Note
Arb was merged into FLINT in 2023.
The documentation on arblib.org will no longer be updated.
See the FLINT documentation instead.
acb.h – complex numbers¶
An acb_t represents a complex number with
error bounds. An acb_t consists of a pair of real number
balls of type arb_struct, representing the real and
imaginary part with separate error bounds.
An acb_t thus represents a rectangle
\([m_1-r_1, m_1+r_1] + [m_2-r_2, m_2+r_2] i\) in the complex plane.
This is used instead of a disk or square representation
(consisting of a complex floating-point midpoint with a single radius),
since it allows implementing many operations more conveniently by splitting
into ball operations on the real and imaginary parts.
It also allows tracking when complex numbers have an exact (for example
exactly zero) real part and an inexact imaginary part, or vice versa.
The interface for the acb_t type is slightly less developed
than that for the arb_t type. In many cases, the user can
easily perform missing operations by directly manipulating the real and
imaginary parts.
Types, macros and constants¶
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type acb_struct¶
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type acb_t¶
An acb_struct consists of a pair of arb_struct:s. An acb_t is defined as an array of length one of type acb_struct, permitting an acb_t to be passed by reference.
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type acb_ptr¶
Alias for
acb_struct *, used for vectors of numbers.
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type acb_srcptr¶
Alias for
const acb_struct *, used for vectors of numbers when passed as constant input to functions.
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acb_realref(x)¶
Macro returning a pointer to the real part of x as an arb_t.
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acb_imagref(x)¶
Macro returning a pointer to the imaginary part of x as an arb_t.
Memory management¶
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slong acb_allocated_bytes(const acb_t x)¶
Returns the total number of bytes heap-allocated internally by this object. The count excludes the size of the structure itself. Add
sizeof(acb_struct)to get the size of the object as a whole.
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slong _acb_vec_allocated_bytes(acb_srcptr vec, slong len)¶
Returns the total number of bytes allocated for this vector, i.e. the space taken up by the vector itself plus the sum of the internal heap allocation sizes for all its member elements.
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double _acb_vec_estimate_allocated_bytes(slong len, slong prec)¶
Estimates the number of bytes that need to be allocated for a vector of len elements with prec bits of precision, including the space for internal limb data. See comments for
_arb_vec_estimate_allocated_bytes().
Basic manipulation¶
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void acb_set_arb_arb(acb_t z, const arb_t x, const arb_t y)¶
Sets the real and imaginary part of z to the values x and y respectively
Input and output¶
The acb_print… functions print to standard output, while acb_fprint… functions print to the stream file.
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void acb_fprintd(FILE *file, const acb_t x, slong digits)¶
Prints x in decimal. The printed value of the radius is not adjusted to compensate for the fact that the binary-to-decimal conversion of both the midpoint and the radius introduces additional error.
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void acb_fprintn(FILE *file, const acb_t x, slong digits, ulong flags)¶
Prints a nice decimal representation of x, using the format of
arb_get_str()(or the correspondingarb_printn()) for the real and imaginary parts.By default, the output shows the midpoint of both the real and imaginary parts with a guaranteed error of at most one unit in the last decimal place. In addition, explicit error bounds are printed so that the displayed decimal interval is guaranteed to enclose x.
Any flags understood by
arb_get_str()can be passed via flags to control the format of the real and imaginary parts.
Random number generation¶
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void acb_randtest(acb_t z, flint_rand_t state, slong prec, slong mag_bits)¶
Generates a random complex number by generating separate random real and imaginary parts.
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void acb_randtest_special(acb_t z, flint_rand_t state, slong prec, slong mag_bits)¶
Generates a random complex number by generating separate random real and imaginary parts. Also generates NaNs and infinities.
Precision and comparisons¶
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int acb_is_int_2exp_si(const acb_t x, slong e)¶
Returns nonzero iff z exactly equals \(n 2^e\) for some integer n.
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int acb_equal(const acb_t x, const acb_t y)¶
Returns nonzero iff x and y are identical as sets, i.e. if the real and imaginary parts are equal as balls.
Note that this is not the same thing as testing whether both x and y certainly represent the same complex number, unless either x or y is exact (and neither contains NaN). To test whether both operands might represent the same mathematical quantity, use
acb_overlaps()oracb_contains(), depending on the circumstance.
