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arXiv 0804.1142hep-phhep-ex
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μ介子g-2与希格斯玻色子质量的边界

The muon g-2 and the bounds on the Higgs boson mass

M. Passera, W. J. Marciano, A. Sirlin

摘要:

在简单回顾μ子g-2的状态后,我们分析了目前实验与标准模型(SM)预测之间的差异可能是由于在确定强子主导阶对后者的贡献时假设错误的可能性。特别地,我们展示了在低能e^+e^-碰撞中强子产生截面的增加如何能够弥合μ子g-2的差异,然而却导致M_H的电弱上限,即SM希格斯玻色子玻色子质量的降低。根据初步的顶夸克质量M_t = 172.6(1.4)GeV和最近的测量Δα_{ \rm had}^{(5)}(M_Z)= 0.02768(22),目前的界为M_H < ~ 150 GeV(95%CL),而直接搜索的下界为M_H > 114.4 GeV(95%CL)。通过详细的分析,我们得出结论,这种解决方案的μ子g-2的差异是不可能的,鉴于目前的实验误差估计。然而,如果这被证明是解决方案,那么M_H的95%CL上限将减少到大约130 GeV,这与实验下限相结合,为这个基本粒子的质量留下了一个狭窄的窗口。

英文摘要:

After a brief review of the muon g-2 status, we analyze the possibility that the present discrepancy between experiment and the Standard Model (SM) prediction may be due to hypothetical errors in the determination of the hadronic leading-order contribution to the latter. In particular, we show how an increase of the hadro-production cross section in low-energy e^+e^- collisions could bridge the muon g-2 discrepancy, leading however to a decrease on the electroweak upper bound on M_H, the SM Higgs boson mass. That bound is currently M_H < ~ 150GeV (95%CL) based on the preliminary top quark mass M_t = 172.6(1.4)GeV and the recent determination Δα_{\rm had}^{(5)}(M_Z) = 0.02768(22), while the direct-search lower bound is M_H > 114.4GeV (95%CL). By means of a detailed analysis we conclude that this solution of the muon g-2 discrepancy is unlikely in view of current experimental error estimates. However, if this turns out to be the solution, the 95%CL upper bound on M_H is reduced to about 130GeV which, in conjunction with the experimental lower bound, leaves a narrow window for the mass of this fundamental particle.

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