s_tan.s

Glibc 2.3.2源代码(解压后有100多M)

.file "tan.s"

// Copyright (C) 2000, 2001, Intel Corporation
// All rights reserved.
// 
// Contributed 2/2/2000 by John Harrison, Ted Kubaska, Bob Norin, Shane Story,
// and Ping Tak Peter Tang of the Computational Software Lab, Intel Corporation.
//
// Redistribution and use in source and binary forms, with or without
// modification, are permitted provided that the following conditions are
// met:
//
// * Redistributions of source code must retain the above copyright
// notice, this list of conditions and the following disclaimer.
//
// * Redistributions in binary form must reproduce the above copyright
// notice, this list of conditions and the following disclaimer in the
// documentation and/or other materials provided with the distribution.
//
// * The name of Intel Corporation may not be used to endorse or promote
// products derived from this software without specific prior written
// permission.
//
// THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS 
// "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT 
// LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR
// A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL INTEL OR ITS 
// CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL,
// EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO, 
// PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR 
// PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY 
// OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY OR TORT (INCLUDING
// NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS 
// SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE. 
// 
// Intel Corporation is the author of this code, and requests that all
// problem reports or change requests be submitted to it directly at 
// http://developer.intel.com/opensource.
//
// History
//==============================================================
// 2/02/00: Initial version
// 4/04/00  Unwind support added
// 12/27/00 Improved speed
//
// API
//==============================================================
// double tan( double x);
//
// Overview of operation
//==============================================================
// If the input value in radians is |x| >= 1.xxxxx 2^10 call the
// older slower version.
//
// The new algorithm is used when |x| <= 1.xxxxx 2^9.
//
// Represent the input X as Nfloat * pi/2 + r
//    where r can be negative and |r| <= pi/4
//
//     tan_W  = x * 2/pi
//     Nfloat = round_int(tan_W)
//
//     tan_r  = x - Nfloat * (pi/2)_hi
//     tan_r  = tan_r - Nfloat * (pi/2)_lo
//
// We have two paths: p8, when Nfloat is even and p9. when Nfloat is odd.
// p8: tan(X) =  tan(r)
// p9: tan(X) = -cot(r)
//
// Each is evaluated as a series. The p9 path requires 1/r.
//
// The coefficients used in the series are stored in a table as
// are the pi constants.
//
// Registers used
//==============================================================
//
// predicate registers used:  
// p6-10
//
// floating-point registers used:  
// f10-15, f32-105
// f8, input
//
// general registers used
// r14-18, r32-43
//

#include "libm_support.h"

// Assembly macros
//==============================================================
TAN_INV_PI_BY_2_2TO64        = f10
TAN_RSHF_2TO64               = f11
TAN_2TOM64                   = f12
TAN_RSHF                     = f13
TAN_W_2TO64_RSH              = f14
TAN_NFLOAT                   = f15

tan_Inv_Pi_by_2              = f32
tan_Pi_by_2_hi               = f33
tan_Pi_by_2_lo               = f34


tan_P0                       = f35
tan_P1                       = f36
tan_P2                       = f37
tan_P3                       = f38 
tan_P4                       = f39 
tan_P5                       = f40 
tan_P6                       = f41
tan_P7                       = f42
tan_P8                       = f43 
tan_P9                       = f44 
tan_P10                      = f45 
tan_P11                      = f46
tan_P12                      = f47 
tan_P13                      = f48
tan_P14                      = f49
tan_P15                      = f50

tan_Q0                       = f51 
tan_Q1                       = f52 
tan_Q2                       = f53 
tan_Q3                       = f54 
tan_Q4                       = f55 
tan_Q5                       = f56 
tan_Q6                       = f57 
tan_Q7                       = f58 
tan_Q8                       = f59
tan_Q9                       = f60
tan_Q10                      = f61

tan_r                        = f62
tan_rsq                      = f63
tan_rcube                    = f64

tan_v18                      = f65
tan_v16                      = f66
tan_v17                      = f67
tan_v12                      = f68
tan_v13                      = f69
tan_v7                       = f70
tan_v8                       = f71
tan_v4                       = f72
tan_v5                       = f73
tan_v15                      = f74
tan_v11                      = f75
tan_v14                      = f76
tan_v3                       = f77
tan_v6                       = f78
tan_v10                      = f79
tan_v2                       = f80
tan_v9                       = f81
tan_v1                       = f82
tan_int_Nfloat               = f83 
tan_Nfloat                   = f84 

