Skip to content
DraconiticResearch
Search Sources API
206,690 studies31 sourcesUpdated 36 min ago
PreprintarXiv licencearXiv

Gravitational Production of Non-minimally Coupled Vector Dark Matter in Warm Inflation

Abstract

We study the purely gravitational production of a massive vector dark matter with a non-minimal coupling to the Einstein tensor, ξGμνXμXν, in warm inflation. The background, V=λϕ4 with a dissipation coefficient linear in temperature, is constrained by CMB observations and parametrized by the dissipation ratio 10−4≤ Q0≤1. We consider both unavoidable production channels: freeze-in from the Standard Model bath through graviton exchange, and cosmological gravitational particle production (CGPP). For freeze-in, we compute the scattering amplitudes including the contact interaction induced by ξ, which enhances the production of light dark matter through the longitudinal mode and suppresses that of heavy dark matter through destructive interference. For CGPP, the slow-roll parameter is not small during warm inflation, which enhances the production of light dark matter by up to three orders of magnitude relative to cold inflation. Combining both channels, CGPP excludes most of the light freeze-in branch, leaving mX≲2.4×10−5 GeV, a narrow window around 1010 GeV for strong dissipation, and mX≳1014--1015 GeV. Only the heavy branch remains viable for all |ξ|≲1.

Related

  1. Gravitational Dark Matter Production from Spectator Field in R2-Higgs Inflation
    Arnab Samanta, Rajesh Mondal, Tanmoy Modak
    arXivPreprintarXiv licenceFull textCosmologyHigh-energy & particle physicsarXiv
  2. Inflationary models in a minimally coupled f(R,T) gravity: Constraints from Planck, BICEP/Keck, and ACT
    Biswajit Deb, Atri Deshamukhya
    New AstronomyPeer-reviewedLicence not statedFull text7 citedCosmologyOpenAlex
  3. Reconciling nonminimally coupled Higgs inflation with ACT DR6 observations through reheating
    Lang Liü, Zhu Yi, Yungui Gong
    Science China Physics Mechanics and AstronomyPeer-reviewedLicence not statedFull text75 citedCosmologyOpenAlex
  4. Gravitational Waves from New Inflation
    Naoya Kitajima, Kamil Mudrunka, Kazunori Nakayama
    arXivPreprintCC BY 4.0Full textCosmologyGravitation & general relativityarXiv
  5. Primordial black holes and gravitational waves from aligned axion inflation
    Nadir Ijaz
    arXivPreprintarXiv licenceFull textCosmologyHigh-energy & particle physicsarXiv
BibTeX
@misc{sereewat2026gravitational,
  title = {{Gravitational Production of Non-minimally Coupled Vector Dark Matter in Warm Inflation}},
  author = {Phongsakorn Sereewat},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.10090},
  eprint = {2611.10090},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.10090},
}
RIS
TY  - UNPB
TI  - Gravitational Production of Non-minimally Coupled Vector Dark Matter in Warm Inflation
AU  - Phongsakorn Sereewat
PY  - 2026
DA  - 2026/11/06
PB  - arXiv
DO  - 10.48550/arxiv.2611.10090
UR  - https://arxiv.org/abs/2611.10090
AB  - We study the purely gravitational production of a massive vector dark matter with a non-minimal coupling to the Einstein tensor, ξG_μνX^μX^ν, in warm inflation. The background, V=λϕ^4 with a dissipation coefficient linear in temperature, is constrained by CMB observations and parametrized by the dissipation ratio 10^−4≤ Q_0≤1. We consider both unavoidable production channels: freeze-in from the Standard Model bath through graviton exchange, and cosmological gravitational particle production (CGPP). For freeze-in, we compute the scattering amplitudes including the contact interaction induced by ξ, which enhances the production of light dark matter through the longitudinal mode and suppresses that of heavy dark matter through destructive interference. For CGPP, the slow-roll parameter is not small during warm inflation, which enhances the production of light dark matter by up to three orders of magnitude relative to cold inflation. Combining both channels, CGPP excludes most of the light freeze-in branch, leaving m_X≲2.4×10^−5 GeV, a narrow window around 10^10 GeV for strong dissipation, and m_X≳10^14--10^15 GeV. Only the heavy branch remains viable for all |ξ|≲1.
ER  -