论文标题
在SU（2）YANG-MILLS热力学的紧急颗粒和稳定的中性血浆球上
On emergent particles and stable neutral plasma balls in SU(2) Yang-Mills thermodynamics
论文作者
论文摘要
For a pure SU(2) Yang-Mills theory in 4D we revisit the spatial (3D), ball-like region of radius $r_0$, in its bulk subject to the pressureless, deconfining phase at $T_0=1.32\,T_c$ where $T_c$ denotes the critical temperature for the onset of the deconfining-preconfining phase transition. Such a region possesses of a finite energy density and represents the self-intersection of a figure-eight shaped center-vortex loop if a BPS monopole of core radius $\sim \frac{r_0}{52.4}$, isolated from its antimonopole by repulsion externally invoked through a transient shift of (anti)caloron holonomy (pair creation), is trapped therein.整个Soliton（涡旋线以及包含单极的质量$ M_0 $的自我交流区域）可以被认为是对限制阶段的无压力和无能基态的激发。纠正$ r_0 $的较早估计值，我们表明涡流自我交流区域与A（n）（anti）Caloron的{\ sl Central Part}相关联，并且该区域通过（1）单位通过（1）单位电荷通过（电磁性双向解释）的单极管电荷。单极核心量子在热力学确定的频率$ω_0$下振动，尚未解决。对于$ t = t_0 $的零压力背景的解剖相位等离子振荡，我们计算{\ sl中性}内的最低频率$ω_0$，并且在其RADIUS $ r_0 $的依赖性方面和均质的空间球（无捕获的单子）。对于$ r_0 = r_0 $ $ω_0$与$ω_0$的比较表明，中性等离子体振荡的振荡比由单极芯的振荡驱动的同一等离子体慢得多。
For a pure SU(2) Yang-Mills theory in 4D we revisit the spatial (3D), ball-like region of radius $r_0$, in its bulk subject to the pressureless, deconfining phase at $T_0=1.32\,T_c$ where $T_c$ denotes the critical temperature for the onset of the deconfining-preconfining phase transition. Such a region possesses of a finite energy density and represents the self-intersection of a figure-eight shaped center-vortex loop if a BPS monopole of core radius $\sim \frac{r_0}{52.4}$, isolated from its antimonopole by repulsion externally invoked through a transient shift of (anti)caloron holonomy (pair creation), is trapped therein. The entire soliton (vortex line plus region of self-intersection of mass $m_0$ containing the monopole) can be considered an excitation of the pressureless and energyless ground state of the confining phase. Correcting an earlier estimate of $r_0$, we show that the vortex-loop self-intersection region associates with the {\sl central part} of a(n) (anti)caloron and that this region carries one unit of electric U(1) charge via the (electric-magnetic dually interpreted) charge of the monopole. The monopole core quantum vibrates at a thermodynamically determined frequency $ω_0$ and is unresolved. For a deconfining-phase plasma oscillation about the zero-pressure background at $T=T_0$ we compute the lowest frequency $Ω_0$ within a {\sl neutral} and homogeneous spatial ball (no trapped monopole) in dependence of its radius $R_0$. For $R_0=r_0$ a comparison of $Ω_0$ with $ω_0$ reveals that the neutral plasma oscillates much slower than the same plasma driven by the oscillation of a monopole core.
