acb_theta_ql_jet_fd, acb_theta_ql_jet
#include <flint/acb_theta.h>void acb_theta_ql_jet_fd(acb_ptr th, acb_srcptr zs, slong nb, const acb_mat_t tau, slong ord, int all, slong prec)sourcevoid acb_theta_ql_jet(acb_ptr th, acb_srcptr zs, slong nb, const acb_mat_t tau, slong ord, int all, slong prec)sourceSet th to the derivatives up to order ord of at the nb pairs , for all and for all (all nonzero) or ; the output is the concatenation of nb times (or ) vectors of derivatives. acb_theta_ql_jet_fd uses finite differences on the output of acb_theta_ql_exact, in time quasi-linear in for fixed ; acb_theta_ql_jet uses direct summation instead when ord is positive and the precision is low (few duplication steps would be needed).
The finite difference method evaluates at for a primitive -th root of unity , , and all ; a discrete Fourier transform gives for each , where are the Taylor coefficients. By the Cauchy formula with the bound of acb_theta_ql_local_bound, the error is at most before division by . The function chooses , strips of their radii, raises the precision to compensate for the division by , and restores certified radii with acb_theta_ql_jet_error and derivatives to order computed at low precision; see Derivatives.
Guides#
The FLINT team, “acb_theta_ql_jet_fd, acb_theta_ql_jet (acb_theta.h),” FLINT: Fast Library for Number Theory, documentation, version 3.7.0-dev, 2026. https://flintlib.org/doc/acb_theta/acb_theta_ql_jet_fd.html (generated 2026-11-02).
@misc{flint-doc-acb-theta-acb-theta-ql-jet-fd,
author = {{The FLINT team}},
title = {{acb\_theta\_ql\_jet\_fd, acb\_theta\_ql\_jet (acb\_theta.h)}},
howpublished = {FLINT: Fast Library for Number Theory, documentation, version 3.7.0-dev},
year = {2026},
url = {https://flintlib.org/doc/acb_theta/acb_theta_ql_jet_fd.html},
note = {Generated 2026-11-02}
}