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Test of parametrized post-Newtonian gravity with galaxy-scale strong lensing systems

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arxiv 1701.00357 v1 pith:6BWIQ7O7 submitted 2017-01-02 astro-ph.CO

Test of parametrized post-Newtonian gravity with galaxy-scale strong lensing systems

classification astro-ph.CO
keywords gammaparameterconstraintcurvaturefoundfuturegalaxy-scalelensing
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Based on a mass-selected sample of galaxy-scale strong gravitational lenses from the SLACS, BELLS, LSD and SL2S surveys and using a well-motivated fiducial set of lens-galaxy parameters we tested the weak-field metric on kiloparsec scales and found a constraint on the post-Newtonian parameter $\gamma = 0.995^{+0.037}_{-0.047}$ under the assumption of a flat $\Lambda$CDM universe with parameters taken from \textit{Planck} observations. General relativity (GR) predicts exactly $\gamma=1$. Uncertainties concerning the total mass density profile, anisotropy of the velocity dispersion and the shape of the light-profile combine to systematic uncertainties of $\sim 25\%$. By applying a cosmological model independent method to the simulated future LSST data, we found a significant degeneracy between the PPN $\gamma$ parameter and spatial curvature of the Universe. Setting a prior on the cosmic curvature parameter $-0.007< \Omega_k <0.006$, we obtained the following constraint on the PPN parameter: $\gamma=1.000^{+0.0023}_{-0.0025}$. We conclude that strong-lensing systems with measured stellar velocity dispersions may serve as another important probe to investigate validity of the GR, if the mass-dynamical structure of the lensing galaxies is accurately constrained in the future lens surveys.

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  1. Testing General Relativity on Galactic Scales via DESI-BAO and Strong Lensing: Circumventing Assumptions on the Hubble Constant, Sound Horizon, and Dark Energy

    astro-ph.CO 2026-03 conditional novelty 5.5

    Model-independent BAO+strong-lensing analysis yields γ_PPN ≈ 1.10–1.15 (P1) and 1.32–1.49 (P2), consistent with GR at 1–2.5σ depending on the lens mass model.