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While no copyright violation occurred, the license which 'Numerical Recipes' operates under is not amenable to Python, so to prevent confusion it's easier to simply remove its mention.
2155 lines
68 KiB
C
2155 lines
68 KiB
C
/* Math module -- standard C math library functions, pi and e */
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/* Here are some comments from Tim Peters, extracted from the
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discussion attached to http://bugs.python.org/issue1640. They
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describe the general aims of the math module with respect to
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special values, IEEE-754 floating-point exceptions, and Python
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exceptions.
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These are the "spirit of 754" rules:
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1. If the mathematical result is a real number, but of magnitude too
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large to approximate by a machine float, overflow is signaled and the
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result is an infinity (with the appropriate sign).
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2. If the mathematical result is a real number, but of magnitude too
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small to approximate by a machine float, underflow is signaled and the
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result is a zero (with the appropriate sign).
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3. At a singularity (a value x such that the limit of f(y) as y
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approaches x exists and is an infinity), "divide by zero" is signaled
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and the result is an infinity (with the appropriate sign). This is
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complicated a little by that the left-side and right-side limits may
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not be the same; e.g., 1/x approaches +inf or -inf as x approaches 0
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from the positive or negative directions. In that specific case, the
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sign of the zero determines the result of 1/0.
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4. At a point where a function has no defined result in the extended
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reals (i.e., the reals plus an infinity or two), invalid operation is
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signaled and a NaN is returned.
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And these are what Python has historically /tried/ to do (but not
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always successfully, as platform libm behavior varies a lot):
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For #1, raise OverflowError.
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For #2, return a zero (with the appropriate sign if that happens by
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accident ;-)).
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For #3 and #4, raise ValueError. It may have made sense to raise
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Python's ZeroDivisionError in #3, but historically that's only been
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raised for division by zero and mod by zero.
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*/
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/*
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In general, on an IEEE-754 platform the aim is to follow the C99
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standard, including Annex 'F', whenever possible. Where the
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standard recommends raising the 'divide-by-zero' or 'invalid'
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floating-point exceptions, Python should raise a ValueError. Where
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the standard recommends raising 'overflow', Python should raise an
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OverflowError. In all other circumstances a value should be
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returned.
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*/
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#include "Python.h"
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#include "_math.h"
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/*
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sin(pi*x), giving accurate results for all finite x (especially x
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integral or close to an integer). This is here for use in the
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reflection formula for the gamma function. It conforms to IEEE
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754-2008 for finite arguments, but not for infinities or nans.
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*/
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static const double pi = 3.141592653589793238462643383279502884197;
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static const double sqrtpi = 1.772453850905516027298167483341145182798;
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static const double logpi = 1.144729885849400174143427351353058711647;
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static double
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sinpi(double x)
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{
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double y, r;
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int n;
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/* this function should only ever be called for finite arguments */
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assert(Py_IS_FINITE(x));
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y = fmod(fabs(x), 2.0);
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n = (int)round(2.0*y);
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assert(0 <= n && n <= 4);
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switch (n) {
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case 0:
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r = sin(pi*y);
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break;
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case 1:
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r = cos(pi*(y-0.5));
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break;
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case 2:
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/* N.B. -sin(pi*(y-1.0)) is *not* equivalent: it would give
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-0.0 instead of 0.0 when y == 1.0. */
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r = sin(pi*(1.0-y));
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break;
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case 3:
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r = -cos(pi*(y-1.5));
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break;
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case 4:
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r = sin(pi*(y-2.0));
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break;
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default:
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assert(0); /* should never get here */
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r = -1.23e200; /* silence gcc warning */
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}
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return copysign(1.0, x)*r;
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}
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/* Implementation of the real gamma function. In extensive but non-exhaustive
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random tests, this function proved accurate to within <= 10 ulps across the
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entire float domain. Note that accuracy may depend on the quality of the
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system math functions, the pow function in particular. Special cases
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follow C99 annex F. The parameters and method are tailored to platforms
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whose double format is the IEEE 754 binary64 format.
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Method: for x > 0.0 we use the Lanczos approximation with parameters N=13
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and g=6.024680040776729583740234375; these parameters are amongst those
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used by the Boost library. Following Boost (again), we re-express the
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Lanczos sum as a rational function, and compute it that way. The
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coefficients below were computed independently using MPFR, and have been
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double-checked against the coefficients in the Boost source code.
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For x < 0.0 we use the reflection formula.
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There's one minor tweak that deserves explanation: Lanczos' formula for
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Gamma(x) involves computing pow(x+g-0.5, x-0.5) / exp(x+g-0.5). For many x
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values, x+g-0.5 can be represented exactly. However, in cases where it
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can't be represented exactly the small error in x+g-0.5 can be magnified
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significantly by the pow and exp calls, especially for large x. A cheap
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correction is to multiply by (1 + e*g/(x+g-0.5)), where e is the error
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involved in the computation of x+g-0.5 (that is, e = computed value of
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x+g-0.5 - exact value of x+g-0.5). Here's the proof:
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Correction factor
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-----------------
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Write x+g-0.5 = y-e, where y is exactly representable as an IEEE 754
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double, and e is tiny. Then:
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pow(x+g-0.5,x-0.5)/exp(x+g-0.5) = pow(y-e, x-0.5)/exp(y-e)
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= pow(y, x-0.5)/exp(y) * C,
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where the correction_factor C is given by
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C = pow(1-e/y, x-0.5) * exp(e)
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Since e is tiny, pow(1-e/y, x-0.5) ~ 1-(x-0.5)*e/y, and exp(x) ~ 1+e, so:
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C ~ (1-(x-0.5)*e/y) * (1+e) ~ 1 + e*(y-(x-0.5))/y
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But y-(x-0.5) = g+e, and g+e ~ g. So we get C ~ 1 + e*g/y, and
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pow(x+g-0.5,x-0.5)/exp(x+g-0.5) ~ pow(y, x-0.5)/exp(y) * (1 + e*g/y),
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Note that for accuracy, when computing r*C it's better to do
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r + e*g/y*r;
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than
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r * (1 + e*g/y);
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since the addition in the latter throws away most of the bits of
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information in e*g/y.
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*/
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#define LANCZOS_N 13
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static const double lanczos_g = 6.024680040776729583740234375;
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static const double lanczos_g_minus_half = 5.524680040776729583740234375;
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static const double lanczos_num_coeffs[LANCZOS_N] = {
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23531376880.410759688572007674451636754734846804940,
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42919803642.649098768957899047001988850926355848959,
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35711959237.355668049440185451547166705960488635843,
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17921034426.037209699919755754458931112671403265390,
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6039542586.3520280050642916443072979210699388420708,
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1439720407.3117216736632230727949123939715485786772,
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248874557.86205415651146038641322942321632125127801,
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31426415.585400194380614231628318205362874684987640,
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2876370.6289353724412254090516208496135991145378768,
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186056.26539522349504029498971604569928220784236328,
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8071.6720023658162106380029022722506138218516325024,
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210.82427775157934587250973392071336271166969580291,
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2.5066282746310002701649081771338373386264310793408
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};
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/* denominator is x*(x+1)*...*(x+LANCZOS_N-2) */
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static const double lanczos_den_coeffs[LANCZOS_N] = {
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0.0, 39916800.0, 120543840.0, 150917976.0, 105258076.0, 45995730.0,
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13339535.0, 2637558.0, 357423.0, 32670.0, 1925.0, 66.0, 1.0};
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/* gamma values for small positive integers, 1 though NGAMMA_INTEGRAL */
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#define NGAMMA_INTEGRAL 23
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static const double gamma_integral[NGAMMA_INTEGRAL] = {
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1.0, 1.0, 2.0, 6.0, 24.0, 120.0, 720.0, 5040.0, 40320.0, 362880.0,
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3628800.0, 39916800.0, 479001600.0, 6227020800.0, 87178291200.0,
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1307674368000.0, 20922789888000.0, 355687428096000.0,
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6402373705728000.0, 121645100408832000.0, 2432902008176640000.0,
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51090942171709440000.0, 1124000727777607680000.0,
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};
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/* Lanczos' sum L_g(x), for positive x */
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static double
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lanczos_sum(double x)
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{
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double num = 0.0, den = 0.0;
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int i;
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assert(x > 0.0);
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/* evaluate the rational function lanczos_sum(x). For large
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x, the obvious algorithm risks overflow, so we instead
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rescale the denominator and numerator of the rational
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function by x**(1-LANCZOS_N) and treat this as a
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rational function in 1/x. This also reduces the error for
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larger x values. The choice of cutoff point (5.0 below) is
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somewhat arbitrary; in tests, smaller cutoff values than
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this resulted in lower accuracy. */
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if (x < 5.0) {
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for (i = LANCZOS_N; --i >= 0; ) {
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num = num * x + lanczos_num_coeffs[i];
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den = den * x + lanczos_den_coeffs[i];
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}
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}
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else {
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for (i = 0; i < LANCZOS_N; i++) {
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num = num / x + lanczos_num_coeffs[i];
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den = den / x + lanczos_den_coeffs[i];
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}
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}
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return num/den;
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}
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/* Constant for +infinity, generated in the same way as float('inf'). */
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static double
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m_inf(void)
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{
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#ifndef PY_NO_SHORT_FLOAT_REPR
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return _Py_dg_infinity(0);
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#else
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return Py_HUGE_VAL;
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#endif
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}
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/* Constant nan value, generated in the same way as float('nan'). */
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/* We don't currently assume that Py_NAN is defined everywhere. */
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#if !defined(PY_NO_SHORT_FLOAT_REPR) || defined(Py_NAN)
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static double
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m_nan(void)
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{
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#ifndef PY_NO_SHORT_FLOAT_REPR
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return _Py_dg_stdnan(0);
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#else
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return Py_NAN;
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#endif
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}
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#endif
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static double
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m_tgamma(double x)
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{
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double absx, r, y, z, sqrtpow;
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/* special cases */
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if (!Py_IS_FINITE(x)) {
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if (Py_IS_NAN(x) || x > 0.0)
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return x; /* tgamma(nan) = nan, tgamma(inf) = inf */
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else {
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errno = EDOM;
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return Py_NAN; /* tgamma(-inf) = nan, invalid */
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}
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}
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if (x == 0.0) {
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errno = EDOM;
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/* tgamma(+-0.0) = +-inf, divide-by-zero */
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return copysign(Py_HUGE_VAL, x);
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}
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/* integer arguments */
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if (x == floor(x)) {
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if (x < 0.0) {
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errno = EDOM; /* tgamma(n) = nan, invalid for */
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return Py_NAN; /* negative integers n */
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}
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if (x <= NGAMMA_INTEGRAL)
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return gamma_integral[(int)x - 1];
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}
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absx = fabs(x);
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/* tiny arguments: tgamma(x) ~ 1/x for x near 0 */
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if (absx < 1e-20) {
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r = 1.0/x;
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if (Py_IS_INFINITY(r))
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errno = ERANGE;
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return r;
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}
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/* large arguments: assuming IEEE 754 doubles, tgamma(x) overflows for
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x > 200, and underflows to +-0.0 for x < -200, not a negative
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integer. */
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if (absx > 200.0) {
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if (x < 0.0) {
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return 0.0/sinpi(x);
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}
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else {
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errno = ERANGE;
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return Py_HUGE_VAL;
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}
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}
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y = absx + lanczos_g_minus_half;
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/* compute error in sum */
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if (absx > lanczos_g_minus_half) {
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/* note: the correction can be foiled by an optimizing
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compiler that (incorrectly) thinks that an expression like
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a + b - a - b can be optimized to 0.0. This shouldn't
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happen in a standards-conforming compiler. */
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double q = y - absx;
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z = q - lanczos_g_minus_half;
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}
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else {
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double q = y - lanczos_g_minus_half;
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z = q - absx;
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}
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z = z * lanczos_g / y;
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if (x < 0.0) {
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r = -pi / sinpi(absx) / absx * exp(y) / lanczos_sum(absx);
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r -= z * r;
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if (absx < 140.0) {
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r /= pow(y, absx - 0.5);
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}
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else {
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sqrtpow = pow(y, absx / 2.0 - 0.25);
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r /= sqrtpow;
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r /= sqrtpow;
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}
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}
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else {
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r = lanczos_sum(absx) / exp(y);
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r += z * r;
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if (absx < 140.0) {
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r *= pow(y, absx - 0.5);
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}
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else {
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sqrtpow = pow(y, absx / 2.0 - 0.25);
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r *= sqrtpow;
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r *= sqrtpow;
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}
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}
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if (Py_IS_INFINITY(r))
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errno = ERANGE;
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return r;
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}
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/*
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lgamma: natural log of the absolute value of the Gamma function.
