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https://github.com/vale981/arb
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310 lines
12 KiB
ReStructuredText
310 lines
12 KiB
ReStructuredText
.. _acb-dirichlet:
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**acb_dirichlet.h** -- Dirichlet L-functions, zeta functions, and related functions
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===================================================================================
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*Warning: the interfaces in this module are experimental and may change
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without notice.*
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This module allows working with values of Dirichlet characters, Dirichlet L-functions,
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and related functions. Working with Dirichlet characters is documented in
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:ref:`dirichlet`.
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A Dirichlet L-function is the analytic continuation of an L-series
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.. math ::
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L(s,\chi) = \sum_{k=1}^\infty \frac{\chi(k)}{k^s}
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where `\chi(k)` is a Dirichlet character.
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The code in other modules for computing the Riemann zeta function,
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Hurwitz zeta function and polylogarithm will possibly be migrated to this
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module in the future.
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Character evaluation
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-------------------------------------------------------------------------------
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.. function:: void acb_dirichlet_chi(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, ulong n, slong prec)
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Sets *res* to `\chi(n)`, the value of the Dirichlet character *chi*
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at the integer *n*.
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.. function:: void acb_dirichlet_chi_vec(acb_ptr v, const dirichlet_group_t G, const dirichlet_char_t chi, slong nv, slong prec)
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Compute the *nv* first Dirichlet values.
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Roots of unity
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-------------------------------------------------------------------------------
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.. type:: acb_dirichlet_powers_struct
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.. type:: acb_dirichlet_powers_t
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This structure allows to compute *n* powers of a fixed root of unity of order *m*
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using precomputations. Extremal cases are
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- all powers are stored: `O(m)` initialization + storage, `O(n)` evaluations
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- nothing stored: `O(1)` initialization + storage, `O(\log(m)n)` evaluations
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- `k` step decomposition: `O(k m^{\frac1k})` init + storage, `O((k-1)n)` evaluations.
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Currently, only baby-step giant-step decomposition (i.e. `k=2`)
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is implemented, allowing to obtain each power using one multiplication.
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.. function:: void acb_dirichlet_powers_init(acb_dirichlet_powers_t t, ulong order, slong num, slong prec)
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Initialize the powers structure for *num* evaluations of powers of the root of unity
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of order *order*.
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.. function:: void acb_dirichlet_powers_clear(acb_dirichlet_powers_t t)
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Clears *t*.
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.. function:: void acb_dirichlet_power(acb_t z, const acb_dirichlet_powers_t t, ulong n, slong prec)
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Sets *z* to `x^n` where *t* contains precomputed powers of `x`.
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Gauss and Jacobi sums
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-------------------------------------------------------------------------------
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.. function:: void acb_dirichlet_gauss_sum_naive(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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.. function:: void acb_dirichlet_gauss_sum_factor(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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.. function:: void acb_dirichlet_gauss_sum_order2(acb_t res, const dirichlet_char_t chi, slong prec)
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.. function:: void acb_dirichlet_gauss_sum_theta(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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.. function:: void acb_dirichlet_gauss_sum(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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.. function:: void acb_dirichlet_gauss_sum_ui(acb_t res, const dirichlet_group_t G, ulong a, slong prec)
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Sets *res* to the Gauss sum
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.. math::
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G_q(a) = \sum_{x \bmod q} \chi_q(a, x) e^{\frac{2i\pi x}q}
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- the *naive* version computes the sum as defined.
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- the *factor* version writes it as a product of local Gauss sums by chinese
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remainder theorem.
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- the *order2* version assumes *chi* is real and primitive and returns
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`i^p\sqrt q` where `p` is the parity of `\chi`.
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- the *theta* version assumes that *chi* is primitive to obtain the Gauss
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sum by functional equation of the theta series at `t=1`. An abort will be
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raised if the theta series vanishes at `t=1`. Only 4 exceptional
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characters of conductor 300 and 600 are known to have this particularity,
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and none with primepower modulus.
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- the default version automatically combines the above methods.
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- the *ui* version only takes the Conrey number *a* as parameter.
