• 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

在FAIR实验中,通过比较UrQMD混合模型和粗粒化方法研究介子的椭圆流及相关情况。

Elliptic flow and of mesons at FAIR comparing the UrQMD hybrid model and the coarse-graining approach.

作者信息

Inghirami Gabriele, van Hees Hendrik, Endres Stephan, Torres-Rincon Juan M, Bleicher Marcus

机构信息

1Frankfurt Institute for Advanced Studies (FIAS), Ruth-Moufang-Str. 1, 60438 Frankfurt am Main, Germany.

2Institut für Theoretische Physik, Johann Wolfgang Goethe-Universität, Max-von-Laue-Str. 1, 60438 Frankfurt am Main, Germany.

出版信息

Eur Phys J C Part Fields. 2019;79(1):52. doi: 10.1140/epjc/s10052-019-6537-6. Epub 2019 Jan 21.

DOI:10.1140/epjc/s10052-019-6537-6
PMID:30740033
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6341055/
Abstract

We present a study of the elliptic flow and of and mesons in Au+Au collisions at FAIR energies. We propagate the charm quarks and the mesons following a previously applied Langevin dynamics. The evolution of the background medium is modeled in two different ways: (I) we use the UrQMD hydrodynamics + Boltzmann transport hybrid approach including a phase transition to QGP and (II) with the coarse-graining approach employing also an equation of state with QGP. The latter approach has previously been used to describe di-lepton data at various energies very successfully. This comparison allows us to explore the effects of partial thermalization and viscous effects on the charm propagation. We explore the centrality dependencies of the collisions, the variation of the decoupling temperature and various hadronization parameters. We find that the initial partonic phase is responsible for the creation of most of the mesons elliptic flow and that the subsequent hadronic interactions seem to play only a minor role. This indicates that mesons elliptic flow is a smoking gun for a partonic phase at FAIR energies. However, the results suggest that the magnitude and the details of the elliptic flow strongly depend on the dynamics of the medium and on the hadronization procedure, which is related to the medium properties as well. Therefore, even at FAIR energies the charm quark might constitute a very useful tool to probe the quark-gluon plasma and investigate its physics.

摘要

我们展示了一项关于在FAIR能量下金金碰撞中椭圆流以及介子和介子的研究。我们按照先前应用的朗之万动力学来传播粲夸克和介子。背景介质的演化以两种不同方式建模:(I)我们使用包括向夸克胶子等离子体(QGP)相变的UrQMD流体动力学+玻尔兹曼输运混合方法,以及(II)采用同样带有QGP状态方程的粗粒化方法。后一种方法先前已非常成功地用于描述各种能量下的双轻子数据。这种比较使我们能够探究部分热化和粘性效应在粲夸克传播上的影响。我们探究碰撞的中心度依赖性、解耦温度的变化以及各种强子化参数。我们发现初始的部分子相是产生大多数介子椭圆流的原因,而随后的强子相互作用似乎只起次要作用。这表明介子椭圆流是FAIR能量下存在部分子相的一个确凿证据。然而,结果表明椭圆流的大小和细节强烈依赖于介质的动力学以及强子化过程,而这也与介质性质相关。因此,即使在FAIR能量下,粲夸克可能也是探测夸克胶子等离子体并研究其物理性质的一个非常有用的工具。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/6cab2d109d6d/10052_2019_6537_Fig26_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/9036a8f7ff27/10052_2019_6537_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/3380b3ea202b/10052_2019_6537_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/a15e44f12b27/10052_2019_6537_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/e798f12c6361/10052_2019_6537_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/873a69c99e98/10052_2019_6537_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/4c7de4e516df/10052_2019_6537_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/5c8e40678ac5/10052_2019_6537_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/9fa45267a275/10052_2019_6537_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/1c44810ba63d/10052_2019_6537_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/dadb2813699c/10052_2019_6537_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/a6fe87ea4494/10052_2019_6537_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/86c9225372a1/10052_2019_6537_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/3072d7b14aa8/10052_2019_6537_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/be7d58d8e2a7/10052_2019_6537_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/d32ac7826238/10052_2019_6537_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/c8ed0b584a01/10052_2019_6537_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/f1936a84d98f/10052_2019_6537_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/20cadfa9df21/10052_2019_6537_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/3cbf0eda47e3/10052_2019_6537_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/dfb06b573396/10052_2019_6537_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/b54fa3cae613/10052_2019_6537_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/fa49413e6dd9/10052_2019_6537_Fig22_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/6a47983fa61c/10052_2019_6537_Fig23_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/c00ab591bd3b/10052_2019_6537_Fig24_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/fe9e0c0bdaca/10052_2019_6537_Fig25_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/6cab2d109d6d/10052_2019_6537_Fig26_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/9036a8f7ff27/10052_2019_6537_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/3380b3ea202b/10052_2019_6537_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/a15e44f12b27/10052_2019_6537_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/e798f12c6361/10052_2019_6537_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/873a69c99e98/10052_2019_6537_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/4c7de4e516df/10052_2019_6537_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/5c8e40678ac5/10052_2019_6537_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/9fa45267a275/10052_2019_6537_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/1c44810ba63d/10052_2019_6537_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/dadb2813699c/10052_2019_6537_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/a6fe87ea4494/10052_2019_6537_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/86c9225372a1/10052_2019_6537_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/3072d7b14aa8/10052_2019_6537_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/be7d58d8e2a7/10052_2019_6537_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/d32ac7826238/10052_2019_6537_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/c8ed0b584a01/10052_2019_6537_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/f1936a84d98f/10052_2019_6537_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/20cadfa9df21/10052_2019_6537_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/3cbf0eda47e3/10052_2019_6537_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/dfb06b573396/10052_2019_6537_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/b54fa3cae613/10052_2019_6537_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/fa49413e6dd9/10052_2019_6537_Fig22_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/6a47983fa61c/10052_2019_6537_Fig23_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/c00ab591bd3b/10052_2019_6537_Fig24_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/fe9e0c0bdaca/10052_2019_6537_Fig25_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/28f6/6341055/6cab2d109d6d/10052_2019_6537_Fig26_HTML.jpg

