# Chemical potentials of light hadrons and quarks from yield ratios of   negative to positive particles in high energy $pp$ collisions

**Authors:** Xing-Wei He, Hua-Rong Wei, Fu-Hu Liu

arXiv: 1812.08513 · 2019-03-13

## TL;DR

This study extracts the chemical potentials of light hadrons and quarks in high-energy proton-proton collisions by analyzing yield ratios from transverse momentum spectra, revealing their dependence on momentum and collision energy.

## Contribution

It introduces a method to determine transverse momentum and energy dependent chemical potentials of hadrons and quarks from yield ratios in $pp$ collisions, highlighting their behavior at different energies.

## Key findings

- Chemical potentials approach zero at high $p_T$ and high energies.
- Energy dependent chemical potentials decrease slightly with increasing collision energy.
- Partonic interactions are significant at RHIC and LHC energies.

## Abstract

We describe the transverse momentum spectra of $\pi^\pm$, $K^\pm$, $p$, and $\bar{p}$ produced in proton-proton ($pp$) collisions at different collision energies by using a Tsallis-Pareto-type function, and obtain the yield ratios, $k_{\pi}$, $k_{K}$, and $k_{p}$, of negative to positive particles from the fitting results of transverse momentum spectra and the extracted normalization constants. The transverse momentum dependent and energy dependent chemical potentials of light hadrons ($\pi$, $K$, and $p$) and quarks ($u$, $d$, and $s$) in $pp$ collisions are then extracted successively from the yield ratios. The six types of transverse momentum dependent chemical potentials show the trend of being close to zero in low-$p_T$ region and away from zero in high-$p_T$ region. Meanwhile, the energy dependent chemical potentials seem to decrease slightly with the increase of the collision energy, and the limiting values of the six types of chemical potentials are zero at very high energy in $pp$ collisions, which confirms that the partonic interactions possibly play an important role at RHIC and LHC, especially at LHC.

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Source: https://tomesphere.com/paper/1812.08513