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int acb_eq(const acb_t x, const acb_t y)¶
Returns nonzero iff x and y are certainly equal, as determined by testing that
arb_eq()holds for both the real and imaginary parts.
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int acb_ne(const acb_t x, const acb_t y)¶
Returns nonzero iff x and y are certainly not equal, as determined by testing that
arb_ne()holds for either the real or imaginary parts.
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int acb_overlaps(const acb_t x, const acb_t y)¶
Returns nonzero iff x and y have some point in common.
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void acb_union(acb_t z, const acb_t x, const acb_t y, slong prec)¶
Sets z to a complex interval containing both x and y.
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void acb_get_abs_ubound_arf(arf_t u, const acb_t z, slong prec)¶
Sets u to an upper bound for the absolute value of z, computed using a working precision of prec bits.
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void acb_get_abs_lbound_arf(arf_t u, const acb_t z, slong prec)¶
Sets u to a lower bound for the absolute value of z, computed using a working precision of prec bits.
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void acb_get_rad_ubound_arf(arf_t u, const acb_t z, slong prec)¶
Sets u to an upper bound for the error radius of z (the value is currently not computed tightly).
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void acb_get_mag_lower(mag_t u, const acb_t x)¶
Sets u to a lower bound for the absolute value of x.
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int acb_contains_int(const acb_t x)¶
Returns nonzero iff the complex interval represented by x contains an integer.
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int acb_contains_interior(const acb_t x, const acb_t y)¶
Tests if y is contained in the interior of x. This predicate always evaluates to false if x and y are both real-valued, since an imaginary part of 0 is not considered contained in the interior of the point interval 0. More generally, the same problem occurs for intervals with an exact real or imaginary part. Such intervals must be handled specially by the user where a different interpretation is intended.
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slong acb_rel_error_bits(const acb_t x)¶
Returns the effective relative error of x measured in bits. This is computed as if calling
arb_rel_error_bits()on the real ball whose midpoint is the larger out of the real and imaginary midpoints of x, and whose radius is the larger out of the real and imaginary radiuses of x.
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slong acb_rel_accuracy_bits(const acb_t x)¶
Returns the effective relative accuracy of x measured in bits, equal to the negative of the return value from
acb_rel_error_bits().
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slong acb_rel_one_accuracy_bits(const acb_t x)¶
Given a ball with midpoint m and radius r, returns an approximation of the relative accuracy of \([\max(1,|m|) \pm r]\) measured in bits.
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slong acb_bits(const acb_t x)¶
Returns the maximum of arb_bits applied to the real and imaginary parts of x, i.e. the minimum precision sufficient to represent x exactly.
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void acb_indeterminate(acb_t x)¶
Sets x to \([\operatorname{NaN} \pm \infty] + [\operatorname{NaN} \pm \infty]i\), representing an indeterminate result.
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void acb_trim(acb_t y, const acb_t x)¶
Sets y to a a copy of x with both the real and imaginary parts trimmed (see
arb_trim()).
Complex parts¶
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void acb_arg(arb_t r, const acb_t z, slong prec)¶
Sets r to a real interval containing the complex argument (phase) of z. We define the complex argument have a discontinuity on \((-\infty,0]\), with the special value \(\operatorname{arg}(0) = 0\), and \(\operatorname{arg}(a+0i) = \pi\) for \(a < 0\). Equivalently, if \(z = a+bi\), the argument is given by \(\operatorname{atan2}(b,a)\) (see
arb_atan2()).
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void acb_sgn(acb_t r, const acb_t z, slong prec)¶
Sets r to the complex sign of z, defined as 0 if z is exactly zero and the projection onto the unit circle \(z / |z| = \exp(i \arg(z))\) otherwise.
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void acb_csgn(arb_t r, const acb_t z)¶
Sets r to the extension of the real sign function taking the value 1 for z strictly in the right half plane, -1 for z strictly in the left half plane, and the sign of the imaginary part when z is on the imaginary axis. Equivalently, \(\operatorname{csgn}(z) = z / \sqrt{z^2}\) except that the value is 0 when z is exactly zero.