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.. function:: void acb_dirichlet_jacobi_sum_naive(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi1, const dirichlet_char_t chi2, slong prec)
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.. function:: void acb_dirichlet_jacobi_sum_factor(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi1, const dirichlet_char_t chi2, slong prec)
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.. function:: void acb_dirichlet_jacobi_sum_gauss(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi1, const dirichlet_char_t chi2, slong prec)
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.. function:: void acb_dirichlet_jacobi_sum(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi1, const dirichlet_char_t chi2, slong prec)
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.. function:: void acb_dirichlet_jacobi_sum_ui(acb_t res, const dirichlet_group_t G, ulong a, ulong b, slong prec)
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Computes the Jacobi sum
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.. math::
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J_q(a,b) = \sum_{x \bmod q} \chi_q(a, x)\chi_q(b, 1-x)
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- the *naive* version computes the sum as defined.
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- the *factor* version writes it as a product of local Jacobi sums
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- the *gauss* version assumes `ab` is primitive and uses the formula
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`J_q(a,b)G_q(ab) = G_q(a)G_q(b)`
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- the default version automatically combines the above methods.
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- the *ui* version only takes the Conrey numbers *a* and *b* as parameters.
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Theta sums
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-------------------------------------------------------------------------------
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We call *theta series* of a Dirichlet character the quadratic series
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.. math::
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\Theta_q(a) = \sum_{n\geq 0} \chi_q(a, n) n^p x^{n^2}
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where `p` is the parity of the character `\chi_q(a,\cdot)`.
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For `\Re(t)>0` we write `x(t)=\exp(-\frac{\pi}{N}t^2)` and define
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.. math::
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\Theta_q(a,t) = \sum_{n\geq 0} \chi_q(a, n) x(t)^{n^2}.
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.. function:: void acb_dirichlet_chi_theta_arb(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, const arb_t t, slong prec)
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.. function:: void acb_dirichlet_ui_theta_arb(acb_t res, const dirichlet_group_t G, ulong a, const arb_t t, slong prec)
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Compute the theta series `\Theta_q(a,t)` for real argument `t>0`.
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Beware that if `t<1` the functional equation
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.. math::
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t \theta(a,t) = \epsilon(\chi) \theta\left(\frac1a, \frac1t\right)
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should be used, which is not done automatically (to avoid recomputing the
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Gauss sum).
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.. function:: ulong acb_dirichlet_theta_length(ulong q, const arb_t t, slong prec)
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Compute the number of terms to be summed in the theta series of argument *t*
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so that the tail is less than `2^{-\mathrm{prec}}`.
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.. function:: void acb_dirichlet_qseries_powers_naive(acb_t res, const arb_t x, int p, const ulong * a, const acb_dirichlet_powers_t z, slong len, slong prec)
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.. function:: void acb_dirichlet_qseries_powers_smallorder(acb_t res, const arb_t x, int p, const ulong * a, const acb_dirichlet_powers_t z, slong len, slong prec)
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Compute the series `\sum n^p z^{a_n} x^{n^2}` for exponent list *a*,
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precomputed powers *z* and parity *p* (being 0 or 1).
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The *naive* version sums the series as defined, while the *smallorder*
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variant evaluates the series on the quotient ring by a cyclotomic polynomial
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before evaluating at the root of unity, ignoring its argument *z*.
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Discrete Fourier Transforms (DFT)
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-------------------------------------------------------------------------------
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Let *G* be a finite abelian group, and `\chi` a character of *G*.
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For any map `f:G\to\mathbb C`, the discrete fourier transform
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`\hat f:\hat G\to \mathbb C` is defined by
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.. math::
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\hat f(\chi) = \sum_{x\in G}\chi(x)f(x)
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Fast Fourier Transform techniques allow to compute efficiently
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all values `\hat f(\chi)`.
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For a Dirichlet group `G` modulo `q`, we take advantage
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of the Conrey isomorphism `G \to \hat G` to consider the
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the Fourier transform on Conrey labels as
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.. math::
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g(a) = \sum_{b\bmod q}\chi_q(a,b)f(b)
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.. function:: void acb_dirichlet_dft_conrey(acb_ptr w, acb_srcptr v, const dirichlet_group_t G, slong prec)
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Compute the DFT of *v* using Conrey indices.
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This function assumes *v* and *w* are vectors
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of size *G->phi_q*, whose values correspond to a lexicographic ordering
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of Conrey logs (as obtained using :func:`dirichlet_conrey_next` or
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by :func:`dirichlet_index_conrey`).
