Two related preprints from Astrophysics Letters describe “running vacuum” scenarios in which vacuum energy is not constant but changes with the universe’s expansion. In the running vacuum model (RVM), quantum field theory in curved spacetime makes the vacuum energy density, ρ_vac (equivalently Λ/8πG), a function of the Hubble rate H and its time derivatives. In the late universe, the models predict a very slow evolution of vacuum energy, typically of order δρ_vac ~ O(m_Pl^2 H^2), which is presented as a possible origin of dark energy as dynamical vacuum energy rather than a rigid cosmological constant. For the early universe, the preprints state that vacuum fluctuations can generate higher even powers of H, such as H^4, that drive a short period of fast inflation when H is large and approximately constant; the mechanism is described as “RVM-inflation” and does not require an inflaton field. One preprint also studies how an exact de Sitter vacuum decays into a radiation-dominated FLRW phase and argues this supports a “graceful exit,” with subleading ~H^2 contributions easing the transition. The papers frame the approach as a unified quantum field theory description of inflation and dark energy with potential observational implications.
Running vacuum models propose dynamical vacuum energy unifying inflation and dark energy
Two related preprints from Astrophysics Letters describe “running vacuum” scenarios in which vacuum energy is not constant but changes with the universe’s expansion. In the running vacuum model (RVM),...
- Running vacuum models treat vacuum energy density ρ_vac as a function of the Hubble rate H and its derivatives (ρ_vac = ρ_vac(H, Ḣ, …)).
- The late-time vacuum energy evolves slowly, with a typical estimate δρ_vac of order m_Pl^2 H^2.
- In the early universe, quantum fluctuations can generate higher even powers of H (e.g., H^4) that drive a short, fast inflationary phase where H is approximately constant.
- The proposed inflation mechanism does not require an inflaton field; it arises from quantum effects on a dynamical background.
- One study models decay from an exact de Sitter vacuum to a radiation-era FLRW universe and links it to a graceful exit via subleading ~H^2 contributions.
arXiv:2601.05218v3 Announce Type: replace-cross Abstract: Inflation is a necessary cosmic mechanism to cure basic inconsistencies of the standard model of cosmology. These problems are usually `fixed' by postulating the existence of a scalar field (called the ``inflaton''). However, other less ad hoc options are possible. In the running vacuum model (RVM) framework, the vacuum energy density (VED) $\rho_{\rm vac}$ is a function of the Hubble rate $H$ and its time derivatives. In this context, the VED is dynamical (there is no rigid cosmological constant $\Lambda$). In the FLRW epoch, $\rho_{\rm vac}$ evolves very slowly with expansion. In contrast, in the very early universe the vacuum fluctuations induce higher powers $H^N$ capable of unleashing fast inflation in a short period in which $H\simeq$ const. We call this mechanism `RVM-inflation'. It does not require an inflaton field since inflation is brought about by pure quantum field theory (QFT) effects on the dynamical background. It is different from Starobinsky's inflation, in which $H$ is never constant. In this work, we study a closely related scenario: the decay of the exact de Sitter vacuum into FLRW spacetime in its radiation epoch and the subsequent impact on the current universe, and compare with the RVM. We find that in both cases inflation is driven by $H^4$ powers together with subleading contributions of order $H^2$ that ease a graceful-exit transition into the radiation-dominated epoch, where the FLRW regime starts and ultimately develops a mildly evolving VED in the late universe: $\delta\rho_{\rm vac}\sim {\cal O}(m_{\rm Pl} ^2 H^2)$. The proposal presented here aims at a unified QFT approach to inflation and dark energy (conceived as dynamical vacuum energy) with potentially measurable phenomenological consequences in the present universe, and constitutes a first step toward establishing its full theoretical and phenomenological consistency.
2 hours agoarXiv:2606.05352v2 Announce Type: replace-cross Abstract: The concordance $\Lambda$CDM model, based on a rigid $\Lambda$-term for the entire cosmic history, has been in crisis for a long time. In our expanding Universe, an evolving $\Lambda$ with the expansion is intuitively much more reasonable. In the running vacuum model (RVM) framework, based on quantum field theory (QFT) in curved spacetime, quantum effects induce a vacuum energy density (VED) $\rho_{\rm vac}=\Lambda/(8\pi G)$ which is a function of the Hubble rate $H$ and its time derivatives, $\rho_{\rm vac}=\rho_{\rm vac}(H, \dot{H},\ddot{H},\dots)$. Currently, $\rho_{\rm vac}$ evolves very slowly with the expansion, $\delta\rho_{\rm vac}\sim {\cal O}(m_{Pl} ^2 H^2)$, and this fact provides a possible fundamental origin of dark energy (DE), conceived as dynamical vacuum energy. In the RVM, Newton's $G$ is also evolving, but much more slowly (logarithmically with $H$): $G=G(\ln H)$. In the very early universe, the vacuum fluctuations induce higher (even) powers, e.g. $\sim H^4$, capable of triggering fast inflation in a very short period, in which $H$ is very large and approximately constant. This is the mechanism of `RVM-inflation'. It does not require an `inflaton' field since inflation is brought about by pure QFT effects on the dynamical background. It differs from Starobinsky's inflation, where $H$ is never constant. Furthermore, the dynamics of $\rho_{\rm vac}(H)$ and $G(H)$ can also have implications on the frequently discussed possibility that the fundamental `constants' of Nature can be mildly evolving with the cosmic expansion. Putting things together, a unified QFT framework of dark energy and inflation ensues as a realistic theory for the description of the universe as a whole on fundamental grounds. In it, dynamical VED is predicted and is much welcomed, since it fits in with current DESI measurements, preferring dynamical DE over a rigid $\Lambda$ term.
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