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717 lines
22 KiB
ArmAsm
717 lines
22 KiB
ArmAsm
.file "sincosf.s"
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// Copyright (c) 2000 - 2005, Intel Corporation
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// All rights reserved.
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//
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// Contributed 2000 by the Intel Numerics Group, Intel Corporation
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//
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// Redistribution and use in source and binary forms, with or without
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// modification, are permitted provided that the following conditions are
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// met:
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//
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// * Redistributions of source code must retain the above copyright
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// notice, this list of conditions and the following disclaimer.
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//
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// * Redistributions in binary form must reproduce the above copyright
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// notice, this list of conditions and the following disclaimer in the
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// documentation and/or other materials provided with the distribution.
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//
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// * The name of Intel Corporation may not be used to endorse or promote
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// products derived from this software without specific prior written
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// permission.
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// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
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// "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
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// LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR
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// A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL INTEL OR ITS
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// CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL,
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// EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO,
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// PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR
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// PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY
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// OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY OR TORT (INCLUDING
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// NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS
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// SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
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//
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// Intel Corporation is the author of this code, and requests that all
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// problem reports or change requests be submitted to it directly at
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// http://www.intel.com/software/products/opensource/libraries/num.htm.
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//
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// History
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//==============================================================
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// 02/02/00 Initial version
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// 04/02/00 Unwind support added.
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// 06/16/00 Updated tables to enforce symmetry
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// 08/31/00 Saved 2 cycles in main path, and 9 in other paths.
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// 09/20/00 The updated tables regressed to an old version, so reinstated them
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// 10/18/00 Changed one table entry to ensure symmetry
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// 01/03/01 Improved speed, fixed flag settings for small arguments.
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// 02/18/02 Large arguments processing routine excluded
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// 05/20/02 Cleaned up namespace and sf0 syntax
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// 06/03/02 Insure inexact flag set for large arg result
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// 09/05/02 Single precision version is made using double precision one as base
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// 02/10/03 Reordered header: .section, .global, .proc, .align
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// 03/31/05 Reformatted delimiters between data tables
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//
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// API
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//==============================================================
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// float sinf( float x);
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// float cosf( float x);
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//
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// Overview of operation
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//==============================================================
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//
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// Step 1
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// ======
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// Reduce x to region -1/2*pi/2^k ===== 0 ===== +1/2*pi/2^k where k=4
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// divide x by pi/2^k.
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// Multiply by 2^k/pi.
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// nfloat = Round result to integer (round-to-nearest)
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//
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// r = x - nfloat * pi/2^k
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// Do this as (x - nfloat * HIGH(pi/2^k)) - nfloat * LOW(pi/2^k)
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// for increased accuracy.
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// pi/2^k is stored as two numbers that when added make pi/2^k.
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// pi/2^k = HIGH(pi/2^k) + LOW(pi/2^k)
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// HIGH part is rounded to zero, LOW - to nearest
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//
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// x = (nfloat * pi/2^k) + r
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// r is small enough that we can use a polynomial approximation
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// and is referred to as the reduced argument.
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//
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// Step 3
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// ======
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// Take the unreduced part and remove the multiples of 2pi.
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// So nfloat = nfloat (with lower k+1 bits cleared) + lower k+1 bits
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//
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// nfloat (with lower k+1 bits cleared) is a multiple of 2^(k+1)
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// N * 2^(k+1)
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// nfloat * pi/2^k = N * 2^(k+1) * pi/2^k + (lower k+1 bits) * pi/2^k
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// nfloat * pi/2^k = N * 2 * pi + (lower k+1 bits) * pi/2^k
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// nfloat * pi/2^k = N2pi + M * pi/2^k
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//
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//
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// Sin(x) = Sin((nfloat * pi/2^k) + r)
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// = Sin(nfloat * pi/2^k) * Cos(r) + Cos(nfloat * pi/2^k) * Sin(r)
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//
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// Sin(nfloat * pi/2^k) = Sin(N2pi + Mpi/2^k)
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// = Sin(N2pi)Cos(Mpi/2^k) + Cos(N2pi)Sin(Mpi/2^k)
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// = Sin(Mpi/2^k)
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//
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// Cos(nfloat * pi/2^k) = Cos(N2pi + Mpi/2^k)
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// = Cos(N2pi)Cos(Mpi/2^k) + Sin(N2pi)Sin(Mpi/2^k)
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// = Cos(Mpi/2^k)
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//
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// Sin(x) = Sin(Mpi/2^k) Cos(r) + Cos(Mpi/2^k) Sin(r)
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//
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//
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// Step 4
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// ======
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// 0 <= M < 2^(k+1)
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// There are 2^(k+1) Sin entries in a table.
