SSE2 Sigmoid evaluation stubs using Newton-Raphson reciprocal
PiperOrigin-RevId: 337438275
diff --git a/src/math/sigmoid-sse2-rr2-lut64-p2-nr2.c b/src/math/sigmoid-sse2-rr2-lut64-p2-nr2.c
new file mode 100644
index 0000000..99c14d9
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+++ b/src/math/sigmoid-sse2-rr2-lut64-p2-nr2.c
@@ -0,0 +1,142 @@
+// Copyright 2020 Google LLC
+//
+// This source code is licensed under the BSD-style license found in the
+// LICENSE file in the root directory of this source tree.
+
+#include <assert.h>
+#include <stddef.h>
+
+#include <emmintrin.h>
+
+#include <xnnpack/common.h>
+#include <xnnpack/math-stubs.h>
+
+
+// Table of exp2(k / 64) values decremented (as integer) by (k << 17), k = 0..63
+extern XNN_INTERNAL const float xnn_table_exp2minus_k_over_64[64];
+
+void xnn_math_f32_sigmoid__sse2_rr2_lut64_p2_nr2(
+ size_t n,
+ const float* input,
+ float* output)
+{
+ assert(n % (4 * sizeof(float)) == 0);
+
+ // Floating-point mask with only the sign bit set
+ const __m128 vsign_mask = _mm_set1_ps(-0.0f);
+ // Large number such that ulp(magic bias) == exp2(-6)
+ const __m128 vmagic_bias = _mm_set1_ps(0x1.800000p17f);
+ const __m128 vlog2e = _mm_set1_ps(0x1.715476p0f);
+ // Mask for the lowest 6 bits
+ const __m128i vindex_mask = _mm_set1_epi32(INT32_C(0x3F));
+ // Last 13 bits are zeroes
+ const __m128 vminus_ln2_hi = _mm_set1_ps(-0x1.630000p-1f);
+ const __m128 vminus_ln2_lo = _mm_set1_ps(0x1.BD0106p-13f);
+ // Coefficient of polynomial approximation of exp(t) ~ 1 + t * (1 + t * c2) on [-log(2)/128, log(2)/128]
+ const __m128 vc2 = _mm_set1_ps(0x1.FFFF0Ap-2f);
+ const __m128 vone = _mm_set1_ps(1.0f);
+ const __m128 vminus_two = _mm_set1_ps(-2.0f);
+ // The smallest x for which sigmoidf(x) is normalized.
+ // This number is also the smallest x for which expf(x) is normalized.
+ const __m128 vdenorm_cutoff = _mm_set1_ps(-0x1.5D589Ep+6f);
+
+ for (; n != 0; n -= 4 * sizeof(float)) {
+ const __m128 vx = _mm_load_ps(input);
+ input += 4;
+
+ // General structure of the algorithm:
+ //
+ // / exp(x) / (1 + exp(x)) if x <= 0
+ // f[x] :=
+ // \ 1 - f[-x] if x >= 0
+ //
+ // First we compute f[z] := exp(z) / (1 + exp(z)) where z = -abs(x), then replace result with 1 - f[z] if x >= 0.
+ const __m128 vz = _mm_or_ps(vx, vsign_mask);
+
+ // Compute reduced argument n := round(z / log(2), 6).
+ // We do it by adding a large number (magic bias), which cause rounding of the result to 6 fractional bits, then
+ // subtracing the large number back. The trick with adding large number is valid only within certain bounds
+ // (|z / log(2)| <= 2**16, i.e. |z| <= 0x1.62E43p+15 = 45426.09375), but that is acceptable, because inputs x
+ // outside of [-87.336544, 17.328678] (i.e. z outsize [87.336544, 0]) underflow or saturate sigmoidf(x). We fixup
+ // the result for such inputs at the very end of the algorithm.
+ __m128 vn = _mm_add_ps(_mm_mul_ps(vz, vlog2e), vmagic_bias);
+
+ // Create a floating-point number s (scale) such that s := 2**n for such inputs that sigmoidf(z) is normalized,
+ // i.e. -87.33642 <= z <= 0. As n has 6 fractional bits, we split s == 2**n = 2**int(n) * 2**frac(n). We create s
+ // in two steps:
+ // 1. Fetch 2**frac(n) from the table using the 6 low bits of n, as integer. Note that the fetched values are in
+ // the [1.0, 2.0) range, i.e. their floating-point exponent is 0.
+ // 2. Adjust fecthed value by addition of int(n) to its floating-point exponent. The result is always a normalized
+ // number, because for -87.33642 <= z <= 0 (inputs for which sigmoidf(z) is normalized) we have
+ // -126 <= int(n) <= 0, and thus the adjusted exponent is not lower than -126.
+ //
+ // Shift bits 6:14 into 23:31 (position of floating-point exponent).
