• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

全球概率密度函数(PDF)拟合的压力测试:对MSHT概率密度函数进行闭包测试并首次与神经网络方法进行直接比较。

A stress test of global PDF fits: closure testing the MSHT PDFs and a first direct comparison to the neural net approach.

作者信息

Harland-Lang L A, Cridge T, Thorne R S

机构信息

Department of Physics and Astronomy, University College London, London, WC1E 6BT UK.

Deutsches Elektronen-Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany.

出版信息

Eur Phys J C Part Fields. 2025;85(3):316. doi: 10.1140/epjc/s10052-025-13934-3. Epub 2025 Mar 18.

DOI:10.1140/epjc/s10052-025-13934-3
PMID:40115426
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11920009/
Abstract

We present a first global closure test of the fixed parameterisation (MSHT) approach to PDF fitting. We find that the default MSHT20 parameterisation can reproduce the features of the input set in such a closure test to well within the textbook uncertainties. This provides strong evidence that parameterisation inflexibility in the MSHT20 fit is not a significant issue in the data region. We also present the first completely like-for-like comparison between two global PDF fits, namely MSHT and NNPDF, where the only difference is guaranteed to be due to the fitting methodology. To achieve this, we present a fit to the NNPDF4.0 data and theory inputs, but with the MSHT fixed parameterisation. We find that this gives a moderately, but noticeably, better fit quality than the central NNPDF4.0 fits, both with perturbative and fitted charm, and that this difference persists at the level of the PDFs and benchmark cross sections. The NNPDF4.0 uncertainties are found to be broadly in line with the MSHT results if a textbook tolerance is applied, but to be significantly smaller if a tolerance typical of the MSHT20 fit is applied. This points to an inherent inconsistency between these approaches. We discuss the need for an enlarged tolerance criterion in global PDF fits in detail, and demonstrate the impact of data/theory inconsistencies in the closure test setting; namely, these do not lead to any increase in the PDF uncertainty. We also investigate the impact of restricting the PDF parameterisation to have fewer free parameters than the default MSHT20 case, and find this can be significant at the level of both closure tests and the full fit.

