Volume 430 -
The 39th International Symposium on Lattice Field Theory (LATTICE2022) -
Standard Model Parameters

Log-enhanced discretization errors in integrated correlation functions

Full text:
pdf

Pre-published on:
March 15, 2023

Published on:
April 06, 2023

Abstract

Integrated time-slice correlation functions $G(t)$ with weights $K(t)$ appear, e.g., in

the moments method to determine $\alpha_s$ from heavy quark correlators,

in the muon g-2 determination or in the determination of smoothed spectral

functions.

For the (leading-order-)normalised moment $R_4$ of the pseudo-scalar correlator

we have non-perturbative results down to $a=10^{-2}$ fm and for masses, $m$, of the order of the charm

mass in the quenched approximation. A significant bending of $R_4$ as a function of $a^2$ is observed at small lattice

spacings.

\\

Starting from the Symanzik expansion

of the integrand we derive the asymptotic convergence of the integral at small lattice spacing in the free theory and prove

that the short distance part of the integral leads to $\log(a)$-enhanced

discretisation errors when $G(t)K(t) \sim\, t $ for small $t$.

In the interacting theory an unknown,

function $K(a\Lambda)$ appears.

\\

For the $R_4$-case, we modify the observable to improve the short distance behavior and demonstrate that it results in a very smooth continuum limit. The strong coupling and the $\Lambda$-parameter can then be extracted. In general, and in particular for $g-2$, the short distance part of the integral should be determined by perturbation theory. The (dominating) rest can then be obtained by the controlled continuum limit of the lattice computation.

Integrated time-slice correlation functions $G(t)$ with weights $K(t)$ appear, e.g., in

the moments method to determine $\alpha_s$ from heavy quark correlators,

in the muon g-2 determination or in the determination of smoothed spectral

functions.

For the (leading-order-)normalised moment $R_4$ of the pseudo-scalar correlator

we have non-perturbative results down to $a=10^{-2}$ fm and for masses, $m$, of the order of the charm

mass in the quenched approximation. A significant bending of $R_4$ as a function of $a^2$ is observed at small lattice

spacings.

\\

Starting from the Symanzik expansion

of the integrand we derive the asymptotic convergence of the integral at small lattice spacing in the free theory and prove

that the short distance part of the integral leads to $\log(a)$-enhanced

discretisation errors when $G(t)K(t) \sim\, t $ for small $t$.

In the interacting theory an unknown,

function $K(a\Lambda)$ appears.

\\

For the $R_4$-case, we modify the observable to improve the short distance behavior and demonstrate that it results in a very smooth continuum limit. The strong coupling and the $\Lambda$-parameter can then be extracted. In general, and in particular for $g-2$, the short distance part of the integral should be determined by perturbation theory. The (dominating) rest can then be obtained by the controlled continuum limit of the lattice computation.

DOI: https://doi.org/10.22323/1.430.0358

How to cite

Metadata are provided both in "article" format (very similar to INSPIRE) as this helps creating very compact bibliographies which can be beneficial to authors and readers, and in "proceeding" format which is more detailed and complete.

Open Access

Copyright owned by the author(s) under the term of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License.