Arithmetic¶
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void acb_sub(acb_t z, const acb_t x, const acb_t y, slong prec)¶
Sets z to the difference of x and y.
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void acb_mul_arb(acb_t z, const acb_t x, const arb_t y, slong prec)¶
Sets z to the product of x and y.
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void acb_mul(acb_t z, const acb_t x, const acb_t y, slong prec)¶
Sets z to the product of x and y. If at least one part of x or y is zero, the operations is reduced to two real multiplications. If x and y are the same pointers, they are assumed to represent the same mathematical quantity and the squaring formula is used.
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void acb_mul_2exp_fmpz(acb_t z, const acb_t x, const fmpz_t e)¶
Sets z to x multiplied by \(2^e\), without rounding.
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void acb_cube(acb_t z, const acb_t x, slong prec)¶
Sets z to x cubed, computed efficiently using two real squarings, two real multiplications, and scalar operations.
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void acb_addmul_arb(acb_t z, const acb_t x, const arb_t y, slong prec)¶
Sets z to z plus the product of x and y.
Dot product¶
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void acb_dot_precise(acb_t res, const acb_t s, int subtract, acb_srcptr x, slong xstep, acb_srcptr y, slong ystep, slong len, slong prec)¶
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void acb_dot_simple(acb_t res, const acb_t s, int subtract, acb_srcptr x, slong xstep, acb_srcptr y, slong ystep, slong len, slong prec)¶
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void acb_dot(acb_t res, const acb_t s, int subtract, acb_srcptr x, slong xstep, acb_srcptr y, slong ystep, slong len, slong prec)¶
Computes the dot product of the vectors x and y, setting res to \(s + (-1)^{subtract} \sum_{i=0}^{len-1} x_i y_i\).
The initial term s is optional and can be omitted by passing NULL (equivalently, \(s = 0\)). The parameter subtract must be 0 or 1. The length len is allowed to be negative, which is equivalent to a length of zero. The parameters xstep or ystep specify a step length for traversing subsequences of the vectors x and y; either can be negative to step in the reverse direction starting from the initial pointer. Aliasing is allowed between res and s but not between res and the entries of x and y.
The default version determines the optimal precision for each term and performs all internal calculations using mpn arithmetic with minimal overhead. This is the preferred way to compute a dot product; it is generally much faster and more precise than a simple loop.
The simple version performs fused multiply-add operations in a simple loop. This can be used for testing purposes and is also used as a fallback by the default version when the exponents are out of range for the optimized code.
The precise version computes the dot product exactly up to the final rounding. This can be extremely slow and is only intended for testing.
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void acb_approx_dot(acb_t res, const acb_t s, int subtract, acb_srcptr x, slong xstep, acb_srcptr y, slong ystep, slong len, slong prec)¶
Computes an approximate dot product without error bounds. The radii of the inputs are ignored (only the midpoints are read) and only the midpoint of the output is written.
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void acb_dot_ui(acb_t res, const acb_t initial, int subtract, acb_srcptr x, slong xstep, const ulong *y, slong ystep, slong len, slong prec)¶
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void acb_dot_si(acb_t res, const acb_t initial, int subtract, acb_srcptr x, slong xstep, const slong *y, slong ystep, slong len, slong prec)¶
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void acb_dot_uiui(acb_t res, const acb_t initial, int subtract, acb_srcptr x, slong xstep, const ulong *y, slong ystep, slong len, slong prec)¶
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void acb_dot_siui(acb_t res, const acb_t initial, int subtract, acb_srcptr x, slong xstep, const ulong *y, slong ystep, slong len, slong prec)¶
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void acb_dot_fmpz(acb_t res, const acb_t initial, int subtract, acb_srcptr x, slong xstep, const fmpz *y, slong ystep, slong len, slong prec)¶
Equivalent to
acb_dot(), but with integers in the array y. The uiui and siui versions take an array of double-limb integers as input; the siui version assumes that these represent signed integers in two’s complement form.
Mathematical constants¶
Powers and roots¶
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void acb_sqrt(acb_t r, const acb_t z, slong prec)¶
Sets r to the square root of z. If either the real or imaginary part is exactly zero, only a single real square root is needed. Generally, we use the formula \(\sqrt{a+bi} = u/2 + ib/u, u = \sqrt{2(|a+bi|+a)}\), requiring two real square root extractions.
