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authorDaniel Baumann <daniel.baumann@progress-linux.org>2024-04-28 13:16:40 +0000
committerDaniel Baumann <daniel.baumann@progress-linux.org>2024-04-28 13:16:40 +0000
commit47ab3d4a42e9ab51c465c4322d2ec233f6324e6b (patch)
treea61a0ffd83f4a3def4b36e5c8e99630c559aa723 /src/math/j1.go
parentInitial commit. (diff)
downloadgolang-1.18-47ab3d4a42e9ab51c465c4322d2ec233f6324e6b.tar.xz
golang-1.18-47ab3d4a42e9ab51c465c4322d2ec233f6324e6b.zip
Adding upstream version 1.18.10.upstream/1.18.10upstream
Signed-off-by: Daniel Baumann <daniel.baumann@progress-linux.org>
Diffstat (limited to 'src/math/j1.go')
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diff --git a/src/math/j1.go b/src/math/j1.go
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+// Copyright 2010 The Go Authors. All rights reserved.
+// Use of this source code is governed by a BSD-style
+// license that can be found in the LICENSE file.
+
+package math
+
+/*
+ Bessel function of the first and second kinds of order one.
+*/
+
+// The original C code and the long comment below are
+// from FreeBSD's /usr/src/lib/msun/src/e_j1.c and
+// came with this notice. The go code is a simplified
+// version of the original 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.
+// ====================================================
+//
+// __ieee754_j1(x), __ieee754_y1(x)
+// Bessel function of the first and second kinds of order one.
+// Method -- j1(x):
+// 1. For tiny x, we use j1(x) = x/2 - x**3/16 + x**5/384 - ...
+// 2. Reduce x to |x| since j1(x)=-j1(-x), and
+// for x in (0,2)
+// j1(x) = x/2 + x*z*R0/S0, where z = x*x;
+// (precision: |j1/x - 1/2 - R0/S0 |<2**-61.51 )
+// for x in (2,inf)
+// j1(x) = sqrt(2/(pi*x))*(p1(x)*cos(x1)-q1(x)*sin(x1))
+// y1(x) = sqrt(2/(pi*x))*(p1(x)*sin(x1)+q1(x)*cos(x1))
+// where x1 = x-3*pi/4. It is better to compute sin(x1),cos(x1)
+// as follow:
+// cos(x1) = cos(x)cos(3pi/4)+sin(x)sin(3pi/4)
+// = 1/sqrt(2) * (sin(x) - cos(x))
+// sin(x1) = sin(x)cos(3pi/4)-cos(x)sin(3pi/4)
+// = -1/sqrt(2) * (sin(x) + cos(x))
+// (To avoid cancellation, use
+// sin(x) +- cos(x) = -cos(2x)/(sin(x) -+ cos(x))
+// to compute the worse one.)
+//
+// 3 Special cases
+// j1(nan)= nan
+// j1(0) = 0
+// j1(inf) = 0
+//
+// Method -- y1(x):
+// 1. screen out x<=0 cases: y1(0)=-inf, y1(x<0)=NaN
+// 2. For x<2.
+// Since
+// y1(x) = 2/pi*(j1(x)*(ln(x/2)+Euler)-1/x-x/2+5/64*x**3-...)
+// therefore y1(x)-2/pi*j1(x)*ln(x)-1/x is an odd function.
+// We use the following function to approximate y1,
+// y1(x) = x*U(z)/V(z) + (2/pi)*(j1(x)*ln(x)-1/x), z= x**2
+// where for x in [0,2] (abs err less than 2**-65.89)
+// U(z) = U0[0] + U0[1]*z + ... + U0[4]*z**4
+// V(z) = 1 + v0[0]*z + ... + v0[4]*z**5
+// Note: For tiny x, 1/x dominate y1 and hence
+// y1(tiny) = -2/pi/tiny, (choose tiny<2**-54)
+// 3. For x>=2.
+// y1(x) = sqrt(2/(pi*x))*(p1(x)*sin(x1)+q1(x)*cos(x1))
+// where x1 = x-3*pi/4. It is better to compute sin(x1),cos(x1)
+// by method mentioned above.
+
+// J1 returns the order-one Bessel function of the first kind.
