论文标题

辐射强化:从夸克 - 杜伦等离子体的强扎时的光子发射

Radiative hadronization: Photon emission at hadronization from quark-gluon plasma

论文作者

Fujii, Hirotsugu, Itakura, Kazunori, Miyachi, Katsunori, Nonaka, Chiho

论文摘要

我们从相对论重离子碰撞中产生的夸克 - 格鲁隆等离子体的强调阶段调查了光子发射。重组模式的图片表明,在强环化中,夸克和一个古夸公园结合到介子状态,如果没有其他涉及的话,这显然会违反节能。我们在这里考虑重组伴随光子发射的强合过程。这是血浆物理学中已知的“ {\ it辐射重组}”的类似物,例如$ e^ - + p^ + \ to {\ rm h} 0 +γ$,当电磁等离子体回到中性原子质燃气中时发生时发生。 “辐射强化”图片将带来(i)光子产量的增强,(ii)具有类似于Hadron的光子的显着流动,以及(iii)具有热曲线的光子横向动量($ p_t $)分布,其有效温度由夸张的夸克温度给出,其有效温度给出。在这里,作为辐射强化的最简单和现象学的实现,我们修改了重组模型涉及光子发射,并使用该修饰模型评估光子产量。我们对直接光子产量的贡献以及由流体动力模型和及时光子的参数贡献计算的热光子贡献,我们研究了在RHIC和LHC Energies的重型离子碰撞中产生的光子的$ P_T $ spectrum和椭圆流。

We investigate photon emission at the hadronization stage from a quark-gluon plasma created in relativistic heavy-ion collisions. A recombination-model picture suggests that a quark and an antiquark bind into a meson state in hadronization, which would apparently violate the energy conservation if there is nothing else involved. We consider here a hadronization process where the recombination accompanies a photon emission. This is an analog of the "{\it radiative recombination}" known in plasma physics, such as $e^- + p^+ \to {\rm H}^0 +γ$, which occurs when an electromagnetic plasma goes back to a neutral atomic gas. The "radiative hadronization" picture will bring about (i) an enhancement of the photon yield, (ii) significant flow of photons similar to that of hadrons, and (iii) the photon transverse momentum ($p_T$) distribution with a thermal profile whose effective temperature is given by blue-shifted temperature of quarks. Here as a simplest and phenomenological realization of the radiative hadronization, we modify the recombination model to involve a photon emission and evaluate the photon yield with this modified model. Adding this contribution to the direct photon yield along with thermal photon contribution calculated with a hydrodynamic model and a parametrized contribution of prompt photons, we study the $p_T$ spectrum and elliptic flow of the photons produced in heavy-ion collisions at RHIC and LHC energies.

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