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For large arguments, Lanczos' formula works extremely well here.
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*/
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static double
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m_lgamma(double x)
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{
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double r, absx;
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/* special cases */
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if (!Py_IS_FINITE(x)) {
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if (Py_IS_NAN(x))
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return x; /* lgamma(nan) = nan */
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else
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return Py_HUGE_VAL; /* lgamma(+-inf) = +inf */
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}
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/* integer arguments */
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if (x == floor(x) && x <= 2.0) {
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if (x <= 0.0) {
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errno = EDOM; /* lgamma(n) = inf, divide-by-zero for */
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return Py_HUGE_VAL; /* integers n <= 0 */
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}
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else {
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return 0.0; /* lgamma(1) = lgamma(2) = 0.0 */
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}
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}
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absx = fabs(x);
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/* tiny arguments: lgamma(x) ~ -log(fabs(x)) for small x */
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if (absx < 1e-20)
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return -log(absx);
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/* Lanczos' formula. We could save a fraction of a ulp in accuracy by
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having a second set of numerator coefficients for lanczos_sum that
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absorbed the exp(-lanczos_g) term, and throwing out the lanczos_g
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subtraction below; it's probably not worth it. */
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r = log(lanczos_sum(absx)) - lanczos_g;
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r += (absx - 0.5) * (log(absx + lanczos_g - 0.5) - 1);
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if (x < 0.0)
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/* Use reflection formula to get value for negative x. */
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r = logpi - log(fabs(sinpi(absx))) - log(absx) - r;
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if (Py_IS_INFINITY(r))
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errno = ERANGE;
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return r;
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}
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/*
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Implementations of the error function erf(x) and the complementary error
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function erfc(x).
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Method: we use a series approximation for erf for small x, and a continued
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fraction approximation for erfc(x) for larger x;
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combined with the relations erf(-x) = -erf(x) and erfc(x) = 1.0 - erf(x),
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this gives us erf(x) and erfc(x) for all x.
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The series expansion used is:
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erf(x) = x*exp(-x*x)/sqrt(pi) * [
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2/1 + 4/3 x**2 + 8/15 x**4 + 16/105 x**6 + ...]
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The coefficient of x**(2k-2) here is 4**k*factorial(k)/factorial(2*k).
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This series converges well for smallish x, but slowly for larger x.
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The continued fraction expansion used is:
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erfc(x) = x*exp(-x*x)/sqrt(pi) * [1/(0.5 + x**2 -) 0.5/(2.5 + x**2 - )
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3.0/(4.5 + x**2 - ) 7.5/(6.5 + x**2 - ) ...]
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after the first term, the general term has the form:
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k*(k-0.5)/(2*k+0.5 + x**2 - ...).
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This expansion converges fast for larger x, but convergence becomes
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infinitely slow as x approaches 0.0. The (somewhat naive) continued
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fraction evaluation algorithm used below also risks overflow for large x;
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but for large x, erfc(x) == 0.0 to within machine precision. (For
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example, erfc(30.0) is approximately 2.56e-393).
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Parameters: use series expansion for abs(x) < ERF_SERIES_CUTOFF and
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continued fraction expansion for ERF_SERIES_CUTOFF <= abs(x) <
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ERFC_CONTFRAC_CUTOFF. ERFC_SERIES_TERMS and ERFC_CONTFRAC_TERMS are the
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numbers of terms to use for the relevant expansions. */
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#define ERF_SERIES_CUTOFF 1.5
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#define ERF_SERIES_TERMS 25
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#define ERFC_CONTFRAC_CUTOFF 30.0
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#define ERFC_CONTFRAC_TERMS 50
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/*
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Error function, via power series.
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Given a finite float x, return an approximation to erf(x).
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Converges reasonably fast for small x.
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*/
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static double
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m_erf_series(double x)
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{
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double x2, acc, fk, result;
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int i, saved_errno;
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x2 = x * x;
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acc = 0.0;
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fk = (double)ERF_SERIES_TERMS + 0.5;
|
|
for (i = 0; i < ERF_SERIES_TERMS; i++) {
|
|
acc = 2.0 + x2 * acc / fk;
|
|
fk -= 1.0;
|
|
}
|
|
/* Make sure the exp call doesn't affect errno;
|
|
see m_erfc_contfrac for more. */
|
|
saved_errno = errno;
|
|
result = acc * x * exp(-x2) / sqrtpi;
|
|
errno = saved_errno;
|
|
return result;
|
|
}
|
|
|
|
/*
|
|
Complementary error function, via continued fraction expansion.
|
|
|
|
Given a positive float x, return an approximation to erfc(x). Converges
|
|
reasonably fast for x large (say, x > 2.0), and should be safe from
|
|
overflow if x and nterms are not too large. On an IEEE 754 machine, with x
|
|
<= 30.0, we're safe up to nterms = 100. For x >= 30.0, erfc(x) is smaller
|
|
than the smallest representable nonzero float. */
|
|
|
|
static double
|
|
m_erfc_contfrac(double x)
|
|
{
|
|
double x2, a, da, p, p_last, q, q_last, b, result;
|
|
int i, saved_errno;
|
|
|
|
if (x >= ERFC_CONTFRAC_CUTOFF)
|
|
return 0.0;
|
|
|
|
x2 = x*x;
|
|
a = 0.0;
|
|
da = 0.5;
|
|
p = 1.0; p_last = 0.0;
|
|
q = da + x2; q_last = 1.0;
|
|
for (i = 0; i < ERFC_CONTFRAC_TERMS; i++) {
|
|
double temp;
|
|
a += da;
|
|
da += 2.0;
|
|
b = da + x2;
|
|
temp = p; p = b*p - a*p_last; p_last = temp;
|
|
temp = q; q = b*q - a*q_last; q_last = temp;
|
|
}
|
|
/* Issue #8986: On some platforms, exp sets errno on underflow to zero;
|
|
save the current errno value so that we can restore it later. */
|
|
saved_errno = errno;
|
|
result = p / q * x * exp(-x2) / sqrtpi;
|
|
errno = saved_errno;
|
|
return result;
|
|
}
|
|
|
|
/* Error function erf(x), for general x */
|
|
|
|
static double
|
|
m_erf(double x)
|
|
{
|
|
double absx, cf;
|
|
|
|
if (Py_IS_NAN(x))
|
|
return x;
|
|
absx = fabs(x);
|
|
if (absx < ERF_SERIES_CUTOFF)
|
|
return m_erf_series(x);
|
|
else {
|
|
cf = m_erfc_contfrac(absx);
|
|
return x > 0.0 ? 1.0 - cf : cf - 1.0;
|
|
}
|
|
}
|
|
|
|
/* Complementary error function erfc(x), for general x. */
|
|
|
|
static double
|
|
m_erfc(double x)
|
|
{
|
|
double absx, cf;
|
|
|
|
if (Py_IS_NAN(x))
|
|
return x;
|
|
absx = fabs(x);
|
|
if (absx < ERF_SERIES_CUTOFF)
|
|
return 1.0 - m_erf_series(x);
|
|
else {
|
|
cf = m_erfc_contfrac(absx);
|
|
return x > 0.0 ? cf : 2.0 - cf;
|
|
}
|
|
}
|
|
|
|
/*
|
|
wrapper for atan2 that deals directly with special cases before
|
|
delegating to the platform libm for the remaining cases. This
|
|
is necessary to get consistent behaviour across platforms.
|
|
Windows, FreeBSD and alpha Tru64 are amongst platforms that don't
|
|
always follow C99.
|
|
*/
|
|
|
|
static double
|
|
m_atan2(double y, double x)
|
|
{
|
|
if (Py_IS_NAN(x) || Py_IS_NAN(y))
|
|
return Py_NAN;
|
|
if (Py_IS_INFINITY(y)) {
|
|
if (Py_IS_INFINITY(x)) {
|
|
if (copysign(1., x) == 1.)
|
|
/* atan2(+-inf, +inf) == +-pi/4 */
|
|
return copysign(0.25*Py_MATH_PI, y);
|
|
else
|
|
/* atan2(+-inf, -inf) == +-pi*3/4 */
|
|
return copysign(0.75*Py_MATH_PI, y);
|
|
}
|
|
/* atan2(+-inf, x) == +-pi/2 for finite x */
|
|
return copysign(0.5*Py_MATH_PI, y);
|
|
}
|
|
if (Py_IS_INFINITY(x) || y == 0.) {
|
|
if (copysign(1., x) == 1.)
|
|
/* atan2(+-y, +inf) = atan2(+-0, +x) = +-0. */
|
|
return copysign(0., y);
|
|
else
|
|
/* atan2(+-y, -inf) = atan2(+-0., -x) = +-pi. */
|
|
return copysign(Py_MATH_PI, y);
|
|
}
|
|
return atan2(y, x);
|
|
}
|
|
|
|
/*
|
|
Various platforms (Solaris, OpenBSD) do nonstandard things for log(0),
|
|
log(-ve), log(NaN). Here are wrappers for log and log10 that deal with
|
|
special values directly, passing positive non-special values through to
|
|
the system log/log10.
