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arXiv 2510.09482hep-thcond-mat.stat-mech
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通过模糊球上的基态能量定位 Ising CFT

Locating the Ising CFT via the ground-state energy on the fuzzy sphere

Kay Joerg Wiese

AI总结:

通过模糊球上 Ising 模型基态能量的有限尺寸标度分析定位相变点,利用共形微扰理论搜索极小值,精确重现了已知临界曲线并提取了标量相关的标度修正指数。验证了归一化方式的鲁棒性。

摘要:

我们通过对其基态能量的有限尺寸标度分析,定位了模糊球上 Ising 模型的相变点。我们的策略是将后者写为 $E_{GS}(N_m)/N_m = E_{0} + E_1 /N_m + E_{3/2}/N_m^{3/2}+ \dots$,并搜索作为耦合参数函数的 $\chi:=E_{3/2}/E_0$ 的极小值。共形微扰理论预测,在 CFT 附近,$\chi= \chi_{\rm min} + \sum_i \lambda_i^2 N_m^{-\omega_i} + O(\lambda^3)$,其中 $\lambda_i$ 是与维度为 $\Delta_i$ 的算符微扰相关的耦合参数,且 $\omega_i = d - \Delta_i$。该方法以良好的精度找到了 [PRX 13 (2023) 021009] 的临界曲线及其最佳点。改变耦合常数使我们能提取与两个领先标量 $\epsilon$ 和 $\epsilon'$ 相关的标度修正指数 $\omega$。我们发现,当使用能隙、应力张量 $T$ 或第一宇称奇算符 $\sigma$ 而非 $E_0$ 进行归一化时,结果相似。

英文摘要:

We locate the phase-transition line for the Ising model on the fuzzy sphere from a finite-size scaling analysis of its ground-state energy. Our strategy is to write the latter as $E_{GS}(N_m)/N_m = E_{0} + E_1 /N_m + E_{3/2}/N_m^{3/2}+ ...$, and to search for a minimum of $ χ:=E_{3/2}/E_0$ as a function of the couplings. Conformal perturbation theory predicts that around a CFT, $χ= χ_{\rm min} + \sum_i λ_i^2 N_m^{-ω_i} + O(λ^3)$, where $λ_i$ are the couplings associated to perturbations of operators with dimension $Δ_i$, and $ω_i = d-Δ_i$. This procedure finds the critical curve of [PRX 13 (2023) 021009] and their sweet spot with good precision. Varying two coupling constants allows us to extract the correction-to-scaling exponent $ω$ associated to the two leading scalars $ε$, and $ε'$. We find similar results when normalizing by the gap to the stress tensor $T$ or first parity-odd operator $σ$ instead of $E_0$.

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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