Skip to main content

Anomalous Running Gravity

 

How running gravity, anomaly-driven vacuum energy, and quantum error correction combine to explain cosmic tensions, while preserving ΛCDM

Generated image 


 ΛCDM fits the CMB, large-scale structure, and nucleosynthesis exceptionally well.

And yet:

  • The locally measured Hubble constant ($H_0$) is higher than the Planck CMB prediction
  • Weak lensing surveys find lower clustering amplitude ($S_8$) than ΛCDM predicts

These are small but persistent discrepancies.

Rather than discarding ΛCDM, what if these tensions are subtle signals about how vacuum energy and gravity behave dynamically?


1. Core Idea: Mildly Running Gravity

Standard ΛCDM

Vacuum energy is constant: $$\rho_\Lambda = \text{const.}$$

ARG 3.3: Running Gravity with Anomaly Source

In Anomalous Running Gravity (ARG 3.3), we promote vacuum energy and Newton's constant to dynamic quantities sourced by the trace anomaly of quantum fields and a Gauss–Bonnet term:

$$S \supset \int d^4x \sqrt{-g} \frac{b}{(4\pi)^2}\ln\left(\frac{\phi}{\phi_0}\right) E$$

where $E$ is the Euler density.

This naturally generates:

  • Early-time $G$-running near the MeV scale
  • Late-time effects near the dark-energy transition ($z\lesssim 2$)

Gravity compensates to preserve energy conservation:

$$\dot{\rho}_\Lambda + \rho_m \frac{\dot G}{G} \approx 0$$

Present-day variation remains tiny:

$$|\dot G/G|_0 \lesssim 10^{-13}~\mathrm{yr}^{-1}$$

This satisfies local and BBN bounds.


2. Dual-Phase Running

Early Phase

  • MeV-era Gauss–Bonnet source adjusts $G(a)$ near recombination
  • Triggered near matter-radiation equality as relativistic species decouple

Late Phase

  • Braiding and mass evolution tweak expansion at $z\lesssim 2$
  • Emerging from low-energy, IR vacuum fluctuations

Together, they allow $r_d$ and $H_0$ to shift without spoiling the CMB damping tail or BAO geometry.


3. Resolving the Tensions

3.1 Hubble Tension

The late-time evolution modifies effective expansion:

$$H^2 = \frac{8\pi G(a)}{3}(\rho_m+\rho_r+\rho_\Lambda) - H \frac{\dot G}{G}$$

ARG 3.3 produces: $$H_0 \sim 72.5-73.5~\mathrm{km/s/Mpc}$$

without violating the CMB angular scale.


3.2 $S_8$ Tension

Structure growth is suppressed by:

  1. Mildly weaker gravity: $G(a) < G_0$ at intermediate redshifts
  2. Braiding friction: Kinetic mixing between $\phi$ and metric perturbations slows growth

Growth equation: $$\ddot{\delta}_m + \left(2H + \frac{\dot G}{G}\right)\dot{\delta}_m - 4\pi G(a)\rho_m \delta_m = 0$$

Result: $$S_8 \sim 0.75-0.77$$

matching weak-lensing observations.


3.3 Soft ISW Prior: Low-$\ell$ CMB Power

ARG 3.3 enforces a soft prior on braiding vs. Planck mass evolution:

$$\alpha_{\rm B}(z)-\alpha_{\rm M}(z) \sim \mathcal{N}(0, \sigma_\epsilon^2),\quad \sigma_\epsilon \ll 1$$

Effects:

  • Nudges late ISW effect toward zero: $(\Phi+\Psi)' \approx 0$ at $z\lesssim 2$
  • Reduces low-$\ell$ CMB power
  • Generates mild gravitational slip:

$$\eta = \frac{\Phi}{\Psi} \sim 1.02-1.05 \quad \text{at } z \sim 0.5$$

This is a concrete, observable signature.


