid_idx + 1], giy * giy_mult, memory_order_relaxed);
}
"""
kernel = mx.fast.metal_kernel(
name="grid_sample_grad",
input_names=["x", "grid", "cotangent"],
output_names=["x_grad", "grid_grad"],
source=source,
atomic_outputs=True,
)
# pad the output channels to simd group size
# so that our `simd_sum`s don't overlap.
simdgroup_size = 32
C_padded = (C + simdgroup_size - 1) // simdgroup_size * simdgroup_size
grid_size = B * gN * gM * C_padded
outputs = kernel(
inputs=[x, grid, cotangent],
template=[("T", x.dtype)],
output_shapes=[x.shape, grid.shape],
output_dtypes=[x.dtype, x.dtype],
grid=(grid_size, 1, 1),
threadgroup=(256, 1, 1),
init_value=0,
)
return outputs[0], outputs[1]
There's an even larger speed up for the vjp:
``676.4ms -> 16.7ms => 40x speed up``