Custom Metal Kernels#
MLX supports writing custom Metal kernels through the Python and C++ APIs.
Simple Example#
Let’s write a custom kernel that computes exp
elementwise:
def exp_elementwise(a: mx.array):
source = """
uint elem = thread_position_in_grid.x;
T tmp = inp[elem];
out[elem] = metal::exp(tmp);
"""
kernel = mx.fast.metal_kernel(
name="myexp",
input_names=["inp"],
output_names=["out"],
source=source,
)
outputs = kernel(
inputs=[a],
template=[("T", mx.float32)],
grid=(a.size, 1, 1),
threadgroup=(256, 1, 1),
output_shapes=[a.shape],
output_dtypes=[a.dtype],
)
return outputs[0]
a = mx.random.normal(shape=(4, 16)).astype(mx.float16)
b = exp_elementwise(a)
assert mx.allclose(b, mx.exp(a))
Note
We are only required to pass the body of the Metal kernel in source
.
The full function signature will be generated using:
- The shapes/dtypes of
inputs
In the above,
a
is anmx.array
of typemx.float16
and we pass it with the keyinp
so we will addconst device float16_t* inp
to the signature.inp_shape
,inp_strides
andinp_ndim
are also added for convenience if they are present insource
.
- The shapes/dtypes of
- The list of
output_dtypes
In the above,
out
is anmx.array
of typemx.float16
so we adddevice float16_t* out
.
- The list of
- Template parameters passed using
template
In the above,
template=[("T", mx.float32)]
adds a template oftemplate <typename T>
to the function and instantiates the template withcustom_kernel_myexp_float<float>
. Template parameters can bemx.core.Dtype
,int
orbool
.
- Template parameters passed using
- Metal attributes used in
source
such as[[thread_position_in_grid]]
These will be added as function arguments. All the attributes defined in Table 5.8 of the Metal Shading Language Specification are supported.
- Metal attributes used in
Putting this all together, the generated function signature for myexp
is as follows:
template <typename T>
[[kernel]] void custom_kernel_myexp_float(
const device float16_t* inp [[buffer(0)]],
device float16_t* out [[buffer(1)]],
uint3 thread_position_in_grid [[thread_position_in_grid]]) {
uint elem = thread_position_in_grid.x;
T tmp = inp[elem];
out[elem] = metal::exp(tmp);
}
template [[host_name("custom_kernel_myexp_float")]] [[kernel]] decltype(custom_kernel_myexp_float<float>) custom_kernel_myexp_float<float>;
Note: grid
and threadgroup
are parameters to the Metal dispatchThreads function.
This means we will launch mx.prod(grid)
threads, subdivided into threadgroup
size threadgroups.
For optimal performance, each thread group dimension should be less than or equal to the corresponding grid dimension.
Passing verbose=True
to mx.fast.metal_kernel.__call__
will print the generated code for debugging purposes.
Using Shape/Strides#
mx.fast.metal_kernel
supports an argument ensure_row_contiguous
which is True
by default.
This will copy the mx.array
inputs if needed before the kernel is launched to ensure that the memory layout is row contiguous.
Generally this makes writing the kernel easier, since we don’t have to worry about gaps or the ordering of the dims
when indexing.
If we want to avoid this copy, metal_kernel
automatically passes a_shape
, a_strides
and a_ndim
for each
input array a
if any are present in source
.
We can then use MLX’s built in indexing utils to fetch the right elements for each thread.
Let’s convert myexp
above to support arbitrarily strided arrays without relying on a copy from ensure_row_contiguous
:
def exp_elementwise(a: mx.array):
source = """
uint elem = thread_position_in_grid.x;
// Utils from `mlx/backend/metal/kernels/utils.h` are automatically included
uint loc = elem_to_loc(elem, inp_shape, inp_strides, inp_ndim);
T tmp = inp[loc];
// Output arrays are always row contiguous
out[elem] = metal::exp(tmp);
"""
kernel = mx.fast.metal_kernel(
name="myexp_strided",
input_names=["inp"],
output_names=["out"],
source=source
)
outputs = kernel(
inputs=[a],
template=[("T", mx.float32)],
grid=(a.size, 1, 1),
threadgroup=(256, 1, 1),
output_shapes=[a.shape],
output_dtypes=[a.dtype],
ensure_row_contiguous=False,
)
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:
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:
@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:
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’satomic
features to simultaneously update thex_grad
andgrid_grad
arrays from multiple threadgroups. See section 6.15 of the Metal Shading Language Specification for more details.
We can then implement the backwards pass as follows:
@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