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// There are 2^(k+1) Cos entries in a table.
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//
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// Get Sin(Mpi/2^k) and Cos(Mpi/2^k) by table lookup.
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//
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//
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// Step 5
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// ======
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// Calculate Cos(r) and Sin(r) by polynomial approximation.
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//
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// Cos(r) = 1 + r^2 q1 + r^4 q2 = Series for Cos
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// Sin(r) = r + r^3 p1 + r^5 p2 = Series for Sin
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//
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// and the coefficients q1, q2 and p1, p2 are stored in a table
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//
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//
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// Calculate
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// Sin(x) = Sin(Mpi/2^k) Cos(r) + Cos(Mpi/2^k) Sin(r)
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//
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// as follows
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//
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// S[m] = Sin(Mpi/2^k) and C[m] = Cos(Mpi/2^k)
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// rsq = r*r
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//
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//
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// P = P1 + r^2*P2
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// Q = Q1 + r^2*Q2
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//
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// rcub = r * rsq
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// Sin(r) = r + rcub * P
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// = r + r^3p1 + r^5p2 = Sin(r)
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//
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// The coefficients are not exactly these values, but almost.
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//
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// p1 = -1/6 = -1/3!
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// p2 = 1/120 = 1/5!
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// p3 = -1/5040 = -1/7!
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// p4 = 1/362889 = 1/9!
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//
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// P = r + r^3 * P
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//
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// Answer = S[m] Cos(r) + C[m] P
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//
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// Cos(r) = 1 + rsq Q
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// Cos(r) = 1 + r^2 Q
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// Cos(r) = 1 + r^2 (q1 + r^2q2)
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// Cos(r) = 1 + r^2q1 + r^4q2
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//
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// S[m] Cos(r) = S[m](1 + rsq Q)
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// S[m] Cos(r) = S[m] + S[m] rsq Q
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// S[m] Cos(r) = S[m] + s_rsq Q
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// Q = S[m] + s_rsq Q
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//
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// Then,
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//
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// Answer = Q + C[m] P
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// Registers used
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//==============================================================
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// general input registers:
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// r14 -> r19
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// r32 -> r45
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// predicate registers used:
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// p6 -> p14
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// floating-point registers used
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// f9 -> f15
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// f32 -> f61
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// Assembly macros
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//==============================================================
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sincosf_NORM_f8 = f9
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sincosf_W = f10
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sincosf_int_Nfloat = f11
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sincosf_Nfloat = f12
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sincosf_r = f13
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sincosf_rsq = f14
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sincosf_rcub = f15
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sincosf_save_tmp = f15
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sincosf_Inv_Pi_by_16 = f32
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sincosf_Pi_by_16_1 = f33
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sincosf_Pi_by_16_2 = f34
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sincosf_Inv_Pi_by_64 = f35
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sincosf_Pi_by_16_3 = f36
