Q\mathbb Q-linear dependence of certain Bessel moments

preprint2021arXivOpen access

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+1d t∣k∈Z≥0}, \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 a∈Z∩[1,b) a\in\mathbb Z\cap[1,b), our upper bound for the Q \mathbb Q-linear dimension is ⌊(a+b−1)/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+b−1)/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)]6td t=72∫0∞[I0(t)]2[K0(t)]6t3d t\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.

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