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void acb_sqrt_analytic(acb_t r, const acb_t z, int analytic, slong prec)¶
Computes the square root. If analytic is set, gives a NaN-containing result if z touches the branch cut.
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void acb_rsqrt(acb_t r, const acb_t z, slong prec)¶
Sets r to the reciprocal square root of z. If either the real or imaginary part is exactly zero, only a single real reciprocal square root is needed. Generally, we use the formula \(1/\sqrt{a+bi} = ((a+r) - bi)/v, r = |a+bi|, v = \sqrt{r |a+bi+r|^2}\), requiring one real square root and one real reciprocal square root.
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void acb_rsqrt_analytic(acb_t r, const acb_t z, int analytic, slong prec)¶
Computes the reciprocal square root. If analytic is set, gives a NaN-containing result if z touches the branch cut.
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void acb_quadratic_roots_fmpz(acb_t r1, acb_t r2, const fmpz_t a, const fmpz_t b, const fmpz_t c, slong prec)¶
Sets r1 and r2 to the roots of the quadratic polynomial \(ax^2 + bx + c\). Requires that a is nonzero. This function is implemented so that both roots are computed accurately even when direct use of the quadratic formula would lose accuracy.
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void acb_root_ui(acb_t r, const acb_t z, ulong k, slong prec)¶
Sets r to the principal k-th root of z.
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void acb_pow_si(acb_t y, const acb_t b, slong e, slong prec)¶
Sets \(y = b^e\) using binary exponentiation (with an initial division if \(e < 0\)). Note that these functions can get slow if the exponent is extremely large (in such cases
acb_pow()may be superior).
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void acb_pow(acb_t z, const acb_t x, const acb_t y, slong prec)¶
Sets \(z = x^y\), computed using binary exponentiation if \(y\) if a small exact integer, as \(z = (x^{1/2})^{2y}\) if \(y\) is a small exact half-integer, and generally as \(z = \exp(y \log x)\).
Exponentials and logarithms¶
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void acb_exp(acb_t y, const acb_t z, slong prec)¶
Sets y to the exponential function of z, computed as \(\exp(a+bi) = \exp(a) \left( \cos(b) + \sin(b) i \right)\).
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void acb_exp_invexp(acb_t s, acb_t t, const acb_t z, slong prec)¶
Sets \(s = \exp(z)\) and \(t = \exp(-z)\).
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void acb_expm1(acb_t res, const acb_t z, slong prec)¶
Sets res to \(\exp(z)-1\), using a more accurate method when \(z \approx 0\).
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void acb_log(acb_t y, const acb_t z, slong prec)¶
Sets y to the principal branch of the natural logarithm of z, computed as \(\log(a+bi) = \frac{1}{2} \log(a^2 + b^2) + i \operatorname{arg}(a+bi)\).
Trigonometric functions¶
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void acb_sin_cos(acb_t s, acb_t c, const acb_t z, slong prec)¶
Sets \(s = \sin(z)\), \(c = \cos(z)\), evaluated as \(\sin(a+bi) = \sin(a)\cosh(b) + i \cos(a)\sinh(b)\), \(\cos(a+bi) = \cos(a)\cosh(b) - i \sin(a)\sinh(b)\).
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void acb_tan(acb_t s, const acb_t z, slong prec)¶
Sets \(s = \tan(z) = \sin(z) / \cos(z)\). For large imaginary parts, the function is evaluated in a numerically stable way as \(\pm i\) plus a decreasing exponential factor.
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void acb_cot(acb_t s, const acb_t z, slong prec)¶
Sets \(s = \cot(z) = \cos(z) / \sin(z)\). For large imaginary parts, the function is evaluated in a numerically stable way as \(\pm i\) plus a decreasing exponential factor.
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void acb_sin_cos_pi(acb_t s, acb_t c, const acb_t z, slong prec)¶
Sets \(s = \sin(\pi z)\), \(c = \cos(\pi z)\), evaluating the trigonometric factors of the real and imaginary part accurately via
arb_sin_cos_pi().
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void acb_tan_pi(acb_t s, const acb_t z, slong prec)¶
Sets \(s = \tan(\pi z)\). Uses the same algorithm as
acb_tan(), but evaluates the sine and cosine accurately viaarb_sin_cos_pi().
