EÖEmre Özülker

Emre Özülker

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Emre Özülker has a total of 54 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Open Access

    Exploring the growth-index ( γ ) tension with Λ s CDM

    by Luis A. Escamilla, Özgür Akarsu, Eleonora Di Valentino, Emre Özülker, J. Alberto Vazquez

    Recent observational analyses have revealed a significant tension in the growth index γ , which characterizes the growth rate of cosmic structures. When γ is treated as a free parameter within lambda cold dark matter ( Λ CDM ), the PL 18 + f σ 8 combination yields γ ≈ 0.64 , in ∼ 4 σ tension with the theoretically expected value γ ≈ 0.55 (assuming general relativity), suggesting a preference for suppressed late-time growth relative to the standard expectation. In this work, we investigate whether the Λ s CDM framework—featuring a rapid sign-switching cosmological constant (mirror anti–de Sitter-to-de Sitter (AdS-to-dS) transition) in the late universe at redshift z † ∼ 2 —can alleviate the γ tension together with the H 0 and S 8 tensions. We find that γ Λ s CDM is able to reduce the γ and H 0 tensions relative to γ Λ CDM while maintaining low S 8 values. For PL 18 + f σ 8 , the combination underlying the γ tension, γ Λ s CDM yields z † > 1.58 (95% CL) and reduces the γ and H 0 discrepancies from 3.7 σ and 4.2 σ in γ Λ CDM to 2.1 σ and 1.1 σ , respectively, while leaving χ min 2 essentially unchanged. The largest improvement among the free- z † analyses is obtained for PL 18 + f σ 8 + PP & SH 0 ES , for which the marginalized posterior constraint is z † = 1.8 2 − 0.28 + 0.32 (95% CL); the γ and H 0 tensions are reduced to 1.8 σ and 0.6 σ , respectively, and the model also provides an improved fit to the data. The efficacy of the mechanism is, however, dataset dependent: the standard 3D BAO measurements used in the present analysis—from SDSS-IV/eBOSS and the first year of DESI observations—tend to push the transition to higher redshifts, z † ≳ 2.3 – 2.4 , and weaken the simultaneous alleviation, particularly of the H 0 tension. We also examine the benchmark case with fixed z † = 1.7 , previously identified in studies of the standard ( γ ≃ 0.55 ) Λ s CDM framework as a redshift of interest for alleviating multiple major cosmological tensions—including those in H 0 , M B , and S 8 . For the restricted combinations in which it is considered, this benchmark yields low residual tensions (e.g., a 1.6 σ γ tension and an effectively vanishing H 0 tension for PL 18 + f σ 8 ), albeit with somewhat worse fits than γ Λ CDM . It is, however, excluded at more than 2 σ by the free- z † analyses once either the uncalibrated PantheonPlus SN Ia sample or the 3D BAO data are included. Our results indicate that Λ s CDM can contribute to the joint alleviation of multiple cosmological tensions, although its impact is dataset dependent.

  • Top Cited Papers
    Open Access

    Updated constraints on omnipotent dark energy: A comprehensive analysis with CMB and BAO data

    by Enrico Specogna, Shahnawaz A. Adil, Emre Özülker, Eleonora Di Valentino, Rafael C. Nunes, Özgür Akarsu, Anjan A. Sen

    In this work, we present updated observational constraints on the parameter space of the DMS20 dark-energy model, a member of the (ODE) class. Our analysis combines multiple cosmic microwave background datasets—including measurements from the Planck satellite (PL18), the South Pole Telescope (SPT), and the Wilkinson Microwave Anisotropy Probe (WMAP)—with Type Ia supernova data from the Pantheon + catalog (PP), and baryon acoustic oscillation measurements from the Dark Energy Spectroscopic Instrument and Sloan Digital Sky Survey. We find that certain data combinations, such as SPT + WMAP + BAO and P L 18 + BAO , can reduce the significance of the H 0 tension below 1 σ , but with considerably large uncertainties. However, the inclusion of PP data restores the tension in H 0 . To provide a comprehensive view of the ODE phenomenology, we also investigate the evolution of its energy density, emphasizing its dynamical behavior at low redshifts. Our results generically exhibit multiple phantom divide line crossings in a single expansion history; if confirmed, this points beyond the simplest minimally coupled canonical single-field quintessence/phantom descriptions and motivates more general dark-sector realizations.


  • Top Cited Papers
    Open Access

    The Local Distance Network: A community consensus report on the measurement of the Hubble constant at ∼1% precision

    by Stefano Casertano, Gagandeep Anand, Richard I. Anderson, Rachael Beaton, Anupam Bhardwaj, John P. Blakeslee, Paula Boubel, Louise Breuval, Dillon Brout, Michele Cantiello, et al.

