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arXiv 2303.03474hep-thcond-mat.str-el
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来自弦图的large p SYK

Large p SYK from chord diagrams

Baur Mukhametzhanov

AI总结:

本文澄清了large p SYK与double-scaled SYK两种可精确求解极限之间的关系,并从后者出发推导前者极限下的欧几里得2n点关联函数和长时out-of-time-order四点函数,关键步骤是确定U_q(su(1,1)) 6j符号的渐近行为。

摘要:

有限温度下的p-body SYK模型表现出次最大混沌,并包含对偶JT引力的类弦修正。它可以在两个不同的极限下精确求解:“large p” SYK(1 ≪ p ≪ N)和“double-scaled” SYK(N, p → ∞,且λ = 2p²/N固定)。我们澄清了二者之间的关系。从double-scaled极限下的精确结果出发,我们推导了large p极限下的若干可观测量。我们计算了欧几里得2n点关联函数以及长洛伦兹时间下的out-of-time-order四点函数。为了计算这些关联函数,我们找到了U_q(su(1,1)) 6j符号的相关渐近行为。

英文摘要:

The p-body SYK model at finite temperature exhibits submaximal chaos and contains stringy-like corrections to the dual JT gravity. It can be solved exactly in two different limits: "large p" SYK $1 \ll p \ll N$ and "double-scaled" SYK $N,p \to \infty$ with $λ= 2 p^2/N$ fixed. We clarify the relation between the two. Starting from the exact results in the double-scaled limit, we derive several observables in the large p limit. We compute euclidean $2n$-point correlators and out-of-time-order four-point function at long lorentzian times. To compute the correlators we find the relevant asymptototics of the $U_{q}(su(1,1))$ 6j-symbol.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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