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void acb_cot_pi(acb_t s, const acb_t z, slong prec)¶
Sets \(s = \cot(\pi z)\). Uses the same algorithm as
acb_cot(), but evaluates the sine and cosine accurately viaarb_sin_cos_pi().
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void acb_csc_pi(acb_t res, const acb_t z, slong prec)¶
Computes \(\csc(\pi x) = 1 / \sin(\pi z)\). Evaluates the sine accurately via
acb_sin_pi().
Inverse trigonometric functions¶
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void acb_asin(acb_t res, const acb_t z, slong prec)¶
Sets res to \(\operatorname{asin}(z) = -i \log(iz + \sqrt{1-z^2})\).
Hyperbolic functions¶
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void acb_coth(acb_t s, const acb_t z, slong prec)¶
Respectively computes \(\sinh(z) = -i\sin(iz)\), \(\cosh(z) = \cos(iz)\), \(\tanh(z) = -i\tan(iz)\), \(\coth(z) = i\cot(iz)\).
Inverse hyperbolic functions¶
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void acb_asinh(acb_t res, const acb_t z, slong prec)¶
Sets res to \(\operatorname{asinh}(z) = -i \operatorname{asin}(iz)\).
Lambert W function¶
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void acb_lambertw_asymp(acb_t res, const acb_t z, const fmpz_t k, slong L, slong M, slong prec)¶
Sets res to the Lambert W function \(W_k(z)\) computed using L and M terms in the bivariate series giving the asymptotic expansion at zero or infinity. This algorithm is valid everywhere, but the error bound is only finite when \(|\log(z)|\) is sufficiently large.
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int acb_lambertw_check_branch(const acb_t w, const fmpz_t k, slong prec)¶
Tests if w definitely lies in the image of the branch \(W_k(z)\). This function is used internally to verify that a computed approximation of the Lambert W function lies on the intended branch. Note that this will necessarily evaluate to false for points exactly on (or overlapping) the branch cuts, where a different algorithm has to be used.
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void acb_lambertw_bound_deriv(mag_t res, const acb_t z, const acb_t ez1, const fmpz_t k)¶
Sets res to an upper bound for \(|W_k'(z)|\). The input ez1 should contain the precomputed value of \(ez+1\).
Along the real line, the directional derivative of \(W_k(z)\) is understood to be taken. As a result, the user must handle the branch cut discontinuity separately when using this function to bound perturbations in the value of \(W_k(z)\).
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void acb_lambertw(acb_t res, const acb_t z, const fmpz_t k, int flags, slong prec)¶
Sets res to the Lambert W function \(W_k(z)\) where the index k selects the branch (with \(k = 0\) giving the principal branch). The placement of branch cuts follows [CGHJK1996].
If flags is nonzero, nonstandard branch cuts are used.
If flags is set to ACB_LAMBERTW_LEFT, computes \(W_{\mathrm{left}|k}(z)\) which corresponds to \(W_k(z)\) in the upper half plane and \(W_{k+1}(z)\) in the lower half plane, connected continuously to the left of the branch points. In other words, the branch cut on \((-\infty,0)\) is rotated counterclockwise to \((0,+\infty)\). (For \(k = -1\) and \(k = 0\), there is also a branch cut on \((-1/e,0)\), continuous from below instead of from above to maintain counterclockwise continuity.)
If flags is set to ACB_LAMBERTW_MIDDLE, computes \(W_{\mathrm{middle}}(z)\) which corresponds to \(W_{-1}(z)\) in the upper half plane and \(W_{1}(z)\) in the lower half plane, connected continuously through \((-1/e,0)\) with branch cuts on \((-\infty,-1/e)\) and \((0,+\infty)\). \(W_{\mathrm{middle}}(z)\) extends the real analytic function \(W_{-1}(x)\) defined on \((-1/e,0)\) to a complex analytic function, whereas the standard branch \(W_{-1}(z)\) has a branch cut along the real segment.
The algorithm used to compute the Lambert W function is described in [Joh2017b].