|
|
*/
|
|
|
|
static double
|
|
m_log(double x)
|
|
{
|
|
if (Py_IS_FINITE(x)) {
|
|
if (x > 0.0)
|
|
return log(x);
|
|
errno = EDOM;
|
|
if (x == 0.0)
|
|
return -Py_HUGE_VAL; /* log(0) = -inf */
|
|
else
|
|
return Py_NAN; /* log(-ve) = nan */
|
|
}
|
|
else if (Py_IS_NAN(x))
|
|
return x; /* log(nan) = nan */
|
|
else if (x > 0.0)
|
|
return x; /* log(inf) = inf */
|
|
else {
|
|
errno = EDOM;
|
|
return Py_NAN; /* log(-inf) = nan */
|
|
}
|
|
}
|
|
|
|
/*
|
|
log2: log to base 2.
|
|
|
|
Uses an algorithm that should:
|
|
|
|
(a) produce exact results for powers of 2, and
|
|
(b) give a monotonic log2 (for positive finite floats),
|
|
assuming that the system log is monotonic.
|
|
*/
|
|
|
|
static double
|
|
m_log2(double x)
|
|
{
|
|
if (!Py_IS_FINITE(x)) {
|
|
if (Py_IS_NAN(x))
|
|
return x; /* log2(nan) = nan */
|
|
else if (x > 0.0)
|
|
return x; /* log2(+inf) = +inf */
|
|
else {
|
|
errno = EDOM;
|
|
return Py_NAN; /* log2(-inf) = nan, invalid-operation */
|
|
}
|
|
}
|
|
|
|
if (x > 0.0) {
|
|
#ifdef HAVE_LOG2
|
|
return log2(x);
|
|
#else
|
|
double m;
|
|
int e;
|
|
m = frexp(x, &e);
|
|
/* We want log2(m * 2**e) == log(m) / log(2) + e. Care is needed when
|
|
* x is just greater than 1.0: in that case e is 1, log(m) is negative,
|
|
* and we get significant cancellation error from the addition of
|
|
* log(m) / log(2) to e. The slight rewrite of the expression below
|
|
* avoids this problem.
|
|
*/
|
|
if (x >= 1.0) {
|
|
return log(2.0 * m) / log(2.0) + (e - 1);
|
|
}
|
|
else {
|
|
return log(m) / log(2.0) + e;
|
|
}
|
|
#endif
|
|
}
|
|
else if (x == 0.0) {
|
|
errno = EDOM;
|
|
return -Py_HUGE_VAL; /* log2(0) = -inf, divide-by-zero */
|
|
}
|
|
else {
|
|
errno = EDOM;
|
|
return Py_NAN; /* log2(-inf) = nan, invalid-operation */
|
|
}
|
|
}
|
|
|
|
static double
|
|
m_log10(double x)
|
|
{
|
|
if (Py_IS_FINITE(x)) {
|
|
if (x > 0.0)
|
|
return log10(x);
|
|
errno = EDOM;
|
|
if (x == 0.0)
|
|
return -Py_HUGE_VAL; /* log10(0) = -inf */
|
|
else
|
|
return Py_NAN; /* log10(-ve) = nan */
|
|
}
|
|
else if (Py_IS_NAN(x))
|
|
return x; /* log10(nan) = nan */
|
|
else if (x > 0.0)
|
|
return x; /* log10(inf) = inf */
|
|
else {
|
|
errno = EDOM;
|
|
return Py_NAN; /* log10(-inf) = nan */
|
|
}
|
|
}
|
|
|
|
|
|
static PyObject *
|
|
math_gcd(PyObject *self, PyObject *args)
|
|
{
|
|
PyObject *a, *b, *g;
|
|
|
|
if (!PyArg_ParseTuple(args, "OO:gcd", &a, &b))
|
|
return NULL;
|
|
|
|
a = PyNumber_Index(a);
|
|
if (a == NULL)
|
|
return NULL;
|
|
b = PyNumber_Index(b);
|
|
if (b == NULL) {
|
|
Py_DECREF(a);
|
|
return NULL;
|
|
}
|
|
g = _PyLong_GCD(a, b);
|
|
Py_DECREF(a);
|
|
Py_DECREF(b);
|
|
return g;
|
|
}
|
|
|
|
PyDoc_STRVAR(math_gcd_doc,
|
|
"gcd(x, y) -> int\n\
|
|
greatest common divisor of x and y");
|
|
|
|
|
|
/* Call is_error when errno != 0, and where x is the result libm
|
|
* returned. is_error will usually set up an exception and return
|
|
* true (1), but may return false (0) without setting up an exception.
|
|
*/
|
|
static int
|
|
is_error(double x)
|
|
{
|
|
int result = 1; /* presumption of guilt */
|
|
assert(errno); /* non-zero errno is a precondition for calling */
|
|
if (errno == EDOM)
|
|
PyErr_SetString(PyExc_ValueError, "math domain error");
|
|
|
|
else if (errno == ERANGE) {
|
|
/* ANSI C generally requires libm functions to set ERANGE
|
|
* on overflow, but also generally *allows* them to set
|
|
* ERANGE on underflow too. There's no consistency about
|
|
* the latter across platforms.
|
|
* Alas, C99 never requires that errno be set.
|
|
* Here we suppress the underflow errors (libm functions
|
|
* should return a zero on underflow, and +- HUGE_VAL on
|
|
* overflow, so testing the result for zero suffices to
|
|
* distinguish the cases).
|
|
*
|
|
* On some platforms (Ubuntu/ia64) it seems that errno can be
|
|
* set to ERANGE for subnormal results that do *not* underflow
|
|
* to zero. So to be safe, we'll ignore ERANGE whenever the
|
|
* function result is less than one in absolute value.
|
|
*/
|
|
if (fabs(x) < 1.0)
|
|
result = 0;
|
|
else
|
|
PyErr_SetString(PyExc_OverflowError,
|
|
"math range error");
|
|
}
|
|
else
|
|
/* Unexpected math error */
|
|
PyErr_SetFromErrno(PyExc_ValueError);
|
|
return result;
|
|
}
|
|
|
|
/*
|
|
math_1 is used to wrap a libm function f that takes a double
|
|
arguments and returns a double.
|
|
|
|
The error reporting follows these rules, which are designed to do
|
|
the right thing on C89/C99 platforms and IEEE 754/non IEEE 754
|
|
platforms.
|
|
|
|
- a NaN result from non-NaN inputs causes ValueError to be raised
|
|
- an infinite result from finite inputs causes OverflowError to be
|
|
raised if can_overflow is 1, or raises ValueError if can_overflow
|
|
is 0.
|
|
- if the result is finite and errno == EDOM then ValueError is
|
|
raised
|
|
- if the result is finite and nonzero and errno == ERANGE then
|
|
OverflowError is raised
|
|
|
|
The last rule is used to catch overflow on platforms which follow
|
|
C89 but for which HUGE_VAL is not an infinity.
|
|
|
|
For the majority of one-argument functions these rules are enough
|
|
to ensure that Python's functions behave as specified in 'Annex F'
|
|
of the C99 standard, with the 'invalid' and 'divide-by-zero'
|
|
floating-point exceptions mapping to Python's ValueError and the
|
|
'overflow' floating-point exception mapping to OverflowError.
|
|
math_1 only works for functions that don't have singularities *and*
|
|
the possibility of overflow; fortunately, that covers everything we
|
|
care about right now.
|
|
*/
|
|
|
|
static PyObject *
|
|
math_1_to_whatever(PyObject *arg, double (*func) (double),
|
|
PyObject *(*from_double_func) (double),
|
|
int can_overflow)
|
|
{
|
|
double x, r;
|
|
x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_1", return 0);
|
|
r = (*func)(x);
|
|
PyFPE_END_PROTECT(r);
|
|
if (Py_IS_NAN(r) && !Py_IS_NAN(x)) {
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"math domain error"); /* invalid arg */
|
|
return NULL;
|
|
}
|
|
if (Py_IS_INFINITY(r) && Py_IS_FINITE(x)) {
|
|
if (can_overflow)
|
|
PyErr_SetString(PyExc_OverflowError,
|
|
"math range error"); /* overflow */
|
|
else
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"math domain error"); /* singularity */
|
|
return NULL;
|
|
}
|
|
if (Py_IS_FINITE(r) && errno && is_error(r))
|
|
/* this branch unnecessary on most platforms */
|
|
return NULL;
|
|
|
|
return (*from_double_func)(r);
|
|
}
|
|
|
|
/* variant of math_1, to be used when the function being wrapped is known to
|
|
set errno properly (that is, errno = EDOM for invalid or divide-by-zero,
|
|
errno = ERANGE for overflow). */
|
|
|
|
static PyObject *
|
|
math_1a(PyObject *arg, double (*func) (double))
|
|
{
|
|
double x, r;
|
|
x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_1a", return 0);
|
|
r = (*func)(x);
|
|
PyFPE_END_PROTECT(r);
|
|
if (errno && is_error(r))
|
|
return NULL;
|
|
return PyFloat_FromDouble(r);
|
|
}
|
|
|
|
/*
|
|
math_2 is used to wrap a libm function f that takes two double
|
|
arguments and returns a double.
|
|
|
|
The error reporting follows these rules, which are designed to do
|
|
the right thing on C89/C99 platforms and IEEE 754/non IEEE 754
|
|
platforms.
|
|
|
|
- a NaN result from non-NaN inputs causes ValueError to be raised
|
|
- an infinite result from finite inputs causes OverflowError to be
|
|
raised.
|
|
- if the result is finite and errno == EDOM then ValueError is
|
|
raised
|
|
- if the result is finite and nonzero and errno == ERANGE then
|
|
OverflowError is raised
|
|
|
|
The last rule is used to catch overflow on platforms which follow
|
|
C89 but for which HUGE_VAL is not an infinity.
|
|
|
|
For most two-argument functions (copysign, fmod, hypot, atan2)
|
|
these rules are enough to ensure that Python's functions behave as
|
|
specified in 'Annex F' of the C99 standard, with the 'invalid' and
|
|
'divide-by-zero' floating-point exceptions mapping to Python's
|
|
ValueError and the 'overflow' floating-point exception mapping to
|
|
OverflowError.