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sincosf_r_exact = f37
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sincosf_Sm = f38
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sincosf_Cm = f39
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sincosf_P1 = f40
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sincosf_Q1 = f41
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sincosf_P2 = f42
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sincosf_Q2 = f43
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sincosf_P3 = f44
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sincosf_Q3 = f45
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sincosf_P4 = f46
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sincosf_Q4 = f47
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sincosf_P_temp1 = f48
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sincosf_P_temp2 = f49
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sincosf_Q_temp1 = f50
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sincosf_Q_temp2 = f51
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sincosf_P = f52
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sincosf_Q = f53
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sincosf_srsq = f54
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sincosf_SIG_INV_PI_BY_16_2TO61 = f55
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sincosf_RSHF_2TO61 = f56
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sincosf_RSHF = f57
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sincosf_2TOM61 = f58
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sincosf_NFLOAT = f59
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sincosf_W_2TO61_RSH = f60
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fp_tmp = f61
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/////////////////////////////////////////////////////////////
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sincosf_AD_1 = r33
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sincosf_AD_2 = r34
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sincosf_exp_limit = r35
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sincosf_r_signexp = r36
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sincosf_AD_beta_table = r37
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sincosf_r_sincos = r38
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sincosf_r_exp = r39
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sincosf_r_17_ones = r40
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sincosf_GR_sig_inv_pi_by_16 = r14
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sincosf_GR_rshf_2to61 = r15
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sincosf_GR_rshf = r16
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sincosf_GR_exp_2tom61 = r17
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sincosf_GR_n = r18
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sincosf_GR_m = r19
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sincosf_GR_32m = r19
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sincosf_GR_all_ones = r19
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gr_tmp = r41
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GR_SAVE_PFS = r41
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GR_SAVE_B0 = r42
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GR_SAVE_GP = r43
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RODATA
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.align 16
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// Pi/16 parts
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LOCAL_OBJECT_START(double_sincosf_pi)
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data8 0xC90FDAA22168C234, 0x00003FFC // pi/16 1st part
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data8 0xC4C6628B80DC1CD1, 0x00003FBC // pi/16 2nd part
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LOCAL_OBJECT_END(double_sincosf_pi)
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// Coefficients for polynomials
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LOCAL_OBJECT_START(double_sincosf_pq_k4)
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data8 0x3F810FABB668E9A2 // P2
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data8 0x3FA552E3D6DE75C9 // Q2
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data8 0xBFC555554447BC7F // P1
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data8 0xBFDFFFFFC447610A // Q1
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LOCAL_OBJECT_END(double_sincosf_pq_k4)
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// Sincos table (S[m], C[m])
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LOCAL_OBJECT_START(double_sin_cos_beta_k4)
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data8 0x0000000000000000 // sin ( 0 Pi / 16 )
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data8 0x3FF0000000000000 // cos ( 0 Pi / 16 )
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//
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data8 0x3FC8F8B83C69A60B // sin ( 1 Pi / 16 )
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data8 0x3FEF6297CFF75CB0 // cos ( 1 Pi / 16 )
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//
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data8 0x3FD87DE2A6AEA963 // sin ( 2 Pi / 16 )
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data8 0x3FED906BCF328D46 // cos ( 2 Pi / 16 )
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//
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data8 0x3FE1C73B39AE68C8 // sin ( 3 Pi / 16 )
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data8 0x3FEA9B66290EA1A3 // cos ( 3 Pi / 16 )
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//
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data8 0x3FE6A09E667F3BCD // sin ( 4 Pi / 16 )
