glibc/sysdeps/ieee754/ldbl-128ibm/e_acosl.c
Wilco Dijkstra 220622dde5 Add libm_alias_finite for _finite symbols
This patch adds a new macro, libm_alias_finite, to define all _finite
symbol.  It sets all _finite symbol as compat symbol based on its first
version (obtained from the definition at built generated first-versions.h).

The <fn>f128_finite symbols were introduced in GLIBC 2.26 and so need
special treatment in code that is shared between long double and float128.
It is done by adding a list, similar to internal symbol redifinition,
on sysdeps/ieee754/float128/float128_private.h.

Alpha also needs some tricky changes to ensure we still emit 2 compat
symbols for sqrt(f).

Passes buildmanyglibc.

Co-authored-by: Adhemerval Zanella <adhemerval.zanella@linaro.org>
Reviewed-by: Siddhesh Poyarekar <siddhesh@sourceware.org>
2020-01-03 10:02:04 -03:00

318 lines
9.4 KiB
C

/*
* ====================================================
* Copyright (C) 1993 by Sun Microsystems, Inc. All rights reserved.
*
* Developed at SunPro, a Sun Microsystems, Inc. business.
* Permission to use, copy, modify, and distribute this
* software is freely granted, provided that this notice
* is preserved.
* ====================================================
*/
/*
Long double expansions are
Copyright (C) 2001 Stephen L. Moshier <moshier@na-net.ornl.gov>
and are incorporated herein by permission of the author. The author
reserves the right to distribute this material elsewhere under different
copying permissions. These modifications are distributed here under
the following terms:
This 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.
This 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 this library; if not, see
<https://www.gnu.org/licenses/>. */
/* __ieee754_acosl(x)
* Method :
* acos(x) = pi/2 - asin(x)
* acos(-x) = pi/2 + asin(x)
* For |x| <= 0.375
* acos(x) = pi/2 - asin(x)
* Between .375 and .5 the approximation is
* acos(0.4375 + x) = acos(0.4375) + x P(x) / Q(x)
* Between .5 and .625 the approximation is
* acos(0.5625 + x) = acos(0.5625) + x rS(x) / sS(x)
* For x > 0.625,
* acos(x) = 2 asin(sqrt((1-x)/2))
* computed with an extended precision square root in the leading term.
* For x < -0.625
* acos(x) = pi - 2 asin(sqrt((1-|x|)/2))
*
* Special cases:
* if x is NaN, return x itself;
* if |x|>1, return NaN with invalid signal.
*
* Functions needed: sqrtl.
*/
#include <math.h>
#include <math_private.h>
#include <libm-alias-finite.h>
static const long double
one = 1.0L,
pio2_hi = 1.5707963267948966192313216916397514420986L,
pio2_lo = 4.3359050650618905123985220130216759843812E-35L,
/* acos(0.5625 + x) = acos(0.5625) + x rS(x) / sS(x)
-0.0625 <= x <= 0.0625
peak relative error 3.3e-35 */
rS0 = 5.619049346208901520945464704848780243887E0L,
rS1 = -4.460504162777731472539175700169871920352E1L,
rS2 = 1.317669505315409261479577040530751477488E2L,
rS3 = -1.626532582423661989632442410808596009227E2L,
rS4 = 3.144806644195158614904369445440583873264E1L,
