Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\sqrt{s_{NN}}=7.7$ to 200 GeV
A. Adare, S. Afanasiev, C. Aidala, N.N. Ajitanand, Y. Akiba, R., Akimoto, H. Al-Bataineh, J. Alexander, M. Alfred, A. Al-Jamel, H. Al-Ta'ani,, A. Angerami, K. Aoki, N. Apadula, L. Aphecetche, Y. Aramaki, R. Armendariz,, S.H. Aronson, J. Asai, H. Asano, E.C. Aschenauer

TL;DR
This paper reports measurements of charged-particle multiplicity and transverse energy at midrapidity across various collision systems and energies, revealing that quark participant scaling better describes the data than nucleon participant scaling.
Contribution
It provides comprehensive midrapidity distributions for multiple collision systems and energies, emphasizing the importance of quark participant scaling in heavy-ion collisions.
Findings
Midrapidity data are better described by quark participant scaling.
The ratio of transverse energy to charged particle multiplicity remains constant across centralities.
Estimated energy densities increase with collision energy and system size.
Abstract
Measurements of midrapidity charged particle multiplicity distributions, , and midrapidity transverse-energy distributions, , are presented for a variety of collision systems and energies. Included are distributions for AuAu collisions at , 130, 62.4, 39, 27, 19.6, 14.5, and 7.7 GeV, CuCu collisions at and 62.4 GeV, CuAu collisions at GeV, UU collisions at GeV, Au collisions at GeV, HeAu collisions at GeV, and collisions at GeV. Centrality-dependent distributions at midrapidity are presented in terms of the number of nucleon participants, , and the number of constituent quark participants, . For all collisions down to…
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