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Universal Bound on the Duration of a Kination Era
Phys. Rev. Lett. 135, 101002 – Published 2 September, 2025
DOI: https://doi.org/10.1103/k7ty-gwjg
Abstract
We show that primordial adiabatic curvature fluctuations generate an instability of the scalar field sourcing a kination era. We demonstrate that the generated higher Fourier modes constitute a radiationlike component dominating over the kination background after about 11 e-folds of cosmic expansion. Current constraints on the extra number of neutrino flavors thus imply the observational bound of approximately 10 e-folds, representing the most stringent bound to date on the stiffness of the equation of state of the pre–Big Bang–nucleosynthesis universe.
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References (110)
- R. Allahverdi et al., Open J. Astrophys. 4 (2021), 10.21105/astro.2006.16182.
- Y. B. Zel’dovich, Sov. Phys. JETP 14 (1962), http://jetp.ras.ru/cgi-bin/dn/e_014_05_1143.pdf.
- B. Spokoiny, Phys. Lett. B 315, 40 (1993).
- M. Joyce, Phys. Rev. D 55, 1875 (1997).
- P. G. Ferreira and M. Joyce, Phys. Rev. D 58, 023503 (1998).
- M. Joyce, Habilitation thesis, Laboratoire de physique nucleaire et des hautes Energies (LPNHE), Paris (2001), https://supernovae.in2p3.fr/~joyce/mjoyce_habilitation.pdf.
- P. J. E. Peebles and A. Vilenkin, Phys. Rev. D 59, 063505 (1999).
- K. Dimopoulos and J. W. F. Valle, Astropart. Phys. 18, 287 (2002).
- J. P. Conlon, R. Kallosh, A. D. Linde, and F. Quevedo, J. Cosmol. Astropart. Phys. 09 (2008) 011.
- J. P. Conlon and F. Revello, J. High Energy Phys. 11 (2022) 155.
- F. Apers, J. P. Conlon, E. J. Copeland, M. Mosny, and F. Revello, J. Cosmol. Astropart. Phys. 08 (2024) 018.
- B. Li, T. Rindler-Daller, and P. R. Shapiro, Phys. Rev. D 89, 083536 (2014).
- R. T. Co, D. Dunsky, N. Fernandez, A. Ghalsasi, L. J. Hall, K. Harigaya, and J. Shelton, J. High Energy Phys. 09 (2022) 116.
- Y. Gouttenoire, G. Servant, and P. Simakachorn, arXiv:2108.10328.
- Y. Gouttenoire, G. Servant, and P. Simakachorn, arXiv:2111.01150.
- P. Simakachorn, Charting cosmological history and new particle physics with primordial gravitational waves, Ph.D. thesis, U. Hamburg (main), Hamburg University, 2022.
- K. Harigaya, K. Inomata, and T. Terada, Phys. Rev. D 108, L081303 (2023).
- K. Harigaya, K. Inomata, and T. Terada, Phys. Rev. D 108, 123538 (2023).
- D. J. H. Chung and S. C. Tadepalli, Phys. Rev. D 111, 083527 (2025).
- H. Duval, S. Kuroyanagi, A. Mariotti, A. Romero-Rodríguez, and M. Sakellariadou, Phys. Rev. D 110, 103503 (2024).
- I. Affleck and M. Dine, Nucl. Phys. B249, 361 (1985).
- R. T. Co and K. Harigaya, Phys. Rev. Lett. 124, 111602 (2020).
- R. T. Co, L. J. Hall, and K. Harigaya, Phys. Rev. Lett. 124, 251802 (2020).
- C.-F. Chang and Y. Cui, Phys. Rev. D 102, 015003 (2020).
- R. T. Co, N. Fernandez, A. Ghalsasi, L. J. Hall, and K. Harigaya, J. High Energy Phys. 03 (2021) 017.
- C. Eröncel, R. Sato, G. Servant, and P. Sørensen, J. Cosmol. Astropart. Phys. 10 (2022) 053.
- C. Eröncel and G. Servant, J. Cosmol. Astropart. Phys. 01 (2023) 009.
- C. Eröncel, R. Sato, G. Servant, and P. Sørensen, arXiv:2408.08355.
- M. S. Turner, Phys. Rev. D 28, 1243 (1983).
- V. Poulin, T. L. Smith, D. Grin, T. Karwal, and M. Kamionkowski, Phys. Rev. D 98, 083525 (2018).
- V. Poulin, T. L. Smith, T. Karwal, and M. Kamionkowski, Phys. Rev. Lett. 122, 221301 (2019).
- P. Agrawal, F.-Y. Cyr-Racine, D. Pinner, and L. Randall, Phys. Dark Universe 42, 101347 (2023).