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data8 0x3FE6A09E667F3BCD // cos ( 4 Pi / 16 )
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//
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data8 0x3FEA9B66290EA1A3 // sin ( 5 Pi / 16 )
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data8 0x3FE1C73B39AE68C8 // cos ( 5 Pi / 16 )
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//
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data8 0x3FED906BCF328D46 // sin ( 6 Pi / 16 )
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data8 0x3FD87DE2A6AEA963 // cos ( 6 Pi / 16 )
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//
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data8 0x3FEF6297CFF75CB0 // sin ( 7 Pi / 16 )
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data8 0x3FC8F8B83C69A60B // cos ( 7 Pi / 16 )
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//
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data8 0x3FF0000000000000 // sin ( 8 Pi / 16 )
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data8 0x0000000000000000 // cos ( 8 Pi / 16 )
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//
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data8 0x3FEF6297CFF75CB0 // sin ( 9 Pi / 16 )
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data8 0xBFC8F8B83C69A60B // cos ( 9 Pi / 16 )
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//
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data8 0x3FED906BCF328D46 // sin ( 10 Pi / 16 )
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data8 0xBFD87DE2A6AEA963 // cos ( 10 Pi / 16 )
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//
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data8 0x3FEA9B66290EA1A3 // sin ( 11 Pi / 16 )
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data8 0xBFE1C73B39AE68C8 // cos ( 11 Pi / 16 )
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//
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data8 0x3FE6A09E667F3BCD // sin ( 12 Pi / 16 )
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data8 0xBFE6A09E667F3BCD // cos ( 12 Pi / 16 )
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//
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data8 0x3FE1C73B39AE68C8 // sin ( 13 Pi / 16 )
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data8 0xBFEA9B66290EA1A3 // cos ( 13 Pi / 16 )
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//
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data8 0x3FD87DE2A6AEA963 // sin ( 14 Pi / 16 )
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data8 0xBFED906BCF328D46 // cos ( 14 Pi / 16 )
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//
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data8 0x3FC8F8B83C69A60B // sin ( 15 Pi / 16 )
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data8 0xBFEF6297CFF75CB0 // cos ( 15 Pi / 16 )
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//
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data8 0x0000000000000000 // sin ( 16 Pi / 16 )
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data8 0xBFF0000000000000 // cos ( 16 Pi / 16 )
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//
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data8 0xBFC8F8B83C69A60B // sin ( 17 Pi / 16 )
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data8 0xBFEF6297CFF75CB0 // cos ( 17 Pi / 16 )
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//
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data8 0xBFD87DE2A6AEA963 // sin ( 18 Pi / 16 )
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data8 0xBFED906BCF328D46 // cos ( 18 Pi / 16 )
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//
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data8 0xBFE1C73B39AE68C8 // sin ( 19 Pi / 16 )
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data8 0xBFEA9B66290EA1A3 // cos ( 19 Pi / 16 )
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//
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data8 0xBFE6A09E667F3BCD // sin ( 20 Pi / 16 )
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data8 0xBFE6A09E667F3BCD // cos ( 20 Pi / 16 )
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//
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data8 0xBFEA9B66290EA1A3 // sin ( 21 Pi / 16 )
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data8 0xBFE1C73B39AE68C8 // cos ( 21 Pi / 16 )
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//
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data8 0xBFED906BCF328D46 // sin ( 22 Pi / 16 )
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data8 0xBFD87DE2A6AEA963 // cos ( 22 Pi / 16 )
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//
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data8 0xBFEF6297CFF75CB0 // sin ( 23 Pi / 16 )
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data8 0xBFC8F8B83C69A60B // cos ( 23 Pi / 16 )
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//
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data8 0xBFF0000000000000 // sin ( 24 Pi / 16 )
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data8 0x0000000000000000 // cos ( 24 Pi / 16 )
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//
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data8 0xBFEF6297CFF75CB0 // sin ( 25 Pi / 16 )
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data8 0x3FC8F8B83C69A60B // cos ( 25 Pi / 16 )
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//
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data8 0xBFED906BCF328D46 // sin ( 26 Pi / 16 )
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data8 0x3FD87DE2A6AEA963 // cos ( 26 Pi / 16 )
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//
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data8 0xBFEA9B66290EA1A3 // sin ( 27 Pi / 16 )
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data8 0x3FE1C73B39AE68C8 // cos ( 27 Pi / 16 )