4. The QEC Connection

Spacetime as Quantum Error Correction

Recent advances suggest spacetime itself is a quantum code:

Key Ideas:

  • Logical qubits encode geometry
  • Expansion generates new degrees of freedom
  • Dark energy = thermodynamic cost of error correction

Landauer energy for erasing errors: $$\rho_{\rm vac}^{\rm QEC} \sim \frac{k_B T \ln 2 , N_{\rm qubits}(z)}{V_{\rm Hubble}(z)}$$


ARG 3.3 ↔ QEC Correspondence

ARG 3.3 QEC Interpretation
Dual-phase vacuum $\rho_{\rm vac}(z)$ Landauer cost of refreshing qubits at two epochs
Running $G(z)$ Feedback from maintaining coherence
Growth suppression Friction from computational energy cost
Late-time $H_0$ enhancement Faster local "refresh rate"

Emergent Viscoelasticity

From the QEC perspective:

Bulk viscosity from error correction: $$\zeta(z) \sim \frac{k_B T \ln 2}{\tau_{\rm QEC}} \frac{dN_{\rm qubits}}{dV}$$

Shear stress with finite relaxation: $$\pi_{\mu\nu}(z, \omega) = - \frac{2 \eta}{1 - i \omega \tau_{\rm QEC}} \sigma_{\mu\nu}$$

Stochastic stress from quantum fluctuations during syndrome readout produces effective local noise.


Topological Protection

QEC codes are inherently topological:

$$\Lambda_{\rm top} \sim \frac{\text{Code distance}}{V_{\rm Hubble}}$$

Key features:

  • ARG 3.3's dual-phase behavior naturally constrained by topological stability
  • Ensures small ~5–8% $G$ variation without fine-tuning
  • Large code distance → stable cosmological constant → $w \approx -1$
  • Berry phase holonomy suppresses quantum corrections

5. Microscopic Interpretation: Entropy Flow

ARG 3.3 can be interpreted as geometric information processing:

Hubble horizon entropy: $$S_H = \frac{\pi}{G H^2}$$

Thermodynamic relation: $$dE = T_H dS_H$$

QEC viewpoint:

  • Spacetime encodes geometric information non-locally
  • Expansion increases effective qubits
  • Maintaining coherence produces friction
  • Maps onto running vacuum energy and growth suppression

6. Unified Einstein Equation

$$\boxed{G_{\mu\nu} + \Lambda_{\rm top} g_{\mu\nu} = 8\pi G(z) T_{\mu\nu}^{\rm matter} + 8 \pi G(z) \xi_{\mu\nu}^{\rm QEC}(z)}$$

Components:

  • ARG 3.3 dual-phase vacuum ↔ $\rho_{\rm vac}(z)$
  • Running $G(z)$ ↔ computational feedback
  • Growth suppression ↔ local QEC overhead
  • Viscous effects ↔ emergent mesoscopic stress
  • Topological Berry phase ↔ global protection of $\Lambda$

7. ΛCDM as a Special Limit

ARG 3.3 reduces to ΛCDM when:

$$\alpha_{\rm B} = \alpha_{\rm M} = 0, \quad b = 0, \quad \Delta G(a) = 0$$

Key point: All local tests, CMB physics, and large-scale structure are preserved.

This is a conservative extension, not a radical alternative.


8. Observable Signatures

What We Predict

Hubble tension:

  • Slightly higher $H_0$ from SN Ia anchors
  • Local variations with cosmic web density

$S_8$ suppression:

  • Mild gravitational slip
  • Braiding friction slows growth

ISW effect:

  • Reduced low-$\ell$ power in CMB

Gravitational slip:

  • $\eta(z)\neq 1$ at intermediate redshifts
  • Testable with weak lensing

Gravitational waves:

  • Frequency-dependent damping from QEC shear viscosity

Dark energy stability:

  • Naturally protected by topological code distance

9. The Bottom Line

ARG 3.3 + QEC provides:

First-principles, anomaly-driven mechanism for mild vacuum-energy running

Newton's constant adjusts slightly to maintain conservation

Naturally produces:

  • Elevated $H_0$
  • Lower $S_8$
  • Mild gravitational slip
  • Reduced low-$\ell$ ISW power

ΛCDM preserved as the exact infrared fixed point

 Conservative extension with testable predictions


10. Wrap

Three Perspectives, One Framework

Macroscopic (ARG 3.3): Running vacuum energy + running gravity

Mesoscopic (Viscoelastic): Bulk and shear viscosity from quantum coarse-graining

Microscopic (QEC): Computational cost of maintaining spacetime coherence

All three are manifestations of the same underlying physics.


