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arXiv 1909.00540hep-thgr-qchep-phnucl-th
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解析的自引力$4$ -重子、可穿越的NUT-AdS虫洞、有限体积的平坦时空多Skyrmions和$SU(3)$ -Skyrme模型中的一个新跃迁

Analytic self-gravitating $4$-Baryons, traversable NUT-AdS wormholes, flat space-time multi-Skyrmions at finite volume and a novel transition in the $SU(3)$-Skyrme model

Eloy Ayón-Beato, Fabrizio Canfora, Marcela Lagos, Julio Oliva, Aldo Vera

摘要:

通过将广义刺猬假设与Balachandran等人开发的方法相结合,我们为$SU(3)$ -Skyrme-Einstein- $Λ$理论构建了第一个四维解析的具有较高重子电荷的自引力Skyrmions。描述非嵌入解的第一个(数值)例子。这些是真正的$SU(3)$解析解,而不是$SU(2)$到$SU(3)$的平凡嵌入,它的几何形状是比安奇九世宇宙的几何形状。选择Skyrme参数,使得Skyrme场方程在重子荷为4的扇区中一致满足。场方程减少到一个动力学系统的三个比安奇IX标度因子。具体的解决方案进行了明确的分析。构造了拓扑非平凡$SU(3)$ -sigma孤子支持NUT-AdS渐近的可穿越虫孔.自引力解也承认一个合适的平坦极限,使电荷为4的Skyrmion被限制在一个有限体积的盒子里,从而保持了$SU(3)$ Skyrme场方程的可积性。这种形式主义揭示了一种新的过渡在有限的重子密度所产生的嵌入和非嵌入的解决方案之间的竞争,其中非嵌入的解决方案在高密度占上风,而在低密度被抑制。

英文摘要:

We construct the first analytic self-gravitating Skyrmions with higher Baryon charge in four dimensions for the $SU(3)$-Skyrme-Einstein-$Λ$ theory by combining the generalized hedgehog ansatz with the approach developed by Balachandran et al. to describe the first (numerical) example of a non-embedded solution. These are genuine $SU(3)$ analytic solutions instead of trivial embeddings of $SU(2)$ into $SU(3)$ and its geometry is that of a Bianchi IX Universe. The Skyrme ansatz is chosen in such a way that the Skyrme field equations are identically satisfied in the sector with Baryon charge 4. The field equations reduce to a dynamical system for the three Bianchi IX scale factors. Particular solutions are explicitly analyzed. Traversable wormholes with NUT-AdS asymptotics supported by a topologically non-trivial $SU(3)$-sigma soliton are also constructed. The self-gravitating solutions admit also a suitable flat limit giving rise to Skyrmions of charge 4 confined in a box of finite volume maintaining the integrability of the $SU(3)$ Skyrme field equations. This formalism discloses a novel transition at finite Baryon density arising from the competition between embedded and non-embedded solutions in which the non-embedded solutions prevail at high density while are suppressed at low densities.

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