rS5 = 9.806674443470740708765165604769099559553E1L,
rS6 = -5.708468492052010816555762842394927806920E1L,
rS7 = -1.396540499232262112248553357962639431922E1L,
rS8 = 1.126243289311910363001762058295832610344E1L,
rS9 = 4.956179821329901954211277873774472383512E-1L,
rS10 = -3.313227657082367169241333738391762525780E-1L,
sS0 = -4.645814742084009935700221277307007679325E0L,
sS1 = 3.879074822457694323970438316317961918430E1L,
sS2 = -1.221986588013474694623973554726201001066E2L,
sS3 = 1.658821150347718105012079876756201905822E2L,
sS4 = -4.804379630977558197953176474426239748977E1L,
sS5 = -1.004296417397316948114344573811562952793E2L,
sS6 = 7.530281592861320234941101403870010111138E1L,
sS7 = 1.270735595411673647119592092304357226607E1L,
sS8 = -1.815144839646376500705105967064792930282E1L,
sS9 = -7.821597334910963922204235247786840828217E-2L,
/* 1.000000000000000000000000000000000000000E0 */
acosr5625 = 9.7338991014954640492751132535550279812151E-1L,
pimacosr5625 = 2.1682027434402468335351320579240000860757E0L,
/* acos(0.4375 + x) = acos(0.4375) + x rS(x) / sS(x)
-0.0625 <= x <= 0.0625
peak relative error 2.1e-35 */
P0 = 2.177690192235413635229046633751390484892E0L,
P1 = -2.848698225706605746657192566166142909573E1L,
P2 = 1.040076477655245590871244795403659880304E2L,
P3 = -1.400087608918906358323551402881238180553E2L,
P4 = 2.221047917671449176051896400503615543757E1L,
P5 = 9.643714856395587663736110523917499638702E1L,
P6 = -5.158406639829833829027457284942389079196E1L,
P7 = -1.578651828337585944715290382181219741813E1L,
P8 = 1.093632715903802870546857764647931045906E1L,
P9 = 5.448925479898460003048760932274085300103E-1L,
P10 = -3.315886001095605268470690485170092986337E-1L,
Q0 = -1.958219113487162405143608843774587557016E0L,
Q1 = 2.614577866876185080678907676023269360520E1L,
Q2 = -9.990858606464150981009763389881793660938E1L,
Q3 = 1.443958741356995763628660823395334281596E2L,
Q4 = -3.206441012484232867657763518369723873129E1L,
Q5 = -1.048560885341833443564920145642588991492E2L,
Q6 = 6.745883931909770880159915641984874746358E1L,
Q7 = 1.806809656342804436118449982647641392951E1L,
Q8 = -1.770150690652438294290020775359580915464E1L,
Q9 = -5.659156469628629327045433069052560211164E-1L,
/* 1.000000000000000000000000000000000000000E0 */
acosr4375 = 1.1179797320499710475919903296900511518755E0L,
pimacosr4375 = 2.0236129215398221908706530535894517323217E0L,
/* asin(x) = x + x^3 pS(x^2) / qS(x^2)
0 <= x <= 0.5
peak relative error 1.9e-35 */
pS0 = -8.358099012470680544198472400254596543711E2L,
pS1 = 3.674973957689619490312782828051860366493E3L,
pS2 = -6.730729094812979665807581609853656623219E3L,
pS3 = 6.643843795209060298375552684423454077633E3L,
pS4 = -3.817341990928606692235481812252049415993E3L,
pS5 = 1.284635388402653715636722822195716476156E3L,
pS6 = -2.410736125231549204856567737329112037867E2L,
pS7 = 2.219191969382402856557594215833622156220E1L,
pS8 = -7.249056260830627156600112195061001036533E-1L,
pS9 = 1.055923570937755300061509030361395604448E-3L,