- S. Sánchez López, K. Dimopoulos, A. Karam, and E. Tomberg, Eur. Phys. J. C 83, 1152 (2023).
- J. D. Barrow and M. S. Turner, Nature (London) 292, 35 (1981).
- M. S. Turner and L. M. Widrow, Nature (London) 326, 206 (1987).
- F. Niedermann and M. S. Sloth, Phys. Rev. D 103, L041303 (2021).
- F. Niedermann and M. S. Sloth, Phys. Rev. D 102, 063527 (2020).
- V. Sahni, M. Sami, and T. Souradeep, Phys. Rev. D 65, 023518 (2001).
- H. Tashiro, T. Chiba, and M. Sasaki, Classical Quantum Gravity 21, 1761 (2004).
- M. Sami and V. Sahni, Phys. Rev. D 70, 083513 (2004).
- M. Artymowski, O. Czerwinska, Z. Lalak, and M. Lewicki, J. Cosmol. Astropart. Phys. 04 (2018) 046.
- L. Aresté Saló and J. de Haro, Eur. Phys. J. C 77, 798 (2017).
- D. G. Figueroa and E. H. Tanin, J. Cosmol. Astropart. Phys. 10 (2019) 050.
- M. Giovannini, Phys. Rev. D 58, 083504 (1998).
- M. Giovannini, PMC Phys. A 4, 1 (2010).
- M. Giovannini, Phys. Rev. D 105, 103524 (2022).
- M. Giovannini, Phys. Rev. D 108, 123508 (2023).
- A. Riazuelo and J.-P. Uzan, Phys. Rev. D 62, 083506 (2000).
- N. Seto and J. Yokoyama, J. Phys. Soc. Jpn. 72, 3082 (2003).
- L. A. Boyle and A. Buonanno, Phys. Rev. D 78, 043531 (2008).
- K. Nakayama, S. Saito, Y. Suwa, and J. Yokoyama, Phys. Rev. D 77, 124001 (2008).
- K. Nakayama, S. Saito, Y. Suwa, and J. Yokoyama, J. Cosmol. Astropart. Phys. 06 (2008) 020.
- R. Durrer and J. Hasenkamp, Phys. Rev. D 84, 064027 (2011).
- S. Kuroyanagi, K. Nakayama, and S. Saito, Phys. Rev. D 84, 123513 (2011).
- S. Kuroyanagi, T. Chiba, and T. Takahashi, J. Cosmol. Astropart. Phys. 11 (2018) 038.
- R. Jinno, T. Moroi, and K. Nakayama, Phys. Rev. D 86, 123502 (2012).
- P. D. Lasky et al., Phys. Rev. X 6, 011035 (2016).
- B. Li, P. R. Shapiro, and T. Rindler-Daller, Phys. Rev. D 96, 063505 (2017).
- K. Saikawa and S. Shirai, J. Cosmol. Astropart. Phys. 05 (2018) 035.
- D. G. Figueroa and E. H. Tanin, J. Cosmol. Astropart. Phys. 08 (2019) 011.
- R. R. Caldwell, T. L. Smith, and D. G. E. Walker, Phys. Rev. D 100, 043513 (2019).
- N. Bernal and F. Hajkarim, Phys. Rev. D 100, 063502 (2019).
- F. D’Eramo and K. Schmitz, Phys. Rev. Res. 1, 013010 (2019).
- G. Servant and P. Simakachorn, Phys. Rev. D 109, 103538 (2024).
- B. Li and P. R. Shapiro, J. Cosmol. Astropart. Phys. 10 (2021) 024.
- Y. Cui, M. Lewicki, D. E. Morrissey, and J. D. Wells, Phys. Rev. D 97, 123505 (2018).
- Y. Cui, M. Lewicki, D. E. Morrissey, and J. D. Wells, J. High Energy Phys. 01 (2019) 081.
- D. Bettoni, G. Domènech, and J. Rubio, J. Cosmol. Astropart. Phys. 02 (2019) 034.
- P. Auclair et al., J. Cosmol. Astropart. Phys. 04 (2020) 034.
- N. Ramberg and L. Visinelli, Phys. Rev. D 99, 123513 (2019).
- C.-F. Chang and Y. Cui, Phys. Dark Universe 29, 100604 (2020).
- Y. Gouttenoire, G. Servant, and P. Simakachorn, J. Cosmol. Astropart. Phys. 07 (2020) 032.
- Y. Gouttenoire, G. Servant, and P. Simakachorn, J. Cosmol. Astropart. Phys. 07 (2020) 016.
