1 /* Single-precision AdvSIMD expm1
3 Copyright (C) 2023 Free Software Foundation, Inc.
4 This file is part of the GNU C Library.
6 The GNU C Library is free software; you can redistribute it and/or
7 modify it under the terms of the GNU Lesser General Public
8 License as published by the Free Software Foundation; either
9 version 2.1 of the License, or (at your option) any later version.
11 The GNU C Library is distributed in the hope that it will be useful,
12 but WITHOUT ANY WARRANTY; without even the implied warranty of
13 MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU
14 Lesser General Public License for more details.
16 You should have received a copy of the GNU Lesser General Public
17 License along with the GNU C Library; if not, see
18 <https://www.gnu.org/licenses/>. */
21 #include "poly_advsimd_f32.h"
23 static const struct data
26 float32x4_t invln2
, ln2_lo
, ln2_hi
, shift
;
27 int32x4_t exponent_bias
;
31 float32x4_t oflow_bound
;
34 /* Generated using fpminimax with degree=5 in [-log(2)/2, log(2)/2]. */
35 .poly
= { V4 (0x1.fffffep
-2), V4 (0x1.5554aep
-3), V4 (0x1.555736p
-5),
36 V4 (0x1.12287cp
-7), V4 (0x1.6b55a2p
-10) },
37 .invln2
= V4 (0x1.715476p
+0f
),
38 .ln2_hi
= V4 (0x1.62e4p
-1f
),
39 .ln2_lo
= V4 (0x1.7f7d1cp
-20f
),
40 .shift
= V4 (0x1.8p23f
),
41 .exponent_bias
= V4 (0x3f800000),
43 /* Value above which expm1f(x) should overflow. Absolute value of the
44 underflow bound is greater than this, so it catches both cases - there is
45 a small window where fallbacks are triggered unnecessarily. */
46 .oflow_bound
= V4 (0x1.5ebc4p
+6),
48 /* asuint(oflow_bound) - asuint(0x1p-23), shifted left by 1 for absolute
50 .thresh
= V4 (0x1d5ebc40),
54 /* asuint(0x1p-23), shifted by 1 for abs compare. */
55 #define TinyBound v_u32 (0x34000000 << 1)
57 static float32x4_t VPCS_ATTR NOINLINE
58 special_case (float32x4_t x
, float32x4_t y
, uint32x4_t special
)
60 return v_call_f32 (expm1f
, x
, y
, special
);
63 /* Single-precision vector exp(x) - 1 function.
64 The maximum error is 1.51 ULP:
65 _ZGVnN4v_expm1f (0x1.8baa96p-2) got 0x1.e2fb9p-2
66 want 0x1.e2fb94p-2. */
67 float32x4_t VPCS_ATTR
V_NAME_F1 (expm1
) (float32x4_t x
)
69 const struct data
*d
= ptr_barrier (&data
);
70 uint32x4_t ix
= vreinterpretq_u32_f32 (x
);
73 /* If fp exceptions are to be triggered correctly, fall back to scalar for
74 |x| < 2^-23, |x| > oflow_bound, Inf & NaN. Add ix to itself for
75 shift-left by 1, and compare with thresh which was left-shifted offline -
76 this is effectively an absolute compare. */
78 = vcgeq_u32 (vsubq_u32 (vaddq_u32 (ix
, ix
), TinyBound
), d
->thresh
);
79 if (__glibc_unlikely (v_any_u32 (special
)))
80 x
= v_zerofy_f32 (x
, special
);
82 /* Handles very large values (+ve and -ve), +/-NaN, +/-Inf. */
83 uint32x4_t special
= vceqzq_u32 (vcaltq_f32 (x
, d
->oflow_bound
));
86 /* Reduce argument to smaller range:
87 Let i = round(x / ln2)
88 and f = x - i * ln2, then f is in [-ln2/2, ln2/2].
89 exp(x) - 1 = 2^i * (expm1(f) + 1) - 1
90 where 2^i is exact because i is an integer. */
91 float32x4_t j
= vsubq_f32 (vfmaq_f32 (d
->shift
, d
->invln2
, x
), d
->shift
);
92 int32x4_t i
= vcvtq_s32_f32 (j
);
93 float32x4_t f
= vfmsq_f32 (x
, j
, d
->ln2_hi
);
94 f
= vfmsq_f32 (f
, j
, d
->ln2_lo
);
96 /* Approximate expm1(f) using polynomial.
97 Taylor expansion for expm1(x) has the form:
98 x + ax^2 + bx^3 + cx^4 ....
99 So we calculate the polynomial P(f) = a + bf + cf^2 + ...
100 and assemble the approximation expm1(f) ~= f + f^2 * P(f). */
101 float32x4_t p
= v_horner_4_f32 (f
, d
->poly
);
102 p
= vfmaq_f32 (f
, vmulq_f32 (f
, f
), p
);
104 /* Assemble the result.
105 expm1(x) ~= 2^i * (p + 1) - 1
107 int32x4_t u
= vaddq_s32 (vshlq_n_s32 (i
, 23), d
->exponent_bias
);
108 float32x4_t t
= vreinterpretq_f32_s32 (u
);
110 if (__glibc_unlikely (v_any_u32 (special
)))
111 return special_case (vreinterpretq_f32_u32 (ix
),
112 vfmaq_f32 (vsubq_f32 (t
, v_f32 (1.0f
)), p
, t
),
115 /* expm1(x) ~= p * t + (t - 1). */
116 return vfmaq_f32 (vsubq_f32 (t
, v_f32 (1.0f
)), p
, t
);