|
|
*/
|
|
|
|
static PyObject *
|
|
math_1(PyObject *arg, double (*func) (double), int can_overflow)
|
|
{
|
|
return math_1_to_whatever(arg, func, PyFloat_FromDouble, can_overflow);
|
|
}
|
|
|
|
static PyObject *
|
|
math_1_to_int(PyObject *arg, double (*func) (double), int can_overflow)
|
|
{
|
|
return math_1_to_whatever(arg, func, PyLong_FromDouble, can_overflow);
|
|
}
|
|
|
|
static PyObject *
|
|
math_2(PyObject *args, double (*func) (double, double), char *funcname)
|
|
{
|
|
PyObject *ox, *oy;
|
|
double x, y, r;
|
|
if (! PyArg_UnpackTuple(args, funcname, 2, 2, &ox, &oy))
|
|
return NULL;
|
|
x = PyFloat_AsDouble(ox);
|
|
y = PyFloat_AsDouble(oy);
|
|
if ((x == -1.0 || y == -1.0) && PyErr_Occurred())
|
|
return NULL;
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_2", return 0);
|
|
r = (*func)(x, y);
|
|
PyFPE_END_PROTECT(r);
|
|
if (Py_IS_NAN(r)) {
|
|
if (!Py_IS_NAN(x) && !Py_IS_NAN(y))
|
|
errno = EDOM;
|
|
else
|
|
errno = 0;
|
|
}
|
|
else if (Py_IS_INFINITY(r)) {
|
|
if (Py_IS_FINITE(x) && Py_IS_FINITE(y))
|
|
errno = ERANGE;
|
|
else
|
|
errno = 0;
|
|
}
|
|
if (errno && is_error(r))
|
|
return NULL;
|
|
else
|
|
return PyFloat_FromDouble(r);
|
|
}
|
|
|
|
#define FUNC1(funcname, func, can_overflow, docstring) \
|
|
static PyObject * math_##funcname(PyObject *self, PyObject *args) { \
|
|
return math_1(args, func, can_overflow); \
|
|
}\
|
|
PyDoc_STRVAR(math_##funcname##_doc, docstring);
|
|
|
|
#define FUNC1A(funcname, func, docstring) \
|
|
static PyObject * math_##funcname(PyObject *self, PyObject *args) { \
|
|
return math_1a(args, func); \
|
|
}\
|
|
PyDoc_STRVAR(math_##funcname##_doc, docstring);
|
|
|
|
#define FUNC2(funcname, func, docstring) \
|
|
static PyObject * math_##funcname(PyObject *self, PyObject *args) { \
|
|
return math_2(args, func, #funcname); \
|
|
}\
|
|
PyDoc_STRVAR(math_##funcname##_doc, docstring);
|
|
|
|
FUNC1(acos, acos, 0,
|
|
"acos(x)\n\nReturn the arc cosine (measured in radians) of x.")
|
|
FUNC1(acosh, m_acosh, 0,
|
|
"acosh(x)\n\nReturn the inverse hyperbolic cosine of x.")
|
|
FUNC1(asin, asin, 0,
|
|
"asin(x)\n\nReturn the arc sine (measured in radians) of x.")
|
|
FUNC1(asinh, m_asinh, 0,
|
|
"asinh(x)\n\nReturn the inverse hyperbolic sine of x.")
|
|
FUNC1(atan, atan, 0,
|
|
"atan(x)\n\nReturn the arc tangent (measured in radians) of x.")
|
|
FUNC2(atan2, m_atan2,
|
|
"atan2(y, x)\n\nReturn the arc tangent (measured in radians) of y/x.\n"
|
|
"Unlike atan(y/x), the signs of both x and y are considered.")
|
|
FUNC1(atanh, m_atanh, 0,
|
|
"atanh(x)\n\nReturn the inverse hyperbolic tangent of x.")
|
|
|
|
static PyObject * math_ceil(PyObject *self, PyObject *number) {
|
|
_Py_IDENTIFIER(__ceil__);
|
|
PyObject *method, *result;
|
|
|
|
method = _PyObject_LookupSpecial(number, &PyId___ceil__);
|
|
if (method == NULL) {
|
|
if (PyErr_Occurred())
|
|
return NULL;
|
|
return math_1_to_int(number, ceil, 0);
|
|
}
|
|
result = PyObject_CallFunctionObjArgs(method, NULL);
|
|
Py_DECREF(method);
|
|
return result;
|
|
}
|
|
|
|
PyDoc_STRVAR(math_ceil_doc,
|
|
"ceil(x)\n\nReturn the ceiling of x as an int.\n"
|
|
"This is the smallest integral value >= x.");
|
|
|
|
FUNC2(copysign, copysign,
|
|
"copysign(x, y)\n\nReturn a float with the magnitude (absolute value) "
|
|
"of x but the sign \nof y. On platforms that support signed zeros, "
|
|
"copysign(1.0, -0.0) \nreturns -1.0.\n")
|
|
FUNC1(cos, cos, 0,
|
|
"cos(x)\n\nReturn the cosine of x (measured in radians).")
|
|
FUNC1(cosh, cosh, 1,
|
|
"cosh(x)\n\nReturn the hyperbolic cosine of x.")
|
|
FUNC1A(erf, m_erf,
|
|
"erf(x)\n\nError function at x.")
|
|
FUNC1A(erfc, m_erfc,
|
|
"erfc(x)\n\nComplementary error function at x.")
|
|
FUNC1(exp, exp, 1,
|
|
"exp(x)\n\nReturn e raised to the power of x.")
|
|
FUNC1(expm1, m_expm1, 1,
|
|
"expm1(x)\n\nReturn exp(x)-1.\n"
|
|
"This function avoids the loss of precision involved in the direct "
|
|
"evaluation of exp(x)-1 for small x.")
|
|
FUNC1(fabs, fabs, 0,
|
|
"fabs(x)\n\nReturn the absolute value of the float x.")
|
|
|
|
static PyObject * math_floor(PyObject *self, PyObject *number) {
|
|
_Py_IDENTIFIER(__floor__);
|
|
PyObject *method, *result;
|
|
|
|
method = _PyObject_LookupSpecial(number, &PyId___floor__);
|
|
if (method == NULL) {
|
|
if (PyErr_Occurred())
|
|
return NULL;
|
|
return math_1_to_int(number, floor, 0);
|
|
}
|
|
result = PyObject_CallFunctionObjArgs(method, NULL);
|
|
Py_DECREF(method);
|
|
return result;
|
|
}
|
|
|
|
PyDoc_STRVAR(math_floor_doc,
|
|
"floor(x)\n\nReturn the floor of x as an int.\n"
|
|
"This is the largest integral value <= x.");
|
|
|
|
FUNC1A(gamma, m_tgamma,
|
|
"gamma(x)\n\nGamma function at x.")
|
|
FUNC1A(lgamma, m_lgamma,
|
|
"lgamma(x)\n\nNatural logarithm of absolute value of Gamma function at x.")
|
|
FUNC1(log1p, m_log1p, 0,
|
|
"log1p(x)\n\nReturn the natural logarithm of 1+x (base e).\n"
|
|
"The result is computed in a way which is accurate for x near zero.")
|
|
FUNC1(sin, sin, 0,
|
|
"sin(x)\n\nReturn the sine of x (measured in radians).")
|
|
FUNC1(sinh, sinh, 1,
|
|
"sinh(x)\n\nReturn the hyperbolic sine of x.")
|
|
FUNC1(sqrt, sqrt, 0,
|
|
"sqrt(x)\n\nReturn the square root of x.")
|
|
FUNC1(tan, tan, 0,
|
|
"tan(x)\n\nReturn the tangent of x (measured in radians).")
|
|
FUNC1(tanh, tanh, 0,
|
|
"tanh(x)\n\nReturn the hyperbolic tangent of x.")
|
|
|
|
/* Precision summation function as msum() by Raymond Hettinger in
|
|
<http://aspn.activestate.com/ASPN/Cookbook/Python/Recipe/393090>,
|
|
enhanced with the exact partials sum and roundoff from Mark
|
|
Dickinson's post at <http://bugs.python.org/file10357/msum4.py>.
|
|
See those links for more details, proofs and other references.
|
|
|
|
Note 1: IEEE 754R floating point semantics are assumed,
|
|
but the current implementation does not re-establish special
|
|
value semantics across iterations (i.e. handling -Inf + Inf).
|
|
|
|
Note 2: No provision is made for intermediate overflow handling;
|
|
therefore, sum([1e+308, 1e-308, 1e+308]) returns 1e+308 while
|
|
sum([1e+308, 1e+308, 1e-308]) raises an OverflowError due to the
|
|
overflow of the first partial sum.
|
|
|
|
Note 3: The intermediate values lo, yr, and hi are declared volatile so
|
|
aggressive compilers won't algebraically reduce lo to always be exactly 0.0.
|
|
Also, the volatile declaration forces the values to be stored in memory as
|
|
regular doubles instead of extended long precision (80-bit) values. This
|
|
prevents double rounding because any addition or subtraction of two doubles
|
|
can be resolved exactly into double-sized hi and lo values. As long as the
|
|
hi value gets forced into a double before yr and lo are computed, the extra
|
|
bits in downstream extended precision operations (x87 for example) will be
|
|
exactly zero and therefore can be losslessly stored back into a double,
|
|
thereby preventing double rounding.
|
|
|
|
Note 4: A similar implementation is in Modules/cmathmodule.c.
|
|
Be sure to update both when making changes.
|
|
|
|
Note 5: The signature of math.fsum() differs from builtins.sum()
|
|
because the start argument doesn't make sense in the context of
|
|
accurate summation. Since the partials table is collapsed before
|
|
returning a result, sum(seq2, start=sum(seq1)) may not equal the
|
|
accurate result returned by sum(itertools.chain(seq1, seq2)).
|
|
*/
|
|
|
|
#define NUM_PARTIALS 32 /* initial partials array size, on stack */
|
|
|
|
/* Extend the partials array p[] by doubling its size. */
|
|
static int /* non-zero on error */
|
|
_fsum_realloc(double **p_ptr, Py_ssize_t n,
|
|
double *ps, Py_ssize_t *m_ptr)
|
|
{
|
|
void *v = NULL;
|
|
Py_ssize_t m = *m_ptr;
|
|
|
|
m += m; /* double */
|
|
if (n < m && (size_t)m < ((size_t)PY_SSIZE_T_MAX / sizeof(double))) {
|
|
double *p = *p_ptr;
|
|
if (p == ps) {
|
|
v = PyMem_Malloc(sizeof(double) * m);
|
|
if (v != NULL)
|
|
memcpy(v, ps, sizeof(double) * n);
|
|
}
|
|
else
|
|
v = PyMem_Realloc(p, sizeof(double) * m);
|
|
}
|
|
if (v == NULL) { /* size overflow or no memory */
|
|
PyErr_SetString(PyExc_MemoryError, "math.fsum partials");
|
|
return 1;
|
|
}
|
|
*p_ptr = (double*) v;
|
|
*m_ptr = m;
|
|
return 0;
|
|
}
|
|
|
|
/* Full precision summation of a sequence of floats.