- C.-F. Chang and Y. Cui, J. High Energy Phys. 03 (2022) 114.
- D. J. H. Chung and P. Zhou, Phys. Rev. D 82, 024027 (2010).
- N. Aghanim et al. (Planck Collaboration), Astron. Astrophys. 641, A6 (2020); 652, C4(E) (2021).
The power spectrum of a physical variable is the Fourier spectrum of the correlation function . In this Letter, we use the dimensionless power spectrum .
- N. Aghanim et al. (Planck Collaboration), Astron. Astrophys. 641, A6 (2020).
- P. A. R. Ade et al. (BICEP and Keck Collaborations), Phys. Rev. Lett. 127, 151301 (2021).
- V. Mukhanov, Physical Foundations of Cosmology (Cambridge University Press, Oxford, 2005).
- J. Martin, C. Ringeval, and V. Vennin, J. Cosmol. Astropart. Phys. 07 (2024) 087.
- A. A. Starobinsky, Adv. Ser. Astrophys. Cosmol. 3, 130 (1987).
- B. Whitt, Phys. Lett. 145B, 176 (1984).
- Y. Ema, Phys. Lett. B 770, 403 (2017).
- See Supplemental Material at http://link.aps.org/supplemental/10.1103/k7ty-gwjg for the scalar and tensor power spectra predicted by Starobinsky inflation, the impact of dark radiation on , and the derivation showing that kination fluctuations behave as radiation, which includes Ref. [86].
- M. Cielo, M. Escudero, G. Mangano, and O. Pisanti, Phys. Rev. D 108, L121301 (2023).
- P. Peter and J.-P. Uzan, Primordial Cosmology, Oxford Graduate Texts (Oxford University Press, New York, 2013).
- J. Martin, C. Ringeval, and V. Vennin, Europhys. Lett. 148, 29002 (2024).
- C. Caprini and D. G. Figueroa, Classical Quantum Gravity 35, 163001 (2018).
- S. Navas et al. (Particle Data Group), Phys. Rev. D 110, 030001 (2024).
- C. Pitrou, A. Coc, J.-P. Uzan, and E. Vangioni, Phys. Rep. 754, 1 (2018).
- D. J. Brooker, Mod. Phys. Lett. A 34, 1950131 (2019).
- N. K. Stein and W. H. Kinney, J. Cosmol. Astropart. Phys. 03 (2023) 027.
- J. P. Conlon and F. Quevedo, J. High Energy Phys. 01 (2006) 146.
- J. Martin, C. Ringeval, and V. Vennin, Phys. Dark Universe 5–6, 75 (2014).
- D. Baumann, Cosmology (Cambridge University Press, Cambridge, England, 2022).
We have checked with osmoattice [98, 99] that the scalar field energy density redshifts like radiation in the non-linear regime where the gradient energy density becomes comparable to the kinetic energy density. The details will be reported in the companion paper [100].
- D. G. Figueroa, A. Florio, F. Torrenti, and W. Valkenburg, J. Cosmol. Astropart. Phys. 04 (2021) 035.
- D. G. Figueroa, A. Florio, F. Torrenti, and W. Valkenburg, Comput. Phys. Commun. 283, 108586 (2023).
- C. Eröncel et al. (2025).
- K. Redmond, A. Trezza, and A. L. Erickcek, Phys. Rev. D 98, 063504 (2018).
- P. J. Peebles, The Large-Scale Structure of the Universe (Princeton University Press, Princeton, NJ, 1980).
- F. Bernardeau, S. Colombi, E. Gaztanaga, and R. Scoccimarro, Phys. Rep. 367, 1 (2002).
Prior to our Letter, the instability of kination had been demonstrated in the context of oscillating scalar condensates [105] where the fluctuations arise from the fragmentation of the scalar field rather than being sourced by curvature perturbations.
- K. D. Lozanov and M. A. Amin, Phys. Rev. D 97, 023533 (2018).
- K. N. Abazajian et al. (CMB-S4 Collaboration), arXiv:1610.02743.
- C. Dvorkin et al., in Proceedings of the US Community Study on the Future of Particle Physics (Snowmass 2021) (2022), https://inspirehep.net/conferences/1803127?ui-citation-summary=true.
In addition to those originating from adiabatic curvature fluctuations, kination fluctuations could also arise from isocurvature perturbations, which, however, depend on the scalar field dynamics during inflation and are left for future study.
- C. Eröncel, Y. Gouttenoire, R. Sato, G. Servant, and P. Simakachorn, arXiv:2503.04880.
- A. Bodas, R. T. Co, A. Ghalsasi, K. Harigaya, and L.-T. Wang, arXiv:2503.04888.