Rising factorials¶
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void acb_rising_ui(acb_t z, const acb_t x, ulong n, slong prec)¶
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void acb_rising(acb_t z, const acb_t x, const acb_t n, slong prec)¶
Computes the rising factorial \(z = x (x+1) (x+2) \cdots (x+n-1)\). These functions are aliases for
acb_hypgeom_rising_ui()andacb_hypgeom_rising().
Gamma function¶
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void acb_gamma(acb_t y, const acb_t x, slong prec)¶
Computes the gamma function \(y = \Gamma(x)\). This is an alias for
acb_hypgeom_gamma().
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void acb_rgamma(acb_t y, const acb_t x, slong prec)¶
Computes the reciprocal gamma function \(y = 1/\Gamma(x)\), avoiding division by zero at the poles of the gamma function. This is an alias for
acb_hypgeom_rgamma().
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void acb_lgamma(acb_t y, const acb_t x, slong prec)¶
Computes the logarithmic gamma function \(y = \log \Gamma(x)\). This is an alias for
acb_hypgeom_lgamma().The branch cut of the logarithmic gamma function is placed on the negative half-axis, which means that \(\log \Gamma(z) + \log z = \log \Gamma(z+1)\) holds for all \(z\), whereas \(\log \Gamma(z) \ne \log(\Gamma(z))\) in general. In the left half plane, the reflection formula with correct branch structure is evaluated via
acb_log_sin_pi().
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void acb_digamma(acb_t y, const acb_t x, slong prec)¶
Computes the digamma function \(y = \psi(x) = (\log \Gamma(x))' = \Gamma'(x) / \Gamma(x)\).
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void acb_log_sin_pi(acb_t res, const acb_t z, slong prec)¶
Computes the logarithmic sine function defined by
\[S(z) = \log(\pi) - \log \Gamma(z) + \log \Gamma(1-z)\]which is equal to
\[S(z) = \int_{1/2}^z \pi \cot(\pi t) dt\]where the path of integration goes through the upper half plane if \(0 < \arg(z) \le \pi\) and through the lower half plane if \(-\pi < \arg(z) \le 0\). Equivalently,
\[S(z) = \log(\sin(\pi(z-n))) \mp n \pi i, \quad n = \lfloor \operatorname{re}(z) \rfloor\]where the negative sign is taken if \(0 < \arg(z) \le \pi\) and the positive sign is taken otherwise (if the interval \(\arg(z)\) does not certainly satisfy either condition, the union of both cases is computed). After subtracting n, we have \(0 \le \operatorname{re}(z) < 1\). In this strip, we use use \(S(z) = \log(\sin(\pi(z)))\) if the imaginary part of z is small. Otherwise, we use \(S(z) = i \pi (z-1/2) + \log((1+e^{-2i\pi z})/2)\) in the lower half-plane and the conjugated expression in the upper half-plane to avoid exponent overflow.
The function is evaluated at the midpoint and the propagated error is computed from \(S'(z)\) to get a continuous change when \(z\) is non-real and \(n\) spans more than one possible integer value.
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void acb_polygamma(acb_t res, const acb_t s, const acb_t z, slong prec)¶
Sets res to the value of the generalized polygamma function \(\psi(s,z)\).
If s is a nonnegative order, this is simply the s-order derivative of the digamma function. If \(s = 0\), this function simply calls the digamma function internally. For integers \(s \ge 1\), it calls the Hurwitz zeta function. Note that for small integers \(s \ge 1\), it can be faster to use
acb_poly_digamma_series()and read off the coefficients.The generalization to other values of s is due to Espinosa and Moll [EM2004]:
\[\psi(s,z) = \frac{\zeta'(s+1,z) + (\gamma + \psi(-s)) \zeta(s+1,z)}{\Gamma(-s)}\]
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void acb_log_barnes_g(acb_t res, const acb_t z, slong prec)¶
Computes Barnes G-function or the logarithmic Barnes G-function, respectively. The logarithmic version has branch cuts on the negative real axis and is continuous elsewhere in the complex plane, in analogy with the logarithmic gamma function. The functional equation
\[\log G(z+1) = \log \Gamma(z) + \log G(z).\]holds for all z.