相似文献

1
Elliptic flow and of mesons at FAIR comparing the UrQMD hybrid model and the coarse-graining approach.在FAIR实验中,通过比较UrQMD混合模型和粗粒化方法研究介子的椭圆流及相关情况。
Eur Phys J C Part Fields. 2019;79(1):52. doi: 10.1140/epjc/s10052-019-6537-6. Epub 2019 Jan 21.
2
Hadronization and Charm-Hadron Ratios in Heavy-Ion Collisions.重离子碰撞中的强子化与粲强子比率
Phys Rev Lett. 2020 Jan 31;124(4):042301. doi: 10.1103/PhysRevLett.124.042301.
3
D(s) meson as a quantitative probe of diffusion and hadronization in nuclear collisions.D(s) 介子作为探测核碰撞中扩散和强子化的定量探针。
Phys Rev Lett. 2013 Mar 15;110(11):112301. doi: 10.1103/PhysRevLett.110.112301. Epub 2013 Mar 11.
4
Elliptic flow for phi mesons and (anti)deuterons in Au+Au collisions at square root of sNN=200 GeV.在质心能量平方根√sNN = 200 GeV的金离子与金离子碰撞中,π介子和(反)氘核的椭圆流
Phys Rev Lett. 2007 Aug 3;99(5):052301. doi: 10.1103/PhysRevLett.99.052301. Epub 2007 Jul 31.
5
Elliptic flow of thermal photons in relativistic nuclear collisions.相对论性核碰撞中热光子的椭圆流
Phys Rev Lett. 2006 May 26;96(20):202302. doi: 10.1103/PhysRevLett.96.202302.
6
Nonperturbative heavy-quark diffusion in the quark-gluon plasma.夸克-胶子等离子体中的非微扰重夸克扩散
Phys Rev Lett. 2008 May 16;100(19):192301. doi: 10.1103/PhysRevLett.100.192301. Epub 2008 May 13.
7
Influence of shear viscosity of quark-gluon plasma on elliptic flow in ultrarelativistic heavy-ion collisions.夸克-胶子等离子体的剪切黏度对相对论重离子碰撞中椭圆流的影响。
Phys Rev Lett. 2011 May 27;106(21):212302. doi: 10.1103/PhysRevLett.106.212302. Epub 2011 May 26.
8
Observation of D_{s}^{±}/D^{0} Enhancement in Au+Au Collisions at sqrt[s_{NN}]=200  GeV.在\(\sqrt{s_{NN}} = 200\)GeV的金离子与金离子碰撞中对\(D_{s}^{±}/D^{0}\)增强的观测
Phys Rev Lett. 2021 Aug 27;127(9):092301. doi: 10.1103/PhysRevLett.127.092301.
9
200 A GeV Au + Au collisions serve a nearly perfect quark-gluon liquid.200 A GeV Au + Au 碰撞几乎提供了完美的夸克-胶子液体。
Phys Rev Lett. 2011 May 13;106(19):192301. doi: 10.1103/PhysRevLett.106.192301. Epub 2011 May 9.
10
Collectivity of J/ψ Mesons in Heavy-Ion Collisions.重离子碰撞中J/ψ介子的集体性
Phys Rev Lett. 2022 Apr 22;128(16):162301. doi: 10.1103/PhysRevLett.128.162301.

本文引用的文献

1
Gluon PDF constraints from the ratio of forward heavy-quark production at the LHC at [Formula: see text] and 13 TeV.来自大型强子对撞机在[公式:见原文]和13 TeV时前向重夸克产生比率的胶子部分子分布函数约束。
Eur Phys J C Part Fields. 2015;75:610. doi: 10.1140/epjc/s10052-015-3814-x. Epub 2015 Dec 22.
2
Relativistic Langevin dynamics in expanding media.膨胀介质中的相对论性朗之万动力学。
Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Sep;88(3):032138. doi: 10.1103/PhysRevE.88.032138. Epub 2013 Sep 27.
3
Nonperturbative heavy-quark diffusion in the quark-gluon plasma.
夸克-胶子等离子体中的非微扰重夸克扩散
Phys Rev Lett. 2008 May 16;100(19):192301. doi: 10.1103/PhysRevLett.100.192301. Epub 2008 May 13.
4
Heavy quark energy loss in a nuclear medium.核介质中的重夸克能量损失
Phys Rev Lett. 2004 Aug 13;93(7):072301. doi: 10.1103/PhysRevLett.93.072301. Epub 2004 Aug 11.
5
Landau-Pomeranchuk-Migdal effect in QCD and radiative energy loss in a quark-gluon plasma.量子色动力学中的朗道-波梅兰丘克-米格尔效应与夸克-胶子等离子体中的辐射能量损失
Phys Rev D Part Fields. 1995 Apr 1;51(7):3436-3446. doi: 10.1103/physrevd.51.3436.
6
Diffusion of charmed quarks in the quark-gluon plasma.粲夸克在夸克-胶子等离子体中的扩散。
Phys Rev D Part Fields. 1988 May 1;37(9):2484-2491. doi: 10.1103/physrevd.37.2484.