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//
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data8 0xBFE6A09E667F3BCD // sin ( 28 Pi / 16 )
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data8 0x3FE6A09E667F3BCD // cos ( 28 Pi / 16 )
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//
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data8 0xBFE1C73B39AE68C8 // sin ( 29 Pi / 16 )
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data8 0x3FEA9B66290EA1A3 // cos ( 29 Pi / 16 )
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//
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data8 0xBFD87DE2A6AEA963 // sin ( 30 Pi / 16 )
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data8 0x3FED906BCF328D46 // cos ( 30 Pi / 16 )
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//
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data8 0xBFC8F8B83C69A60B // sin ( 31 Pi / 16 )
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data8 0x3FEF6297CFF75CB0 // cos ( 31 Pi / 16 )
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//
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data8 0x0000000000000000 // sin ( 32 Pi / 16 )
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data8 0x3FF0000000000000 // cos ( 32 Pi / 16 )
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LOCAL_OBJECT_END(double_sin_cos_beta_k4)
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.section .text
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////////////////////////////////////////////////////////
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// There are two entry points: sin and cos
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// If from sin, p8 is true
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// If from cos, p9 is true
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GLOBAL_IEEE754_ENTRY(sinf)
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{ .mlx
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alloc r32 = ar.pfs,1,13,0,0
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movl sincosf_GR_sig_inv_pi_by_16 = 0xA2F9836E4E44152A //signd of 16/pi
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}
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{ .mlx
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addl sincosf_AD_1 = @ltoff(double_sincosf_pi), gp
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movl sincosf_GR_rshf_2to61 = 0x47b8000000000000 // 1.1 2^(63+63-2)
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};;
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{ .mfi
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ld8 sincosf_AD_1 = [sincosf_AD_1]
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fnorm.s1 sincosf_NORM_f8 = f8 // Normalize argument
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cmp.eq p8,p9 = r0, r0 // set p8 (clear p9) for sin
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}
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{ .mib
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mov sincosf_GR_exp_2tom61 = 0xffff-61 // exponent of scale 2^-61
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mov sincosf_r_sincos = 0x0 // 0 for sin
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br.cond.sptk _SINCOSF_COMMON // go to common part
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};;
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GLOBAL_IEEE754_END(sinf)
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GLOBAL_IEEE754_ENTRY(cosf)
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{ .mlx
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alloc r32 = ar.pfs,1,13,0,0
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movl sincosf_GR_sig_inv_pi_by_16 = 0xA2F9836E4E44152A //signd of 16/pi
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}
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{ .mlx
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addl sincosf_AD_1 = @ltoff(double_sincosf_pi), gp
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movl sincosf_GR_rshf_2to61 = 0x47b8000000000000 // 1.1 2^(63+63-2)
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};;
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{ .mfi
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ld8 sincosf_AD_1 = [sincosf_AD_1]
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fnorm.s1 sincosf_NORM_f8 = f8 // Normalize argument
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cmp.eq p9,p8 = r0, r0 // set p9 (clear p8) for cos
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}
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{ .mib
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mov sincosf_GR_exp_2tom61 = 0xffff-61 // exponent of scale 2^-61
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mov sincosf_r_sincos = 0x8 // 8 for cos
|
|
nop.b 999
|
|
};;
|
|
|
|
////////////////////////////////////////////////////////
|
|
// All entry points end up here.
|
|
// If from sin, sincosf_r_sincos is 0 and p8 is true
|
|
// If from cos, sincosf_r_sincos is 8 = 2^(k-1) and p9 is true
|
|
// We add sincosf_r_sincos to N
|
|
|
|
///////////// Common sin and cos part //////////////////
|
|
_SINCOSF_COMMON:
|
|
|
|
// Form two constants we need
|
|
// 16/pi * 2^-2 * 2^63, scaled by 2^61 since we just loaded the significand
|
|
// 1.1000...000 * 2^(63+63-2) to right shift int(W) into the low significand
|
|
// fcmp used to set denormal, and invalid on snans
|
|
{ .mfi
|
|
setf.sig sincosf_SIG_INV_PI_BY_16_2TO61 = sincosf_GR_sig_inv_pi_by_16
|
|
fclass.m p6,p0 = f8, 0xe7 // if x=0,inf,nan
|
|
mov sincosf_exp_limit = 0x10017
|
|
}
|
|
{ .mlx
|
|
setf.d sincosf_RSHF_2TO61 = sincosf_GR_rshf_2to61
|
|
movl sincosf_GR_rshf = 0x43e8000000000000 // 1.1000 2^63
|
|
};; // Right shift
|
|
|
|
// Form another constant
|
|
// 2^-61 for scaling Nfloat
|
|
// 0x10017 is register_bias + 24.