摘要

我们展示了对用于部分子分布函数(PDF)拟合的固定参数化(MSHT)方法的首次全局闭合测试。我们发现,在这种闭合测试中,默认的MSHT20参数化能够将输入集的特征重现到教科书不确定性范围内。这有力地证明了在数据区域中,MSHT20拟合中参数化的不灵活性并非重大问题。我们还展示了两种全局PDF拟合(即MSHT和NNPDF)之间的首次完全同类比较,其中唯一的差异必定源于拟合方法。为实现这一点,我们展示了对NNPDF4.0数据和理论输入的拟合,但采用MSHT固定参数化。我们发现,无论是对于微扰粲夸克还是拟合粲夸克,这都给出了比NNPDF4.0中心拟合适度但明显更好的拟合质量,并且这种差异在部分子分布函数和基准截面水平上持续存在。如果应用教科书公差,发现NNPDF4.0的不确定性与MSHT结果大致相符,但如果应用MSHT20拟合的典型公差,则明显更小。这表明这些方法之间存在内在不一致性。我们详细讨论了在全局PDF拟合中扩大公差标准的必要性,并展示了闭合测试设置中数据/理论不一致性的影响;即,这些不会导致部分子分布函数不确定性增加。我们还研究了将部分子分布函数参数化限制为比默认的MSHT20情况具有更少自由参数的影响,发现在闭合测试和完整拟合水平上这都可能很显著。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4bfab9d9d57d/10052_2025_13934_Fig43_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/5126a909dea3/10052_2025_13934_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/bccf3e911198/10052_2025_13934_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d333c596805a/10052_2025_13934_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/97a0a0cca9b9/10052_2025_13934_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/b8a190f52064/10052_2025_13934_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4132ed9610a3/10052_2025_13934_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d888cdada096/10052_2025_13934_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/8ab26f1391f8/10052_2025_13934_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/0632014d1c3a/10052_2025_13934_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/7335afc616a9/10052_2025_13934_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/7baf15d515cf/10052_2025_13934_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/147a40ba6967/10052_2025_13934_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/9cf8f3f48e41/10052_2025_13934_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/15d58dd1087e/10052_2025_13934_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/389c06fbd1d9/10052_2025_13934_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/87851522968a/10052_2025_13934_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/5057a5859f97/10052_2025_13934_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/9a2d51271b9c/10052_2025_13934_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/c84ff8eca6b6/10052_2025_13934_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d0c2fd55f697/10052_2025_13934_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/e314e42dc0ea/10052_2025_13934_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/2b429e56a23b/10052_2025_13934_Fig22_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/a40aab135c3c/10052_2025_13934_Fig23_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/2483e838f572/10052_2025_13934_Fig24_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/1af75120a97a/10052_2025_13934_Fig25_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/02cb5a3d8e1a/10052_2025_13934_Fig26_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/3c50f266e19d/10052_2025_13934_Fig27_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4f0ff84a6aaa/10052_2025_13934_Fig28_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/e7df9498256c/10052_2025_13934_Fig29_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/5b968b524f91/10052_2025_13934_Fig30_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d55586d74ba9/10052_2025_13934_Fig31_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/f1ad2b68879d/10052_2025_13934_Fig32_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/90a3a16f0866/10052_2025_13934_Fig33_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d97c165c1987/10052_2025_13934_Fig34_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/b1dcf488205b/10052_2025_13934_Fig35_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/71bed0c3e4ad/10052_2025_13934_Fig36_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/dfb32fb2c3da/10052_2025_13934_Fig37_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/1b1dd8af16a8/10052_2025_13934_Fig39_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/b1224ee67575/10052_2025_13934_Fig41_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4bfab9d9d57d/10052_2025_13934_Fig43_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/5126a909dea3/10052_2025_13934_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/bccf3e911198/10052_2025_13934_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d333c596805a/10052_2025_13934_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/97a0a0cca9b9/10052_2025_13934_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/b8a190f52064/10052_2025_13934_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4132ed9610a3/10052_2025_13934_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d888cdada096/10052_2025_13934_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/8ab26f1391f8/10052_2025_13934_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/0632014d1c3a/10052_2025_13934_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/7335afc616a9/10052_2025_13934_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/7baf15d515cf/10052_2025_13934_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/147a40ba6967/10052_2025_13934_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/9cf8f3f48e41/10052_2025_13934_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/15d58dd1087e/10052_2025_13934_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/389c06fbd1d9/10052_2025_13934_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/87851522968a/10052_2025_13934_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/5057a5859f97/10052_2025_13934_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/9a2d51271b9c/10052_2025_13934_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/c84ff8eca6b6/10052_2025_13934_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d0c2fd55f697/10052_2025_13934_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/e314e42dc0ea/10052_2025_13934_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/2b429e56a23b/10052_2025_13934_Fig22_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/a40aab135c3c/10052_2025_13934_Fig23_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/2483e838f572/10052_2025_13934_Fig24_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/1af75120a97a/10052_2025_13934_Fig25_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/02cb5a3d8e1a/10052_2025_13934_Fig26_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/3c50f266e19d/10052_2025_13934_Fig27_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4f0ff84a6aaa/10052_2025_13934_Fig28_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/e7df9498256c/10052_2025_13934_Fig29_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/5b968b524f91/10052_2025_13934_Fig30_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d55586d74ba9/10052_2025_13934_Fig31_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/f1ad2b68879d/10052_2025_13934_Fig32_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/90a3a16f0866/10052_2025_13934_Fig33_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/d97c165c1987/10052_2025_13934_Fig34_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/b1dcf488205b/10052_2025_13934_Fig35_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/71bed0c3e4ad/10052_2025_13934_Fig36_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/dfb32fb2c3da/10052_2025_13934_Fig37_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/1b1dd8af16a8/10052_2025_13934_Fig39_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/b1224ee67575/10052_2025_13934_Fig41_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b467/11920009/4bfab9d9d57d/10052_2025_13934_Fig43_HTML.jpg

