2007
DOI: 10.1016/j.physletb.2007.01.001
|View full text |Cite
|
Sign up to set email alerts
|

Korteweg–de Vries solitons in relativistic hydrodynamics

Abstract: In a previous work, assuming that the nucleus can be treated as a perfect fluid, we have studied the propagation of perturbations in the baryon density. For a given equation of state we have derived a Korteweg -de Vries (KdV) equation from Euler and continuity equations in nonrelativistic hydrodynamics. Here, using a more general equation of state, we extend our formalism to relativistic hydrodynamics.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
35
0
4

Year Published

2009
2009
2020
2020

Publication Types

Select...
6

Relationship

3
3

Authors

Journals

citations
Cited by 20 publications
(39 citation statements)
references
References 17 publications
(29 reference statements)
0
35
0
4
Order By: Relevance
“…Following the same formalism already used for nuclear matter in [17,18,19,20] we will now expand both (5) and (24) in powers of a small parameter σ and combine these two equations to find one single differential equation which governs the space-time evolution of the perturbation in the baryon density. We write (5) and (24) in one cartesian dimension (x) in terms of the dimensionless variables:…”
Section: Wave Equation At Zero Temperaturementioning
confidence: 99%
See 4 more Smart Citations
“…Following the same formalism already used for nuclear matter in [17,18,19,20] we will now expand both (5) and (24) in powers of a small parameter σ and combine these two equations to find one single differential equation which governs the space-time evolution of the perturbation in the baryon density. We write (5) and (24) in one cartesian dimension (x) in terms of the dimensionless variables:…”
Section: Wave Equation At Zero Temperaturementioning
confidence: 99%
“…The other one is to have a third order spatial derivative term. This term comes from the equation of state of the fluid and it appears because the Lagrangian density contains higher derivative couplings [17,18,19] or because of the Laplacians appearing in the equations of motion of the fields of the theory [20]. This happens, for example, in the non-linear Walecka model of nuclear matter at zero and finite temperature.…”
Section: Introductionmentioning
confidence: 99%
See 3 more Smart Citations