tan_NORM_f8                  = f85 
tan_W                        = f86

tan_y0                       = f87
tan_d                        = f88 
tan_y1                       = f89 
tan_dsq                      = f90 
tan_y2                       = f91 
tan_d4                       = f92 
tan_inv_r                    = f93 

tan_z1                       = f94
tan_z2                       = f95
tan_z3                       = f96
tan_z4                       = f97
tan_z5                       = f98
tan_z6                       = f99
tan_z7                       = f100
tan_z8                       = f101
tan_z9                       = f102
tan_z10                      = f103
tan_z11                      = f104
tan_z12                      = f105


/////////////////////////////////////////////////////////////

tan_GR_sig_inv_pi_by_2       = r14
tan_GR_rshf_2to64            = r15
tan_GR_exp_2tom64            = r16
tan_GR_n                     = r17
tan_GR_rshf                  = r18

tan_AD                       = r33
tan_GR_10009                 = r34 
tan_GR_17_ones               = r35 
tan_GR_N_odd_even            = r36 
tan_GR_N                     = r37 
tan_signexp                  = r38
tan_exp                      = r39
tan_ADQ                      = r40

GR_SAVE_PFS                  = r41 
GR_SAVE_B0                   = r42       
GR_SAVE_GP                   = r43      


#ifdef _LIBC
.rodata
#else
.data
#endif

.align 16

double_tan_constants:
ASM_TYPE_DIRECTIVE(double_tan_constants,@object)
//   data8 0xA2F9836E4E44152A, 0x00003FFE // 2/pi
   data8 0xC90FDAA22168C234, 0x00003FFF // pi/2 hi

   data8 0xBEEA54580DDEA0E1 // P14 
   data8 0x3ED3021ACE749A59 // P15
   data8 0xBEF312BD91DC8DA1 // P12 
   data8 0x3EFAE9AFC14C5119 // P13
   data8 0x3F2F342BF411E769 // P8
   data8 0x3F1A60FC9F3B0227 // P9
   data8 0x3EFF246E78E5E45B // P10
   data8 0x3F01D9D2E782875C // P11
   data8 0x3F8226E34C4499B6 // P4
   data8 0x3F6D6D3F12C236AC // P5
   data8 0x3F57DA1146DCFD8B // P6
   data8 0x3F43576410FE3D75 // P7
   data8 0x3FD5555555555555 // P0
   data8 0x3FC11111111111C2 // P1
   data8 0x3FABA1BA1BA0E850 // P2
   data8 0x3F9664F4886725A7 // P3
ASM_SIZE_DIRECTIVE(double_tan_constants)

double_Q_tan_constants:
ASM_TYPE_DIRECTIVE(double_Q_tan_constants,@object)
   data8 0xC4C6628B80DC1CD1, 0x00003FBF // pi/2 lo
   data8 0x3E223A73BA576E48 // Q8
   data8 0x3DF54AD8D1F2CA43 // Q9
   data8 0x3EF66A8EE529A6AA // Q4
   data8 0x3EC2281050410EE6 // Q5
   data8 0x3E8D6BB992CC3CF5 // Q6
   data8 0x3E57F88DE34832E4 // Q7
   data8 0x3FD5555555555555 // Q0
   data8 0x3F96C16C16C16DB8 // Q1
   data8 0x3F61566ABBFFB489 // Q2
   data8 0x3F2BBD77945C1733 // Q3
   data8 0x3D927FB33E2B0E04 // Q10
ASM_SIZE_DIRECTIVE(double_Q_tan_constants)


   
.align 32
.global tan#
#ifdef _LIBC
.global __tan#
#endif

////////////////////////////////////////////////////////



.section .text
.proc  tan#
#ifdef _LIBC
.proc  __tan#
#endif
.align 32
tan: 
#ifdef _LIBC
__tan: 
#endif
// The initial fnorm will take any unmasked faults and
// normalize any single/double unorms

