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arXiv 2404.16601hep-th
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非AdS全息中的旋转弦与反常维数

Rotating strings and anomalous dimensions in Non-AdS holography

Meseret Asrat

AI总结:

本文研究了非AdS弦背景中刚性旋转闭合弦的构型,计算了大角动量极限下的能量与角动量差,发现该量及特定条件下能量和角动量均存在上界,并揭示了其与二维CFT中算子反常维数及单迹TTbar变形的对偶关系。

摘要:

在本文中,我们考虑在渐近非AdS弦背景中的某些刚性旋转闭合弦构型。该弦背景是 $AdS_{3} \times {\cal M}_7$ 的变形。它在 $AdS_{3}$ 和渐近线性膨胀子 ${\rm I\\!R} \times S^1 \times {\rm I\\!R}$ 时空(乘以内部紧致流形 ${\cal M}_7$)之间进行插值。我们计算了量 $E - J$(在大 $J$ 极限下),其中 $E$ 是能量,$J$ 是旋转弦的角动量。在对偶于 $AdS_{3}$(乘以 ${\cal M}_7$)上弦论的二维 CFT 中,它给出了某些扭度二及更高算子的反常维数。我们在变形背景中表明 $E - J$ 是有界的。在变形耦合的特殊值下,我们还表明,对于包含 $n > 2$ 个尖点或尖刺的旋转闭合弦,$E$ 和 $J$ 都是有界的。在对偶于 $AdS_{3}$(乘以 ${\cal M}_7$)上弦论的 CFT 中,旋转的尖点弦描述了扭度 $n$ 大于二的算子。一般而言,在变形耦合的其他值处,我们证明了此特征仅由那些 $n > n_0$ 的尖点弦所展现,其中 $n_0$ 仅由变形耦合决定。我们还给出了 $E$ 和 $J$ 之间简单的精确 Regge 关系。我们还研究了类光 Wilson 环密切相关的尖点反常维数。我们讨论了在耦合空间中沿变形远离 CFT 时 $E - J$ 所度量的物理量。在长弦部分,该变形对偶于单迹 $T{\bar T}$ 变形的轨道理论。我们确定了相关的变形 sinh-Gordon 模型,该模型在经典上描述了边界附近的(长)弦。这提供了非轨道理论中单迹 $T{\bar T}$ 变形的一个实例。

英文摘要:

In this paper we consider certain rigidly rotating closed string configurations in an asymptotically non-AdS string background. The string background is a deformation of $AdS_3 \times {\cal M}_7$. It interpolates between $AdS_3 $ and asymptotically linear dilaton ${\rm I\!R} \times S^1 \times {\rm I\!R}$ spacetime (times the internal compact manifold ${\cal M}_7$). We compute the quantity $E - J$ (in the large $J$ limit) where $E$ is the energy and $J$ is the angular momentum of the spinning strings. In the two dimensional CFT dual to string theory on $AdS_3$ (times ${\cal M}_7$) it gives the anomalous dimensions of certain twist two and higher operators. We show in the deformed background that $E - J$ is bounded. At a special value of the deformation coupling we also show that for spinning closed strings containing $n > 2$ cusps or spikes both $E$ and $J$ are bounded. In the CFT dual to string theory on $AdS_3$ (times ${\cal M}_7$) the spinning cusped strings describe operators with twist $n$ larger than two. In general, at other values of the deformation coupling, we demonstrate that this feature is exhibited only by those cusped strings with $n > n_0$ where $n_0$ is determined only by the deformation coupling. We also give simple exact Regge relations between $E$ and $J$. We also study the closely related cusp anomalous dimension of a light-like Wilson loop. We comment on what $E - J$ measures away from the CFT along the deformation in the coupling space. In the long string sector the deformation is dual to a single trace $T{\bar T}$ deformed orbifold theory. We determine the associated deformed sinh-Gordon model that classically describes the (long) strings near the boundary. This provides an example of single trace $T{\bar T}$ deformation in non-orbifold theories.

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