TY - JOUR
T1 - Disappearing inflaton potential via heavy field dynamics
AU - Kitajima, Naoya
AU - Takahashi, Fuminobu
N1 - Funding Information:
This work is supported by MEXT Grant-in-Aid for Scientific research on Innovative Areas (No.15H05889 (F.T.) and No. 23104008 (N.K. and F.T.)), Scientific Research (A) No. 26247042 and (B) No. 26287039 (F.T.), and Young Scientists (B) (No. 24740135 (F.T.)), and World Premier International Research Center Initiative (WPI Initiative), MEXT, Japan (F.T.).
Publisher Copyright:
© 2016, Institute of Physics. All rights reserved.
PY - 2016/2/17
Y1 - 2016/2/17
N2 - We propose a possibility that the inflaton potential is significantly modified after inflation due to heavy field dynamics. During inflation such a heavy scalar field may be stabilized at a value deviated from the low-energy minimum. In extreme cases, the inflaton potential vanishes and the inflaton becomes almost massless at some time after inflation. Such transition of the inflaton potential has interesting implications for primordial density perturbations, reheating, creation of unwanted relics, dark radiation, and experimental search for light degrees of freedom. To be concrete, we consider a chaotic inflation in supergravity where the inflaton mass parameter is promoted to a modulus field, finding that the inflaton becomes stable after the transition and contributes to dark matter. Another example is a hilltop inflation (also called new inflation) by the MSSM Higgs field which acquires a large expectation value just after inflation, but it returns to the origin after the transition and finally rolls down to the electroweak vacuum. Interestingly, the smallness of the electroweak scale compared to the Planck scale is directly related to the flatness of the inflaton potential.
AB - We propose a possibility that the inflaton potential is significantly modified after inflation due to heavy field dynamics. During inflation such a heavy scalar field may be stabilized at a value deviated from the low-energy minimum. In extreme cases, the inflaton potential vanishes and the inflaton becomes almost massless at some time after inflation. Such transition of the inflaton potential has interesting implications for primordial density perturbations, reheating, creation of unwanted relics, dark radiation, and experimental search for light degrees of freedom. To be concrete, we consider a chaotic inflation in supergravity where the inflaton mass parameter is promoted to a modulus field, finding that the inflaton becomes stable after the transition and contributes to dark matter. Another example is a hilltop inflation (also called new inflation) by the MSSM Higgs field which acquires a large expectation value just after inflation, but it returns to the origin after the transition and finally rolls down to the electroweak vacuum. Interestingly, the smallness of the electroweak scale compared to the Planck scale is directly related to the flatness of the inflaton potential.
KW - inflation
KW - particle physics - cosmology connection
KW - physics of the early universe
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U2 - 10.1088/1475-7516/2016/02/041
DO - 10.1088/1475-7516/2016/02/041
M3 - Article
AN - SCOPUS:84960126176
SN - 1475-7516
VL - 2016
JO - Journal of Cosmology and Astroparticle Physics
JF - Journal of Cosmology and Astroparticle Physics
IS - 2
M1 - 041
ER -