+//
+// Special cases are:
+// J1(±Inf) = 0
+// J1(NaN) = NaN
+func J1(x float64) float64 {
+ const (
+ TwoM27 = 1.0 / (1 << 27) // 2**-27 0x3e40000000000000
+ Two129 = 1 << 129 // 2**129 0x4800000000000000
+ // R0/S0 on [0, 2]
+ R00 = -6.25000000000000000000e-02 // 0xBFB0000000000000
+ R01 = 1.40705666955189706048e-03 // 0x3F570D9F98472C61
+ R02 = -1.59955631084035597520e-05 // 0xBEF0C5C6BA169668
+ R03 = 4.96727999609584448412e-08 // 0x3E6AAAFA46CA0BD9
+ S01 = 1.91537599538363460805e-02 // 0x3F939D0B12637E53
+ S02 = 1.85946785588630915560e-04 // 0x3F285F56B9CDF664
+ S03 = 1.17718464042623683263e-06 // 0x3EB3BFF8333F8498
+ S04 = 5.04636257076217042715e-09 // 0x3E35AC88C97DFF2C
+ S05 = 1.23542274426137913908e-11 // 0x3DAB2ACFCFB97ED8
+ )
+ // special cases
+ switch {
+ case IsNaN(x):
+ return x
+ case IsInf(x, 0) || x == 0:
+ return 0
+ }
+
+ sign := false
+ if x < 0 {
+ x = -x
+ sign = true
+ }
+ if x >= 2 {
+ s, c := Sincos(x)
+ ss := -s - c
+ cc := s - c
+
+ // make sure x+x does not overflow
+ if x < MaxFloat64/2 {
+ z := Cos(x + x)
+ if s*c > 0 {
+ cc = z / ss
+ } else {
+ ss = z / cc
+ }
+ }
+
+ // j1(x) = 1/sqrt(pi) * (P(1,x)*cc - Q(1,x)*ss) / sqrt(x)
+ // y1(x) = 1/sqrt(pi) * (P(1,x)*ss + Q(1,x)*cc) / sqrt(x)
+
+ var z float64
+ if x > Two129 {
+ z = (1 / SqrtPi) * cc / Sqrt(x)
+ } else {
+ u := pone(x)
+ v := qone(x)
+ z = (1 / SqrtPi) * (u*cc - v*ss) / Sqrt(x)
+ }
+ if sign {
+ return -z
+ }
+ return z
+ }
+ if x < TwoM27 { // |x|<2**-27
+ return 0.5 * x // inexact if x!=0 necessary
+ }
+ z := x * x
+ r := z * (R00 + z*(R01+z*(R02+z*R03)))
+ s := 1.0 + z*(S01+z*(S02+z*(S03+z*(S04+z*S05))))
+ r *= x
+ z = 0.5*x + r/s
+ if sign {
+ return -z
+ }
+ return z
+}
+
+// Y1 returns the order-one Bessel function of the second kind.
+//
+// Special cases are:
+// Y1(+Inf) = 0
+// Y1(0) = -Inf
+// Y1(x < 0) = NaN
+// Y1(NaN) = NaN
+func Y1(x float64) float64 {
+ const (
+ TwoM54 = 1.0 / (1 << 54) // 2**-54 0x3c90000000000000
+ Two129 = 1 << 129 // 2**129 0x4800000000000000
+ U00 = -1.96057090646238940668e-01 // 0xBFC91866143CBC8A
+ U01 = 5.04438716639811282616e-02 // 0x3FA9D3C776292CD1
+ U02 = -1.91256895875763547298e-03 // 0xBF5F55E54844F50F
+ U03 = 2.35252600561610495928e-05 // 0x3EF8AB038FA6B88E
+ U04 = -9.19099158039878874504e-08 // 0xBE78AC00569105B8
+ V00 = 1.99167318236649903973e-02 // 0x3F94650D3F4DA9F0
+ V01 = 2.02552581025135171496e-04 // 0x3F2A8C896C257764
+ V02 = 1.35608801097516229404e-06 // 0x3EB6C05A894E8CA6
+ V03 = 6.22741452364621501295e-09 // 0x3E3ABF1D5BA69A86
+ V04 = 1.66559246207992079114e-11 // 0x3DB25039DACA772A
+ )
+ // special cases
+ switch {
+ case x < 0 || IsNaN(x):
+ return NaN()
+ case IsInf(x, 1):
+ return 0
+ case x == 0:
+ return Inf(-1)
+ }
+
+ if x >= 2 {
+ s, c := Sincos(x)
+ ss := -s - c
+ cc := s - c
+
+ // make sure x+x does not overflow
+ if x < MaxFloat64/2 {
+ z := Cos(x + x)
+ if s*c > 0 {
+ cc = z / ss
+ } else {
+ ss = z / cc
+ }
+ }
+ // y1(x) = sqrt(2/(pi*x))*(p1(x)*sin(x0)+q1(x)*cos(x0))
+ // where x0 = x-3pi/4
+ // Better formula:
+ // cos(x0) = cos(x)cos(3pi/4)+sin(x)sin(3pi/4)
+ // = 1/sqrt(2) * (sin(x) - cos(x))
+ // sin(x0) = sin(x)cos(3pi/4)-cos(x)sin(3pi/4)
+ // = -1/sqrt(2) * (cos(x) + sin(x))
+ // To avoid cancellation, use
+ // sin(x) +- cos(x) = -cos(2x)/(sin(x) -+ cos(x))
+ // to compute the worse one.