|
|
|
|
def msum(iterable):
|
|
partials = [] # sorted, non-overlapping partial sums
|
|
for x in iterable:
|
|
i = 0
|
|
for y in partials:
|
|
if abs(x) < abs(y):
|
|
x, y = y, x
|
|
hi = x + y
|
|
lo = y - (hi - x)
|
|
if lo:
|
|
partials[i] = lo
|
|
i += 1
|
|
x = hi
|
|
partials[i:] = [x]
|
|
return sum_exact(partials)
|
|
|
|
Rounded x+y stored in hi with the roundoff stored in lo. Together hi+lo
|
|
are exactly equal to x+y. The inner loop applies hi/lo summation to each
|
|
partial so that the list of partial sums remains exact.
|
|
|
|
Sum_exact() adds the partial sums exactly and correctly rounds the final
|
|
result (using the round-half-to-even rule). The items in partials remain
|
|
non-zero, non-special, non-overlapping and strictly increasing in
|
|
magnitude, but possibly not all having the same sign.
|
|
|
|
Depends on IEEE 754 arithmetic guarantees and half-even rounding.
|
|
*/
|
|
|
|
static PyObject*
|
|
math_fsum(PyObject *self, PyObject *seq)
|
|
{
|
|
PyObject *item, *iter, *sum = NULL;
|
|
Py_ssize_t i, j, n = 0, m = NUM_PARTIALS;
|
|
double x, y, t, ps[NUM_PARTIALS], *p = ps;
|
|
double xsave, special_sum = 0.0, inf_sum = 0.0;
|
|
volatile double hi, yr, lo;
|
|
|
|
iter = PyObject_GetIter(seq);
|
|
if (iter == NULL)
|
|
return NULL;
|
|
|
|
PyFPE_START_PROTECT("fsum", Py_DECREF(iter); return NULL)
|
|
|
|
for(;;) { /* for x in iterable */
|
|
assert(0 <= n && n <= m);
|
|
assert((m == NUM_PARTIALS && p == ps) ||
|
|
(m > NUM_PARTIALS && p != NULL));
|
|
|
|
item = PyIter_Next(iter);
|
|
if (item == NULL) {
|
|
if (PyErr_Occurred())
|
|
goto _fsum_error;
|
|
break;
|
|
}
|
|
x = PyFloat_AsDouble(item);
|
|
Py_DECREF(item);
|
|
if (PyErr_Occurred())
|
|
goto _fsum_error;
|
|
|
|
xsave = x;
|
|
for (i = j = 0; j < n; j++) { /* for y in partials */
|
|
y = p[j];
|
|
if (fabs(x) < fabs(y)) {
|
|
t = x; x = y; y = t;
|
|
}
|
|
hi = x + y;
|
|
yr = hi - x;
|
|
lo = y - yr;
|
|
if (lo != 0.0)
|
|
p[i++] = lo;
|
|
x = hi;
|
|
}
|
|
|
|
n = i; /* ps[i:] = [x] */
|
|
if (x != 0.0) {
|
|
if (! Py_IS_FINITE(x)) {
|
|
/* a nonfinite x could arise either as
|
|
a result of intermediate overflow, or
|
|
as a result of a nan or inf in the
|
|
summands */
|
|
if (Py_IS_FINITE(xsave)) {
|
|
PyErr_SetString(PyExc_OverflowError,
|
|
"intermediate overflow in fsum");
|
|
goto _fsum_error;
|
|
}
|
|
if (Py_IS_INFINITY(xsave))
|
|
inf_sum += xsave;
|
|
special_sum += xsave;
|
|
/* reset partials */
|
|
n = 0;
|
|
}
|
|
else if (n >= m && _fsum_realloc(&p, n, ps, &m))
|
|
goto _fsum_error;
|
|
else
|
|
p[n++] = x;
|
|
}
|
|
}
|
|
|
|
if (special_sum != 0.0) {
|
|
if (Py_IS_NAN(inf_sum))
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"-inf + inf in fsum");
|
|
else
|
|
sum = PyFloat_FromDouble(special_sum);
|
|
goto _fsum_error;
|
|
}
|
|
|
|
hi = 0.0;
|
|
if (n > 0) {
|
|
hi = p[--n];
|
|
/* sum_exact(ps, hi) from the top, stop when the sum becomes
|
|
inexact. */
|
|
while (n > 0) {
|
|
x = hi;
|
|
y = p[--n];
|
|
assert(fabs(y) < fabs(x));
|
|
hi = x + y;
|
|
yr = hi - x;
|
|
lo = y - yr;
|
|
if (lo != 0.0)
|
|
break;
|
|
}
|
|
/* Make half-even rounding work across multiple partials.
|
|
Needed so that sum([1e-16, 1, 1e16]) will round-up the last
|
|
digit to two instead of down to zero (the 1e-16 makes the 1
|
|
slightly closer to two). With a potential 1 ULP rounding
|
|
error fixed-up, math.fsum() can guarantee commutativity. */
|
|
if (n > 0 && ((lo < 0.0 && p[n-1] < 0.0) ||
|
|
(lo > 0.0 && p[n-1] > 0.0))) {
|
|
y = lo * 2.0;
|
|
x = hi + y;
|
|
yr = x - hi;
|
|
if (y == yr)
|
|
hi = x;
|
|
}
|
|
}
|
|
sum = PyFloat_FromDouble(hi);
|
|
|
|
_fsum_error:
|
|
PyFPE_END_PROTECT(hi)
|
|
Py_DECREF(iter);
|
|
if (p != ps)
|
|
PyMem_Free(p);
|
|
return sum;
|
|
}
|
|
|
|
#undef NUM_PARTIALS
|
|
|
|
PyDoc_STRVAR(math_fsum_doc,
|
|
"fsum(iterable)\n\n\
|
|
Return an accurate floating point sum of values in the iterable.\n\
|
|
Assumes IEEE-754 floating point arithmetic.");
|
|
|
|
/* Return the smallest integer k such that n < 2**k, or 0 if n == 0.
|
|
* Equivalent to floor(lg(x))+1. Also equivalent to: bitwidth_of_type -
|
|
* count_leading_zero_bits(x)
|
|
*/
|
|
|
|
/* XXX: This routine does more or less the same thing as
|
|
* bits_in_digit() in Objects/longobject.c. Someday it would be nice to
|
|
* consolidate them. On BSD, there's a library function called fls()
|
|
* that we could use, and GCC provides __builtin_clz().
|
|
*/
|
|
|
|
static unsigned long
|
|
bit_length(unsigned long n)
|
|
{
|
|
unsigned long len = 0;
|
|
while (n != 0) {
|
|
++len;
|
|
n >>= 1;
|
|
}
|
|
return len;
|
|
}
|
|
|
|
static unsigned long
|
|
count_set_bits(unsigned long n)
|
|
{
|
|
unsigned long count = 0;
|
|
while (n != 0) {
|
|
++count;
|
|
n &= n - 1; /* clear least significant bit */
|
|
}
|
|
return count;
|
|
}
|
|
|
|
/* Divide-and-conquer factorial algorithm
|
|
*
|
|
* Based on the formula and psuedo-code provided at:
|
|
* http://www.luschny.de/math/factorial/binarysplitfact.html
|
|
*
|
|
* Faster algorithms exist, but they're more complicated and depend on
|
|
* a fast prime factorization algorithm.
|
|
*
|
|
* Notes on the algorithm
|
|
* ----------------------
|
|
*
|
|
* factorial(n) is written in the form 2**k * m, with m odd. k and m are
|
|
* computed separately, and then combined using a left shift.
|
|
*
|
|
* The function factorial_odd_part computes the odd part m (i.e., the greatest
|
|
* odd divisor) of factorial(n), using the formula:
|
|
*
|
|
* factorial_odd_part(n) =
|
|
*
|
|
* product_{i >= 0} product_{0 < j <= n / 2**i, j odd} j
|
|
*
|
|
* Example: factorial_odd_part(20) =
|
|
*
|
|
* (1) *
|
|
* (1) *
|
|
* (1 * 3 * 5) *
|
|
* (1 * 3 * 5 * 7 * 9)
|
|
* (1 * 3 * 5 * 7 * 9 * 11 * 13 * 15 * 17 * 19)
|
|
*
|
|
* Here i goes from large to small: the first term corresponds to i=4 (any
|
|
* larger i gives an empty product), and the last term corresponds to i=0.
|
|
* Each term can be computed from the last by multiplying by the extra odd
|
|
* numbers required: e.g., to get from the penultimate term to the last one,
|
|
* we multiply by (11 * 13 * 15 * 17 * 19).
|
|
*
|
|
* To see a hint of why this formula works, here are the same numbers as above
|
|
* but with the even parts (i.e., the appropriate powers of 2) included. For
|
|
* each subterm in the product for i, we multiply that subterm by 2**i:
|
|
*
|
|
* factorial(20) =
|
|
*
|
|
* (16) *
|
|
* (8) *
|
|
* (4 * 12 * 20) *
|
|
* (2 * 6 * 10 * 14 * 18) *
|
|
* (1 * 3 * 5 * 7 * 9 * 11 * 13 * 15 * 17 * 19)
|
|
*
|
|
* The factorial_partial_product function computes the product of all odd j in
|
|
* range(start, stop) for given start and stop. It's used to compute the
|
|
* partial products like (11 * 13 * 15 * 17 * 19) in the example above. It
|
|
* operates recursively, repeatedly splitting the range into two roughly equal
|
|
* pieces until the subranges are small enough to be computed using only C
|
|
* integer arithmetic.
|
|
*
|
|
* The two-valuation k (i.e., the exponent of the largest power of 2 dividing
|
|
* the factorial) is computed independently in the main math_factorial
|
|
* function. By standard results, its value is:
|
|
*
|
|
* two_valuation = n//2 + n//4 + n//8 + ....
|
|
*
|
|
* It can be shown (e.g., by complete induction on n) that two_valuation is
|
|
* equal to n - count_set_bits(n), where count_set_bits(n) gives the number of
|
|
* '1'-bits in the binary expansion of n.
|
|
*/
|
|
|
|
/* factorial_partial_product: Compute product(range(start, stop, 2)) using
|
|
* divide and conquer. Assumes start and stop are odd and stop > start.
|
|
* max_bits must be >= bit_length(stop - 2). */
|
|
|
|
static PyObject *
|
|
factorial_partial_product(unsigned long start, unsigned long stop,
|
|
unsigned long max_bits)
|
|
{
|
|
unsigned long midpoint, num_operands;
|
|
PyObject *left = NULL, *right = NULL, *result = NULL;
|
|
|
|
/* If the return value will fit an unsigned long, then we can
|
|
* multiply in a tight, fast loop where each multiply is O(1).
