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arXiv 2607.17346hep-thcond-mat.dis-nncond-mat.stat-mechmath-phmath.MPquant-ph

克里洛夫可观测量的信息内容:一种机器学习方法

The Information Content of Krylov Observables: A Machine Learning Approach

Ritam Basu

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中文总结 AI 辅助

该研究用机器学习量化克里洛夫空间可观测量的信息,训练小型残差网络等,发现其能确定热场温度,无法重构精细谱形式因子,二阶矩信息盈余是混沌标志,还推导了相关机制和界限。

中文摘要 AI 辅助

我们采用机器学习来量化三个克里洛夫空间可观测量所携带的信息:展宽复杂度$\mathcal{C}(t)$、离散维格纳负性$N(t)$以及归一化负性$\chi(t)=N(t)/|S(t)|$,其中$S(t)$为生存振幅,最近被提议作为二阶矩下落探针(arXiv:2607.04065)。在跨越高斯酉系综(GUE)、高斯正交系综(GOE)和泊松系综、可积的$SL(2,\mathbb{R})$/共形场论(CFT)扇区以及混沌插值$H(\varepsilon)=H_{SL(2,\mathbb{R})}+\varepsilon R_0 W_{GUE}$的约57000个有标签演化的一半数据上训练小型残差网络(16 - 32个神经元)和提升树。任意一个矩都能在$R^2\simeq 0.999$时确定热场温度。两者都无法重构精细谱形式因子(每个系综中$R^2\simeq 0.18$);对目标进行平滑处理也无法修复此问题,且宽窗口虽有助于消除凹陷 - 斜坡物理现象本身,但谱形式因子严格细化了两个矩。不过在$R^2 = 0.861$时能恢复粗略的$e^S$平台,主要来自$\mathcal{C}(t)$的前20%。一条曲线能以高达98%的准确率识别对称类。在可积扇区,可观测量在信息上是等价的,正如精确的负二项从属要求的那样,而负性最能解决$(h,\alpha)$简并($N\to h$:0.999)。沿着插值,$\chi$相对于$\mathcal{C}$的不对称差距随着混沌开启,随着能级统计过渡到GUE从 +0.33增长到 +0.77,而原始$N$差距衰减到零。因此,二阶矩信息盈余是混沌的一个标志,由归一化负性专门携带,并且我们为此推导了一种分析机制和一个定量界限。

英文摘要

We employ machine learning to quantify the information carried by three Krylov-space observables: the spread complexity $\mathcal{C}(t)$, the discrete Wigner negativity $N(t)$, and the normalized negativity $χ(t)=N(t)/|S(t)|$, with $S(t)$ the survival amplitude, recently proposed as a second-moment infall probe (arXiv:2607.04065). Small residual networks (16-32 neurons) and boosted trees are trained on half of $\sim 57{,}000$ labeled evolutions spanning the GUE, GOE and Poisson ensembles, the integrable $SL(2,\mathbb{R})$/CFT sector, and the chaos interpolation $H(\varepsilon)=H_{SL(2,\mathbb{R})}+\varepsilon R_0 W_{GUE}$. Either moment determines the thermofield temperature at $R^2\simeq 0.999$. Neither reconstructs the fine spectral form factor ($R^2\simeq 0.18$ in every ensemble); smoothing the target does not repair this, and windows wide enough to help erase the dip-ramp physics itself: the SFF strictly refines both moments. The coarse $e^S$ plateau is nevertheless recovered at $R^2=0.861$, mostly from the first 20% of $\mathcal{C}(t)$. A single curve identifies the symmetry class at up to 98% accuracy. In the integrable sector the observables are informationally equivalent, as exact negative-binomial slaving demands, while the negativity best resolves the $(h,α)$ degeneracy ($N\to h$: 0.999). Along the interpolation the asymmetry gap of $χ$ over $\mathcal{C}$ switches on with chaos, growing from +0.33 to +0.77 as the level statistics cross to GUE, while the raw-$N$ gap decays to zero. The second-moment informational surplus is therefore a signature of chaos, carried specifically by the normalized negativity, and we derive an analytical mechanism and a quantitative bound for it.

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