+
+ var z float64
+ if x > Two129 {
+ z = (1 / SqrtPi) * ss / Sqrt(x)
+ } else {
+ u := pone(x)
+ v := qone(x)
+ z = (1 / SqrtPi) * (u*ss + v*cc) / Sqrt(x)
+ }
+ return z
+ }
+ if x <= TwoM54 { // x < 2**-54
+ return -(2 / Pi) / x
+ }
+ z := x * x
+ u := U00 + z*(U01+z*(U02+z*(U03+z*U04)))
+ v := 1 + z*(V00+z*(V01+z*(V02+z*(V03+z*V04))))
+ return x*(u/v) + (2/Pi)*(J1(x)*Log(x)-1/x)
+}
+
+// For x >= 8, the asymptotic expansions of pone is
+// 1 + 15/128 s**2 - 4725/2**15 s**4 - ..., where s = 1/x.
+// We approximate pone by
+// pone(x) = 1 + (R/S)
+// where R = pr0 + pr1*s**2 + pr2*s**4 + ... + pr5*s**10
+// S = 1 + ps0*s**2 + ... + ps4*s**10
+// and
+// | pone(x)-1-R/S | <= 2**(-60.06)
+
+// for x in [inf, 8]=1/[0,0.125]
+var p1R8 = [6]float64{
+ 0.00000000000000000000e+00, // 0x0000000000000000
+ 1.17187499999988647970e-01, // 0x3FBDFFFFFFFFFCCE
+ 1.32394806593073575129e+01, // 0x402A7A9D357F7FCE
+ 4.12051854307378562225e+02, // 0x4079C0D4652EA590
+ 3.87474538913960532227e+03, // 0x40AE457DA3A532CC
+ 7.91447954031891731574e+03, // 0x40BEEA7AC32782DD
+}
+var p1S8 = [5]float64{
+ 1.14207370375678408436e+02, // 0x405C8D458E656CAC
+ 3.65093083420853463394e+03, // 0x40AC85DC964D274F
+ 3.69562060269033463555e+04, // 0x40E20B8697C5BB7F
+ 9.76027935934950801311e+04, // 0x40F7D42CB28F17BB
+ 3.08042720627888811578e+04, // 0x40DE1511697A0B2D
+}
+
+// for x in [8,4.5454] = 1/[0.125,0.22001]
+var p1R5 = [6]float64{
+ 1.31990519556243522749e-11, // 0x3DAD0667DAE1CA7D
+ 1.17187493190614097638e-01, // 0x3FBDFFFFE2C10043
+ 6.80275127868432871736e+00, // 0x401B36046E6315E3
+ 1.08308182990189109773e+02, // 0x405B13B9452602ED
+ 5.17636139533199752805e+02, // 0x40802D16D052D649
+ 5.28715201363337541807e+02, // 0x408085B8BB7E0CB7
+}
+var p1S5 = [5]float64{
+ 5.92805987221131331921e+01, // 0x404DA3EAA8AF633D
+ 9.91401418733614377743e+02, // 0x408EFB361B066701
+ 5.35326695291487976647e+03, // 0x40B4E9445706B6FB
+ 7.84469031749551231769e+03, // 0x40BEA4B0B8A5BB15
+ 1.50404688810361062679e+03, // 0x40978030036F5E51
+}
+
+// for x in[4.5453,2.8571] = 1/[0.2199,0.35001]
+var p1R3 = [6]float64{
+ 3.02503916137373618024e-09, // 0x3E29FC21A7AD9EDD
+ 1.17186865567253592491e-01, // 0x3FBDFFF55B21D17B
+ 3.93297750033315640650e+00, // 0x400F76BCE85EAD8A
+ 3.51194035591636932736e+01, // 0x40418F489DA6D129
+ 9.10550110750781271918e+01, // 0x4056C3854D2C1837
+ 4.85590685197364919645e+01, // 0x4048478F8EA83EE5
+}
+var p1S3 = [5]float64{
+ 3.47913095001251519989e+01, // 0x40416549A134069C
