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Trapped Quintessential Inflation.

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Trapped Quintessential Inflation. / Bueno-Sanchez, Juan Carlos; Dimopoulos, Konstantinos.
In: Physics Letters B, Vol. 642, No. 4, 16.11.2006, p. 294-301.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Bueno-Sanchez, JC & Dimopoulos, K 2006, 'Trapped Quintessential Inflation.', Physics Letters B, vol. 642, no. 4, pp. 294-301. https://doi.org/10.1016/j.physletb.2006.09.045

APA

Bueno-Sanchez, J. C., & Dimopoulos, K. (2006). Trapped Quintessential Inflation. Physics Letters B, 642(4), 294-301. https://doi.org/10.1016/j.physletb.2006.09.045

Vancouver

Bueno-Sanchez JC, Dimopoulos K. Trapped Quintessential Inflation. Physics Letters B. 2006 Nov 16;642(4):294-301. doi: 10.1016/j.physletb.2006.09.045

Author

Bueno-Sanchez, Juan Carlos ; Dimopoulos, Konstantinos. / Trapped Quintessential Inflation. In: Physics Letters B. 2006 ; Vol. 642, No. 4. pp. 294-301.

Bibtex

@article{15e569c932b64c999410f160fb0f9f76,
title = "Trapped Quintessential Inflation.",
abstract = "Quintessential inflation is studied using a string modulus as the inflaton–quintessence field. The modulus begins its evolution at the steep part of its scalar potential, which is due to non-perturbative effects (e.g. gaugino condensation). It is assumed that the modulus crosses an enhanced symmetry point (ESP) in field space. Particle production at the ESP temporarily traps the modulus resulting in a brief period of inflation. More inflation follows, due to the flatness of the potential, since the ESP generates either an extremum (maximum or minimum) or a flat inflection point in the scalar potential. Eventually, the potential becomes steep again and inflation is terminated. After reheating the modulus freezes due to cosmological friction at a large value, such that its scalar potential is dominated by contributions due to fluxes in the extra dimensions or other effects. The modulus remains frozen until the present, when it can become quintessence and account for the dark energy necessary to explain the observed accelerated expansion.",
author = "Bueno-Sanchez, {Juan Carlos} and Konstantinos Dimopoulos",
year = "2006",
month = nov,
day = "16",
doi = "10.1016/j.physletb.2006.09.045",
language = "English",
volume = "642",
pages = "294--301",
journal = "Physics Letters B",
issn = "0370-2693",
publisher = "ELSEVIER SCIENCE BV",
number = "4",

}

RIS

TY - JOUR

T1 - Trapped Quintessential Inflation.

AU - Bueno-Sanchez, Juan Carlos

AU - Dimopoulos, Konstantinos

PY - 2006/11/16

Y1 - 2006/11/16

N2 - Quintessential inflation is studied using a string modulus as the inflaton–quintessence field. The modulus begins its evolution at the steep part of its scalar potential, which is due to non-perturbative effects (e.g. gaugino condensation). It is assumed that the modulus crosses an enhanced symmetry point (ESP) in field space. Particle production at the ESP temporarily traps the modulus resulting in a brief period of inflation. More inflation follows, due to the flatness of the potential, since the ESP generates either an extremum (maximum or minimum) or a flat inflection point in the scalar potential. Eventually, the potential becomes steep again and inflation is terminated. After reheating the modulus freezes due to cosmological friction at a large value, such that its scalar potential is dominated by contributions due to fluxes in the extra dimensions or other effects. The modulus remains frozen until the present, when it can become quintessence and account for the dark energy necessary to explain the observed accelerated expansion.

AB - Quintessential inflation is studied using a string modulus as the inflaton–quintessence field. The modulus begins its evolution at the steep part of its scalar potential, which is due to non-perturbative effects (e.g. gaugino condensation). It is assumed that the modulus crosses an enhanced symmetry point (ESP) in field space. Particle production at the ESP temporarily traps the modulus resulting in a brief period of inflation. More inflation follows, due to the flatness of the potential, since the ESP generates either an extremum (maximum or minimum) or a flat inflection point in the scalar potential. Eventually, the potential becomes steep again and inflation is terminated. After reheating the modulus freezes due to cosmological friction at a large value, such that its scalar potential is dominated by contributions due to fluxes in the extra dimensions or other effects. The modulus remains frozen until the present, when it can become quintessence and account for the dark energy necessary to explain the observed accelerated expansion.

U2 - 10.1016/j.physletb.2006.09.045

DO - 10.1016/j.physletb.2006.09.045

M3 - Journal article

VL - 642

SP - 294

EP - 301

JO - Physics Letters B

JF - Physics Letters B

SN - 0370-2693

IS - 4

ER -