qS0 = -5.014859407482408326519083440151745519205E3L,
qS1 = 2.430653047950480068881028451580393430537E4L,
qS2 = -4.997904737193653607449250593976069726962E4L,
qS3 = 5.675712336110456923807959930107347511086E4L,
qS4 = -3.881523118339661268482937768522572588022E4L,
qS5 = 1.634202194895541569749717032234510811216E4L,
qS6 = -4.151452662440709301601820849901296953752E3L,
qS7 = 5.956050864057192019085175976175695342168E2L,
qS8 = -4.175375777334867025769346564600396877176E1L;
/* 1.000000000000000000000000000000000000000E0 */
long double
__ieee754_acosl (long double x)
{
long double a, z, r, w, p, q, s, t, f2;
if (__glibc_unlikely (isnan (x)))
return x + x;
a = __builtin_fabsl (x);
if (a == 1.0L)
{
if (x > 0.0L)
return 0.0; /* acos(1) = 0 */
else
return (2.0 * pio2_hi) + (2.0 * pio2_lo); /* acos(-1)= pi */
}
else if (a > 1.0L)
{
return (x - x) / (x - x); /* acos(|x| > 1) is NaN */
}
if (a < 0.5L)
{
if (a < 0x1p-106L)
return pio2_hi + pio2_lo;
if (a < 0.4375L)
{
/* Arcsine of x. */
z = x * x;
p = (((((((((pS9 * z
+ pS8) * z
+ pS7) * z
+ pS6) * z
+ pS5) * z
+ pS4) * z
+ pS3) * z
+ pS2) * z
+ pS1) * z
+ pS0) * z;
q = (((((((( z
+ qS8) * z
+ qS7) * z
+ qS6) * z
+ qS5) * z
+ qS4) * z
+ qS3) * z
+ qS2) * z
+ qS1) * z
+ qS0;
r = x + x * p / q;
z = pio2_hi - (r - pio2_lo);
return z;
}
/* .4375 <= |x| < .5 */
t = a - 0.4375L;
p = ((((((((((P10 * t
+ P9) * t
+ P8) * t
+ P7) * t
+ P6) * t
+ P5) * t
+ P4) * t
+ P3) * t
+ P2) * t
+ P1) * t
+ P0) * t;
q = (((((((((t
+ Q9) * t
+ Q8) * t
+ Q7) * t
+ Q6) * t
+ Q5) * t
+ Q4) * t
+ Q3) * t
+ Q2) * t
+ Q1) * t
+ Q0;
r = p / q;
if (x < 0.0L)
r = pimacosr4375 - r;
else
r = acosr4375 + r;
return r;
}
else if (a < 0.625L)
{
t = a - 0.5625L;
p = ((((((((((rS10 * t
+ rS9) * t
+ rS8) * t
+ rS7) * t
+ rS6) * t
+ rS5) * t
+ rS4) * t
+ rS3) * t
+ rS2) * t
+ rS1) * t
+ rS0) * t;
q = (((((((((t
+ sS9) * t
+ sS8) * t
+ sS7) * t
+ sS6) * t
+ sS5) * t
+ sS4) * t
+ sS3) * t
+ sS2) * t
+ sS1) * t
+ sS0;
if (x < 0.0L)
r = pimacosr5625 - p / q;
else
r = acosr5625 + p / q;
return r;
}
else
{ /* |x| >= .625 */
double shi, slo;
z = (one - a) * 0.5;
s = sqrtl (z);
/* Compute an extended precision square root from
the Newton iteration s -> 0.5 * (s + z / s).
The change w from s to the improved value is
w = 0.5 * (s + z / s) - s = (s^2 + z)/2s - s = (z - s^2)/2s.
Express s = f1 + f2 where f1 * f1 is exactly representable.
w = (z - s^2)/2s = (z - f1^2 - 2 f1 f2 - f2^2)/2s .
s + w has extended precision. */
ldbl_unpack (s, &shi, &slo);
a = shi;
f2 = slo;
w = z - a * a;
w = w - 2.0 * a * f2;
w = w - f2 * f2;
w = w / (2.0 * s);
/* Arcsine of s. */
p = (((((((((pS9 * z
+ pS8) * z
+ pS7) * z
+ pS6) * z
+ pS5) * z
+ pS4) * z
+ pS3) * z
+ pS2) * z
+ pS1) * z
+ pS0) * z;
q = (((((((( z
+ qS8) * z
+ qS7) * z
+ qS6) * z
+ qS5) * z
+ qS4) * z
+ qS3) * z
+ qS2) * z
+ qS1) * z
+ qS0;
r = s + (w + s * p / q);
if (x < 0.0L)
w = pio2_hi + (pio2_lo - r);
else
w = r;
return 2.0 * w;
}
}
libm_alias_finite (__ieee754_acosl, __acosl)