Constraints on dark matter-dark energy interaction from strong lensing ✛ ✎ ✦

Original: "Strong gravitational lensing constraints on interacting dark energy models"
arXiv:2607.04460 · 2026-07-05 · arXiv non-exclusive · independent analysis · 3 min
Analysis of strong gravitational lensing data points to a strong interaction between dark matter and dark energy, capable of easing the Hubble tension.

Context

The standard ΛCDM cosmological model, based on Einstein's field equations, is supported by observations of the cosmic microwave background and supernovae, but faces the cosmic coincidence puzzle — why are the densities of dark matter (whose existence was proved by Vera Rubin) and dark energy comparable today? Another problem is the Hubble tension: the discrepancy in the expansion rate of the universe between early (Planck) and late universe (supernovae of Adam Riess) measurements. The hypothesis of interaction between the dark components, proposed to alleviate these contradictions, involves an energy exchange that can synchronize their evolution.

Methods

The scientists combined two complementary datasets of strong gravitational lensing: a sample of 143 lenses on early-type galaxies (measuring velocity dispersion, Einstein radius, redshifts of lens and source) and a system of 28 multiple images from 12 families in the Abell 1689 cluster, captured by the Hubble telescope. For the galaxies, the observed ratio of angular diameter distances Dls/Ds was compared with the theoretical one derived from the Friedmann equations for the interacting model, within the singular isothermal sphere approximation. The cluster mass was reconstructed simultaneously with cosmological parameters by minimizing the deviations of image positions. The search for the best-fit values (Ωdm0, β) was performed using a Bayesian Monte Carlo method with Markov chains in the LENSTOOL software package.

Results

The joint analysis yielded a dark matter density parameter Ωdm0 = 0.253+0.018-0.004 and a coupling constant β = -0.83+0.10-0.08. The negative sign of β indicates an energy transfer from dark energy to dark matter, which accelerates the dilution of the latter and sustains a perpetually accelerating expansion. The reconstructed expansion history H(z) lies systematically below standard ΛCDM at intermediate and high redshifts, while remaining consistent with cosmic chronometer data within 3σ. The transition to acceleration, defined by q(zt)=0, occurs at zt = 2.33 — significantly earlier than in ΛCDM (zt ≈ 0.64), indicating the deep influence of interaction on the dynamics of cosmological expansion.

Implications

The results strengthen the hypothesis that interaction in the dark sector could be a real physical process, not just a mathematical trick. Such a strong negative coupling challenges the standard picture and calls for a revision of structure growth models, since the additional energy influx into matter affects the evolution of density perturbations. Moreover, gravitational lensing confirms its status as a powerful cosmological probe, capable of competing with traditional methods.

Future development

The topic can advance by including data from other probes — supernovae, baryon acoustic oscillations, cosmic microwave background — for cross-checking and parameter refinement. Full-scale hydrodynamical simulations incorporating the interaction will be needed to compare predictions with observations of large-scale structure. Future sky surveys, such as Euclid and the Rubin Observatory, will significantly increase lens samples, improving sensitivity to subtle effects.

Impact

The work impacts cosmology, gravitational lens astrophysics, and modified gravity theories, offering a new independent method for testing fundamental interactions on cosmological scales.

Next steps

Next steps involve incorporating weak lensing and cluster abundance data, as well as perturbation analysis to predict the matter power spectrum in interacting models.

Key open problems

The research is directly related to unsolved problems in modern physics: the Hubble tension and the cosmic coincidence problem. It also touches on fundamental questions about the nature of dark matter and dark energy.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The authors combined strong lensing data from 143 early-type galaxies and the cluster Abell 1689 to constrain the parameters of a model with interacting dark matter and dark energy. A Bayesian analysis yielded a negative coupling constant, indicating energy transfer from dark energy to dark matter, and a transition to accelerated expansion at z≈2.33, significantly earlier than in ΛCDM.

Where its strength is

This work shows how combining two complementary sets of lensing data yields strong constraints on the interaction in the dark sector, and reveals a notable difference in the expansion history compared to the standard model.

Where it could go next

Worth trying

  • Test whether the negative sign of β persists when cosmic chronometer data are included in the joint analysis.
  • Apply the interacting model to a sample of lenses with measured velocity dispersions to break the degeneracy between parameters.
  • Compare the reconstructed H(z) history with predictions from a model where dark energy has a variable equation of state to identify differences.

Why this may matter

If the interaction in the dark sector is confirmed, it would point to new physics beyond ΛCDM and help explain the accelerated expansion of the universe without invoking a cosmological constant.

The idea of the interaction switching direction resembles a cosmic 'breathing cycle,' in which dark energy alternately gives and takes energy — akin to a mythical ouroboros, but in this model, a unidirectional flow from energy to matter dominates.

In Greg Egan's novel 'Schild's Ladder', vacuum physics and dark energy turn out to be dynamic and capable of phase transitions, which resonates with the idea of an interacting dark sector, where the evolution of the Universe could abruptly change when the sign of the coupling flips.

\dot{\rho}_{\mathrm{dm}} + 3H\rho_{\mathrm{dm}} = Q, \quad \dot{\rho}_{\mathrm{de}} + 3H(\rho_{\mathrm{de}}+p_{\mathrm{de}}) = -Q
The rate of change of the density of each component, taking into account the energy exchange Q.
Q = 3\beta H q \rho_{\mathrm{dm}}
The energy flow is proportional to the dark matter density, the Hubble constant, and the deceleration parameter q.
E(z)^2 = \frac{\Omega_{\mathrm{dm}0} (1+z)^{3(1+\beta)} + (1-\Omega_{\mathrm{dm}0})}{1+\beta}
Defines the expansion evolution as a function of redshift. (The exact expression is more complex, but this captures the essence).

Key numbers

  • Ω_dm0: 0.253 (+0.018/-0.004)
  • β: -0.83 (+0.10/-0.08)
  • z_t for IDE: 2.33
  • z_t for ΛCDM: 0.64
  • number of lens galaxies: 143
Scientists
Fritz ZwickyAlan GuthAlexander FriedmannAndrei LindeGeorges LemaîtreJames Peebles
Concepts
interaction model weak lensing gravitational lensing analysis dark energy black hole interaction dark energy gravitational microlensing coherence time axion detection large-scale structure of the universe quintessence axion photon coupling expansion of the universe Hubble Space Telescope microlensing gravity quantum gravity and symmetry neural network galaxy mapping cosmic acceleration deceleration direct detection experiments fritz zwicky