|
|
// So if f8 >= 2^24, go to large argument routines
|
|
{ .mmi
|
|
getf.exp sincosf_r_signexp = f8
|
|
setf.exp sincosf_2TOM61 = sincosf_GR_exp_2tom61
|
|
addl gr_tmp = -1,r0 // For "inexect" constant create
|
|
};;
|
|
|
|
// Load the two pieces of pi/16
|
|
// Form another constant
|
|
// 1.1000...000 * 2^63, the right shift constant
|
|
{ .mmb
|
|
ldfe sincosf_Pi_by_16_1 = [sincosf_AD_1],16
|
|
setf.d sincosf_RSHF = sincosf_GR_rshf
|
|
(p6) br.cond.spnt _SINCOSF_SPECIAL_ARGS
|
|
};;
|
|
|
|
// Getting argument's exp for "large arguments" filtering
|
|
{ .mmi
|
|
ldfe sincosf_Pi_by_16_2 = [sincosf_AD_1],16
|
|
setf.sig fp_tmp = gr_tmp // constant for inexact set
|
|
nop.i 999
|
|
};;
|
|
|
|
// Polynomial coefficients (Q2, Q1, P2, P1) loading
|
|
{ .mmi
|
|
ldfpd sincosf_P2,sincosf_Q2 = [sincosf_AD_1],16
|
|
nop.m 999
|
|
nop.i 999
|
|
};;
|
|
|
|
// Select exponent (17 lsb)
|
|
{ .mmi
|
|
ldfpd sincosf_P1,sincosf_Q1 = [sincosf_AD_1],16
|
|
nop.m 999
|
|
dep.z sincosf_r_exp = sincosf_r_signexp, 0, 17
|
|
};;
|
|
|
|
// p10 is true if we must call routines to handle larger arguments
|
|
// p10 is true if f8 exp is >= 0x10017 (2^24)
|
|
{ .mfb
|
|
cmp.ge p10,p0 = sincosf_r_exp,sincosf_exp_limit
|
|
nop.f 999
|
|
(p10) br.cond.spnt _SINCOSF_LARGE_ARGS // Go to "large args" routine
|
|
};;
|
|
|
|
// sincosf_W = x * sincosf_Inv_Pi_by_16
|
|
// Multiply x by scaled 16/pi and add large const to shift integer part of W to
|
|
// rightmost bits of significand
|
|
{ .mfi
|
|
nop.m 999
|
|
fma.s1 sincosf_W_2TO61_RSH = sincosf_NORM_f8, sincosf_SIG_INV_PI_BY_16_2TO61, sincosf_RSHF_2TO61
|
|
nop.i 999
|
|
};;
|
|
|
|
// sincosf_NFLOAT = Round_Int_Nearest(sincosf_W)
|
|
// This is done by scaling back by 2^-61 and subtracting the shift constant
|
|
{ .mfi
|
|
nop.m 999
|
|
fms.s1 sincosf_NFLOAT = sincosf_W_2TO61_RSH,sincosf_2TOM61,sincosf_RSHF
|
|
nop.i 999
|
|
};;
|
|
|
|
// get N = (int)sincosf_int_Nfloat
|
|
{ .mfi
|
|
getf.sig sincosf_GR_n = sincosf_W_2TO61_RSH // integer N value
|
|
nop.f 999
|
|
nop.i 999
|
|
};;
|
|
|
|
// Add 2^(k-1) (which is in sincosf_r_sincos=8) to N
|
|
// sincosf_r = -sincosf_Nfloat * sincosf_Pi_by_16_1 + x
|
|
{ .mfi
|
|
add sincosf_GR_n = sincosf_GR_n, sincosf_r_sincos
|
|
