TDLI RESEARCH ACHIEVEMENTS
近日,上海交通大学暗物质物理全国重点实验室常务副主任、李政道研究所和物理与天文学院鸿文讲席教授季向东与其博士后张家璐及合作者,在部分子分布的第一性原理研究中取得新进展。相关成果以“Parton Distribution Functions from Large-Momentum Expansion of Current-Current Correlators”为题发表于《物理评论快报》(Physical Review Letters)。
在大型强子对撞机等高能实验中,质子被加速到接近光速,参与高能碰撞的是其内部的夸克和胶子,统称为“部分子”。每个部分子携带质子的一部分动量,并与另一质子中的部分子发生相互作用。预测某种反应出现的概率,需要知道不同种类的部分子具有各种动量份额的可能性。部分子分布函数描述的正是这些信息,反映了质子沿运动方向的一维动量结构。
这些分布目前主要从实验数据中提取。从描述强相互作用的量子色动力学(QCD)出发,直接把它们算出来,一直是一个难题。格点QCD将时空离散为网格,使质子内部的强相互作用能够用计算机模拟。但部分子分布涉及“光锥关联”:两点之间的空间距离,等于光在两点时间间隔内走过的距离。这类同时涉及空间和真实时间的关联,难以用常规格点方法直接计算。
季向东于2013年提出的大动量有效理论(LaMET)提供了一种做法:先在格点上计算具有较大但有限动量的质子,考察同一时刻、不同空间位置的夸克或胶子之间的关联。在大动量极限下,这些“等时空间关联”与光锥关联包含相同的长距离结构信息;两者的短距离差别,则通过可计算的理论“匹配”加以修正。借助这种对应关系,格点上可计算的空间关联便能用于提取部分子分布。

图1. LaMET中两类关联的示意图。蓝色平面表示同一时刻的空间,灰色锥面表示光锥。左图的两点位于同一时刻,构成空间关联;右图示意趋近光锥方向的关联。LaMET利用大动量下两者的联系,通过理论匹配提取部分子分布。
在LaMET框架下,可以选取不同类型的空间关联来研究同一个部分子分布函数。这次研究采用质子内部的“流-流关联”,考察两个位置的局域夸克流之间的联系。它可以理解为质子对两个局域探测的关联响应,其中包含了夸克的动量分布信息。团队建立了由这类关联提取部分子分布的一圈精度理论公式,并利用格点QCD数据,计算了质子中同位旋矢量部分子分布函数。
这一做法的一个优点,是不需要在两个探测位置之间引入威尔逊线,因而避开了这种联络带来的额外发散,使格点结果的处理更加简便。

图2. 利用流-流关联得到的质子中同位旋矢量分布。横轴x表示夸克携带的质子动量份额。蓝、绿色带分别为本研究的次领头阶固定阶微扰计算与次领头对数精度重求和的初步结果,红色带为实验数据的CT18NNLO全局拟合。
这项探索性研究展示了从流-流关联提取部分子分布的可行性。用不同的关联函数计算同一物理量,可以帮助交叉检验结果,更好地控制计算误差,为进一步认识质子的内部结构提供依据。
上海交通大学李政道研究所博士后张家璐为论文第一作者,美国麻省理工学院张睿、肯塔基大学及劳伦斯伯克利国家实验室Christian Zimmermann为共同通讯作者,上海交通大学季向东教授、德国雷根斯堡大学Andreas Schäfer为共同作者。
本工作获国家自然科学基金、暗物质物理全国重点实验室、鸿文慈善基金和“李政道博士生”奖学金支持,在此深表感谢。
原文链接
https://doi.org/10.1103/vdtk-mps3
Extracting Quark Momentum Distributions in the Proton from Current-Current Correlators
TDLI RESEARCH ACHIEVEMENTS
Professor Xiangdong Ji, Executive Deputy Director of the State Key Laboratory of Dark Matter Physics of Shanghai Jiao Tong University, his postdoctoral researcher Jia-Lu Zhang, and their collaborators have made progress in the first-principles study of parton distributions. Their paper, “Parton Distribution Functions from Large-Momentum Expansion of Current-Current Correlators”, was published in Physical Review Letters.
At the Large Hadron Collider and other high-energy experiments, protons travel at nearly the speed of light. The constituents that take part in hard collisions are quarks and gluons, collectively known as partons. Each carries a fraction of its parent proton’s momentum and can interact with a parton from the other proton. Predicting how often a particular reaction occurs requires knowing how likely it is to find each type of parton with a given momentum fraction. Parton distribution functions encode this information, describing the proton’s one-dimensional momentum structure along its direction of motion.
These distributions are mainly extracted from experimental data. Calculating them directly from quantum chromodynamics (QCD), the theory of the strong interaction, has remained difficult. Lattice QCD divides space and time into a grid so that the strong interactions inside a proton can be simulated on a computer. Parton distributions, however, involve light-cone correlations: the spatial separation between two points equals the distance light travels during their time separation. Such correlations involve both space and real time and are not directly accessible to conventional lattice calculations.
Large-momentum effective theory (LaMET), proposed by Xiangdong Ji in 2013, offers a way to make the calculation possible. Researchers first study a proton with a large but finite momentum on the lattice, calculating correlations between quarks or gluons at different spatial positions at the same time. In the large-momentum limit, these equal-time spatial correlations contain the same long-distance structural information as light-cone correlations. Their short-distance differences are accounted for by a calculable theoretical relation known as matching. This connection allows parton distributions to be extracted from spatial correlations that can be computed on the lattice.

Figure 1. Spatial and light-cone correlations in LaMET. Blue planes represent space at a fixed time; gray cones represent the light cone. The two points on the left are at equal time and form a spatial correlation. The right illustrates a correlation approaching the light-cone direction. LaMET connects the two at large momentum and uses theoretical matching to extract parton distributions.
Within LaMET, different types of spatial correlations can be used to study the same parton distribution. In this work, the team examined current-current correlators between local quark currents at two positions inside the proton. These can be understood as the proton’s correlated response to two local probes, containing information about quark momentum distributions. The researchers derived a one-loop formula for extracting parton distributions from these correlators and used lattice QCD data to calculate the proton’s isovector parton distribution.
An advantage of this approach is that it does not require a Wilson line between the two probe positions. It therefore avoids the additional divergences associated with this connection, simplifying the treatment of the lattice results.

Figure 2. The proton’s isovector parton distribution obtained from current-current correlators. The horizontal axis x is the fraction of proton momentum carried by a quark. Green and blue bands show the exploratory results at NLO and with NLL resummation, respectively. The red band shows the CT18NNLO global fit to experimental data.
This exploratory study demonstrates the feasibility of extracting parton distributions from current-current correlators. Calculating the same physical quantity using different correlation functions helps cross-check results and better control computational uncertainties, providing a basis for further understanding the proton’s internal structure.
Jia-Lu Zhang, a postdoctoral researcher at the Tsung-Dao Lee Institute, Shanghai Jiao Tong University, is the first author; Rui Zhang of the Massachusetts Institute of Technology and Christian Zimmermann of the University of Kentucky and Lawrence Berkeley National Laboratory are the corresponding authors; Professor Xiangdong Ji of Shanghai Jiao Tong University and Andreas Schafer of the University of Regensburg are coauthors.
The authors gratefully acknowledge support from the National Natural Science Foundation of China, the State Key Laboratory of Dark Matter Physics, the Thomas and Linda Lau Family Foundation, and the T. D. Lee Scholarship.
Paper link
https://doi.org/10.1103/vdtk-mps3
文章来源 | 李政道研究所TDLI


