Absorbing discretisation effects with a massive renormalization scheme: the charm-quark mass

Fuente: arXiv
Guardado en:
Detalles Bibliográficos
Autores principales: Del Debbio, Luigi, Erben, Felix, Flynn, Jonathan M., Mukherjee, Rajnandini, Tsang, J. Tobias
Formato: Preprint
Publicado: 2024
Materias:
Acceso en línea:
Etiquetas: Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
_version_ 1866916337278779392
author Del Debbio, Luigi
Erben, Felix
Flynn, Jonathan M.
Mukherjee, Rajnandini
Tsang, J. Tobias
author_facet Del Debbio, Luigi
Erben, Felix
Flynn, Jonathan M.
Mukherjee, Rajnandini
Tsang, J. Tobias
contents We present the first numerical implementation of the massive SMOM (mSMOM) renormalization scheme and use it to calculate the charm quark mass. Based on ensembles with three flavours of dynamical domain wall fermions with lattice spacings in the range 0.11 -- 0.08 fm, we demonstrate that the mass scale which defines the mSMOM scheme can be chosen such that the extrapolation has significantly smaller discretisation effects than the SMOM scheme. Converting our results to the $\overline{\mathrm{MS}}$ scheme we obtain $\overline{m}_c(3\,\mathrm{GeV}) = 1.008(13)\,\mathrm{GeV}$ and $\overline{m}_c(\overline{m}_c) = 1.292(12)\,\mathrm{GeV}$.
format Preprint
id arxiv_https___arxiv_org_abs_2407_18700
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Absorbing discretisation effects with a massive renormalization scheme: the charm-quark mass
Del Debbio, Luigi
Erben, Felix
Flynn, Jonathan M.
Mukherjee, Rajnandini
Tsang, J. Tobias
High Energy Physics - Lattice
High Energy Physics - Phenomenology
We present the first numerical implementation of the massive SMOM (mSMOM) renormalization scheme and use it to calculate the charm quark mass. Based on ensembles with three flavours of dynamical domain wall fermions with lattice spacings in the range 0.11 -- 0.08 fm, we demonstrate that the mass scale which defines the mSMOM scheme can be chosen such that the extrapolation has significantly smaller discretisation effects than the SMOM scheme. Converting our results to the $\overline{\mathrm{MS}}$ scheme we obtain $\overline{m}_c(3\,\mathrm{GeV}) = 1.008(13)\,\mathrm{GeV}$ and $\overline{m}_c(\overline{m}_c) = 1.292(12)\,\mathrm{GeV}$.
title Absorbing discretisation effects with a massive renormalization scheme: the charm-quark mass
topic High Energy Physics - Lattice
High Energy Physics - Phenomenology
url https://arxiv.org/abs/2407.18700