2002
DOI: 10.1016/s0375-9474(02)00680-2
|View full text |Cite
|
Sign up to set email alerts
|

Stability of strange quark matter: MIT bag versus color dielectric model

Abstract: We discuss the properties of strange matter, in particular the minimum of the energy per baryon number as a function of the strangeness fraction. We utilize both the MIT bag model and the Color Dielectric Model and compare the energy per baryon with the masses of hyperons having the corresponding strangeness fraction, which are coherently calculated within both models. We also take into account the perturbative exchange of gluons. The results obtained in the two approaches allow to discuss the stability of str… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

1
18
0

Year Published

2002
2002
2018
2018

Publication Types

Select...
4
2
1

Relationship

0
7

Authors

Journals

citations
Cited by 14 publications
(19 citation statements)
references
References 42 publications
1
18
0
Order By: Relevance
“…We adopted S = 7.15 GeV and Λ = T c , where T c is the value of the critical temperature computed in the model. These parameter values are also consistent with the more general form for g 2 introduced in [40] (see note 4). Notice that the value of the critical temperature is not modified by the perturbative corrections and can therefore be computed before the latter are taken into account.…”
Section: Resultssupporting
confidence: 85%
“…We adopted S = 7.15 GeV and Λ = T c , where T c is the value of the critical temperature computed in the model. These parameter values are also consistent with the more general form for g 2 introduced in [40] (see note 4). Notice that the value of the critical temperature is not modified by the perturbative corrections and can therefore be computed before the latter are taken into account.…”
Section: Resultssupporting
confidence: 85%
“…The high stability of the 56 Fe nucleus (the binding energy per nucleon is maximum at A ≈ 56) requires that to have the strange quark matter as the ground state of the quark matter, the energy per unit of baryonic number should satisfies the condition ρ [9][10].…”
Section: Results and Conclusionmentioning
confidence: 99%
“…The present contribution is largely based on the results of ref. [13], with a special focus on the model dependence of the strangelets stability. We consider homogeneous quark matter made up of u, d and s quarks, without imposing chemical equilibrium on the density of the strange quarks.…”
Section: Introductionmentioning
confidence: 99%