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Negentropy as Diagnostic of Cosmic Density Fields and Dynamical Dark Energy Models

Suman Sarkar

TL;DR

This work introduces negentropy as an information-theoretic scalar to quantify non-Gaussianity in the cosmic density field and to probe dynamical dark energy models. By linking differential entropy of Gaussian and log-normal density fields, and by extending to discrete galaxy distributions with nonlinear bias, the authors define $J(a)$ and its derivatives $\Gamma_1(a)$ and $\Gamma_2(a)$ to track structure formation across cosmic time. They identify characteristic epochs $z_{NG}$ and $z_{TA}$, showing ΛCDM values of $z_{NG}\approx0.81$ and $z_{TA}\approx0.18$, and demonstrate thatnegentropy discriminates between thawing, freezing, and phantom dark-energy scenarios, with BA parametrisation providing particularly tight constraints. The paper also develops a Fisher-matrix framework to forecast DE parameter constraints from negentropy, highlighting that $\Gamma_2(a)$ yields the strongest, least-correlated constraints and pinpointing pivot redshifts around $z_p\sim0.1$–$0.2$, suggesting practical pathways for applying this approach to upcoming surveys and simulations.

Abstract

We employ negentropy ($J$), defined as the difference between the information content of a non-Gaussian probability distribution and a Gaussian with identical variance, as an information-theoretic probe of non-Gaussianity in the cosmic density field. We quantify its sensitivity to dynamical dark energy by studying the evolution of $J(a)$ and its derivatives $Γ_1(a)$ and $Γ_2(a)$ across three parameterisation schemes: CPL, JBP, and BA. We determine the characteristic redshift $z_{NG}$, marking the epoch of maximal non-Gaussian structure formation, and the turnaround redshift $z_{TA}$, when information production transitions due to dark-energy domination, finding $z_{NG}\sim0.81$ and $z_{TA}\sim0.18$ for $Λ$CDM. Our diagnostics clearly discriminate between thawing and freezing quintessence models and phantom dark energy at low redshifts. Thawing models show small departures from $Λ$CDM, freezing models display higher $z_{TA}$, while phantom models exhibit lower $z_{TA}$, reflecting late-time evolution. We provide a practical prescription for measuring negentropy from discrete galaxy distributions, establishing a framework that can be applied to simulations and observations. This information-theoretic approach offers a robust and complementary tool for probing dark energy dynamics, enabling sensitive discrimination between evolving and cosmological-constant scenarios.

Negentropy as Diagnostic of Cosmic Density Fields and Dynamical Dark Energy Models

TL;DR

This work introduces negentropy as an information-theoretic scalar to quantify non-Gaussianity in the cosmic density field and to probe dynamical dark energy models. By linking differential entropy of Gaussian and log-normal density fields, and by extending to discrete galaxy distributions with nonlinear bias, the authors define and its derivatives and to track structure formation across cosmic time. They identify characteristic epochs and , showing ΛCDM values of and , and demonstrate thatnegentropy discriminates between thawing, freezing, and phantom dark-energy scenarios, with BA parametrisation providing particularly tight constraints. The paper also develops a Fisher-matrix framework to forecast DE parameter constraints from negentropy, highlighting that yields the strongest, least-correlated constraints and pinpointing pivot redshifts around , suggesting practical pathways for applying this approach to upcoming surveys and simulations.

Abstract

We employ negentropy (), defined as the difference between the information content of a non-Gaussian probability distribution and a Gaussian with identical variance, as an information-theoretic probe of non-Gaussianity in the cosmic density field. We quantify its sensitivity to dynamical dark energy by studying the evolution of and its derivatives and across three parameterisation schemes: CPL, JBP, and BA. We determine the characteristic redshift , marking the epoch of maximal non-Gaussian structure formation, and the turnaround redshift , when information production transitions due to dark-energy domination, finding and for CDM. Our diagnostics clearly discriminate between thawing and freezing quintessence models and phantom dark energy at low redshifts. Thawing models show small departures from CDM, freezing models display higher , while phantom models exhibit lower , reflecting late-time evolution. We provide a practical prescription for measuring negentropy from discrete galaxy distributions, establishing a framework that can be applied to simulations and observations. This information-theoretic approach offers a robust and complementary tool for probing dark energy dynamics, enabling sensitive discrimination between evolving and cosmological-constant scenarios.
Paper Structure (21 sections, 57 equations, 5 figures, 4 tables)

This paper contains 21 sections, 57 equations, 5 figures, 4 tables.

Figures (5)

  • Figure 1: This figure shows the growth of perturbations in the matter density field and the evolution of differential entropy and negentropy associated with it.
  • Figure 2: The evolution of negentropy estimated for the 3 different parametrisation schemes, for different dark energy models with chosen values of ($w_0$,$w_a$) from Set I (\ref{['tab:w0wa_grid']}). The solid curved lines with different colours represent different physical models of dark energy. The colour coding is done as: {Black:$\Lambda$CDM; Red:Quintessence; Blue:Thawing; Purple:Freezing; Gold:Phantom }
  • Figure 3: Same as \ref{['fig:evol_J_dde_set1']} but for the choice of parameters from Set II, having larger departure from $\Lambda$CDM compared to Set I.
  • Figure 4: Same as \ref{['fig:evol_J_dde_set1']} and \ref{['fig:evol_J_dde_set2']} but for the choice of parameters from Set III, having larger departure from $\Lambda$CDM compared to both Set I and Set II.
  • Figure 5: The contour plots display the Fisher forecast constraints in the ($w_0$,$w_a$) plane, illustrating the sensitivity of $J(a)$, $\Gamma_1(a)$ and $\Gamma_2 (a)$ to the dark energy parameters. Different colours correspond to different dark energy parametrisations. The confidence regions around the fiducial model ($w_0=-1$,$w_a=0$) are shown at $1\sigma$, $2\sigma$ and $3\sigma$ confidence levels, with decreasing opacity.