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Pythia中的强子-离子碰撞与光生过程的矢量介子主导模型。

Hadron-ion collisions in Pythia and the vector-meson dominance model for photoproduction.

作者信息

Helenius Ilkka, Utheim Marius

机构信息

Department of Physics, University of Jyvaskyla, P.O. Box 35, Fl-40014 Jyvaskyla, Finland.

Helsinki Institute of Physics, University of Helsinki, P.O. Box 64, FI-00014 Helsinki, Finland.

出版信息

Eur Phys J C Part Fields. 2024;84(11):1155. doi: 10.1140/epjc/s10052-024-13543-6. Epub 2024 Nov 15.

DOI:10.1140/epjc/s10052-024-13543-6
PMID:39554376
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11568055/
Abstract

We present an extension to the Pythia Monte Carlo event generator that enables simulations of collisions between a generic hadron beam on a nuclear target with energy variation in event-by-event basis. This builds upon Pythia 's module for heavy ions, Angantyr, as well as previous work on simulating hadron-proton collisions. As such, the extensions in this work are largely technical, except for a rudimentary model for hadronic fluctuations. With hadron-ion simulations, we implement an explicit vector-meson dominance (VMD) model that can be used to simulate interactions of hadronic component of real photons in photo-nuclear collisions. Such processes can be studied in ultra-peripheral heavy-ion collisions and in the future also with the upcoming Electron-Ion Collider. Our work also has applications to hadronic showers, e.g. air showers initiated by high-energy cosmic rays. We first validate the VMD model by comparing to HERA photoproduction data on proton target. Then we apply this to generate events for ultra-peripheral heavy-ion collisions at the LHC and present the results corresponding to the event-selection criteria matching to a recent ATLAS analysis. We find that single-particle multiplicity and rapidity distributions are well in line with the measured ones. We also construct the Fourier coefficients from two-particle correlations for the simulated events and study whether the resulting azimuthal anisotropies are consistent with the ATLAS results.

摘要

我们展示了对Pythia蒙特卡罗事件发生器的扩展,该扩展能够逐事件地模拟具有能量变化的通用强子束与核靶之间的碰撞。这是在Pythia的重离子模块Angantyr以及先前模拟强子 - 质子碰撞的工作基础上构建的。因此,除了一个用于强子涨落的初步模型外,这项工作中的扩展在很大程度上是技术性的。通过强子 - 离子模拟,我们实现了一个明确的矢量介子主导(VMD)模型,该模型可用于模拟光核碰撞中实光子强子成分的相互作用。此类过程可在超外围重离子碰撞中进行研究,并且在未来随着即将建成的电子 - 离子对撞机也可进行研究。我们的工作在强子簇射中也有应用,例如由高能宇宙射线引发的空气簇射。我们首先通过与质子靶上的HERA光致产生数据进行比较来验证VMD模型。然后我们将其应用于生成大型强子对撞机超外围重离子碰撞的事件,并给出与最近ATLAS分析相匹配的事件选择标准对应的结果。我们发现单粒子多重性和快度分布与测量结果非常吻合。我们还为模拟事件构建了两粒子关联的傅里叶系数,并研究所得的方位角各向异性是否与ATLAS结果一致。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/155df9f45462/10052_2024_13543_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/e9ab0ff18f33/10052_2024_13543_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/fa5f6bfca0fc/10052_2024_13543_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/0e8c19d62070/10052_2024_13543_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/fe55f15b8a61/10052_2024_13543_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/699aea009ec5/10052_2024_13543_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/fcf7f71262a1/10052_2024_13543_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/72775023b340/10052_2024_13543_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/c5e04a656cc0/10052_2024_13543_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/7c442bb5cd7b/10052_2024_13543_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/155df9f45462/10052_2024_13543_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/e9ab0ff18f33/10052_2024_13543_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/fa5f6bfca0fc/10052_2024_13543_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/0e8c19d62070/10052_2024_13543_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/fe55f15b8a61/10052_2024_13543_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/699aea009ec5/10052_2024_13543_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/fcf7f71262a1/10052_2024_13543_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/72775023b340/10052_2024_13543_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/c5e04a656cc0/10052_2024_13543_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/7c442bb5cd7b/10052_2024_13543_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7544/11568055/155df9f45462/10052_2024_13543_Fig10_HTML.jpg

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