    Context. The direct empirical determination of the local value of the Hubble constant ( H 0 ) has markedly advanced thanks to improved instrumentation, measurement techniques, and distance estimators. However, combining determinations from different estimators is nontrivial due to their correlated calibrations and different analysis methodologies. Aims. Using covariance weighting and leveraging community expertise, we have constructed a rigorous and transparent “Distance Network” to find a consensus value and uncertainty for the locally measured Hubble constant. Methods. Experts across all relevant distance measurement domains were invited to critically review the available datasets spanning parallaxes, detached eclipsing binaries, masers, Cepheids, the tip of the red giant branch, Miras, carbon-rich asymptotic giant branch stars, Type Ia (SNe Ia) and Type II supernovae, surface brightness fluctuations, the fundamental plane, and Tully–Fisher relations. Before any calculations, the group voted for first-rank indicators to define a “baseline” Distance Network. Other indicators were included to assess the robustness and sensitivity of the results. We provide open-source software and data products to support full transparency and future extensions of this effort. Results. Our key findings are as follows: (1) The local H 0 is robustly determined, with first-rank indicators internally consistent within their uncertainties. (2) A covariance-weighted combination yields a relative uncertainty of 1.1% (baseline) or 0.9% (all estimators). (3) The contribution from SNe Ia is consistent across compilations of optical or NIR magnitudes. (4) Removing either Cepheids or the tip of the red giant branch has a minimal effect on the central value of H 0 . (5) Replacing SNe Ia with galaxy-based indicators changes H 0 by less than 0.1 km s −1 Mpc −1 while doubling its uncertainty. (6) The baseline result is H 0 = 73.50 ± 0.81 km s −1 Mpc −1 , 7.1 σ from the early Universe plus ΛCDM result 67.24 ± 0.35 km s −1 Mpc −1 and 5.0 σ from BBN+BAO within a flat ΛCDM DESI DR2 (68.51 ± 0.58 km s −1 Mpc −1 ). Conclusions. A networked approach, such as the one presented here, is invaluable for enabling further progress in Hubble constant measurements, as it provides the much needed advances in accuracy and precision without overreliance on any single method, sample, or group.


  • Open Access

    Do we need wavelets in the late Universe?

    by Luis A. Escamilla, Emre Özülker, Özgür Akarsu, Eleonora Di Valentino, J. A. Vázquez

    We parameterize the Hubble function by adding Hermitian wavelets to the Hubble radius of $Λ$CDM. This allows us to build Hubble functions that oscillate around $Λ$CDM at late times without modifying its angular diameter distance to last scattering. We perform parameter inference and model selection procedures on these new Hubble functions at the background level. In our analyses consisting of a wide variety of cosmological observations, we find that baryon acoustic oscillations (BAO) data play a crucial role in determining the constraints on the wavelet parameters. In particular, we focus on the differences between SDSS- and DESI-BAO datasets and find that wavelets provide a better fit to the data when either of the BAO datasets is present. However, DESI-BAO has a preference for the center of the wavelets to be around $z \sim 0.7$, while SDSS-BAO prefers higher redshifts of $z > 1$. This difference appears to be driven by the discrepancies between these two datasets in their $D_H / r_{\rm d}$ measurements at $z = 0.51$ and $z \sim 2.3$. Finally, we also derive the consequences of the wavelets on a dark energy component. We find that the dark energy density oscillates by construction and also attains negative values at large redshifts ($z\gtrsim2$) as a consequence of the SDSS-BAO data. We conclude that while the early universe and the constraints on the matter density and the Hubble constant remain unchanged, wavelets are favored in the late universe by the BAO data. Specifically, there is a significant improvement at more than $3σ$ in the fit when new DESI-BAO data are included in the analysis.


  • Top Cited Papers

    Omnipotent dark energy: A phenomenological answer to the Hubble tension

    by Shahnawaz A. Adil, Özgür Akarsu, Eleonora Di Valentino, Rafael C. Nunes, Emre Özülker, Anjan A. Sen, Enrico Specogna

    This paper introduces the class of omnipotent dark energy (DE) models characterized by nonmonotonic energy densities that are capable of attaining negative values with corresponding equation of state parameters featuring phantom divide line (PDL) crossings and singularities. These nontrivial features are phenomenologically motivated by findings of previous studies that reconstruct cosmological functions from observations, and the success of extensions of ΛCDM, whose actual or effective DE density is omnipotent, in alleviating the observational discordance within ΛCDM. As an example, we focus on one embodiment of omnipotent DE, viz. the DE parametrization introduced in Di Valentino et al. [Dark energy with phantom crossing and the H0 tension, Entropy 23, 404 (2021)] (DMS20). By updating and extending the datasets used in the original paper where it was introduced, we confirm the effectiveness of DMS20 in alleviating the observational discrepancies. Additionally, we uncover that its negative DE density feature, importance of which was not previously investigated, plays a crucial role in alleviating the tensions, along with the PDL crossing feature that the parametrization presupposes. In particular, we find that there is a positive correlation between the H0 parameter and the scale (ap) at which DE density transitions from negative to positive, in agreement with previous studies that incorporate this transition feature. For our full dataset, the model yields H0=70.05±0.64 (68% CL) relaxing the H0 tension with a preference of crossing to negative DE densities (ap>0 at 99% CL), along with the constraint am=0.922−0.035+0.041 on the scale of the presupposed PDL crossing.