fnma.s1 sincosf_r = sincosf_NFLOAT, sincosf_Pi_by_16_1, sincosf_NORM_f8
|
|
nop.i 999
|
|
};;
|
|
|
|
// Get M (least k+1 bits of N)
|
|
{ .mmi
|
|
and sincosf_GR_m = 0x1f,sincosf_GR_n // Put mask 0x1F -
|
|
nop.m 999 // - select k+1 bits
|
|
nop.i 999
|
|
};;
|
|
|
|
// Add 16*M to address of sin_cos_beta table
|
|
{ .mfi
|
|
shladd sincosf_AD_2 = sincosf_GR_32m, 4, sincosf_AD_1
|
|
(p8) fclass.m.unc p10,p0 = f8,0x0b // If sin denormal input -
|
|
nop.i 999
|
|
};;
|
|
|
|
// Load Sin and Cos table value using obtained index m (sincosf_AD_2)
|
|
{ .mfi
|
|
ldfd sincosf_Sm = [sincosf_AD_2],8 // Sin value S[m]
|
|
(p9) fclass.m.unc p11,p0 = f8,0x0b // If cos denormal input -
|
|
nop.i 999 // - set denormal
|
|
};;
|
|
|
|
// sincosf_r = sincosf_r -sincosf_Nfloat * sincosf_Pi_by_16_2
|
|
{ .mfi
|
|
ldfd sincosf_Cm = [sincosf_AD_2] // Cos table value C[m]
|
|
fnma.s1 sincosf_r_exact = sincosf_NFLOAT, sincosf_Pi_by_16_2, sincosf_r
|
|
nop.i 999
|
|
}
|
|
// get rsq = r*r
|
|
{ .mfi
|
|
nop.m 999
|
|
fma.s1 sincosf_rsq = sincosf_r, sincosf_r, f0 // r^2 = r*r
|
|
nop.i 999
|
|
};;
|
|
|
|
{ .mfi
|
|
nop.m 999
|
|
fmpy.s0 fp_tmp = fp_tmp, fp_tmp // forces inexact flag
|
|
nop.i 999
|
|
};;
|
|
|
|
// Polynomials calculation
|
|
// Q = Q2*r^2 + Q1
|
|
// P = P2*r^2 + P1
|
|
{ .mfi
|
|
nop.m 999
|
|
fma.s1 sincosf_Q = sincosf_rsq, sincosf_Q2, sincosf_Q1
|
|
nop.i 999
|
|
}
|
|
{ .mfi
|
|
nop.m 999
|
|
fma.s1 sincosf_P = sincosf_rsq, sincosf_P2, sincosf_P1
|
|
nop.i 999
|
|
};;
|
|
|
|
// get rcube and S[m]*r^2
|
|
{ .mfi
|
|
nop.m 999
|
|
fmpy.s1 sincosf_srsq = sincosf_Sm,sincosf_rsq // r^2*S[m]
|
|
nop.i 999
|
|
}
|
|
{ .mfi
|
|
nop.m 999
|
|
fmpy.s1 sincosf_rcub = sincosf_r_exact, sincosf_rsq
|
|
nop.i 999
|
|
};;
|
|
|
|
// Get final P and Q
|
|
// Q = Q*S[m]*r^2 + S[m]
|
|
// P = P*r^3 + r
|
|
{ .mfi
|
|
nop.m 999
|
|
fma.s1 sincosf_Q = sincosf_srsq,sincosf_Q, sincosf_Sm
|
|
nop.i 999
|
|
}
|
|
{ .mfi
|
|
nop.m 999
|
|
fma.s1 sincosf_P = sincosf_rcub,sincosf_P,sincosf_r_exact
|
|
nop.i 999
|
|
};;
|
|
|
|
// If sinf(denormal) - force underflow to be set
|
|
.pred.rel "mutex",p10,p11
|
|
{ .mfi
|
|
nop.m 999
|
|
(p10) fmpy.s.s0 fp_tmp = f8,f8 // forces underflow flag
|
|
nop.i 999 // for denormal sine args
