arb_hypgeom_airy_zero
#include <flint/arb_hypgeom.h>void arb_hypgeom_airy_zero(arb_t a, arb_t a_prime, arb_t b, arb_t b_prime, const fmpz_t n, slong prec)sourceSets a, a_prime, b, b_prime to the n-th real zero a_n, a'_n, b_n, b'_n of \operatorname{Ai}, \operatorname{Ai}', \operatorname{Bi}, \operatorname{Bi}' respectively; any of them may be NULL. The zeros are negative and indexed by increasing magnitude starting with n = 1, as in the literature. An index n \le 0 raises an exception.
A starting enclosure comes from a table for n \le 10 and otherwise from the asymptotic expansions a_n \sim -T(\tfrac38 \pi (4n-1)), b_n \sim -T(\tfrac38\pi(4n-3)), a'_n \sim -U(\tfrac38\pi(4n-3)), b'_n \sim -U(\tfrac38\pi(4n-1)) [NIST2012, §9.9], whose truncations give proven bounds for a_n and b_n [PS1991]. The enclosure is refined by interval Newton iteration with doubling precision; for the zeros of the derivatives, for which the asymptotic bounds are not proved, an interval Newton step verifies that the enclosure contains the zero.
References#
- [NIST2012] National Institute of Standards and Technology, Digital Library of Mathematical Functions (2012), https://dlmf.nist.gov/
- [PS1991] G. Pittaluga and L. Sacripante, "Inequalities for the zeros of the Airy functions", SIAM J. Math. Anal. 22:1 (1991), 260-267.
The FLINT team, “arb_hypgeom_airy_zero (arb_hypgeom.h),” FLINT: Fast Library for Number Theory, documentation, version 3.7.0-dev, 2026. https://flintlib.org/doc/arb_hypgeom/arb_hypgeom_airy_zero.html (generated 2026-10-20).
@misc{flint-doc-arb-hypgeom-arb-hypgeom-airy-zero,
author = {{The FLINT team}},
title = {{arb\_hypgeom\_airy\_zero (arb\_hypgeom.h)}},
howpublished = {FLINT: Fast Library for Number Theory, documentation, version 3.7.0-dev},
year = {2026},
url = {https://flintlib.org/doc/arb_hypgeom/arb_hypgeom_airy_zero.html},
note = {Generated 2026-10-20}
}