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首页> 外文期刊>The journal of high energy physics >The bottom quark mass from the ? 1 S $$ oldsymbol{Upsilon} (1S) $$ system at NNNLO
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The bottom quark mass from the ? 1 S $$ oldsymbol{Upsilon} (1S) $$ system at NNNLO

机译:来自 1 s $$ boldsymbol { upsilon}(1s)$$ 系统在NNNLO

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A bstract We obtain an improved determination of the normalization constant of the first infrared renormalon of the pole mass (and the singlet static potential). For N ~( f )= 3 it reads N ~( m )= 0 . 563(26). Charm quark effects in the bottom quark mass determination are carefully investigated. Finally, we determine the bottom quark mass using the NNNLO perturbative expression for the ? 1 S $$ oldsymbol{Upsilon} (1S) $$ mass. We work in the renormalon subtracted scheme, which allows us to control the divergence of the perturbation series due to pole mass renormalon. Our result for the MS ˉ $$ overline{mathrm{MS}} $$ mass reads m ˉ b m b = 4201 43 $$ {overline{m}}_bleft({m}_bight)=4201(43) $$ MeV.
机译:Bstract我们获得了改进的确定极块(和单线态静电)的第一红外Renormalon的归一化常数的确定。对于n〜(f)= 3,它读取n〜(m)= 0。 563(26)。仔细研究了底部夸克质量决定中的魅力夸克效应。最后,我们使用NNNLO扰动表达来确定底夸克质量? 1 s $$ boldsymbol { upsilon}(1s)$$质量。我们在Renormalon减去方案中工作,使我们能够控制由于杆子批量级重型而导致的扰动系列的分歧。我们的结果是MSˉ$$ overline { mathrm {ms}} $$质量读取m∈BMB= 4201 43 $$ { overline {m}} _ b left({m} _b revally)= 4201( 43)$$ MEV。

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