TY - JOUR
T1 - Renormalon subtraction in OPE using Fourier transform
T2 - formulation and application to various observables
AU - Hayashi, Yuuki
AU - Sumino, Yukinari
AU - Takaura, Hiromasa
N1 - Publisher Copyright:
© 2022, The Author(s).
PY - 2022/2
Y1 - 2022/2
N2 - Properly separating and subtracting renormalons in the framework of the op- erator product expansion (OPE) is a way to realize high precision computation of QCD effects in high energy physics. We propose a new method (FTRS method), which enables to subtract multiple renormalons simultaneously from a general observable. It utilizes a property of Fourier transform, and the leading Wilson coefficient is written in a one-parameter integral form whose integrand has suppressed (or vanishing) renormalons. The renormalon subtraction scheme coincides with the usual principal-value prescription at large orders. We perform test analyses and subtract the O(ΛQCD4) renormalon from the Adler function, the O(ΛQCD2) renormalon from the B → Xulν¯ decay width, and the O(ΛQCD) and O(ΛQCD2) renormalons from the B, D meson masses. The analyses show good consistency with theoretical expectations, such as improved convergence and scale dependence. In particular we obtain Λ ¯ FTRS = 0.495 ± 0.053 GeV and (μπ2)FTRS = −0.12 ± 0.23 GeV2 for the non-perturbative parameters of HQET. We explain the formulation and analyses in detail.
AB - Properly separating and subtracting renormalons in the framework of the op- erator product expansion (OPE) is a way to realize high precision computation of QCD effects in high energy physics. We propose a new method (FTRS method), which enables to subtract multiple renormalons simultaneously from a general observable. It utilizes a property of Fourier transform, and the leading Wilson coefficient is written in a one-parameter integral form whose integrand has suppressed (or vanishing) renormalons. The renormalon subtraction scheme coincides with the usual principal-value prescription at large orders. We perform test analyses and subtract the O(ΛQCD4) renormalon from the Adler function, the O(ΛQCD2) renormalon from the B → Xulν¯ decay width, and the O(ΛQCD) and O(ΛQCD2) renormalons from the B, D meson masses. The analyses show good consistency with theoretical expectations, such as improved convergence and scale dependence. In particular we obtain Λ ¯ FTRS = 0.495 ± 0.053 GeV and (μπ2)FTRS = −0.12 ± 0.23 GeV2 for the non-perturbative parameters of HQET. We explain the formulation and analyses in detail.
KW - Effective Field Theories
KW - Nonperturbative Effects
KW - Perturbative QCD
KW - Quark Masses and SM Parameters
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U2 - 10.1007/JHEP02(2022)016
DO - 10.1007/JHEP02(2022)016
M3 - Article
AN - SCOPUS:85124334918
SN - 1126-6708
VL - 2022
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 2
M1 - 16
ER -