A Multi-Phase Transport Model (AMPT) has been extensively used to understand the physics behind the experimental observation. Like other models, the outcome of the AMPT model depends on the initial parameters. Therefore, one needs to choose suitable initial parameters before using the model. Lund string fragmentation function has been used to create quark-antiquarks pairs in the AMPT model. The Lund string fragmentation parameters determine the yields and transverse momentum ($p_{T}$) spectra of particles produced in nucleus-nucleus collisions. The values of Lund string fragmentation parameters were determined by fitting the charged particle yield and $p_{T}$ spectra measured in the experiment. In this paper, we have shown the yield of strange quarks carrying hadrons, e.g. $ϕ$ mesons, are more sensitive to Lund string fragmentation parameters compared to non-strange pions. Using $ϕ$ meson spectra measured at RHIC, we have obtained new sets of Lund parameters for Au+Au collisions at $\sqrt{s_{\mathrm {NN}}}$ = 11.5, 39, and 200 GeV. We have found that using the same set of parameters, we can explain $ϕ$-meson yield at $\sqrt{s_{\mathrm {NN}}}$ = 39 and 200 GeV, however, we need a different set of parameters for $\sqrt{s_{\mathrm {NN}}}$ = 11.5 GeV. This suggests that at low energy, $\sqrt{s_{\mathrm {NN}}}$ = 11.5 GeV, the underlying mechanism for particle production is different compared to top RHIC energies. We have also predicted invariant yield of $π$ and $ϕ$ mesons as a function of $p_{T}$ in U+U collisions at $\sqrt{s_{\mathrm {NN}}}$ = 196 GeV to be measured by STAR experiment.
Constraining the strangeness content of the nucleon by measuring the $ϕ$ meson mass shift in nuclear matter
利用QCD求和规则和最大熵方法研究了有限密度下$ϕ$介子的行为。结果表明，核物质中$ϕ$可能的质量移动与核子的奇异含量密切相关，核子的奇异含量与奇异σ项$σ_{sN} = m_s \langle N | \overline{s}s | N \rangle$成正比.我们的结果进一步表明，根据$σ_{sN}$的值，$ϕ$介子在核物质密度下可以得到正的或负的质量移动。我们发现，这些结果仅弱依赖于潜在的修改的宽度的$ϕ$介子峰和假设的行为的四夸克凝聚在有限密度。为了检验结果的稳定性，我们考虑了对算子乘积展开展开的高阶修正，包括$α_s$修正、奇异夸克质量的高阶项和早期工作中未考虑的高扭曲项.
Investigating forward-backward asymmetry in D-meson production and anisotropic flow in p-Pb collisions at the LHC
Wuhan Textile University（武汉纺织大学）；Shanghai Research Center for Theoretical Nuclear Physics, NSFC and Fudan University（上海理论核物理中心，国家自然科学基金委员会与复旦大学）；Wuhan University of Technology（武汉理工大学）；China University of Geosciences (Wuhan)（中国地质大学（武汉））；East Carolina University（东卡罗来纳大学）；Institute of Modern Physics, Fudan University（复旦大学现代物理研究所）
Open charm production and $Λ_{c}^{+}/D^{0}$ ratio in pp and Au+Au collisions at the RHIC
Key Laboratory of Quark and Lepton Physics (MOE) and Institute of Particle Physics, Central China Normal University（华中师范大学夸克与轻子物理教育部重点实验室和粒子物理研究所）；School of Physics and Mechanics, Wuhan University of Technology（武汉理工大学物理与机电工程学院）；School of Mathematics and Physics, China University of Geosciences (Wuhan)（中国地质大学（武汉）数学与物理学院）
Studies of beauty hadron and non-prompt charm hadron production in pp collisions at $\sqrt{s}$=13 TeV within a transport model approach
School of Mathematics and Physics, China University of Geosciences (Wuhan)（中国地质大学（武汉）数学与统计学院）；Key Laboratory of Quark and Lepton Physics (MOE) and Institute of Particle Physics, Central China Normal University（华中师范大学夸克与轻子物理教育部重点实验室及粒子物理研究所）；Shanghai Research Center for Theoretical Nuclear Physics, NSFC and Fudan University（复旦大学理论核物理上海研究中心）
Towards an automated tool to evaluate the impact of the nuclear modification of the gluon density on quarkonium, D and B meson production in proton-nucleus collisions
我们提出了一个简单的和模型无关的程序来解释核修改的胶子密度编码在核共线PDF集上的两到两个部分子硬过程中的质子-核碰撞的影响。这适用于对夸克偶素、D和B介子产生的良好近似，一般称为H。我们的程序包括参数化的部分子散射振幅的平方，A_{gg -> H X}和约束它从质子-质子数据。这样，我们已经能够以模型无关的方式计算在各种LHC实验的运动学中，在sqrt（s_NN）=5和8 TeV时，J/psi，Upperdance和D^0作为y和P_T的函数的相应核修改因子。这当然是合理的，因为在这种评估中最重要的成分是每个运动学配置的概率。我们对D介子的计算也可以推广到B介子的产生。为了进一步说明该工具的潜力，我们提供了-第一次-预测的核修改因子的eta_c的生产在LHC的pPb碰撞。
