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格点量子色动力学数据的虚部分布与信号改进

洪浩艺 高美琪 桂龙成 华俊 梁剑 史君 邹锦涛

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格点量子色动力学数据的虚部分布与信号改进

洪浩艺, 高美琪, 桂龙成, 华俊, 梁剑, 史君, 邹锦涛

Imaginary-part distribution and signal improvement of lattice quantum chromodynamics data

Hong Hao-Yi, Gao Mei-Qi, Gui Long-Cheng, Hua Jun, Liang Jian, Shi Jun, Zou Jin-Tao
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  • 通过分析淬火近似下高统计量格点两点关联函数实部与虚部对规范场采样的分布, 给出了一种可能的实、虚部分布间的定量关系, 并通过计算实部与虚部的非平庸统计相关性对该关系加以验证. 利用该实、虚部的统计相关性, 格点关联函数的方差可以得到约40%的改进. 这些结果为进一步理解格点计算中统计误差的物理来源以及发展信号改进方案提供了全新的思路.
    Understanding the statistical fluctuations of lattice observables over the gauge configurations is important both theoretically and practically. It provides a physical insight into tackling the famous signal-to-noise problem and the sign problem, and inspires new thoughts in developing methods to improve the signal of lattice calculations. Among many efforts, exploring the relationship between the real part and imaginary part of lattice numerical result is a new method to understand lattice signal and error, because both the real part and imaginary part come from the same sample of gauge field and their distributions on the gauge sample are related in principle. Specifically, by analyzing the distributions of the real part and imaginary part of quenched lattice two-point function with high statistics and non-zero momentum, this work proposes a possible quantitative formula connecting these two distributions as $R(x)=\displaystyle\int {\rm{d}}y S(y-x) \left[I(y) K(U_y)\right]$, where $R(x)$ denotes the real-part distribution, $I(x)$ the imaginary-part distribution, $S(x)$ the underlying signal distribution and $K(U_x)$ a kernel function of the gauge field. This theoretical assumption has universal validity because the kernel function contains the gauge field information that determines all the distributions. The formula is numerically verified by calculating the non-trivial statistical correlations of the real part and the kernel-function-modified imaginary part under the further assumption of the kernel function. It is found that the most naïve guess of $K(U_x)=1$ does not work, which leads to no statistically significant correlation. Meanwhile, the assumption that $K(U_x)$ is only a sign function works well, giving rise to $\sim70\%$ correlation. Then, through the process of adding random distortions to the absolute values of the imaginary part, it is found that even a slight distortion, of around 1% could result in a significant reduction in the correlation between the real part and imaginary part down to less than 50% or lower. This essentially proves that the observed $\sim70\%$ correlation is highly non-trivial and the hypothesis that $K(U_x)$ is a sign function captures at least some of the physical mechanisms behind the scenes. Employing this correlation, the variance of lattice results can be improved by around 40%. It is not a significant improvement in practice; however, this study offers an innovative strategy to understand the source of statistical uncertainties in lattice QCD and to improve the signal-to-noise ratio in lattice calculation. Further research on the ability to use machine learning on various more accurate lattice data will hopefully give better instructions and constraint on the form of the kernel function.
      通信作者: 桂龙成, guilongcheng@hunnu.edu.cn ; 梁剑, jianliang@scnu.edu.cn ; 史君, jun.shi@scnu.edu.cn
    • 基金项目: 国家自然科学基金优秀青年科学基金(批准号: 12222503)、国家自然科学基金(批准号: 12175073, 12175063)、国家自然科学基金青年科学基金(批准号: 12105108, 12205106)、广东省基础与应用基础研究基金自然科学基金(批准号: 2023A1515012712)和湖南省自然科学基金(批准号: 2023JJ30380)资助的课题.
      Corresponding author: Gui Long-Cheng, guilongcheng@hunnu.edu.cn ; Liang Jian, jianliang@scnu.edu.cn ; Shi Jun, jun.shi@scnu.edu.cn
    • Funds: Project supported by the Excellent Young Scientists Fund of the National Natural Science Foundation of China (Grant No. 12222503), the National Natural Science Foundation of China (Grant Nos. 12175073, 12175063), the Young Scientists Fund of the National Natural Science Foundation of China (Grant Nos. 12105108, 12205106), the Natural Science Foundation of Basic and Applied Basic Research of Guangdong Province, China (Grant No. 2023A1515012712), and the Natural Science Foundation of Hunan Province, China (Grant No. 2023JJ30380).
    [1]

    陈莹, 丁亨通, 冯旭, 等 2020 现代物理知识 32 36

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    Chang C C, Nicholson A N, Rinaldi E, et al. 2018 Nature 558 91Google Scholar

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    Liang J, Yang Y B, Draper T, et al. 2018 Phys. Rev. D 98 074505Google Scholar

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    Yang Y B, Gong M, Liang J, et al. 2018 Phys. Rev. D 98 074506Google Scholar

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    Endres M G, Kaplan D B, Lee J W, et al. 2011 Phys. Rev. Lett. 197 201601

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    Gupta R 1997 arXiv: hep-lat/9807028[hep-lat]

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    DeGrand T 2012 Phys. Rev. D 86 014512

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    Wagman M L, Savage M J 2017 arXiv: 1704.07356[hep-lat]

