English

$\mathbb Q$-linear dependence of certain Bessel moments

Number Theory 2022-06-13 v3 High Energy Physics - Theory

Abstract

Let I0I_0 and K0K_0 be modified Bessel functions of the zeroth order. We use Vanhove's differential operators for Feynman integrals to derive upper bounds for dimensions of the Q\mathbb Q-vector space spanned by certain sequences of Bessel moments {0[I0(t)]a[K0(t)]bt2k+1dtkZ0}, \left\{\left.\int_0^\infty [I_0(t)]^a[K_0(t)]^b t^{2k+1}\mathrm{d}\, t\right|k\in\mathbb Z_{\geq0}\right\},where aa and bb are fixed non-negative integers. For aZ[1,b) a\in\mathbb Z\cap[1,b), our upper bound for the Q \mathbb Q-linear dimension is (a+b1)/2\lfloor (a+b-1)/2\rfloor, which improves the Borwein-Salvy bound (a+b+1)/2\lfloor (a+b+1)/2\rfloor. Our new upper bound (a+b1)/2\lfloor (a+b-1)/2\rfloor is not sharp for a=2,b=6 a=2,b=6, due to an exceptional Q \mathbb Q-linear relation 0[I0(t)]2[K0(t)]6tdt=720[I0(t)]2[K0(t)]6t3dt\int_0^\infty [I_0(t)]^2[K_0(t)]^6 t\mathrm{d}\, t=72\int_0^\infty [I_0(t)]^2[K_0(t)]^6 t^{3}\mathrm{d}\, t, which is provable by integrating modular forms.

Keywords

Cite

@article{arxiv.1911.04141,
  title  = {$\mathbb Q$-linear dependence of certain Bessel moments},
  author = {Yajun Zhou},
  journal= {arXiv preprint arXiv:1911.04141},
  year   = {2022}
}

Comments

(v1) i+21 pages. Simplification and extension of some results in Section 5 of arXiv:1706.08308; (v2) i+29 pages; (v3) 20 pages, accepted version

R2 v1 2026-06-23T12:11:18.985Z