|
|
* Compute an upper bound on the number of bits required to store
|
|
* the answer.
|
|
*
|
|
* Storing some integer z requires floor(lg(z))+1 bits, which is
|
|
* conveniently the value returned by bit_length(z). The
|
|
* product x*y will require at most
|
|
* bit_length(x) + bit_length(y) bits to store, based
|
|
* on the idea that lg product = lg x + lg y.
|
|
*
|
|
* We know that stop - 2 is the largest number to be multiplied. From
|
|
* there, we have: bit_length(answer) <= num_operands *
|
|
* bit_length(stop - 2)
|
|
*/
|
|
|
|
num_operands = (stop - start) / 2;
|
|
/* The "num_operands <= 8 * SIZEOF_LONG" check guards against the
|
|
* unlikely case of an overflow in num_operands * max_bits. */
|
|
if (num_operands <= 8 * SIZEOF_LONG &&
|
|
num_operands * max_bits <= 8 * SIZEOF_LONG) {
|
|
unsigned long j, total;
|
|
for (total = start, j = start + 2; j < stop; j += 2)
|
|
total *= j;
|
|
return PyLong_FromUnsignedLong(total);
|
|
}
|
|
|
|
/* find midpoint of range(start, stop), rounded up to next odd number. */
|
|
midpoint = (start + num_operands) | 1;
|
|
left = factorial_partial_product(start, midpoint,
|
|
bit_length(midpoint - 2));
|
|
if (left == NULL)
|
|
goto error;
|
|
right = factorial_partial_product(midpoint, stop, max_bits);
|
|
if (right == NULL)
|
|
goto error;
|
|
result = PyNumber_Multiply(left, right);
|
|
|
|
error:
|
|
Py_XDECREF(left);
|
|
Py_XDECREF(right);
|
|
return result;
|
|
}
|
|
|
|
/* factorial_odd_part: compute the odd part of factorial(n). */
|
|
|
|
static PyObject *
|
|
factorial_odd_part(unsigned long n)
|
|
{
|
|
long i;
|
|
unsigned long v, lower, upper;
|
|
PyObject *partial, *tmp, *inner, *outer;
|
|
|
|
inner = PyLong_FromLong(1);
|
|
if (inner == NULL)
|
|
return NULL;
|
|
outer = inner;
|
|
Py_INCREF(outer);
|
|
|
|
upper = 3;
|
|
for (i = bit_length(n) - 2; i >= 0; i--) {
|
|
v = n >> i;
|
|
if (v <= 2)
|
|
continue;
|
|
lower = upper;
|
|
/* (v + 1) | 1 = least odd integer strictly larger than n / 2**i */
|
|
upper = (v + 1) | 1;
|
|
/* Here inner is the product of all odd integers j in the range (0,
|
|
n/2**(i+1)]. The factorial_partial_product call below gives the
|
|
product of all odd integers j in the range (n/2**(i+1), n/2**i]. */
|
|
partial = factorial_partial_product(lower, upper, bit_length(upper-2));
|
|
/* inner *= partial */
|
|
if (partial == NULL)
|
|
goto error;
|
|
tmp = PyNumber_Multiply(inner, partial);
|
|
Py_DECREF(partial);
|
|
if (tmp == NULL)
|
|
goto error;
|
|
Py_DECREF(inner);
|
|
inner = tmp;
|
|
/* Now inner is the product of all odd integers j in the range (0,
|
|
n/2**i], giving the inner product in the formula above. */
|
|
|
|
/* outer *= inner; */
|
|
tmp = PyNumber_Multiply(outer, inner);
|
|
if (tmp == NULL)
|
|
goto error;
|
|
Py_DECREF(outer);
|
|
outer = tmp;
|
|
}
|
|
Py_DECREF(inner);
|
|
return outer;
|
|
|
|
error:
|
|
Py_DECREF(outer);
|
|
Py_DECREF(inner);
|
|
return NULL;
|
|
}
|
|
|
|
/* Lookup table for small factorial values */
|
|
|
|
static const unsigned long SmallFactorials[] = {
|
|
1, 1, 2, 6, 24, 120, 720, 5040, 40320,
|
|
362880, 3628800, 39916800, 479001600,
|
|
#if SIZEOF_LONG >= 8
|
|
6227020800, 87178291200, 1307674368000,
|
|
20922789888000, 355687428096000, 6402373705728000,
|
|
121645100408832000, 2432902008176640000
|
|
#endif
|
|
};
|
|
|
|
static PyObject *
|
|
math_factorial(PyObject *self, PyObject *arg)
|
|
{
|
|
long x;
|
|
int overflow;
|
|
PyObject *result, *odd_part, *two_valuation;
|
|
|
|
if (PyFloat_Check(arg)) {
|
|
PyObject *lx;
|
|
double dx = PyFloat_AS_DOUBLE((PyFloatObject *)arg);
|
|
if (!(Py_IS_FINITE(dx) && dx == floor(dx))) {
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"factorial() only accepts integral values");
|
|
return NULL;
|
|
}
|
|
lx = PyLong_FromDouble(dx);
|
|
if (lx == NULL)
|
|
return NULL;
|
|
x = PyLong_AsLongAndOverflow(lx, &overflow);
|
|
Py_DECREF(lx);
|
|
}
|
|
else
|
|
x = PyLong_AsLongAndOverflow(arg, &overflow);
|
|
|
|
if (x == -1 && PyErr_Occurred()) {
|
|
return NULL;
|
|
}
|
|
else if (overflow == 1) {
|
|
PyErr_Format(PyExc_OverflowError,
|
|
"factorial() argument should not exceed %ld",
|
|
LONG_MAX);
|
|
return NULL;
|
|
}
|
|
else if (overflow == -1 || x < 0) {
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"factorial() not defined for negative values");
|
|
return NULL;
|
|
}
|
|
|
|
/* use lookup table if x is small */
|
|
if (x < (long)Py_ARRAY_LENGTH(SmallFactorials))
|
|
return PyLong_FromUnsignedLong(SmallFactorials[x]);
|
|
|
|
/* else express in the form odd_part * 2**two_valuation, and compute as
|
|
odd_part << two_valuation. */
|
|
odd_part = factorial_odd_part(x);
|
|
if (odd_part == NULL)
|
|
return NULL;
|
|
two_valuation = PyLong_FromLong(x - count_set_bits(x));
|
|
if (two_valuation == NULL) {
|
|
Py_DECREF(odd_part);
|
|
return NULL;
|
|
}
|
|
result = PyNumber_Lshift(odd_part, two_valuation);
|
|
Py_DECREF(two_valuation);
|
|
Py_DECREF(odd_part);
|
|
return result;
|
|
}
|
|
|
|
PyDoc_STRVAR(math_factorial_doc,
|
|
"factorial(x) -> Integral\n"
|
|
"\n"
|
|
"Find x!. Raise a ValueError if x is negative or non-integral.");
|
|
|
|
static PyObject *
|
|
math_trunc(PyObject *self, PyObject *number)
|
|
{
|
|
_Py_IDENTIFIER(__trunc__);
|
|
PyObject *trunc, *result;
|
|
|
|
if (Py_TYPE(number)->tp_dict == NULL) {
|
|
if (PyType_Ready(Py_TYPE(number)) < 0)
|
|
return NULL;
|
|
}
|
|
|
|
trunc = _PyObject_LookupSpecial(number, &PyId___trunc__);
|
|
if (trunc == NULL) {
|
|
if (!PyErr_Occurred())
|
|
PyErr_Format(PyExc_TypeError,
|
|
"type %.100s doesn't define __trunc__ method",
|
|
Py_TYPE(number)->tp_name);
|
|
return NULL;
|
|
}
|
|
result = PyObject_CallFunctionObjArgs(trunc, NULL);
|
|
Py_DECREF(trunc);
|
|
return result;
|
|
}
|
|
|
|
PyDoc_STRVAR(math_trunc_doc,
|
|
"trunc(x:Real) -> Integral\n"
|
|
"\n"
|
|
"Truncates x to the nearest Integral toward 0. Uses the __trunc__ magic method.");
|
|
|
|
static PyObject *
|
|
math_frexp(PyObject *self, PyObject *arg)
|
|
{
|
|
int i;
|
|
double x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
/* deal with special cases directly, to sidestep platform
|
|
differences */
|
|
if (Py_IS_NAN(x) || Py_IS_INFINITY(x) || !x) {
|
|
i = 0;
|
|
}
|
|
else {
|
|
PyFPE_START_PROTECT("in math_frexp", return 0);
|
|
x = frexp(x, &i);
|
|
PyFPE_END_PROTECT(x);
|
|
}
|
|
return Py_BuildValue("(di)", x, i);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_frexp_doc,
|
|
"frexp(x)\n"
|
|
"\n"
|
|
"Return the mantissa and exponent of x, as pair (m, e).\n"
|
|
"m is a float and e is an int, such that x = m * 2.**e.\n"
|
|
"If x is 0, m and e are both 0. Else 0.5 <= abs(m) < 1.0.");
|
|
|
|
static PyObject *
|
|
math_ldexp(PyObject *self, PyObject *args)
|
|
{
|
|
double x, r;
|
|
PyObject *oexp;
|
|
long exp;
|
|
int overflow;
|
|
if (! PyArg_ParseTuple(args, "dO:ldexp", &x, &oexp))
|
|
return NULL;
|
|
|
|
if (PyLong_Check(oexp)) {
|
|
/* on overflow, replace exponent with either LONG_MAX
|
|
or LONG_MIN, depending on the sign. */
|
|
exp = PyLong_AsLongAndOverflow(oexp, &overflow);
|
|
if (exp == -1 && PyErr_Occurred())
|
|
return NULL;
|
|
if (overflow)
|
|
exp = overflow < 0 ? LONG_MIN : LONG_MAX;
|
|
}
|
|
else {
|
|
PyErr_SetString(PyExc_TypeError,
|
|
"Expected an int as second argument to ldexp.");
|
|
return NULL;
|
|
}
|
|
|
|
if (x == 0. || !Py_IS_FINITE(x)) {
|
|
/* NaNs, zeros and infinities are returned unchanged */
|
|
r = x;
|
|
errno = 0;
|
|
} else if (exp > INT_MAX) {
|
|
/* overflow */
|
|
r = copysign(Py_HUGE_VAL, x);
|
|
errno = ERANGE;
|
|
} else if (exp < INT_MIN) {
|
|
/* underflow to +-0 */
|
|
r = copysign(0., x);
|
|
errno = 0;
|
|
} else {
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_ldexp", return 0);
|
|
r = ldexp(x, (int)exp);
|
|
PyFPE_END_PROTECT(r);
|
|
if (Py_IS_INFINITY(r))
|
|
errno = ERANGE;
|
|
}
|
|
|
|
if (errno && is_error(r))
|
|
return NULL;
|
|
return PyFloat_FromDouble(r);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_ldexp_doc,
|
|
"ldexp(x, i)\n\n\
|
|
Return x * (2**i).");
|
|
|
|
static PyObject *
|
|
math_modf(PyObject *self, PyObject *arg)
|
|
{
|
|
double y, x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
/* some platforms don't do the right thing for NaNs and
|
|
infinities, so we take care of special cases directly. */
|
|
if (!Py_IS_FINITE(x)) {
|
|
if (Py_IS_INFINITY(x))
|
|
return Py_BuildValue("(dd)", copysign(0., x), x);
|
|
else if (Py_IS_NAN(x))
|
|
return Py_BuildValue("(dd)", x, x);
|
|
}
|
|
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_modf", return 0);
|
|
x = modf(x, &y);
|
|
PyFPE_END_PROTECT(x);
|
|
return Py_BuildValue("(dd)", x, y);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_modf_doc,
|
|
"modf(x)\n"
|
|
"\n"
|
|
"Return the fractional and integer parts of x. Both results carry the sign\n"
|
|
"of x and are floats.");
|
|
|
|
/* A decent logarithm is easy to compute even for huge ints, but libm can't
|
|
do that by itself -- loghelper can. func is log or log10, and name is
|
|
"log" or "log10". Note that overflow of the result isn't possible: an int
|
|
can contain no more than INT_MAX * SHIFT bits, so has value certainly less
|
|
than 2**(2**64 * 2**16) == 2**2**80, and log2 of that is 2**80, which is
|
|
small enough to fit in an IEEE single. log and log10 are even smaller.
