论文标题

质子 - 蛋白质和质子铅碰撞中的二元发电机在$ \ sqrt {s _ {\ rm {nn}}} $ = 5.02 TEV

Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV

论文作者

ALICE Collaboration

论文摘要

质子 - 质子 - 质子 - 普罗顿和质子铅碰撞$ \ sqrt {s _ {\ rm {rm {nn}}} $ = 5.02 tev的第一个测量(proton-proton和proton-Lead Collivision在proton-proton和Proton-Lead碰撞中的第一个测量值)用爱丽丝探测器测量Dielectron横截面,作为不变质量$ M _ {\ rm {ee}} $的函数,以及对在范围内的横向动量$ p _ {\ rm {\ rm {t,ee}} $在范围内$ p _ {\ rm {t,ee}} $ <8.0 gev/$ c^{2} $,在两个碰撞系统中。在质子 - 普罗顿碰撞中,魅力和美容横截面是在中等范围内从拟合到两个不同事件发生器的数据的。这补充了以$ \ sqrt {s} $ = 7和13 TEV执行的现有介电测量值。 Fonll计算描述了三个测量值的$ \ sqrt {s} $依赖性的斜率。在质子铅碰撞中测量的二元横截面在当前的精度范围内是一致的,与预期的二元发电机产生,没有任何核物质效应,$ \ rm {e}^{+} \ rm {e}^{e}^{ - } $ pairs $来自开放式重型福特·哈德隆(Hadron decays)。首次在LHC Energies中,直接将质子铅和质子 - 蛋白质碰撞中的二元发射产生以相同的$ \ sqrt {s _ {\ rm {\ rm {nn}}} $通过dielectron核修饰因子$ r _ {\ rm rm {\ rm rm {\ rm {ppb} $ {\ rm {nn}} $进行比较。将测量值与模型计算进行了比较,包括冷核物质效应或热辐射中的其他电介子来源。

The first measurements of dielectron production at midrapidity ($|η_{c}|<0.8$) in proton-proton and proton-lead collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass $m_{\rm{ee}}$ and the pair transverse momentum $p_{\rm{T,ee}}$ in the ranges $m_{\rm{ee}}$ < 3.5 GeV/$c^{2}$ and $p_{\rm{T,ee}}$ < 8.0 GeV/$c^{2}$, in both collision systems. In proton-proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at $\sqrt{s}$ = 7 and 13 TeV. The slope of the $\sqrt{s}$ dependence of the three measurements is described by FONLL calculations. The dielectron cross section measured in proton-lead collisions is in agreement, within the current precision, with the expected dielectron production without any nuclear matter effects for $\rm{e}^{+}\rm{e}^{-}$ pairs from open heavy-flavor hadron decays. For the first time at LHC energies, the dielectron production in proton-lead and proton-proton collisions are directly compared at the same $\sqrt{s_{\rm{NN}}}$ via the dielectron nuclear modification factor $R_{\rm{pPb}}$. The measurements are compared to model calculations including cold nuclear matter effects, or additional sources of dielectrons from thermal radiation.

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