/* Double-precision AdvSIMD inverse tan Copyright (C) 2023-2024 Free Software Foundation, Inc. This file is part of the GNU C Library. The GNU C Library is free software; you can redistribute it and/or modify it under the terms of the GNU Lesser General Public License as published by the Free Software Foundation; either version 2.1 of the License, or (at your option) any later version. The GNU C Library is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU Lesser General Public License for more details. You should have received a copy of the GNU Lesser General Public License along with the GNU C Library; if not, see . */ #include "v_math.h" #include "poly_advsimd_f64.h" static const struct data { float64x2_t pi_over_2; float64x2_t poly[20]; } data = { /* Coefficients of polynomial P such that atan(x)~x+x*P(x^2) on [2**-1022, 1.0]. */ .poly = { V2 (-0x1.5555555555555p-2), V2 (0x1.99999999996c1p-3), V2 (-0x1.2492492478f88p-3), V2 (0x1.c71c71bc3951cp-4), V2 (-0x1.745d160a7e368p-4), V2 (0x1.3b139b6a88ba1p-4), V2 (-0x1.11100ee084227p-4), V2 (0x1.e1d0f9696f63bp-5), V2 (-0x1.aebfe7b418581p-5), V2 (0x1.842dbe9b0d916p-5), V2 (-0x1.5d30140ae5e99p-5), V2 (0x1.338e31eb2fbbcp-5), V2 (-0x1.00e6eece7de8p-5), V2 (0x1.860897b29e5efp-6), V2 (-0x1.0051381722a59p-6), V2 (0x1.14e9dc19a4a4ep-7), V2 (-0x1.d0062b42fe3bfp-9), V2 (0x1.17739e210171ap-10), V2 (-0x1.ab24da7be7402p-13), V2 (0x1.358851160a528p-16), }, .pi_over_2 = V2 (0x1.921fb54442d18p+0), }; #define SignMask v_u64 (0x8000000000000000) #define TinyBound 0x3e10000000000000 /* asuint64(0x1p-30). */ #define BigBound 0x4340000000000000 /* asuint64(0x1p53). */ /* Fast implementation of vector atan. Based on atan(x) ~ shift + z + z^3 * P(z^2) with reduction to [0,1] using z=1/x and shift = pi/2. Maximum observed error is 2.27 ulps: _ZGVnN2v_atan (0x1.0005af27c23e9p+0) got 0x1.9225645bdd7c1p-1 want 0x1.9225645bdd7c3p-1. */ float64x2_t VPCS_ATTR V_NAME_D1 (atan) (float64x2_t x) { const struct data *d = ptr_barrier (&data); /* Small cases, infs and nans are supported by our approximation technique, but do not set fenv flags correctly. Only trigger special case if we need fenv. */ uint64x2_t ix = vreinterpretq_u64_f64 (x); uint64x2_t sign = vandq_u64 (ix, SignMask); #if WANT_SIMD_EXCEPT uint64x2_t ia12 = vandq_u64 (ix, v_u64 (0x7ff0000000000000)); uint64x2_t special = vcgtq_u64 (vsubq_u64 (ia12, v_u64 (TinyBound)), v_u64 (BigBound - TinyBound)); /* If any lane is special, fall back to the scalar routine for all lanes. */ if (__glibc_unlikely (v_any_u64 (special))) return v_call_f64 (atan, x, v_f64 (0), v_u64 (-1)); #endif /* Argument reduction: y := arctan(x) for x < 1 y := pi/2 + arctan(-1/x) for x > 1 Hence, use z=-1/a if x>=1, otherwise z=a. */ uint64x2_t red = vcagtq_f64 (x, v_f64 (1.0)); /* Avoid dependency in abs(x) in division (and comparison). */ float64x2_t z = vbslq_f64 (red, vdivq_f64 (v_f64 (1.0), x), x); float64x2_t shift = vreinterpretq_f64_u64 ( vandq_u64 (red, vreinterpretq_u64_f64 (d->pi_over_2))); /* Use absolute value only when needed (odd powers of z). */ float64x2_t az = vbslq_f64 ( SignMask, vreinterpretq_f64_u64 (vandq_u64 (SignMask, red)), z); /* Calculate the polynomial approximation. Use split Estrin scheme for P(z^2) with deg(P)=19. Use split instead of full scheme to avoid underflow in x^16. The order 19 polynomial P approximates (atan(sqrt(x))-sqrt(x))/x^(3/2). */ float64x2_t z2 = vmulq_f64 (z, z); float64x2_t x2 = vmulq_f64 (z2, z2); float64x2_t x4 = vmulq_f64 (x2, x2); float64x2_t x8 = vmulq_f64 (x4, x4); float64x2_t y = vfmaq_f64 (v_estrin_7_f64 (z2, x2, x4, d->poly), v_estrin_11_f64 (z2, x2, x4, x8, d->poly + 8), x8); /* Finalize. y = shift + z + z^3 * P(z^2). */ y = vfmaq_f64 (az, y, vmulq_f64 (z2, az)); y = vaddq_f64 (y, shift); /* y = atan(x) if x>0, -atan(-x) otherwise. */ y = vreinterpretq_f64_u64 (veorq_u64 (vreinterpretq_u64_f64 (y), sign)); return y; }