从内部时空推导第一代粒子质量

Charlie Beil
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引用次数: 0

摘要

最近引入了内部时空几何,用退化的时空度量来模拟某些量子现象。我们使用这些度量的里奇张量来推导裸上下夸克质量的比值,得到 $m_u/m_d = 9604/19683 (约 .4879$)。在$overline{operatorname{MS}}$方案中,这个值在晶格QCD的$2 \operatorname{GeV}$ 值范围之内,即$.473 \pm .023$。此外,利用列维-塞维塔泊松方程,我们还推导出了着色电子质量与裸夸克质量的比值。对于掺杂电子质量为$.511 (operatorname{MeV}$时,这些比值得出裸夸克质量为$m_u (约2.2440 (operatorname{MeV}$)和$m_d (约4.599 (operatorname{MeV}$)。599 \operatorname{MeV}$,它们都在/接近于晶格QCD的值 $m^{overline\operatorname{MS}}_u =(2.20\pm .10) \operatorname{MeV}$和 $m^{overline\operatorname{MS}}_d =(4.69 \pm .07) \operatorname{MeV}$。最后,利用4元加速度,我们得出了上下夸克质量的比值$\tilde{m}_u/\tilde{m}_d = 48/49 (约0.98元)。这个值在组成夸克模型的 0.97 (sim 1)美元范围内。我们得到的所有比值都是根据第一原理得出的,没有任何自由参数或临时参数。此外,比较奇怪的是,我们的推导没有使用量子场论,而只使用了广义相对论的工具。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A derivation of the first generation particle masses from internal spacetime
Internal spacetime geometry was recently introduced to model certain quantum phenomena using spacetime metrics that are degenerate. We use the Ricci tensors of these metrics to derive a ratio of the bare up and down quark masses, obtaining $m_u/m_d = 9604/19683 \approx .4879$. This value is within the lattice QCD value at $2 \operatorname{GeV}$ in the $\overline{\operatorname{MS}}$-scheme, $.473 \pm .023$. Moreover, using the Levi-Cevita Poisson equation, we derive ratios of the dressed electron mass and bare quark masses. For a dressed electron mass of $.511 \operatorname{MeV}$, these ratios yield the bare quark masses $m_u \approx 2.2440 \operatorname{MeV}$ and $m_d \approx 4.599 \operatorname{MeV}$, which are within/near the lattice QCD values $m^{\overline{\operatorname{MS}}}_u = (2.20\pm .10) \operatorname{MeV}$ and $m^{\overline{\operatorname{MS}}}_d = (4.69 \pm .07) \operatorname{MeV}$. Finally, using $4$-accelerations, we derive the ratio $\tilde{m}_u/\tilde{m}_d = 48/49 \approx .98$ of the constituent up and down quark masses. This value is within the $.97 \sim 1$ range of constituent quark models. All of the ratios we obtain are from first principles alone, with no free or ad hoc parameters. Furthermore, and rather curiously, our derivations do not use quantum field theory, but only tools from general relativity.
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