论文标题
部分可观测时空混沌系统的无模型预测
New phases of $\mathcal{N}=4$ SYM at finite chemical potential
论文作者
论文摘要
我们对超级实力解决方案进行系统的搜索,该解决方案通过广告$ _5 $/cft $ _4 $通讯是对$ \ Mathcal {n} = 4 $ Syms in Pricitie Chemical潜力的热状态双重偶性的。这些解决方案主导了微型人体集合,并最终需要重现ADS黑洞的微观熵。使用分析方法和数值方法的混合,我们用全球广告$ _5 $渐近器来构建和研究带有全球广告的静态带电毛状孤子和黑洞解决方案。它们是在两个不同的一致截断的五个尺寸测量超级重力的两种一致的截断中的(因此可以将其提升到渐近广告$ _5 \ times $ s $ s $^5 $ iib iib supergravity的解决方案)。在由一个带电的标量场组成的“单电荷”截断中,毛茸茸的黑洞存在于临界电荷上方,并与已知的Behrndt-Cvetič-Sabra(BCS)合并,沿着后者家族的超级崇拜的发作确定。最低的质毛黑洞是一个奇异的零熵孤子。在由两个相等的电荷标量磁场组成的“两个电荷”截断中,存在所有电荷的毛茸茸的黑洞,并与已知的BCS黑洞沿其超级发作曲线合并。最低质量毛状黑洞是光滑的超对称零熵孤子。与三个相等的电荷的截断阶段的已知阶段一起,我们的发现可以很好地了解具有三个任意化学势的Sym热状态的整个相空间。
We do a systematic search of supergravity solutions that, via the AdS$_5$/CFT$_4$ correspondence, are dual to thermal states in $\mathcal{N}=4$ SYM at finite chemical potential. These solutions dominate the microcanonical ensemble and are required to ultimately reproduce the microscopic entropy of AdS black holes. Using a mix of analytical and numerical methods, we construct and study static charged hairy solitonic and black hole solutions with global AdS$_5$ asymptotics. They are constructed in two distinct consistent truncations of five dimensional gauged supergravity (and can thus be uplifted to asymptotically AdS$_5\times$S$^5$ solutions of type IIB supergravity). In the "single charge" truncation which consists of one charged scalar field, hairy black holes exist above a critical charge and merge with the known Behrndt-Cvetič-Sabra (BCS) black holes along a curve determined by the onset of superradiance in the latter family. The lowest mass hairy black hole is a singular zero entropy soliton. In the "two charge" truncation which consists of a two equal charged scalar fields, hairy black holes exist for all charges and merge with the known BCS black holes along their superradiant onset curve. The lowest mass hairy black hole is a smooth supersymmetric zero entropy soliton. Together with the known phases of the truncation with three equal charges, our findings permit a good understanding of the full phase space of SYM thermal states with three arbitrary chemical potentials.