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Vacuum Tide: How Cosmic Emptiness Conducts the Universe

Original: "Running Vacuum in the expanding Universe: a unified QFT paradigm for Inflation and Dark Energy"
· Joan Solà Peracaula
The running vacuum model turns quantum ripples of space into a conductor of cosmic evolution: inflation and dark energy are just rhythms of a single vacuum ocean.
Abstract

The standard ΛCDM model with constant dark energy is hitting a wall. In the 'running vacuum' model (RVM), based on quantum field theory in curved spacetime, the vacuum energy density changes with the expansion rate of the Universe (the Hubble parameter). This yields dynamic dark energy—its slow evolution aligns with recent DESI survey data. Moreover, in the early Universe, quantum effects can trigger ultra-fast inflation without the need for a hypothetical inflaton particle. Thus the vacuum, like a stretched membrane whose tension varies over time, becomes a unified explanation for both inflation and the accelerating expansion.

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The cosmic vacuum is not emptiness but a living ocean: its energy swells and subsides, echoing the expansion. Like a lunar tide, vacuum density sensitively responds to Hubble’s tempo—the conductor’s baton of the universe. This “running vacuum” is not frozen: within it pulse quantum fluctuations of all fields—from electronic to hypothetical vortices of Grand Unification.

Classical physics hit a wall: summing zero-point oscillations of fields in flat space yields a terrifying 10^120—many times more than observed dark energy. Pioneers sought a way out. Georges Lemaître in the 1930s linked the cosmological constant to vacuum energy, and after Edwin Hubble’s discovery, it became clear: spacetime breathes. The running vacuum model goes further—it demands calculations in a curved and expanding continuum. Adiabatic renormalization ties the scale to the parameter H, and infinities miraculously cancel, leaving neat H², H⁴ terms... The vacuum ceases to be a catastrophe—it becomes an evolutionary flywheel.

Zero-point oscillations of electromagnetism in flat vacuum are infinite, but in curved spacetime they crystallize into a tiny, tangible quantity—around 10⁻⁴⁷ GeV⁴. Gravity, which created the problem, also solves it: infinity condenses into a fateful droplet.

In the first milliseconds after the Big Bang, when Hubble roared, H⁴ dominated. It became an inflationary hurricane—without any inflaton, it inflated the universe 10²⁶ times, smoothing the horizon and diluting entropy. Today, in the calm of slow expansion, H² rules the dance. It sets the density of dark energy—almost constant, but with a barely perceptible breath. Fresh maps from DESI and the cosmic microwave background catch this rhythm. The vacuum doesn’t just exist—it conducts.

RVM is no elegant abstraction. It is palpable: the gravitational constant G might be drifting—by 10⁻¹³ per year, in harmony with Paul Dirac’s vision. Catching the drift with hyper-precise clocks would rewrite the laws of gravity. A dynamic vacuum also reconciles disputes: where standard ΛCDM cracks in large-scale structure and dark matter data, it sews the edges together. Ahead lie stringy corrections, loops of quantum gravity, with Euclid and Nancy Grace Roman already taking aim.

Today, vacuum energy equals the mass of a couple of protons per cubic meter. But this “pinch” accelerates galaxies and may decide the finale: eternal cold or the crunch of a new Big Bang.

🎯 30 years before the discovery of acceleration, [scientist:Paul Dirac]Paul Dirac[/scientist] suspected G is not constant. The running vacuum model dresses his hunch in rigorous quantum field theory, predicting a drift of about 10⁻¹³ per year—at the edge of sensitivity of modern atomic clocks.

🎬 In Greg Egan’s novel “Quarantine,” the [tag:dark_energy]cosmological constant[/tag] obeys observers—a hint of a living vacuum that responds to the very fabric of reality.

\rho_{\rm vac}(H) \simeq \rho_{\rm vac}^0 + \frac{3\nu_{\rm eff}}{8\pi G_{\rm N}}(H^2 - H_0^2)
Soft dependence on the square of the Hubble parameter via a small coefficient ν_eff
\beta_{\rho_{\rm vac}} = M \frac{\partial \rho_{\rm vac}}{\partial M} \simeq -\frac{3m^2 H^2}{8\pi^2}\left(\xi - \frac{1}{6}\right)
Rate of change of vacuum energy density with renormalization scale; suppressed by factor m^2 H^2
Scientists
Alan GuthAndrei LindeGeorges LemaîtreJames PeeblesAdam RiessBrian Schmidt
Tags
dark energy Quantum Field expansion of the universe spacetime curvature entropy dark matter cosmic microwave background big bang
Laws
Friedmann equationsHubble's lawsecond law of thermodynamicsgravitational lensingNoether's theoremBekenstein-Hawking entropy
Original: arXiv:2606.05352v2 · CC BY · bridge42worlds