|
|
However, intermediate overflow is possible for an int if the number of bits
|
|
in that int is larger than PY_SSIZE_T_MAX. */
|
|
|
|
static PyObject*
|
|
loghelper(PyObject* arg, double (*func)(double), char *funcname)
|
|
{
|
|
/* If it is int, do it ourselves. */
|
|
if (PyLong_Check(arg)) {
|
|
double x, result;
|
|
Py_ssize_t e;
|
|
|
|
/* Negative or zero inputs give a ValueError. */
|
|
if (Py_SIZE(arg) <= 0) {
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"math domain error");
|
|
return NULL;
|
|
}
|
|
|
|
x = PyLong_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred()) {
|
|
if (!PyErr_ExceptionMatches(PyExc_OverflowError))
|
|
return NULL;
|
|
/* Here the conversion to double overflowed, but it's possible
|
|
to compute the log anyway. Clear the exception and continue. */
|
|
PyErr_Clear();
|
|
x = _PyLong_Frexp((PyLongObject *)arg, &e);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
/* Value is ~= x * 2**e, so the log ~= log(x) + log(2) * e. */
|
|
result = func(x) + func(2.0) * e;
|
|
}
|
|
else
|
|
/* Successfully converted x to a double. */
|
|
result = func(x);
|
|
return PyFloat_FromDouble(result);
|
|
}
|
|
|
|
/* Else let libm handle it by itself. */
|
|
return math_1(arg, func, 0);
|
|
}
|
|
|
|
static PyObject *
|
|
math_log(PyObject *self, PyObject *args)
|
|
{
|
|
PyObject *arg;
|
|
PyObject *base = NULL;
|
|
PyObject *num, *den;
|
|
PyObject *ans;
|
|
|
|
if (!PyArg_UnpackTuple(args, "log", 1, 2, &arg, &base))
|
|
return NULL;
|
|
|
|
num = loghelper(arg, m_log, "log");
|
|
if (num == NULL || base == NULL)
|
|
return num;
|
|
|
|
den = loghelper(base, m_log, "log");
|
|
if (den == NULL) {
|
|
Py_DECREF(num);
|
|
return NULL;
|
|
}
|
|
|
|
ans = PyNumber_TrueDivide(num, den);
|
|
Py_DECREF(num);
|
|
Py_DECREF(den);
|
|
return ans;
|
|
}
|
|
|
|
PyDoc_STRVAR(math_log_doc,
|
|
"log(x[, base])\n\n\
|
|
Return the logarithm of x to the given base.\n\
|
|
If the base not specified, returns the natural logarithm (base e) of x.");
|
|
|
|
static PyObject *
|
|
math_log2(PyObject *self, PyObject *arg)
|
|
{
|
|
return loghelper(arg, m_log2, "log2");
|
|
}
|
|
|
|
PyDoc_STRVAR(math_log2_doc,
|
|
"log2(x)\n\nReturn the base 2 logarithm of x.");
|
|
|
|
static PyObject *
|
|
math_log10(PyObject *self, PyObject *arg)
|
|
{
|
|
return loghelper(arg, m_log10, "log10");
|
|
}
|
|
|
|
PyDoc_STRVAR(math_log10_doc,
|
|
"log10(x)\n\nReturn the base 10 logarithm of x.");
|
|
|
|
static PyObject *
|
|
math_fmod(PyObject *self, PyObject *args)
|
|
{
|
|
PyObject *ox, *oy;
|
|
double r, x, y;
|
|
if (! PyArg_UnpackTuple(args, "fmod", 2, 2, &ox, &oy))
|
|
return NULL;
|
|
x = PyFloat_AsDouble(ox);
|
|
y = PyFloat_AsDouble(oy);
|
|
if ((x == -1.0 || y == -1.0) && PyErr_Occurred())
|
|
return NULL;
|
|
/* fmod(x, +/-Inf) returns x for finite x. */
|
|
if (Py_IS_INFINITY(y) && Py_IS_FINITE(x))
|
|
return PyFloat_FromDouble(x);
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_fmod", return 0);
|
|
r = fmod(x, y);
|
|
PyFPE_END_PROTECT(r);
|
|
if (Py_IS_NAN(r)) {
|
|
if (!Py_IS_NAN(x) && !Py_IS_NAN(y))
|
|
errno = EDOM;
|
|
else
|
|
errno = 0;
|
|
}
|
|
if (errno && is_error(r))
|
|
return NULL;
|
|
else
|
|
return PyFloat_FromDouble(r);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_fmod_doc,
|
|
"fmod(x, y)\n\nReturn fmod(x, y), according to platform C."
|
|
" x % y may differ.");
|
|
|
|
static PyObject *
|
|
math_hypot(PyObject *self, PyObject *args)
|
|
{
|
|
PyObject *ox, *oy;
|
|
double r, x, y;
|
|
if (! PyArg_UnpackTuple(args, "hypot", 2, 2, &ox, &oy))
|
|
return NULL;
|
|
x = PyFloat_AsDouble(ox);
|
|
y = PyFloat_AsDouble(oy);
|
|
if ((x == -1.0 || y == -1.0) && PyErr_Occurred())
|
|
return NULL;
|
|
/* hypot(x, +/-Inf) returns Inf, even if x is a NaN. */
|
|
if (Py_IS_INFINITY(x))
|
|
return PyFloat_FromDouble(fabs(x));
|
|
if (Py_IS_INFINITY(y))
|
|
return PyFloat_FromDouble(fabs(y));
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_hypot", return 0);
|
|
r = hypot(x, y);
|
|
PyFPE_END_PROTECT(r);
|
|
if (Py_IS_NAN(r)) {
|
|
if (!Py_IS_NAN(x) && !Py_IS_NAN(y))
|
|
errno = EDOM;
|
|
else
|
|
errno = 0;
|
|
}
|
|
else if (Py_IS_INFINITY(r)) {
|
|
if (Py_IS_FINITE(x) && Py_IS_FINITE(y))
|
|
errno = ERANGE;
|
|
else
|
|
errno = 0;
|
|
}
|
|
if (errno && is_error(r))
|
|
return NULL;
|
|
else
|
|
return PyFloat_FromDouble(r);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_hypot_doc,
|
|
"hypot(x, y)\n\nReturn the Euclidean distance, sqrt(x*x + y*y).");
|
|
|
|
/* pow can't use math_2, but needs its own wrapper: the problem is
|
|
that an infinite result can arise either as a result of overflow
|
|
(in which case OverflowError should be raised) or as a result of
|
|
e.g. 0.**-5. (for which ValueError needs to be raised.)
|
|
*/
|
|
|
|
static PyObject *
|
|
math_pow(PyObject *self, PyObject *args)
|
|
{
|
|
PyObject *ox, *oy;
|
|
double r, x, y;
|
|
int odd_y;
|
|
|
|
if (! PyArg_UnpackTuple(args, "pow", 2, 2, &ox, &oy))
|
|
return NULL;
|
|
x = PyFloat_AsDouble(ox);
|
|
y = PyFloat_AsDouble(oy);
|
|
if ((x == -1.0 || y == -1.0) && PyErr_Occurred())
|
|
return NULL;
|
|
|
|
/* deal directly with IEEE specials, to cope with problems on various
|
|
platforms whose semantics don't exactly match C99 */
|
|
r = 0.; /* silence compiler warning */
|
|
if (!Py_IS_FINITE(x) || !Py_IS_FINITE(y)) {
|
|
errno = 0;
|
|
if (Py_IS_NAN(x))
|
|
r = y == 0. ? 1. : x; /* NaN**0 = 1 */
|
|
else if (Py_IS_NAN(y))
|
|
r = x == 1. ? 1. : y; /* 1**NaN = 1 */
|
|
else if (Py_IS_INFINITY(x)) {
|
|
odd_y = Py_IS_FINITE(y) && fmod(fabs(y), 2.0) == 1.0;
|
|
if (y > 0.)
|
|
r = odd_y ? x : fabs(x);
|
|
else if (y == 0.)
|
|
r = 1.;
|
|
else /* y < 0. */
|
|
r = odd_y ? copysign(0., x) : 0.;
|
|
}
|
|
else if (Py_IS_INFINITY(y)) {
|
|
if (fabs(x) == 1.0)
|
|
r = 1.;
|
|
else if (y > 0. && fabs(x) > 1.0)
|
|
r = y;
|
|
else if (y < 0. && fabs(x) < 1.0) {
|
|
r = -y; /* result is +inf */
|
|
if (x == 0.) /* 0**-inf: divide-by-zero */
|
|
errno = EDOM;
|
|
}
|
|
else
|
|
r = 0.;
|
|
}
|
|
}
|
|
else {
|
|
/* let libm handle finite**finite */
|
|
errno = 0;
|
|
PyFPE_START_PROTECT("in math_pow", return 0);
|
|
r = pow(x, y);
|
|
PyFPE_END_PROTECT(r);
|
|
/* a NaN result should arise only from (-ve)**(finite
|
|
non-integer); in this case we want to raise ValueError. */
|
|
if (!Py_IS_FINITE(r)) {
|
|
if (Py_IS_NAN(r)) {
|
|
errno = EDOM;
|
|
}
|
|
/*
|
|
an infinite result here arises either from:
|
|
(A) (+/-0.)**negative (-> divide-by-zero)
|
|
(B) overflow of x**y with x and y finite
|
|
*/
|
|
else if (Py_IS_INFINITY(r)) {
|
|
if (x == 0.)