For small integers, we directly use the recurrence relation \(G(z+1) = \Gamma(z) G(z)\) together with the initial value \(G(1) = 1\). For general z, we use the formula
\[\log G(z) = (z-1) \log \Gamma(z) - \zeta'(-1,z) + \zeta'(-1).\]
Zeta function¶
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void acb_zeta(acb_t z, const acb_t s, slong prec)¶
Sets z to the value of the Riemann zeta function \(\zeta(s)\). Note: for computing derivatives with respect to \(s\), use
acb_poly_zeta_series()or related methods.This is a wrapper of
acb_dirichlet_zeta().
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void acb_hurwitz_zeta(acb_t z, const acb_t s, const acb_t a, slong prec)¶
Sets z to the value of the Hurwitz zeta function \(\zeta(s, a)\). Note: for computing derivatives with respect to \(s\), use
acb_poly_zeta_series()or related methods.This is a wrapper of
acb_dirichlet_hurwitz().
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void acb_bernoulli_poly_ui(acb_t res, ulong n, const acb_t x, slong prec)¶
Sets res to the value of the Bernoulli polynomial \(B_n(x)\).
Warning: this function is only fast if either n or x is a small integer.
This function reads Bernoulli numbers from the global cache if they are already cached, but does not automatically extend the cache by itself.
Polylogarithms¶
Arithmetic-geometric mean¶
See Algorithms for the arithmetic-geometric mean for implementation details.
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void acb_agm1(acb_t m, const acb_t z, slong prec)¶
Sets m to the arithmetic-geometric mean \(M(z) = \operatorname{agm}(1,z)\), defined such that the function is continuous in the complex plane except for a branch cut along the negative half axis (where it is continuous from above). This corresponds to always choosing an “optimal” branch for the square root in the arithmetic-geometric mean iteration.
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void acb_agm1_cpx(acb_ptr m, const acb_t z, slong len, slong prec)¶
Sets the coefficients in the array m to the power series expansion of the arithmetic-geometric mean at the point z truncated to length len, i.e. \(M(z+x) \in \mathbb{C}[[x]]\).
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void acb_agm(acb_t m, const acb_t x, const acb_t y, slong prec)¶
Sets m to the arithmetic-geometric mean of x and y. The square roots in the AGM iteration are chosen so as to form the “optimal” AGM sequence. This gives a well-defined function of x and y except when \(x / y\) is a negative real number, in which case there are two optimal AGM sequences. In that case, an arbitrary but consistent choice is made (if a decision cannot be made due to inexact arithmetic, the union of both choices is returned).
Other special functions¶
Piecewise real functions¶
The following methods extend common piecewise real functions to piecewise complex analytic functions, useful together with the acb_calc.h module. If analytic is set, evaluation on a discontinuity or non-analytic point gives a NaN result.
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void acb_real_abs(acb_t res, const acb_t z, int analytic, slong prec)¶
The absolute value is extended to \(+z\) in the right half plane and \(-z\) in the left half plane, with a discontinuity on the vertical line \(\operatorname{Re}(z) = 0\).
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void acb_real_sgn(acb_t res, const acb_t z, int analytic, slong prec)¶
The sign function is extended to \(+1\) in the right half plane and \(-1\) in the left half plane, with a discontinuity on the vertical line \(\operatorname{Re}(z) = 0\). If analytic is not set, this is effectively the same function as
acb_csgn().
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void acb_real_heaviside(acb_t res, const acb_t z, int analytic, slong prec)¶
The Heaviside step function (or unit step function) is extended to \(+1\) in the right half plane and \(0\) in the left half plane, with a discontinuity on the vertical line \(\operatorname{Re}(z) = 0\).
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void acb_real_floor(acb_t res, const acb_t z, int analytic, slong prec)¶
The floor function is extended to a piecewise constant function equal to \(n\) in the strips with real part \((n,n+1)\), with discontinuities on the vertical lines \(\operatorname{Re}(z) = n\).
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void acb_real_ceil(acb_t res, const acb_t z, int analytic, slong prec)¶
The ceiling function is extended to a piecewise constant function equal to \(n+1\) in the strips with real part \((n,n+1)\), with discontinuities on the vertical lines \(\operatorname{Re}(z) = n\).
