Higgs-like (pseudo)Scalars in AdS$_4$, Marginal and Irrelevant Deformations in CFT$_3$ and Instantons on $S^3$

Mohammad Naghdi
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Abstract

With a 4-form ansatz of 11-dimensional supergravity over non-dynamical $AdS_4 \times S^7/Z_k$ background, with the internal space as a $S^1$ Hopf fibration on $CP^3$, we get a consistent truncation. The (pseudo)scalars, in the resulting scalar equations in Euclidean AdS$_4$ space, may be viewed as arising from (anti)M-branes wrapping around internal directions in the (Wick-rotated) skew-whiffed M2-branes background (as the resulting theory is for anti-M2-branes) and so, realizing the modes after swapping the three fundamental representations $\textbf{8}_s$, $\textbf{8}_c$, $\textbf{8}_v$ of $SO(8)$. Taking the backreaction on the external and internal spaces, we get massless and massive modes, corresponding to exactly marginal and marginally irrelevant deformations on the boundary CFT$_3$, and write a closed solution for the bulk equation and compute its correction to the background action. Next, considering the Higgs-like (breathing) mode $m^2=18$, having all supersymmetries, parity and scale-invariance broken, by solving the associated bulk equation with mathematical methods, especially the Adomian decomposition method, and analyzing the behavior near the boundary of the solutions, we realize the boundary duals in $SU(4) \times U(1)$-singlet sectors of the ABJM model. Then, introducing new dual deformation $\Delta_+ = 3, 6$ operators made of bi-fundamental scalars, fermions and $U(1)$ gauge fields, we obtain $SO(4)$-invariant solutions as small instantons on a three-sphere with radius at infinity, which actually correspond to collapsing bulk bubbles leading to big-crunch singularities. Content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. Article funded by SCOAP3 and published under licence by Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Science and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd.
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AdS$_4$ 中的希格斯类(伪)标量、CFT$_3$ 中的边际变形和无关变形以及 $S^3$ 上的瞬子
在非动力$AdS_4 \times S^7/Z_k$背景上的11维超引力的4形式解析,内部空间为$CP^3$上的$S^1$霍普夫纤维,我们得到了一致的截断。在欧几里得 AdS$_4$ 空间中得到的标量方程中的(伪)标量,可以看作是(反)M2-ranes 在(Wick-rotated)skew-whiffed M2-ranes背景中围绕内部方向产生的(反)M2-ranes(因为得到的理论是反 M2-ranes),因此,我们可以把这些(伪)标量看作是(反)M2-ranes 在(Wick-rotated)skew-whiffed M2-ranes背景中围绕内部方向产生的、实现了交换$SO(8)$的三个基本表示$\textbf{8}_s$, $\textbf{8}_c$, $\textbf{8}_v$之后的模式。通过外部和内部空间的反作用,我们得到了无质量和大质量模,分别对应于边界 CFT$_3$ 上的精确边际变形和边际无关变形,并写出了体方程的封闭解,计算了它对背景作用的修正。接下来,考虑到希格斯类(呼吸)模式$m^2=18$,所有超对称性、奇偶性和尺度不变性都被打破,通过用数学方法,特别是阿多米分解方法求解相关的体方程,并分析解在边界附近的行为,我们实现了ABJM模型在$SU(4) \times U(1)$-singlet 扇区的边界对偶。然后,引入由双基本标量、费米子和$U(1)$量规场组成的新对偶变形$\Delta_+ = 3, 6$算子,我们得到了$SO(4)$不变解,它是一个半径为无穷大的三球体上的小瞬子,实际上对应于导致大紧缩奇点的塌缩体泡。本作品内容可根据知识共享署名 3.0 许可条款使用。如需进一步传播本作品,必须注明作者、作品名称、期刊引文和 DOI。文章由 SCOAP3 资助,由中国物理学会、中国科学院高能物理研究所、中国科学院近代物理研究所和 IOP Publishing Ltd. 授权出版。
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