Cosmic tensions may simply be the first glimpses of vacuum energy doing what quantum field theory predicts:

  • Anomaly physics (trace anomaly, Gauss-Bonnet)
  • Geometric information flow (QEC, entropy)

Rather than a crisis for cosmology, these tensions are hints that:

  • Spacetime is computational
  • Gravity is emergent
  • Dark energy is the overhead of maintaining quantum coherence
  • ΛCDM is the noiseless, trivial-topology limit

The universe isn't broken. We're just seeing the computational microstructure for the first time.

Comments

Popular posts from this blog

Blurring the horizon - the quantum width of the cosmic event horizon

A 2021 paper by Zurek applied a random walk argument to a black hole horizon.   Credit, Zurek, 2021 Zurek called this a blurring of the horizon (a fuzzy, or uncertain horizon), and also went through some equivalent derivations, which basically supported the idea this length scale is the quantum uncertainty in the position of the BH horizon, aka a dynamic quantum width of an event horizon (a concept which would therefore also apply to the universe's own CEH). The Bekenstein-Hawking entropy gives the number of quantum degrees of freedom that can fluctuate. Below, we step out our own cosmic de-Sitter derivation of the random walk argument, obtaining the same result as Zurek did, so its certainly correct! \begin{equation} \Delta x^2 =2 DT \end{equation} In this equation, $\Delta x$ is the position uncertainty, $D$ is the Einstein diffusion coefficient and $T$ is the time between measurements (aka the relaxation time).    So, lets look at the Einstein diffusion co...

The Virial Horizon

  In general relativity, defining "energy" is notoriously difficult. A specific point of confusion often arises in de Sitter space: Why is the quasi-local energy of the horizon exactly double the effective gravitational mass? By imposing a fundamental consistency condition— Horizon Uncertainty—we can re-derive the thermodynamics of the de Sitter horizon. We find that the horizon behaves exactly like a quantum-stretched membrane, where the "factor of two" is simply the result of the Virial Theorem applied to spacetime itself. Horizon Position Uncertainty Whether through holographic arguments, diffusion models, or entanglement entropy, a causal horizon is never sharp. Its position fluctuates. The variance of the horizon position $\Delta x^2$  scales with the geometric mean of the Planck length $L_p$ ​ and the horizon radius $l_{\Lambda}$ ​ :  \begin{equation}     \Delta x^2 = L_P \, l_\Lambda, \qquad L_P = \sqrt{\frac{G\hbar}{c^3}} \end{equation}    W...

Our cosmic event horizon on a string

In this post, we introduced the idea that in the presence of a positive cosmological constant, there is a minimum (local) mass $m_{GR}$   McDormand swinging a cosmic light-like mass-energy $m_{GR}$, with a "cosmic string" of radius $l_{\Lambda}$, giving a centripetal force $F_{local}=m_{GR} \ c^2/l_{\Lambda}$.    Let's think about that string for a bit. In fact, a great number of physicists have spent their entire careers tied up unraveling string theory . For a classical string, which lives in D = 10 dimensions, associated with Nambu-Goto action, the the string tension $T_G$ is a local force, or energy per unit length (dimensions $MLT^{-2}$): \begin{equation} \notag T_G = \frac{1}{2\pi \alpha \prime} \end{equation}$\alpha \prime$ is the Regge slope parameter, set here with dimensions of inverse force.  The wavelength of the stringy mass-energy standing wave (such that it does not interfere with itself), is the circumference of the circle, and we know it moves...