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Related papers: Baryon Number Transport via Gluonic Junctions

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During the early development of Quantum Chromodynamics, it was proposed that baryon number could be carried by a non-perturbative Y-shaped topology of gluon fields, called the gluon junction, rather than by the valence quarks as in the QCD…

Recent SPS data on the rapidity distribution of protons in p+S, p+Au and S+S collisions at 200 AGeV and preliminary Pb+Pb collisions at 160 AGeV are compared to HIJING and VENUS calculations as well as to predictions based on the…

Nuclear Theory · Physics 2022-02-23 M. Gyulassy , V. Topor Pop , S. E. Vance

The nucleon exhibits a rich internal structure governed by Quantum Chromodynamics (QCD), where its electric charge arises from valence quarks, while its spin and mass emerge from complex interactions among valence quarks, sea (anti-)quarks,…

High Energy Physics - Phenomenology · Physics 2025-11-19 Niseem Magdy , Prithwish Tribedy , Chun Yuen Tsang , Zhangbu Xu

A new version, v2.0, of the HIJING/B\=B Monte Carlo nuclear collision event generator is introduced in order to explore further the possible role of baryon junctions loops in the baryon/meson anomaly (2 $< p_{T} <$ 5 GeV/c) observed in 200A…

Nuclear Theory · Physics 2009-10-09 V. Topor Pop , M. Gyulassy , J. Barrette , C. Gale , X. N. Wang , N. Xu

Recent results from the H1 experiment [1] have confirmed the existence of a substantial baryon asymmetry of the proton sea at small $x$ with magnitude predicted in hep-ph/9607486. This is a strong support for the idea [3] that baryon number…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. Z. Kopeliovich , B. Povh

The baryon junction exchange mechanism recently proposed to explain valence baryon number transport in nuclear collisions is extended to study midrapidity anti-hyperon production. Baryon junction-anti-junction (J anti-J) loops are shown to…

Nuclear Theory · Physics 2009-10-09 Stephen E. Vance , Miklos Gyulassy

The process of baryon number transfer due to string junction propagation in rapidity is considered. It has a significant effect in the net baryon production in $pp$ collisions at mid-rapidities and an even larger effect in the forward…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Bopp , Yu. M. Shabelski

The process of baryon number transfer due to string junction propagation in rapidity is considered. It has a significant effect in the net baryon production in $pp$ collisions at mid-rapidities and an even larger effect in the forward…

High Energy Physics - Phenomenology · Physics 2009-11-07 G. H. Arakelyan , A. Capella , A. B. Kaidalov , Yu. M. Shabelski

Baryon quantum number is believed to be conserved since baryogenesis in the early Universe. While fractionally charged valence quarks are understood conventionally to each carry a baryon number of 1/3, the baryon junction, a…

Nuclear Experiment · Physics 2024-08-29 STAR Collaboration

In the constituent quark model, each quark inside a baryon carries 1/3 unit of the baryon number. An alternative picture exists where the center of a Y-shaped topology of gluon fields, called the baryon junction, carries a unit baryon…

Nuclear Theory · Physics 2025-03-07 Chun Yuen Tsang , Rongrong Ma , Prithwish Tribedy , Zhangbu Xu

In this report I will give an experimental overview on nuclear stopping in hadron collisions, and relate observations to understanding of baryon transport. Baryon number transport is not only evidenced via net-proton distributions but also…

Nuclear Experiment · Physics 2015-06-26 F. Videbaek

The baryon number transfer is studied in elementary and complex hadronic interactions at the CERN experiment NA49 at the SPS, at 158 AGeV beam energy (\sqrt{s}=17.2 GeV). A two component picture is proposed, which builds up the net proton…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Varga

It is not obvious which partons in the proton carry its baryon number (BN). We present arguments that BN is associated with a specific topology of gluonic fields, rather than with the valence quarks. The BN distribution is easily confused…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. T Garvey , B. Z. Kopeliovich , B. Povh

Although strange quarks are produced in $s\bar{s}$ pairs, the ratio of $\Omega^{-}$ to ${\bar{\Omega}}^{+}$ is greater than one in heavy-ion collisions at lower RHIC energies. Thus the produced $\Omega$ hyperons must carry net baryon…

Nuclear Theory · Physics 2023-03-22 Xiatong Wu , Weijie Dong , Xiaozhou Yu , Hui Li , Gang Wang , Huan Zhong Huang , Zi-Wei Lin

Jet quenching of quarks and gluons in central A+A collisions suppresses the high-p_T meson production and exposes novel baryon dynamics that we attribute to (gluonic) baryon junctions. This mechanism predicts baryon enhancement in a finite…

High Energy Physics - Phenomenology · Physics 2009-10-09 Ivan Vitev , Miklos Gyulassy

We consider the phenomenological implications of the assumption that baryons are systems of three quarks connected through gluon string junction. The transfer of baryon number in rapidity space due to the string junction propagation is…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. H. Arakelyan , C. Merino , C. Pajares , Yu. M. Shabelski

The process of baryon number transfer due to string junction propagation in rapidity space is considered. It leads to a significant effect in the net baryon production in pA collisions at mid-rapidities and an even more significant effect…

High Energy Physics - Phenomenology · Physics 2012-07-30 F. W. Bopp , Yu. M. Shabelski

Constituent quarks in a nucleon are the essential elements in the standard ``quark model" associated with the electric charge, spin, mass, and baryon number of a nucleon. Quantum Chromodynamics (QCD) describes nucleon as a composite object…

High Energy Physics - Phenomenology · Physics 2025-03-10 Niseem Magdy , Abhay Deshpande , Roy Lacey , Wenliang Li , Prithwish Tribedy , Zhangbu Xu

We report the measurement of Lamda and Anti-Lamda yields and inverse slope parameters in d + Au collisions at sqrt(s_NN) = 200 GeV at forward and backward rapidities (y = +- 2.75), using data from the STAR forward time projection chambers.…

Nuclear Experiment · Physics 2008-11-26 STAR Collaboration , B. I. Abelev

QCD as a gauge non-Abelian theory imposes severe constraints on the structure of the baryon wave function. We point out that, contrary to a widely accepted belief, the traces of baryon number in a high-energy process can reside in a…

Nuclear Theory · Physics 2009-10-30 D. Kharzeev
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