+ 3.36762458747825746741e+02, // 0x40750C3307F1A75F
+ 1.04687139975775130551e+03, // 0x40905B7C5037D523
+ 8.90811346398256432622e+02, // 0x408BD67DA32E31E9
+ 1.03787932439639277504e+02, // 0x4059F26D7C2EED53
+}
+
+// for x in [2.8570,2] = 1/[0.3499,0.5]
+var p1R2 = [6]float64{
+ 1.07710830106873743082e-07, // 0x3E7CE9D4F65544F4
+ 1.17176219462683348094e-01, // 0x3FBDFF42BE760D83
+ 2.36851496667608785174e+00, // 0x4002F2B7F98FAEC0
+ 1.22426109148261232917e+01, // 0x40287C377F71A964
+ 1.76939711271687727390e+01, // 0x4031B1A8177F8EE2
+ 5.07352312588818499250e+00, // 0x40144B49A574C1FE
+}
+var p1S2 = [5]float64{
+ 2.14364859363821409488e+01, // 0x40356FBD8AD5ECDC
+ 1.25290227168402751090e+02, // 0x405F529314F92CD5
+ 2.32276469057162813669e+02, // 0x406D08D8D5A2DBD9
+ 1.17679373287147100768e+02, // 0x405D6B7ADA1884A9
+ 8.36463893371618283368e+00, // 0x4020BAB1F44E5192
+}
+
+func pone(x float64) float64 {
+ var p *[6]float64
+ var q *[5]float64
+ if x >= 8 {
+ p = &p1R8
+ q = &p1S8
+ } else if x >= 4.5454 {
+ p = &p1R5
+ q = &p1S5
+ } else if x >= 2.8571 {
+ p = &p1R3
+ q = &p1S3
+ } else if x >= 2 {
+ p = &p1R2
+ q = &p1S2
+ }
+ z := 1 / (x * x)
+ r := p[0] + z*(p[1]+z*(p[2]+z*(p[3]+z*(p[4]+z*p[5]))))
+ s := 1.0 + z*(q[0]+z*(q[1]+z*(q[2]+z*(q[3]+z*q[4]))))
+ return 1 + r/s
+}
+
+// For x >= 8, the asymptotic expansions of qone is
+// 3/8 s - 105/1024 s**3 - ..., where s = 1/x.
+// We approximate qone by
+// qone(x) = s*(0.375 + (R/S))
+// where R = qr1*s**2 + qr2*s**4 + ... + qr5*s**10
+// S = 1 + qs1*s**2 + ... + qs6*s**12
+// and
+// | qone(x)/s -0.375-R/S | <= 2**(-61.13)
+
+// for x in [inf, 8] = 1/[0,0.125]
+var q1R8 = [6]float64{
+ 0.00000000000000000000e+00, // 0x0000000000000000
+ -1.02539062499992714161e-01, // 0xBFBA3FFFFFFFFDF3
+ -1.62717534544589987888e+01, // 0xC0304591A26779F7
+ -7.59601722513950107896e+02, // 0xC087BCD053E4B576
+ -1.18498066702429587167e+04, // 0xC0C724E740F87415
+ -4.84385124285750353010e+04, // 0xC0E7A6D065D09C6A
+}
+var q1S8 = [6]float64{
+ 1.61395369700722909556e+02, // 0x40642CA6DE5BCDE5
+ 7.82538599923348465381e+03, // 0x40BE9162D0D88419
+ 1.33875336287249578163e+05, // 0x4100579AB0B75E98
+ 7.19657723683240939863e+05, // 0x4125F65372869C19
+ 6.66601232617776375264e+05, // 0x412457D27719AD5C
+ -2.94490264303834643215e+05, // 0xC111F9690EA5AA18
+}
+
+// for x in [8,4.5454] = 1/[0.125,0.22001]
+var q1R5 = [6]float64{
+ -2.08979931141764104297e-11, // 0xBDB6FA431AA1A098
