English

Redshift drift exploration for interacting dark energy

Cosmology and Nongalactic Astrophysics 2015-08-06 v2

Abstract

By detecting redshift drift in the spectra of Lyman-α\alpha forest of distant quasars, Sandage-Loeb (SL) test directly measures the expansion of the universe, covering the "redshift desert" of 2z52 \lesssim z \lesssim5. Thus this method is definitely an important supplement to the other geometric measurements and will play a crucial role in cosmological constraints. In this paper, we quantify the ability of SL test signal by a CODEX-like spectrograph for constraining interacting dark energy. Four typical interacting dark energy models are considered: (i) Q=γHρcQ=\gamma H\rho_c, (ii) Q=γHρdeQ=\gamma H\rho_{de}, (iii) Q=γH0ρcQ=\gamma H_0\rho_c, and (iv) Q=γH0ρdeQ=\gamma H_0\rho_{de}. The results show that for all the considered interacting dark energy models, relative to the current joint SN+BAO+CMB+H0H_0 observations, the constraints on Ωm\Omega_m and H0H_0 would be improved by about 60\% and 30--40\%, while the constraints on ww and γ\gamma would be slightly improved, with a 30-yr observation of SL test. We also explore the impact of SL test on future joint geometric observations. In this analysis, we take the model with Q=γHρcQ=\gamma H\rho_c as an example, and simulate future SN and BAO data based on the space-based project WFIRST. We find that in the future geometric constraints, the redshift drift observations would help break the geometric degeneracies in a meaningful way, thus the measurement precisions of Ωm\Omega_m, H0H_0, ww, and γ\gamma could be substantially improved using future probes.

Keywords

Cite

@article{arxiv.1501.03874,
  title  = {Redshift drift exploration for interacting dark energy},
  author = {Jia-Jia Geng and Yun-He Li and Jing-Fei Zhang and Xin Zhang},
  journal= {arXiv preprint arXiv:1501.03874},
  year   = {2015}
}

Comments

6 pages, 5 figures; accepted for publication in EPJC. arXiv admin note: text overlap with arXiv:1407.7123

R2 v1 2026-06-22T08:03:10.231Z