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Phantom fluid cosmology: Impact of a phantom hidden sector on cosmological observables

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arxiv 2308.12989 v2 pith:7R5HSSYX submitted 2023-08-24 hep-ph astro-ph.CO

Phantom fluid cosmology: Impact of a phantom hidden sector on cosmological observables

classification hep-ph astro-ph.CO
keywords phantomcosmologicaldarkfluidvacuumcauseconstraintscosmology
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Phantom scalar theories are widely considered in cosmology, but rarely at the quantum level, where they give rise to negative-energy ghost particles. These cause decay of the vacuum into gravitons and photons, violating observational gamma-ray limits unless the ghosts are effective degrees of freedom with a cutoff $\Lambda$ at the few-MeV scale. We update the constraints on this scale, finding that $\Lambda \lesssim 19$ MeV. We further explore the possible coupling of ghosts to a light, possibly massless, hidden sector particle, such as a sterile neutrino. Vacuum decays can then cause the dark matter density of the universe to grow at late times. The combined phantom plus dark matter fluid has an effective equation of state $w < -1$, and functions as a new source of dark energy. We derive constraints from cosmological observables on the rate of vacuum decay into such a phantom fluid. We find a mild preference for the ghost model over the standard cosmological one, and a modest amelioration of the Hubble and $S_8$ tensions.

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Cited by 2 Pith papers

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  1. UV-complete and stable Quintom Dark Energy models in the light of DESI DR2

    hep-ph 2026-03 unverdicted novelty 6.0

    Quintom dark energy is UV-completed in 5D NPGHU, producing a modified Quintom-B model whose massive gauge ghost fits DESI with negligible fine-tuning and remains stable for Λ ~ O(10)H0.

  2. UV-complete and stable Quintom Dark Energy models in the light of DESI DR2

    hep-ph 2026-03 reject novelty 6.0

    A 5D lattice gauge model is presented as the first UV-completion of Quintom dark energy, claiming DESI-compatible phantom crossing with stability, but the model's field amplitude makes its dark-energy density negligible.