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    Wagman M L 2017 arXiv: 1711.00062[hep-lat]

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    Sheikholeslami B, Wohlert R 1985 Nucl. Phys. B 259 572Google Scholar

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    Gui L C, Dong J M, Chen Y, et al. 2019 Phys. Rev. D 100 054511

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    Parisi G 1984 Phys. Rep. 103 203Google Scholar

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    Lepage G P 1989 Proceedings of Theoretical Advanced Study Institute in Elementary Particle Physics (TASI89) Boulder, Colorado, United States, June 5–30, 1989 p97

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    Burnier Y, Rothkopf A 2013 Phys. Rev. Lett. 111 182003Google Scholar

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    Hansen M, Lupo A, Tantalo N 2019 Phys. Rev. D 99 094508

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    Chen S Y, Ding H T, Liu F Y, et al. 2021 arXiv: 2110.13521 [hep-lat]

  • 图 1  纵坐标为对数坐标情况下, 不同量子数和不同动量的两点关联函数

    Fig. 1.  Two-point correlations function with different quantum numbers and momenta when the vertical axis is in log scale

    图 2  $ p^2=1 $的赝标两点函数其实部(上半部分)虚部(下半部分)在规范组态上的分布, 从左至右分别对应$ t/a_t=1 $, 30和90的情况

    Fig. 2.  The real-part (upper panel) and imaginary-part (lower panel) distributions of the pseudoscalar two-point functions with $ p^2=1 $ over gauge configurations. From left to right, the figures are for $ t/a_t=1 $, 30 and 90, respectively.

    图 3  赝标单位动量两点关联函数实部与虚部的统计相关性. 蓝色虚线表示原始数据, 橙色实线表示符号修正过的数据

    Fig. 3.  Statistical correlations between the real and imaginary parts of the pseudoscalar two-point correlation function with unit momentum, where the blue dashed line represents the original data, and the orange solid one is for the data after sign-correction.

    图 4  在修正符号的基础上, 考虑对虚部的值进行扰动后的赝标单位动量两点关联函数实部与虚部的统计相关性

    Fig. 4.  On the basis of sign-correction, the statistical correlations between the real and imaginary parts of the pseudoscalar two-point correlation function with unit momentum after distortions on the absolute values of the imaginary parts.

    图 5  不同量子数两点关联函数的方差改进

    Fig. 5.  The variance improvements of two-point correlation functions with different quantum numbers.

    图 6  不同动量矢量两点关联函数的方差改进

    Fig. 6.  The variance improvements of two-point correlation functions with different momenta.

  • [1]

    陈莹, 丁亨通, 冯旭, 等 2020 现代物理知识 32 36

    Chen Y, Ding H T, Feng X, et al. 2020 Modern Physics 32 36

    [2]

    Chang C C, Nicholson A N, Rinaldi E, et al. 2018 Nature 558 91Google Scholar

    [3]

    Borsanyi Sz, Fodor Z, Guenther J N, et al. 2021 Nature 593 51Google Scholar

    [4]

    Yang Y B, Liang J, Bi Y J, et al. 2018 Phys. Rev. Lett. 121 212001Google Scholar

    [5]

    Joó Bálint, Jung C, Christ N H, et al. 2019 Eur. Phys. J. A 55 199Google Scholar

    [6]

    Liu K F, Liang J, Yang Y B 2018 Phys. Rev. D 97 034507Google Scholar

    [7]

    Liang J, Alexandru A, Draper T, et al. 2023 arXiv: 2301.04331 [hep-lat]

    [8]

    Liang J, Yang Y B, Draper T, et al. 2018 Phys. Rev. D 98 074505Google Scholar

    [9]

    Yang Y B, Gong M, Liang J, et al. 2018 Phys. Rev. D 98 074506Google Scholar

    [10]

    Endres M G, Kaplan D B, Lee J W, et al. 2011 Phys. Rev. Lett. 197 201601

    [11]

    Gupta R 1997 arXiv: hep-lat/9807028[hep-lat]

    [12]

    DeGrand T 2012 Phys. Rev. D 86 014512

    [13]

    Wagman M L, Savage M J 2017 arXiv: 1704.07356[hep-lat]

    [14]

    Wagman M L 2017 arXiv: 1711.00062[hep-lat]

    [15]

    Sheikholeslami B, Wohlert R 1985 Nucl. Phys. B 259 572Google Scholar

    [16]

    Gui L C, Dong J M, Chen Y, et al. 2019 Phys. Rev. D 100 054511

    [17]

    Parisi G 1984 Phys. Rep. 103 203Google Scholar

    [18]

    Lepage G P 1989 Proceedings of Theoretical Advanced Study Institute in Elementary Particle Physics (TASI89) Boulder, Colorado, United States, June 5–30, 1989 p97

    [19]

    Burnier Y, Rothkopf A 2013 Phys. Rev. Lett. 111 182003Google Scholar

    [20]

    Hansen M, Lupo A, Tantalo N 2019 Phys. Rev. D 99 094508

    [21]

    Chen S Y, Ding H T, Liu F Y, et al. 2021 arXiv: 2110.13521 [hep-lat]

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出版历程
  • 收稿日期:  2023-05-27
  • 修回日期:  2023-06-30
  • 上网日期:  2023-07-13
  • 刊出日期:  2023-10-20

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