+ -1.02539050241375426231e-01, // 0xBFBA3FFFCB597FEF
+ -8.05644828123936029840e+00, // 0xC0201CE6CA03AD4B
+ -1.83669607474888380239e+02, // 0xC066F56D6CA7B9B0
+ -1.37319376065508163265e+03, // 0xC09574C66931734F
+ -2.61244440453215656817e+03, // 0xC0A468E388FDA79D
+}
+var q1S5 = [6]float64{
+ 8.12765501384335777857e+01, // 0x405451B2FF5A11B2
+ 1.99179873460485964642e+03, // 0x409F1F31E77BF839
+ 1.74684851924908907677e+04, // 0x40D10F1F0D64CE29
+ 4.98514270910352279316e+04, // 0x40E8576DAABAD197
+ 2.79480751638918118260e+04, // 0x40DB4B04CF7C364B
+ -4.71918354795128470869e+03, // 0xC0B26F2EFCFFA004
+}
+
+// for x in [4.5454,2.8571] = 1/[0.2199,0.35001] ???
+var q1R3 = [6]float64{
+ -5.07831226461766561369e-09, // 0xBE35CFA9D38FC84F
+ -1.02537829820837089745e-01, // 0xBFBA3FEB51AEED54
+ -4.61011581139473403113e+00, // 0xC01270C23302D9FF
+ -5.78472216562783643212e+01, // 0xC04CEC71C25D16DA
+ -2.28244540737631695038e+02, // 0xC06C87D34718D55F
+ -2.19210128478909325622e+02, // 0xC06B66B95F5C1BF6
+}
+var q1S3 = [6]float64{
+ 4.76651550323729509273e+01, // 0x4047D523CCD367E4
+ 6.73865112676699709482e+02, // 0x40850EEBC031EE3E
+ 3.38015286679526343505e+03, // 0x40AA684E448E7C9A
+ 5.54772909720722782367e+03, // 0x40B5ABBAA61D54A6
+ 1.90311919338810798763e+03, // 0x409DBC7A0DD4DF4B
+ -1.35201191444307340817e+02, // 0xC060E670290A311F
+}
+
+// for x in [2.8570,2] = 1/[0.3499,0.5]
+var q1R2 = [6]float64{
+ -1.78381727510958865572e-07, // 0xBE87F12644C626D2
+ -1.02517042607985553460e-01, // 0xBFBA3E8E9148B010
+ -2.75220568278187460720e+00, // 0xC006048469BB4EDA
+ -1.96636162643703720221e+01, // 0xC033A9E2C168907F
+ -4.23253133372830490089e+01, // 0xC04529A3DE104AAA
+ -2.13719211703704061733e+01, // 0xC0355F3639CF6E52
+}
+var q1S2 = [6]float64{
+ 2.95333629060523854548e+01, // 0x403D888A78AE64FF
+ 2.52981549982190529136e+02, // 0x406F9F68DB821CBA
+ 7.57502834868645436472e+02, // 0x4087AC05CE49A0F7
+ 7.39393205320467245656e+02, // 0x40871B2548D4C029
+ 1.55949003336666123687e+02, // 0x40637E5E3C3ED8D4
+ -4.95949898822628210127e+00, // 0xC013D686E71BE86B
+}
+
+func qone(x float64) float64 {
+ var p, q *[6]float64
+ if x >= 8 {
+ p = &q1R8
+ q = &q1S8
+ } else if x >= 4.5454 {
+ p = &q1R5
+ q = &q1S5
+ } else if x >= 2.8571 {
+ p = &q1R3
+ q = &q1S3
+ } else if x >= 2 {
+ p = &q1R2
+ q = &q1S2
+ }
+ z := 1 / (x * x)
+ r := p[0] + z*(p[1]+z*(p[2]+z*(p[3]+z*(p[4]+z*p[5]))))
+ s := 1 + z*(q[0]+z*(q[1]+z*(q[2]+z*(q[3]+z*(q[4]+z*q[5])))))
+ return (0.375 + r/s) / x
+}