{ .mlx
      alloc          r32=ar.pfs,1,11,0,0               
      movl tan_GR_sig_inv_pi_by_2 = 0xA2F9836E4E44152A // significand of 2/pi
}
{ .mlx
      addl           tan_AD   = @ltoff(double_tan_constants), gp
      movl tan_GR_rshf_2to64 = 0x47e8000000000000 // 1.1000 2^(63+63+1)
}
;;

{ .mfi
      ld8 tan_AD = [tan_AD]
      fnorm     tan_NORM_f8  = f8                      
      mov tan_GR_exp_2tom64 = 0xffff-64 // exponent of scaling factor 2^-64
}
{ .mlx
      nop.m 999
      movl tan_GR_rshf = 0x43e8000000000000 // 1.1000 2^63 for right shift
}
;;


// Form two constants we need
//   2/pi * 2^1 * 2^63, scaled by 2^64 since we just loaded the significand
//   1.1000...000 * 2^(63+63+1) to right shift int(W) into the significand
{ .mmi
      setf.sig TAN_INV_PI_BY_2_2TO64 = tan_GR_sig_inv_pi_by_2
      setf.d TAN_RSHF_2TO64 = tan_GR_rshf_2to64
      mov       tan_GR_17_ones     = 0x1ffff             ;;
}


// Form another constant
//   2^-64 for scaling Nfloat
//   1.1000...000 * 2^63, the right shift constant
{ .mmf
      setf.exp TAN_2TOM64 = tan_GR_exp_2tom64
      adds tan_ADQ = double_Q_tan_constants - double_tan_constants, tan_AD
      fclass.m.unc  p6,p0 = f8, 0x07  // Test for x=0
}
;;


// Form another constant
//   2^-64 for scaling Nfloat
//   1.1000...000 * 2^63, the right shift constant
{ .mmf
      setf.d TAN_RSHF = tan_GR_rshf
      ldfe      tan_Pi_by_2_hi = [tan_AD],16 
      fclass.m.unc  p7,p0 = f8, 0x23  // Test for x=inf
}
;;

{ .mfb
      ldfe      tan_Pi_by_2_lo = [tan_ADQ],16           
      fclass.m.unc  p8,p0 = f8, 0xc3  // Test for x=nan
(p6)  br.ret.spnt    b0    ;;         // Exit for x=0
}

{ .mfi
      ldfpd     tan_P14,tan_P15 = [tan_AD],16                         
(p7)  frcpa.s0  f8,p9=f0,f0           // Set qnan indef if x=inf
      mov       tan_GR_10009 = 0x10009
}
{ .mib
      ldfpd      tan_Q8,tan_Q9  = [tan_ADQ],16                        
      nop.i 999
(p7)  br.ret.spnt    b0    ;;         // Exit for x=inf
}

{ .mfi
      ldfpd      tan_P12,tan_P13 = [tan_AD],16                         
(p8)  fma.d f8=f8,f1,f8               // Set qnan if x=nan
      nop.i 999
}
{ .mib
      ldfpd      tan_Q4,tan_Q5  = [tan_ADQ],16                        
      nop.i 999
(p8)  br.ret.spnt    b0    ;;         // Exit for x=nan
}

{ .mmi
      getf.exp  tan_signexp    = tan_NORM_f8                 
      ldfpd      tan_P8,tan_P9  = [tan_AD],16                         
      nop.i 999 ;;
}

// Multiply x by scaled 2/pi and add large const to shift integer part of W to 
//   rightmost bits of significand
{ .mfi
      ldfpd      tan_Q6,tan_Q7  = [tan_ADQ],16
      fma.s1 TAN_W_2TO64_RSH = tan_NORM_f8,TAN_INV_PI_BY_2_2TO64,TAN_RSHF_2TO64
      nop.i 999 ;;
}

{ .mmi
      ldfpd      tan_P10,tan_P11 = [tan_AD],16                         
      nop.m 999
      and       tan_exp = tan_GR_17_ones, tan_signexp         ;;
}


// p7 is true if we must call DBX TAN
// p7 is true if f8 exp is > 0x10009 (which includes all ones
//    NAN or inf)
{ .mmi
      ldfpd      tan_Q0,tan_Q1  = [tan_ADQ],16                         
      cmp.ge.unc  p7,p0 = tan_exp,tan_GR_10009               
      nop.i 999 ;;