Atypical k-essence cosmologies

We analyze the implications of having a divergent speed of sound in k-essence cosmological models. We first study a known theory of that kind, for which the Lagrangian density depends linearly on the time derivative of the k-field. We show that when k-essence is the only source consistency requires...

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Autor principal: Chimento, L.P
Otros Autores: Lazkoz, R.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2005
Acceso en línea:Registro en Scopus
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100 1 |a Chimento, L.P. 
245 1 0 |a Atypical k-essence cosmologies 
260 |c 2005 
270 1 0 |m Chimento, L.P.; Dpto. de Física, Fac. de Ciencias Exactas y Naturales, Universidad de Buenos Aires, 1428 Buenos Aires, Argentina; email: chimento@df.uba.ar 
506 |2 openaire  |e Política editorial 
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504 |a Chimento, L.P., Feinstein, A., (2004) Mod. Phys. Lett. A, 19, p. 761 
504 |a Aguirregabiria, J.M., Chimento, L.P., Lazkoz, R., (2004) Phys. Rev. D, 70, p. 023509 
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520 3 |a We analyze the implications of having a divergent speed of sound in k-essence cosmological models. We first study a known theory of that kind, for which the Lagrangian density depends linearly on the time derivative of the k-field. We show that when k-essence is the only source consistency requires that the potential of the k-field be of the inverse square form. Then, we review the known result that the corresponding power-law solutions can be mapped to power-law solutions of theories with no divergence in the speed of sound. After that, we argue that the requirement of a divergent sound speed at some point fixes uniquely the form of the Lagrangian to be exactly the one considered earlier and prove the asymptotic stability of the most interesting solutions belonging to the divergent theory. Then, we discuss the implications of having not just k-essence but also matter. This is interesting because introducing another component breaks the rigidity of the theory, and the form of the potential ceases to be unique as happened in the pure k-essence case. Finally, we show the finiteness of the effective sound speed under an appropiate definition. © 2005 The American Physical Society.  |l eng 
593 |a Dpto. de Física, Fac. de Ciencias Exactas y Naturales, Universidad de Buenos Aires, 1428 Buenos Aires, Argentina 
593 |a Fis. Teorikoa eta Zientziaren H. S., Zientzia eta Teknol. Fakultatea, Euskal Herriko Unibertsitatea, 644 Posta Kutxatila, 48080 Bilbao, Spain 
690 1 0 |a ARTICLE 
690 1 0 |a COSMOLOGICAL PHENOMENA 
690 1 0 |a COSMOS 
690 1 0 |a DENSITY 
690 1 0 |a LANGRANGIAN MODEL 
690 1 0 |a MATHEMATICAL MODEL 
690 1 0 |a POWER LAW SOLUTION 
690 1 0 |a PROBLEM SOLVING 
690 1 0 |a RIGIDITY 
690 1 0 |a SOUND 
690 1 0 |a VELOCITY 
700 1 |a Lazkoz, R. 
773 0 |d 2005  |g v. 71  |h pp. 023505-1-023505-7  |k n. 2  |p Phys Rev D Part Fields Gravit Cosmol  |x 15507998  |t Physical Review D - Particles, Fields, Gravitation and Cosmology 
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