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arXiv 0704.2072nucl-ex
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氢气中μ子俘获率的测量及质子赝标耦合$g_P$的确定

Measurement of the Rate of Muon Capture in Hydrogen Gas and Determination of the Proton's Pseudoscalar Coupling $g_P$

V. A. Andreev, T. I. Banks, T. A. Case, D. B. Chitwood, S. M. Clayton, K. M. Crowe, J. Deutsch, J. Egger, S. J. Freedman, V. A. Ganzha, T. Gorringe, F. E. Gray,… 展开作者

V. A. Andreev, T. I. Banks, T. A. Case, D. B. Chitwood, S. M. Clayton, K. M. Crowe, J. Deutsch, J. Egger, S. J. Freedman, V. A. Ganzha, T. Gorringe, F. E. Gray, D. W. Hertzog, M. Hildebrandt, P. Kammel, B. Kiburg, S. Knaack, P. A. Kravtsov, A. G. Krivshich, B. Lauss, K. L. Lynch, E. M. Maev, O. E. Maev, F. Mulhauser, C. S. Özben, C. Petitjean, G. E. Petrov, R. Prieels, G. N. Schapkin, G. G. Semenchuk, M. A. Soroka, V. Tishchenko, A. A. Vasilyev, A. A. Vorobyov, M. E. Vznuzdaev, P. Winter

摘要:

利用一种基于时间投影室的新实验技术,在超净贫氘氢气中,在1 MPa的压力下,测量了质子捕获核μ介子的速率。捕获率由测量的$μ^-$在氢气中的消失率与$μ^+$衰变率的世界平均值之间的差值获得。与液态氢相比,靶的低气体密度为1%,这是避免μ子分子形成引起的不确定性的关键。从$μp$原子的超精细单重基态的俘获率被测量为$Λ_S=725.0 \pm 17.4 s^{-1}$,由此提取核子的诱导赝标耦合$g_P(q^2=-0.88 m_μ^2)=7.3 \pm 1.1$。这一结果与基于QCD的近似手征对称性的$g_P$的理论预测是一致的。

英文摘要:

The rate of nuclear muon capture by the proton has been measured using a new experimental technique based on a time projection chamber operating in ultra-clean, deuterium-depleted hydrogen gas at 1 MPa pressure. The capture rate was obtained from the difference between the measured $μ^-$ disappearance rate in hydrogen and the world average for the $μ^+$ decay rate. The target's low gas density of 1% compared to liquid hydrogen is key to avoiding uncertainties that arise from the formation of muonic molecules. The capture rate from the hyperfine singlet ground state of the $μp$ atom is measured to be $Λ_S=725.0 \pm 17.4 s^{-1}$, from which the induced pseudoscalar coupling of the nucleon, $g_P(q^2=-0.88 m_μ^2)=7.3 \pm 1.1$, is extracted. This result is consistent with theoretical predictions for $g_P$ that are based on the approximate chiral symmetry of QCD.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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