|
|
}
|
|
// If cosf(denormal) - force denormal to be set
|
|
{ .mfi
|
|
nop.m 999
|
|
(p11) fma.s.s0 fp_tmp = f8, f1, f8 // forces denormal flag
|
|
nop.i 999 // for denormal cosine args
|
|
};;
|
|
|
|
|
|
// Final calculation
|
|
// result = C[m]*P + Q
|
|
{ .mfb
|
|
nop.m 999
|
|
fma.s.s0 f8 = sincosf_Cm, sincosf_P, sincosf_Q
|
|
br.ret.sptk b0 // Exit for common path
|
|
};;
|
|
|
|
////////// x = 0/Inf/NaN path //////////////////
|
|
_SINCOSF_SPECIAL_ARGS:
|
|
.pred.rel "mutex",p8,p9
|
|
// sinf(+/-0) = +/-0
|
|
// sinf(Inf) = NaN
|
|
// sinf(NaN) = NaN
|
|
{ .mfi
|
|
nop.m 999
|
|
(p8) fma.s.s0 f8 = f8, f0, f0 // sinf(+/-0,NaN,Inf)
|
|
nop.i 999
|
|
}
|
|
// cosf(+/-0) = 1.0
|
|
// cosf(Inf) = NaN
|
|
// cosf(NaN) = NaN
|
|
{ .mfb
|
|
nop.m 999
|
|
(p9) fma.s.s0 f8 = f8, f0, f1 // cosf(+/-0,NaN,Inf)
|
|
br.ret.sptk b0 // Exit for x = 0/Inf/NaN path
|
|
};;
|
|
|
|
GLOBAL_IEEE754_END(cosf)
|
|
|
|
//////////// x >= 2^24 - large arguments routine call ////////////
|
|
LOCAL_LIBM_ENTRY(__libm_callout_sincosf)
|
|
_SINCOSF_LARGE_ARGS:
|
|
.prologue
|
|
{ .mfi
|
|
mov sincosf_GR_all_ones = -1 // 0xffffffff
|
|
nop.f 999
|
|
.save ar.pfs,GR_SAVE_PFS
|
|
mov GR_SAVE_PFS = ar.pfs
|
|
}
|
|
;;
|
|
|
|
{ .mfi
|
|
mov GR_SAVE_GP = gp
|
|
nop.f 999
|
|
.save b0, GR_SAVE_B0
|
|
mov GR_SAVE_B0 = b0
|
|
}
|
|
.body
|
|
|
|
{ .mbb
|
|
setf.sig sincosf_save_tmp = sincosf_GR_all_ones // inexact set
|
|
nop.b 999
|
|
(p8) br.call.sptk.many b0 = __libm_sin_large# // sinf(large_X)
|
|
};;
|
|
|
|
{ .mbb
|
|
cmp.ne p9,p0 = sincosf_r_sincos, r0 // set p9 if cos
|
|
nop.b 999
|
|
(p9) br.call.sptk.many b0 = __libm_cos_large# // cosf(large_X)
|
|
};;
|
|
|
|
{ .mfi
|
|
mov gp = GR_SAVE_GP
|
|
fma.s.s0 f8 = f8, f1, f0 // Round result to single
|
|
mov b0 = GR_SAVE_B0
|
|
}
|
|
{ .mfi // force inexact set
|
|
nop.m 999
|
|
fmpy.s0 sincosf_save_tmp = sincosf_save_tmp, sincosf_save_tmp
|
|
nop.i 999
|
|
};;
|
|
|
|
{ .mib
|
|
nop.m 999
|
|
mov ar.pfs = GR_SAVE_PFS
|
|
br.ret.sptk b0 // Exit for large arguments routine call
|
|
};;
|
|
LOCAL_LIBM_END(__libm_callout_sincosf)
|
|
|
|
.type __libm_sin_large#, @function
|
|
.global __libm_sin_large#
|
|
.type __libm_cos_large#, @function
|
|
.global __libm_cos_large#
|