+ const __m128i ve = _mm_slli_epi32(_mm_castps_si128(vn), 17);
+
+ // Use bits 0:6 bits of n, as integer, as an index for table lookup of l := 2**frac(n).
+ const __m128i vidx = _mm_slli_epi32(_mm_and_si128(_mm_castps_si128(vn), vindex_mask), 2);
+#if XNN_ARCH_X86_64
+ const uint64_t vidx_lo = (uint64_t) _mm_cvtsi128_si64(vidx);
+ const uint64_t vidx_hi = (uint64_t) _mm_cvtsi128_si64(_mm_unpackhi_epi64(vidx, vidx));
+ const __m128i vl0 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + (uint32_t) vidx_lo)));
+ const __m128i vl2 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + (uint32_t) vidx_hi)));
+ const __m128i vl1 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + (uint32_t) (vidx_lo >> 32))));
+ const __m128i vl3 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + (uint32_t) (vidx_hi >> 32))));
+#else
+ const uint32_t vidx0 = (uint32_t) _mm_cvtsi128_si32(vidx);
+ const uint32_t vidx1 = (uint32_t) _mm_extract_epi16(vidx, 2);
+ const uint32_t vidx2 = (uint32_t) _mm_extract_epi16(vidx, 4);
+ const uint32_t vidx3 = (uint32_t) _mm_extract_epi16(vidx, 6);
+ const __m128i vl0 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + vidx0)));
+ const __m128i vl2 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + vidx2)));
+ const __m128i vl1 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + vidx1)));
+ const __m128i vl3 = _mm_cvtsi32_si128(*((const int*) ((uintptr_t) xnn_table_exp2minus_k_over_64 + vidx3)));
+#endif
+ const __m128i vl = _mm_unpacklo_epi64(_mm_unpacklo_epi32(vl0, vl1), _mm_unpacklo_epi32(vl2, vl3));
+ // Adjust exponent of the value l fetched from the table to get the final s value.
+ const __m128 vs = _mm_castsi128_ps(_mm_add_epi32(vl, ve));
+
+ // Subtract the large number back to get the final n := round(z / log(2), 6) as a floating-point number.
+ vn = _mm_sub_ps(vn, vmagic_bias);
+
+ // Compute reduced argument t := z - n * log(2).
+ // Use Cody-Waite range reduction method (note two constants to represent log(2)) to improve accuracy.
+ __m128 vt = _mm_add_ps(_mm_mul_ps(vn, vminus_ln2_hi), vz);
+ vt = _mm_add_ps(_mm_mul_ps(vn, vminus_ln2_lo), vt);
+
+ // Compute degree-2 polynomial approximation for exp(t) on [-log(2)/128, log(2)/128].
+ // P(t) = 1 + t * (1 + t * c2) = 1 + (t + t * (t * c2)) = 1 + p
+ __m128 vp = _mm_mul_ps(vt, vc2);
+ vp = _mm_add_ps(vt, _mm_mul_ps(vp, vt));
+
+ // Reconstruct the exp(z) value:
+ // e = s * (1 + t * (1 + t * c2))
+ // = s * (1 + p)
+ // = s + s * p
+ const __m128 vy = _mm_add_ps(vs, _mm_mul_ps(vs, vp));
+
+ // Denominator of the sigmoid fraction: 1.0 + exp(z)
+ const __m128 vd = _mm_add_ps(vy, vone);
+
+ // Use Newton-Raphson method (2 iterations) to compute reciprocal of denominator.
+ // Note: 1 < d <= 2, because z >= 0.0 and 0 < exp(-z) <= 1.0.
+ // Thus the reciprocal of the denominator never overflows.
+ __m128 vr = _mm_rcp_ps(vd);
+ vr = _mm_mul_ps(vr, _mm_add_ps(_mm_mul_ps(vr, vd), vminus_two));
+ vr = _mm_mul_ps(vr, _mm_sub_ps(vminus_two, _mm_mul_ps(vr, vd)));
+
+ // Reconstruct sigmoid(z) = exp(z) / (1.0 + exp(z))
+ __m128 vf = _mm_mul_ps(vy, vr);
+
+ // For inputs below denormal cutoff, replace output with +0.0f.
+ // Note that for NaN inputs, comparison result is false, and outputs are left unchanged.
+ vf = _mm_andnot_ps(_mm_cmplt_ps(vz, vdenorm_cutoff), vf);
+
+ // Reconstruct sigmoid(x) = x < 0 ? sigmoid(z) : 1.0 - sigmoid(z)
+ const __m128 vm = _mm_castsi128_ps(_mm_cmpgt_epi32(_mm_setzero_si128(), _mm_castps_si128(vx)));
+ vf = _mm_or_ps(_mm_and_ps(vm, vf), _mm_andnot_ps(vm, _mm_sub_ps(vone, vf)));
+
+ _mm_store_ps(output, vf);
+ output += 4;
+ }
+}