|
|
errno = EDOM;
|
|
else
|
|
errno = ERANGE;
|
|
}
|
|
}
|
|
}
|
|
|
|
if (errno && is_error(r))
|
|
return NULL;
|
|
else
|
|
return PyFloat_FromDouble(r);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_pow_doc,
|
|
"pow(x, y)\n\nReturn x**y (x to the power of y).");
|
|
|
|
static const double degToRad = Py_MATH_PI / 180.0;
|
|
static const double radToDeg = 180.0 / Py_MATH_PI;
|
|
|
|
static PyObject *
|
|
math_degrees(PyObject *self, PyObject *arg)
|
|
{
|
|
double x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
return PyFloat_FromDouble(x * radToDeg);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_degrees_doc,
|
|
"degrees(x)\n\n\
|
|
Convert angle x from radians to degrees.");
|
|
|
|
static PyObject *
|
|
math_radians(PyObject *self, PyObject *arg)
|
|
{
|
|
double x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
return PyFloat_FromDouble(x * degToRad);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_radians_doc,
|
|
"radians(x)\n\n\
|
|
Convert angle x from degrees to radians.");
|
|
|
|
static PyObject *
|
|
math_isfinite(PyObject *self, PyObject *arg)
|
|
{
|
|
double x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
return PyBool_FromLong((long)Py_IS_FINITE(x));
|
|
}
|
|
|
|
PyDoc_STRVAR(math_isfinite_doc,
|
|
"isfinite(x) -> bool\n\n\
|
|
Return True if x is neither an infinity nor a NaN, and False otherwise.");
|
|
|
|
static PyObject *
|
|
math_isnan(PyObject *self, PyObject *arg)
|
|
{
|
|
double x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
return PyBool_FromLong((long)Py_IS_NAN(x));
|
|
}
|
|
|
|
PyDoc_STRVAR(math_isnan_doc,
|
|
"isnan(x) -> bool\n\n\
|
|
Return True if x is a NaN (not a number), and False otherwise.");
|
|
|
|
static PyObject *
|
|
math_isinf(PyObject *self, PyObject *arg)
|
|
{
|
|
double x = PyFloat_AsDouble(arg);
|
|
if (x == -1.0 && PyErr_Occurred())
|
|
return NULL;
|
|
return PyBool_FromLong((long)Py_IS_INFINITY(x));
|
|
}
|
|
|
|
PyDoc_STRVAR(math_isinf_doc,
|
|
"isinf(x) -> bool\n\n\
|
|
Return True if x is a positive or negative infinity, and False otherwise.");
|
|
|
|
static PyObject *
|
|
math_isclose(PyObject *self, PyObject *args, PyObject *kwargs)
|
|
{
|
|
double a, b;
|
|
double rel_tol = 1e-9;
|
|
double abs_tol = 0.0;
|
|
double diff = 0.0;
|
|
long result = 0;
|
|
|
|
static char *keywords[] = {"a", "b", "rel_tol", "abs_tol", NULL};
|
|
|
|
|
|
if (!PyArg_ParseTupleAndKeywords(args, kwargs, "dd|$dd:isclose",
|
|
keywords,
|
|
&a, &b, &rel_tol, &abs_tol
|
|
))
|
|
return NULL;
|
|
|
|
/* sanity check on the inputs */
|
|
if (rel_tol < 0.0 || abs_tol < 0.0 ) {
|
|
PyErr_SetString(PyExc_ValueError,
|
|
"tolerances must be non-negative");
|
|
return NULL;
|
|
}
|
|
|
|
if ( a == b ) {
|
|
/* short circuit exact equality -- needed to catch two infinities of
|
|
the same sign. And perhaps speeds things up a bit sometimes.
|
|
*/
|
|
Py_RETURN_TRUE;
|
|
}
|
|
|
|
/* This catches the case of two infinities of opposite sign, or
|
|
one infinity and one finite number. Two infinities of opposite
|
|
sign would otherwise have an infinite relative tolerance.
|
|
Two infinities of the same sign are caught by the equality check
|
|
above.
|
|
*/
|
|
|
|
if (Py_IS_INFINITY(a) || Py_IS_INFINITY(b)) {
|
|
Py_RETURN_FALSE;
|
|
}
|
|
|
|
/* now do the regular computation
|
|
this is essentially the "weak" test from the Boost library
|
|
*/
|
|
|
|
diff = fabs(b - a);
|
|
|
|
result = (((diff <= fabs(rel_tol * b)) ||
|
|
(diff <= fabs(rel_tol * a))) ||
|
|
(diff <= abs_tol));
|
|
|
|
return PyBool_FromLong(result);
|
|
}
|
|
|
|
PyDoc_STRVAR(math_isclose_doc,
|
|
"is_close(a, b, *, rel_tol=1e-09, abs_tol=0.0) -> bool\n"
|
|
"\n"
|
|
"Determine whether two floating point numbers are close in value.\n"
|
|
"\n"
|
|
" rel_tol\n"
|
|
" maximum difference for being considered \"close\", relative to the\n"
|
|
" magnitude of the input values\n"
|
|
" abs_tol\n"
|
|
" maximum difference for being considered \"close\", regardless of the\n"
|
|
" magnitude of the input values\n"
|
|
"\n"
|
|
"Return True if a is close in value to b, and False otherwise.\n"
|
|
"\n"
|
|
"For the values to be considered close, the difference between them\n"
|
|
"must be smaller than at least one of the tolerances.\n"
|
|
"\n"
|
|
"-inf, inf and NaN behave similarly to the IEEE 754 Standard. That\n"
|
|
"is, NaN is not close to anything, even itself. inf and -inf are\n"
|
|
"only close to themselves.");
|
|
|
|
static PyMethodDef math_methods[] = {
|
|
{"acos", math_acos, METH_O, math_acos_doc},
|
|
{"acosh", math_acosh, METH_O, math_acosh_doc},
|
|
{"asin", math_asin, METH_O, math_asin_doc},
|
|
{"asinh", math_asinh, METH_O, math_asinh_doc},
|
|
{"atan", math_atan, METH_O, math_atan_doc},
|
|
{"atan2", math_atan2, METH_VARARGS, math_atan2_doc},
|
|
{"atanh", math_atanh, METH_O, math_atanh_doc},
|
|
{"ceil", math_ceil, METH_O, math_ceil_doc},
|
|
{"copysign", math_copysign, METH_VARARGS, math_copysign_doc},
|
|
{"cos", math_cos, METH_O, math_cos_doc},
|
|
{"cosh", math_cosh, METH_O, math_cosh_doc},
|
|
{"degrees", math_degrees, METH_O, math_degrees_doc},
|
|
{"erf", math_erf, METH_O, math_erf_doc},
|
|
{"erfc", math_erfc, METH_O, math_erfc_doc},
|
|
{"exp", math_exp, METH_O, math_exp_doc},
|
|
{"expm1", math_expm1, METH_O, math_expm1_doc},
|
|
{"fabs", math_fabs, METH_O, math_fabs_doc},
|
|
{"factorial", math_factorial, METH_O, math_factorial_doc},
|
|
{"floor", math_floor, METH_O, math_floor_doc},
|
|
{"fmod", math_fmod, METH_VARARGS, math_fmod_doc},
|
|
{"frexp", math_frexp, METH_O, math_frexp_doc},
|
|
{"fsum", math_fsum, METH_O, math_fsum_doc},
|
|
{"gamma", math_gamma, METH_O, math_gamma_doc},
|
|
{"gcd", math_gcd, METH_VARARGS, math_gcd_doc},
|
|
{"hypot", math_hypot, METH_VARARGS, math_hypot_doc},
|
|
{"isclose", (PyCFunction) math_isclose, METH_VARARGS | METH_KEYWORDS,
|
|
math_isclose_doc},
|
|
{"isfinite", math_isfinite, METH_O, math_isfinite_doc},
|
|
{"isinf", math_isinf, METH_O, math_isinf_doc},
|
|
{"isnan", math_isnan, METH_O, math_isnan_doc},
|
|
{"ldexp", math_ldexp, METH_VARARGS, math_ldexp_doc},
|
|
{"lgamma", math_lgamma, METH_O, math_lgamma_doc},
|
|
{"log", math_log, METH_VARARGS, math_log_doc},
|
|
{"log1p", math_log1p, METH_O, math_log1p_doc},
|
|
{"log10", math_log10, METH_O, math_log10_doc},
|
|
{"log2", math_log2, METH_O, math_log2_doc},
|
|
{"modf", math_modf, METH_O, math_modf_doc},
|
|
{"pow", math_pow, METH_VARARGS, math_pow_doc},
|
|
{"radians", math_radians, METH_O, math_radians_doc},
|
|
{"sin", math_sin, METH_O, math_sin_doc},
|
|
{"sinh", math_sinh, METH_O, math_sinh_doc},
|
|
{"sqrt", math_sqrt, METH_O, math_sqrt_doc},
|
|
{"tan", math_tan, METH_O, math_tan_doc},
|
|
{"tanh", math_tanh, METH_O, math_tanh_doc},
|
|
{"trunc", math_trunc, METH_O, math_trunc_doc},
|
|
{NULL, NULL} /* sentinel */
|
|
};
|
|
|
|
|
|
PyDoc_STRVAR(module_doc,
|
|
"This module is always available. It provides access to the\n"
|
|
"mathematical functions defined by the C standard.");
|
|
|
|
|
|
static struct PyModuleDef mathmodule = {
|
|
PyModuleDef_HEAD_INIT,
|
|
"math",
|
|
module_doc,
|
|
-1,
|
|
math_methods,
|
|
NULL,
|
|
NULL,
|
|
NULL,
|
|
NULL
|
|
};
|
|
|
|
PyMODINIT_FUNC
|
|
PyInit_math(void)
|
|
{
|
|
PyObject *m;
|
|
|
|
m = PyModule_Create(&mathmodule);
|
|
if (m == NULL)
|
|
goto finally;
|
|
|
|
PyModule_AddObject(m, "pi", PyFloat_FromDouble(Py_MATH_PI));
|
|
PyModule_AddObject(m, "e", PyFloat_FromDouble(Py_MATH_E));
|
|
PyModule_AddObject(m, "inf", PyFloat_FromDouble(m_inf()));
|
|
#if !defined(PY_NO_SHORT_FLOAT_REPR) || defined(Py_NAN)
|
|
PyModule_AddObject(m, "nan", PyFloat_FromDouble(m_nan()));
|
|
#endif
|
|
|
|
finally:
|
|
return m;
|
|
}
|