相似文献

1
A stress test of global PDF fits: closure testing the MSHT PDFs and a first direct comparison to the neural net approach.全球概率密度函数(PDF)拟合的压力测试:对MSHT概率密度函数进行闭包测试并首次与神经网络方法进行直接比较。
Eur Phys J C Part Fields. 2025;85(3):316. doi: 10.1140/epjc/s10052-025-13934-3. Epub 2025 Mar 18.
2
A first determination of the strong coupling at approximate LO order in a global PDF fit.在全局部分子分布函数拟合中,对近似领头阶的强耦合进行首次确定。
Eur Phys J C Part Fields. 2024;84(10):1009. doi: 10.1140/epjc/s10052-024-13320-5. Epub 2024 Oct 7.
3
A determination of the charm content of the proton: The NNPDF Collaboration.质子粲夸克含量的测定:NNPDF合作组
Eur Phys J C Part Fields. 2016;76(11):647. doi: 10.1140/epjc/s10052-016-4469-y. Epub 2016 Nov 24.
4
SIMUnet: an open-source tool for simultaneous global fits of EFT Wilson coefficients and PDFs.SIMUnet:一种用于同时全局拟合有效场论威尔逊系数和部分子分布函数的开源工具。
Eur Phys J C Part Fields. 2024;84(8):805. doi: 10.1140/epjc/s10052-024-13079-9. Epub 2024 Aug 12.
5
Parton distributions from high-precision collider data: NNPDF Collaboration.来自高精度对撞机数据的部分子分布:NNPDF合作组
Eur Phys J C Part Fields. 2017;77(10):663. doi: 10.1140/epjc/s10052-017-5199-5. Epub 2017 Oct 4.
6
Uncertainties on [Formula: see text] in the MMHT2014 global PDF analysis and implications for SM predictions.MMHT2014全局概率密度函数分析中关于[公式:见正文]的不确定性及其对标准模型预测的影响。
Eur Phys J C Part Fields. 2015;75(9):435. doi: 10.1140/epjc/s10052-015-3630-3. Epub 2015 Sep 21.
7
Impact of the heavy-quark matching scales in PDF fits.PDF拟合中重夸克匹配标度的影响。
Eur Phys J C Part Fields. 2017;77(12):837. doi: 10.1140/epjc/s10052-017-5407-3. Epub 2017 Dec 7.
8
A determination of the fragmentation functions of pions, kaons, and protons with faithful uncertainties: The NNPDF Collaboration.对π介子、K介子和质子的碎裂函数进行具有可靠不确定性的测定:NNPDF合作组。
Eur Phys J C Part Fields. 2017;77(8):516. doi: 10.1140/epjc/s10052-017-5088-y. Epub 2017 Aug 3.
9
The effect of LHC jet data on MSTW PDFs.大型强子对撞机喷注数据对MSTW部分子分布函数的影响。
Eur Phys J C Part Fields. 2014;74(7):2934. doi: 10.1140/epjc/s10052-014-2934-z. Epub 2014 Jul 1.
10
The impact of the final HERA combined data on PDFs obtained from a global fit.HERA最终组合数据对通过全局拟合得到的部分子分布函数(PDFs)的影响。
Eur Phys J C Part Fields. 2016;76(4):186. doi: 10.1140/epjc/s10052-016-4020-1. Epub 2016 Apr 6.

本文引用的文献

1
A first determination of the strong coupling at approximate LO order in a global PDF fit.在全局部分子分布函数拟合中,对近似领头阶的强耦合进行首次确定。
Eur Phys J C Part Fields. 2024;84(10):1009. doi: 10.1140/epjc/s10052-024-13320-5. Epub 2024 Oct 7.
2
Can New Physics Hide inside the Proton?新物理能否藏在质子中?
Phys Rev Lett. 2019 Sep 27;123(13):132001. doi: 10.1103/PhysRevLett.123.132001.
3
Parton distributions with small- resummation: evidence for BFKL dynamics in HERA data.具有小重整化的部分子分布:HERA数据中BFKL动力学的证据。
Eur Phys J C Part Fields. 2018;78(4):321. doi: 10.1140/epjc/s10052-018-5774-4. Epub 2018 Apr 20.
4
Precision measurement and interpretation of inclusive , and production cross sections with the ATLAS detector.利用ATLAS探测器对包含性、以及产生截面进行精确测量和解释。
Eur Phys J C Part Fields. 2017;77(6):367. doi: 10.1140/epjc/s10052-017-4911-9. Epub 2017 Jun 2.
5
Measurements of top-quark pair differential cross-sections in the lepton+jets channel in collisions at [Formula: see text] using the ATLAS detector.利用ATLAS探测器,在[公式:见正文]的碰撞中,对轻子+喷注道中顶夸克对的微分截面进行测量。
Eur Phys J C Part Fields. 2016;76(10):538. doi: 10.1140/epjc/s10052-016-4366-4. Epub 2016 Oct 3.
6
A determination of the charm content of the proton: The NNPDF Collaboration.质子粲夸克含量的测定:NNPDF合作组
Eur Phys J C Part Fields. 2016;76(11):647. doi: 10.1140/epjc/s10052-016-4469-y. Epub 2016 Nov 24.
7
Parton distributions in the LHC era: MMHT 2014 PDFs.大型强子对撞机时代的部分子分布:MMHT 2014部分子分布函数
Eur Phys J C Part Fields. 2015;75(5):204. doi: 10.1140/epjc/s10052-015-3397-6. Epub 2015 May 9.
8
Measurement of the electron charge asymmetry in inclusive W production in pp collisions at sqrt[s]=7  TeV.在 sqrt[s]=7 TeV 的 pp 碰撞中,对 W 产生的包含性中的电子电荷不对称性的测量。
Phys Rev Lett. 2012 Sep 14;109(11):111806. doi: 10.1103/PhysRevLett.109.111806. Epub 2012 Sep 11.