Mass of the bottom quark from Upsilon(1S) at NNNLO: An update

César Ayala; Gorazd Cvetič; Antonio Pineda

doi:10.1088/1742-6596/762/1/012063

Mass of the bottom quark from Upsilon(1S) at NNNLO: An update

César Ayala
, Gorazd Cvetič
, Antonio Pineda

University of Valencia
Universidad Técnica Federico Santa Maria
Autonomous University of Barcelona

Research output: Contribution to journal › Conference article › peer-review

14 Scopus citations

Abstract

We update our perturbative determination of MS mass m_b(m_b), by including the recently obtained four-loop coefficient in the relation between the pole and MS mass. First the renormalon subtracted (RS or RS') mass is determined from the known mass of the Y(1S) meson, where we use the renormalon residue N_m obtained from the asymptotic behavior of the coefficient of the 3-loop static singlet potential. MS mass is then obtained using the 4-loop renormalon-free relation between the RS (RS') and MS mass. We argue that the effects of the charm quark mass are accounted for by effectively using N_f = 3 in the mass relations. The extracted value is m_b(m_b) = 4222(40) MeV, where the uncertainty is dominated by the renormalization scale dependence.

Original language	English
Article number	012063
Journal	Journal of Physics: Conference Series
Volume	762
Issue number	1
DOIs	https://doi.org/10.1088/1742-6596/762/1/012063
State	Published - 21 Nov 2016
Externally published	Yes
Event	17th International Workshop on Advanced Computing and Analysis Techniques in Physics Research, ACAT 2016 - Valparaiso, Chile Duration: 18 Jan 2016 → 22 Jan 2016

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10.1088/1742-6596/762/1/012063

Cite this

@article{2a655da094774af6afaf50e947f42d09,

title = "Mass of the bottom quark from Upsilon(1S) at NNNLO: An update",

abstract = "We update our perturbative determination of MS mass mb(mb), by including the recently obtained four-loop coefficient in the relation between the pole and MS mass. First the renormalon subtracted (RS or RS') mass is determined from the known mass of the Y(1S) meson, where we use the renormalon residue Nm obtained from the asymptotic behavior of the coefficient of the 3-loop static singlet potential. MS mass is then obtained using the 4-loop renormalon-free relation between the RS (RS') and MS mass. We argue that the effects of the charm quark mass are accounted for by effectively using Nf = 3 in the mass relations. The extracted value is mb(mb) = 4222(40) MeV, where the uncertainty is dominated by the renormalization scale dependence.",

author = "C{\'e}sar Ayala and Gorazd Cveti{\v c} and Antonio Pineda",

year = "2016",

month = nov,

day = "21",

doi = "10.1088/1742-6596/762/1/012063",

language = "English",

volume = "762",

journal = "Journal of Physics: Conference Series",

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note = "17th International Workshop on Advanced Computing and Analysis Techniques in Physics Research, ACAT 2016 ; Conference date: 18-01-2016 Through 22-01-2016",

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TY - JOUR

T1 - Mass of the bottom quark from Upsilon(1S) at NNNLO

T2 - 17th International Workshop on Advanced Computing and Analysis Techniques in Physics Research, ACAT 2016

AU - Ayala, César

AU - Cvetič, Gorazd

AU - Pineda, Antonio

PY - 2016/11/21

Y1 - 2016/11/21

N2 - We update our perturbative determination of MS mass mb(mb), by including the recently obtained four-loop coefficient in the relation between the pole and MS mass. First the renormalon subtracted (RS or RS') mass is determined from the known mass of the Y(1S) meson, where we use the renormalon residue Nm obtained from the asymptotic behavior of the coefficient of the 3-loop static singlet potential. MS mass is then obtained using the 4-loop renormalon-free relation between the RS (RS') and MS mass. We argue that the effects of the charm quark mass are accounted for by effectively using Nf = 3 in the mass relations. The extracted value is mb(mb) = 4222(40) MeV, where the uncertainty is dominated by the renormalization scale dependence.

AB - We update our perturbative determination of MS mass mb(mb), by including the recently obtained four-loop coefficient in the relation between the pole and MS mass. First the renormalon subtracted (RS or RS') mass is determined from the known mass of the Y(1S) meson, where we use the renormalon residue Nm obtained from the asymptotic behavior of the coefficient of the 3-loop static singlet potential. MS mass is then obtained using the 4-loop renormalon-free relation between the RS (RS') and MS mass. We argue that the effects of the charm quark mass are accounted for by effectively using Nf = 3 in the mass relations. The extracted value is mb(mb) = 4222(40) MeV, where the uncertainty is dominated by the renormalization scale dependence.

UR - https://www.scopus.com/pages/publications/85002252562

U2 - 10.1088/1742-6596/762/1/012063

DO - 10.1088/1742-6596/762/1/012063

M3 - Conference article

AN - SCOPUS:85002252562

SN - 1742-6588

VL - 762

JO - Journal of Physics: Conference Series

JF - Journal of Physics: Conference Series

IS - 1

M1 - 012063

Y2 - 18 January 2016 through 22 January 2016

ER -

Mass of the bottom quark from Upsilon(1S) at NNNLO: An update

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