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For example, if `q=15`, the Conrey elements are stored in following
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order
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======= ============= =====================
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index log = [e,f] number = 7^e 11^f
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======= ============= =====================
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0 [0, 0] 1
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1 [0, 1] 7
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2 [0, 2] 4
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3 [0, 3] 13
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4 [0, 4] 1
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5 [1, 0] 11
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6 [1, 1] 2
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7 [1, 2] 14
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8 [1, 3] 8
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9 [1, 4] 11
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======= ============= =====================
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.. function:: void acb_dirichlet_dft(acb_ptr w, acb_srcptr v, const dirichlet_group_t G, slong prec)
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Compute the DFT of *v* using Conrey numbers.
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This function assumes *v* and *w* are vectors of size *G->q*.
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All values at index not coprime to *G->q* are ignored.
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Euler products
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-------------------------------------------------------------------------------
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.. function:: void _acb_dirichlet_euler_product_real_ui(arb_t res, ulong s, const signed char * chi, int mod, int reciprocal, slong prec)
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Sets *res* to `L(s,\chi)` where `\chi` is a real Dirichlet character
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given by the explicit list *chi* of character values at
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0, 1, ..., *mod* - 1. If *reciprocal* is set, computes `1 / L(s,\chi)`
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(this is faster if the reciprocal can be used directly).
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This function uses the Euler product, and is only intended for use when
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*s* is large. An error bound is computed via :func:`mag_hurwitz_zeta_uiui`.
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Since
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.. math ::
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\frac{1}{L(s,\chi)} = \prod_{p} \left(1 - \frac{\chi(p)}{p^s}\right)
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= \sum_{k=1}^{\infty} \frac{\mu(k)\chi(k)}{k^s}
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and the truncated product gives all smooth-index terms in the series, we have
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.. math ::
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\left|\prod_{p < N} \left(1 - \frac{\chi(p)}{p^s}\right) - \frac{1}{L(s,\chi)}\right|
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\le \sum_{k=N}^{\infty} \frac{1}{k^s} = \zeta(s,N).
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Simple functions
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-------------------------------------------------------------------------------
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.. function:: void acb_dirichlet_eta(acb_t res, const acb_t s, slong prec)
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Sets *res* to the Dirichlet eta function
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`\eta(s) = \sum_{k=1}^{\infty} (-1)^k / k^s = (1-2^{1-s}) \zeta(s)`,
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also known as the alternating zeta function.
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Note that the alternating character `\{1,-1\}` is not itself
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a Dirichlet character.
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L-functions
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-------------------------------------------------------------------------------
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.. function:: void acb_dirichlet_root_number_theta(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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.. function:: void acb_dirichlet_root_number(acb_t res, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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Sets *res* to the root number `\epsilon(\chi)` for a primitive character *chi*,
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which appears in the functional equation (where `p` is the parity of `\chi`):
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.. math::
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(\frac{q}{π})^{\frac{s+p}2}\Gamma(\frac{s+p}2) L(s, \chi) = \epsilon(\chi) (\frac{q}{π})^{\frac{1-s+p}2}\Gamma(\frac{1-s+p}2) L(1 - s, \overline\chi)
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- The *theta* variant uses the evaluation at `t=1` of the Theta series.
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- The default version computes it via the gauss sum.
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.. function:: void acb_dirichlet_l_hurwitz(acb_t res, const acb_t s, const dirichlet_group_t G, const dirichlet_char_t chi, slong prec)
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Compute `L(s,\chi)` using decomposition in terms of the Hurwitz zeta function
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.. math::
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L(s,\chi) = q^{-s}\sum_{k=1}^{q-1} \chi(k) \,\zeta\!\left(s,\frac kq\right).
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If `s = 1` and `\chi` is non-principal, the deflated Hurwitz zeta function
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is used to avoid poles.
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This formula is slow for large *q*.
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.. function:: void acb_dirichlet_l_vec_hurwitz(acb_ptr res, const acb_t s, const dirichlet_group_t G, slong prec)
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Compute all values `L(s,\chi)` for `\chi` mod `q`, by Hurwitz formula and
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discrete Fourier transform.
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*res* is assumed to have length *G->phi_q* and values are stored by lexicographically ordered
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Conrey logs. See :func:`acb_dirichlet_dft_conrey`.
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