Exact solutions of quintessence models of dark energy

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SUMMARY

The discussion focuses on constructing cosmological models using quintessence, specifically through the minimally coupled scalar field represented by the Klein-Gordon equation: $$ \ddot{\phi} + 3 H \dot{\phi} + \frac{\partial V(\phi)}{\partial \phi} = 0 $$. Participants highlight the necessity of integrating the Friedmann equations with the scalar field energy density $$ \rho_\phi $$ as a source. However, the lack of a known analytical form for the scalar field $$ \phi(t) $$ complicates the integration process. Special solutions, such as the slow-roll approximation and tracker quintessence models, are suggested as potential avenues for addressing cosmological constant issues.

PREREQUISITES
  • Understanding of the Klein-Gordon equation in cosmology
  • Familiarity with Friedmann equations and their applications
  • Knowledge of scalar field dynamics in cosmological models
  • Concept of energy density in the context of dark energy
NEXT STEPS
  • Research the integration of the Klein-Gordon equation with Friedmann equations
  • Study the slow-roll approximation in inflationary cosmology
  • Examine tracker quintessence models and their implications for dark energy
  • Explore potential forms of scalar field potentials $$ V(\phi) $$ and their effects on cosmological solutions
USEFUL FOR

Astronomers, theoretical physicists, and cosmologists interested in dark energy models and the dynamics of scalar fields in the universe.

Diferansiyel
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Hi everyone,

I got the basic ideas quintessence (minimally coupled) and derived the KG equation for scalar field:

$$ \ddot{\phi} + 3 H \dot{\phi} + \frac{\partial V(\phi)}{\partial \phi} = 0 $$
where $$H=\frac{\dot{a}}{a}$$ and $\phi$ is the scalar field.

There are various models depending on the choice of potential of the field, however I do not understand how to construct cosmological model from these potentials? Obviously, there is an differential equation that must be solved but does it even have an analytical solution?

P.S: I am open your resource suggestions.
 
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Diferansiyel said:
There are various models depending on the choice of potential of the field, however I do not understand how to construct cosmological model from these potentials? Obviously, there is an differential equation that must be solved but does it even have an analytical solution?
Have you looked at the Friedmann Equations with the scalar field as the energy source?
 
bapowell said:
Have you looked at the Friedmann Equations with the scalar field as the energy source?

Dear bapowell,

It is possible to use the energy density of the scalar field (## \rho_\phi ##) in Friedmann equations, the problem is that we don't know the exact form of the scalar field ## \phi(t) ##, therefore integration can't be accomplished. There must be some other constrains on ## \phi(t) ##
 
Diferansiyel said:
Dear bapowell,

It is possible to use the energy density of the scalar field (## \rho_\phi ##) in Friedmann equations, the problem is that we don't know the exact form of the scalar field ## \phi(t) ##, therefore integration can't be accomplished. There must be some other constrains on ## \phi(t) ##
For a given V(\phi), you must specify \phi(t_0) and \dot{\phi}(t_0). Then you can solve the Klein-Gordon and Friedmann equations together to obtain your cosmology.
 
bapowell said:
For a given V(\phi), you must specify \phi(t_0) and \dot{\phi}(t_0). Then you can solve the Klein-Gordon and Friedmann equations together to obtain your cosmology.

So there are "special" solutions depending on the behaviour of scalar field like slow-roll approximation in the inflationary cosmology. In fact, tracker quintessence models propose some solutions to cosmological constant problems. Maybe I should examine these fields.
 

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