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void acb_real_max(acb_t res, const acb_t x, const acb_t y, int analytic, slong prec)¶
The real function \(\max(x,y)\) is extended to a piecewise analytic function of two variables by returning \(x\) when \(\operatorname{Re}(x) \ge \operatorname{Re}(y)\) and returning \(y\) when \(\operatorname{Re}(x) < \operatorname{Re}(y)\), with discontinuities where \(\operatorname{Re}(x) = \operatorname{Re}(y)\).
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void acb_real_min(acb_t res, const acb_t x, const acb_t y, int analytic, slong prec)¶
The real function \(\min(x,y)\) is extended to a piecewise analytic function of two variables by returning \(x\) when \(\operatorname{Re}(x) \le \operatorname{Re}(y)\) and returning \(y\) when \(\operatorname{Re}(x) > \operatorname{Re}(y)\), with discontinuities where \(\operatorname{Re}(x) = \operatorname{Re}(y)\).
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void acb_real_sqrtpos(acb_t res, const acb_t z, int analytic, slong prec)¶
Extends the real square root function on \([0,+\infty)\) to the usual complex square root on the cut plane. Like
arb_sqrtpos(), only the nonnegative part of z is considered if z is purely real and analytic is not set. This is useful for integrating \(\sqrt{f(x)}\) where it is known that \(f(x) \ge 0\): unlikeacb_sqrt_analytic(), no spurious imaginary terms \([\pm \varepsilon] i\) are created when the balls computed for \(f(x)\) straddle zero.
Vector functions¶
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int _acb_vec_is_zero(acb_srcptr vec, slong len)¶
Returns nonzero iff all entries in x are zero.
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int _acb_vec_is_real(acb_srcptr v, slong len)¶
Returns nonzero iff all entries in x have zero imaginary part.
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void _acb_vec_set(acb_ptr res, acb_srcptr vec, slong len)¶
Sets res to a copy of vec.
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void _acb_vec_set_round(acb_ptr res, acb_srcptr vec, slong len, slong prec)¶
Sets res to a copy of vec, rounding each entry to prec bits.
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void _acb_vec_neg(acb_ptr res, acb_srcptr vec, slong len)¶
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void _acb_vec_add(acb_ptr res, acb_srcptr vec1, acb_srcptr vec2, slong len, slong prec)¶
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void _acb_vec_sub(acb_ptr res, acb_srcptr vec1, acb_srcptr vec2, slong len, slong prec)¶
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void _acb_vec_scalar_mul_2exp_si(acb_ptr res, acb_srcptr vec, slong len, slong c)¶
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void _acb_vec_scalar_mul_onei(acb_ptr res, acb_srcptr vec, slong len)¶
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void _acb_vec_scalar_div_fmpz(acb_ptr res, acb_srcptr vec, slong len, const fmpz_t c, slong prec)¶
Performs the respective scalar operation elementwise.
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slong _acb_vec_bits(acb_srcptr vec, slong len)¶
Returns the maximum of
arb_bits()for all entries in vec.
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void _acb_vec_set_powers(acb_ptr xs, const acb_t x, slong len, slong prec)¶
Sets xs to the powers \(1, x, x^2, \ldots, x^{len-1}\).
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void _acb_vec_unit_roots(acb_ptr z, slong order, slong len, slong prec)¶
Sets z to the powers \(1,z,z^2,\dots z^{\mathrm{len}-1}\) where \(z=\exp(\frac{2i\pi}{\mathrm{order}})\) to precision prec. order can be taken negative.
In order to avoid precision loss, this function does not simply compute powers of a primitive root.
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void _acb_vec_add_error_mag_vec(acb_ptr res, mag_srcptr err, slong len)¶
Adds the magnitude of each entry in err to the radius of the corresponding entry in res.
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void _acb_vec_indeterminate(acb_ptr vec, slong len)¶
Applies
acb_indeterminate()elementwise.
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void _acb_vec_trim(acb_ptr res, acb_srcptr vec, slong len)¶
Applies
acb_trim()elementwise.
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int _acb_vec_get_unique_fmpz_vec(fmpz *res, acb_srcptr vec, slong len)¶
Calls
acb_get_unique_fmpz()elementwise and returns nonzero if all entries can be rounded uniquely to integers. If any entry in vec cannot be rounded uniquely to an integer, returns zero.