Melting Hadrons, Boiling Quarks - From Hagedorn Temperature to Ultra-Relativistic Heavy-Ion Collisions at CERN 2016
DOI: 10.1007/978-3-319-17545-4_25
|View full text |Cite
|
Sign up to set email alerts
|

How We Got to QCD Matter from the Hadron Side: 1984

Abstract: Rolf Hagedorn reminisces in 1984 about limiting temperature, the development of the statistical bootstrap model (SBM). He argues that consideration of hadrons of finite size allowed the generalization of SBM into a sophisticated relativistic van der Waals-type gas, leading on to a theory of phase transformation from melting hadrons to boiling quarks.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
27
0

Year Published

2016
2016
2022
2022

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 19 publications
(29 citation statements)
references
References 107 publications
2
27
0
Order By: Relevance
“…We find a smooth transformation, a position clearly taken by Hagedorn as of the early 1980s, see for example Ref. [10]. We can say that hadrons dissolve into their constituents, quarks, and that this phase transformation has been established near T H = 145 + −7 MeV [11,12].…”
Section: Hot Hagedorn Universesupporting
confidence: 66%
“…We find a smooth transformation, a position clearly taken by Hagedorn as of the early 1980s, see for example Ref. [10]. We can say that hadrons dissolve into their constituents, quarks, and that this phase transformation has been established near T H = 145 + −7 MeV [11,12].…”
Section: Hot Hagedorn Universesupporting
confidence: 66%
“…and, substituting it into Equations (26) and (27), one can calculate the beta function in the one loop approximation. By considering the asymptotic limit (q − 1)µ λ 0 /ε i , one obtains…”
Section: Effective Coupling and β-Functionmentioning
confidence: 99%
“…The Hadron Resonance Gas (HRG) model describes the confined phase of the QCD equation of state (EoS) at finite temperature below ∼ 150 MeV as a multicomponent gas of non-interacting massive stable and point-like particles [1,2], which are usually taken as the conventional hadrons listed in the review by the Particle Data Group (PDG) [3]. One of the greatest achievements of this approach has been the study of the trace anomaly, ( − 3P )/T 4 with energy density and P the pressure.…”
Section: Introductionmentioning
confidence: 99%