首次测量了不相干的J/ψ光子核生产的依赖性
S Acharya1, D Adamová2, A Adler3
1Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France.
Physical review letters
|May 3, 2024
概括
介绍了在超外围碰撞中对J/ψ向量质子产生截面的首次测量. 在模型中包含量子波动可以提高数据的一致性,特别是关于曼德尔斯塔姆的变量依赖性.
科学领域:
- 高能核物理 高能核物理
- 量子色态动力学 是一个量子色态动力学.
- 粒子物理学的粒子物理学.
背景情况:
- J/ψ矢量质子是核环境的关键探测器.
- 了解光子核生产机制,可以了解子密度和量子波动.
- 之前的测量缺乏详细的研究作为一个函数的曼德尔斯塔姆变量.
研究的目的:
- 为了介绍第一个测量J/ψ矢量质子不连贯的光子核生产截面与曼德尔斯塔姆的变量.
- 将实验数据与理论模型预测进行比较.
- 为了研究量子波动在子密度中的作用.
主要方法:
- 利用大强子对撞机的ALICE探测器进行数据收集.
- 分析了 (Pb) 原子核的超外围碰撞,其质量中心能量为5.02 TeV.
- 在五个时间间隔 (0.04 GeV2) 中测量了 J/ψ 产量在中速 (何时下降<0.8) 时.
主要成果:
- 首次测量了J/ψ生产的横截面作为曼德尔斯塔姆变量的函数.
- 忽略了子密度的量子波动的模型预测了比数据中观察到的更的度依赖.
- 纳入量子波动的模型更好地描述了测量到的量子依赖性.
结论:
- 该研究提供了关键的实验数据来限制J/ψ生产的理论模型.
- 子密度的量子波动在描述截面的依赖性方面发挥着重要作用.
- 这项测量有助于我们更好地理解光子核相互作用与子内部结构之间的相互作用.
相关概念视频
Thomson's e/m Experiment
3.6K
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
3.6K
Atomic Nuclei: Nuclear Spin State Population Distribution
973
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
973
Atomic Emission Spectroscopy: Interference
182
In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
182
Atomic Nuclei: Nuclear Magnetic Moment
1.1K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
1.1K
Atomic Absorption Spectroscopy: Interference
745
Interference leads to systematic error in atomic absorption (AA) measurements by enhancing or diminishing the analytical signal or the background. These interferences can be grouped into three main categories: spectral interference, chemical interference, and physical interference.
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
Spectral interference occurs when signals from other elements or molecules overlap with the analyte signal, falsely elevating or masking the analyte's absorbance. This interference can be corrected using Zeeman,...
745
Interpreting ¹H NMR Signal Splitting: The (n + 1) Rule
1.3K
In the AX proton spin system, proton A can sense the two spin states of a coupled proton X, resulting in a doublet NMR signal with two peaks of equal (1:1) intensity. When proton A is coupled to two equivalent protons (AX2 spin system), the spin states of each X can be aligned with or against the external field, creating three possible scenarios. This results in a 1:2:1 triplet signal, where the central peak corresponds to the chemical shift of A and is twice as large or intense as the...
1.3K


