论文标题
关于Abelian U（1）QED量规相互作用的夸克禁令的问题
On the question of quark confinement in the Abelian U(1) QED gauge interaction
论文作者
论文摘要
如果我们将轻夸克近似为无质量，并将schwinger限制机制应用于轻夸克，我们将得出一个结论，即在Abelian U（1+1）d的Abelian U（1）QED量表中的轻Quark $ Q $及其Antiquark $ \ bar Q $将被限制在Abelian U（1+1）d的Abelian U（1）QED量表中的相互作用。从科尔曼，杰基和苏斯金德的工作中，我们可以进一步推断出，即使在（1+1）d中的大量夸克中，施温格限制机制仍然存在。在（1+1）d中，（3+1）d中（3+1）d中的通量管的理想化是在（1+1）d中使用（1+1）d中的这样的Q $ Q $一维开口字符串，类似于QCD结合$ q \ bar q $打开字符串的情况吗？如果是这样，QED限制的$ Q \ bar Q $玻色子可能会在许多MEV的群众区域中以中性QED媒介物的形式出现（PRC81（2010）064903＆JHEP2020（8）165）。是否有可能仅在QED中产生夸克和古夸克来形成of Qed的介体？是否存在Qed介子（或Qed介子）存在的实验证据？异常软光子，X17粒子和E38粒子的观察结果表明，它们可能具有这种Qed介子存在的实验证据。对X17和E38颗粒的进一步确认和研究将对（3+1）d中的QED中的Quark限制问题确定。讨论了Quark限制在QED相互作用中的含义。
If we approximate light quarks as massless and apply the Schwinger confinement mechanism to light quarks, we will reach the conclusion that a light quark $q$ and its antiquark $\bar q$ will be confined as a $q\bar q$ boson in the Abelian U(1) QED gauge interaction in (1+1)D, as in an open string. From the work of Coleman, Jackiw, and Susskind, we can infer further that the Schwinger confinement mechanism persists even for massive quarks in (1+1)D. Could such a QED-confined $q\bar q$ one-dimensional open string in (1+1)D be the idealization of a flux tube in the physical world in (3+1)D, similar to the case of QCD-confined $q\bar q$ open string? If so, the QED-confined $q\bar q$ bosons may show up as neutral QED mesons in the mass region of many tens of MeV (PRC81(2010)064903 & JHEP2020(8)165). Is it ever possible that a quark and an antiquark be produced and interact in QED alone to form a confined QED meson? Is there any experimental evidence for the existence of a QED meson (or QED mesons)? The observations of the anomalous soft photons, the X17 particle, and the E38 particle suggest that they may bear the experimental evidence for the existence of such QED mesons. Further confirmation and investigations on the X17 and E38 particles will shed definitive light on the question of quark confinement in QED in (3+1)D. Implications of quark confinement in the QED interaction are discussed.