  • Open Access

    Omnipotent dark energy: A phenomenological answer to the Hubble tension

    by Shahnawaz A. Adil, Ozgur Akarsu, Eleonora Di Valentino, Rafael C. Nunes, Emre Ozulker, Anjan A. Sen, Enrico Specogna

    This paper introduces the class of omnipotent dark energy (DE) models characterized by nonmonotonic energy densities that are capable of attaining negative values with corresponding equation of state parameters featuring phantom divide line (PDL) crossings and singularities. These nontrivial features are phenomenologically motivated by findings of previous studies that reconstruct cosmological functions from observations, and the success of extensions of $Λ$CDM, whose actual or effective DE density is omnipotent, in alleviating the observational discordance within $Λ$CDM. As an example, we focus on one embodiment of omnipotent DE, viz., the DE parametrization introduced in Di Valentino et al. [Dark energy with phantom crossing and the H0 tension, Entropy 23, 404 (2021)] (DMS20). By updating and extending the datasets used in the original paper where it was introduced, we confirm the effectiveness of DMS20 in alleviating the observational discrepancies. Additionally, we uncover that its negative DE density feature, importance of which was not previously investigated, plays a crucial role in alleviating the tensions, along with the PDL crossing feature that the parametrization presupposes. In particular, we find that there is a positive correlation between the $H_0$ parameter and the scale ($a_p$) at which DE density transitions from negative to positive, in agreement with previous studies that incorporate this transition feature. For our full dataset, the model yields $H_0=70.05 \pm 0.64$ (68% CL) relaxing the $H_0$ tension with a preference of crossing to negative DE densities ($a_p>0$ at 99% CL), along with the constraint $a_m=0.922^{+0.041}_{-0.035}$ on the scale of the presupposed PDL crossing.

  • Open Access

    Relaxing cosmological tensions with a sign switching cosmological constant: Improved results with Planck, BAO, and Pantheon data

    by Ozgur Akarsu, Suresh Kumar, Emre Ozulker, J. Alberto Vazquez, Anita Yadav

    We present a further observational analysis of the $\Lambda_{\rm s}$CDM model proposed in Akarsu et al. [Phys. Rev. D 104, 123512 (2021)]. This model is based on the recent conjecture suggesting the Universe has transitioned from anti-de Sitter vacua to de Sitter vacua (viz., the cosmological constant switches sign from negative to positive), at redshift ${z_\dagger\sim2}$, inspired by the graduated dark energy model proposed in Akarsu et al. [Phys. Rev. D 101, 063528 (2020)]. $\Lambda_{\rm s}$CDM was previously claimed to simultaneously relax five cosmological discrepancies, namely, the $H_0$, $S_8$, and $M_B$ tensions along with the Ly-$\alpha$ and $\omega_{\rm b}$ anomalies, which prevail within the standard $\Lambda$CDM model as well as its canonical/simple extensions. In the present work, we extend the previous analysis by constraining the model using the Pantheon data (with and without the SH0ES $M_B$ prior) and/or the completed BAO data along with the full Planck CMB data. We find that $\Lambda_{\rm s}$CDM exhibits a better fit to the data compared to $\Lambda$CDM, and simultaneously relaxes the six discrepancies of $\Lambda$CDM, viz., the $H_0$, $M_B$, $S_8$, Ly-$\alpha$, $t_0$, and $\omega_{\rm b}$ discrepancies, all of which are discussed in detail. When the $M_B$ prior is included in the analyses, $\Lambda_{\rm s}$CDM performs significantly better in relaxing the $H_0$, $M_B$, and $S_8$ tensions with the constraint ${z_\dagger\sim1.8}$ even when the Ly-$\alpha$ data (which imposed the $z_\dagger\sim2$ constraint in the previous studies) are excluded. In contrast, the presence of the $M_B$ prior causes only negligible improvements for $\Lambda$CDM. Thus, the $\Lambda_{\rm s}$CDM model provides remedy to various cosmological tensions simultaneously, only that the galaxy BAO data hinder its success to some extent.

  • Top Cited Papers

    Relaxing cosmological tensions with a sign switching cosmological constant: Improved results with Planck, BAO, and Pantheon data

    by Özgür Akarsu, Suresh Kumar, Emre Özülker, J. Alberto Vazquez, Anita Yadav

    We present a further observational analysis of the ΛsCDM model proposed in Akarsu et al. [ Phys. Rev. D 104, 123512 (2021)]. This model is based on the recent conjecture suggesting the Universe has transitioned from anti–de Sitter vacua to de Sitter vacua (viz., the cosmological constant switches sign from negative to positive), at redshift z†∼2, inspired by the graduated dark energy model proposed in Akarsu et al. [ Phys. Rev. D 101, 063528 (2020)]. ΛsCDM was previously claimed to simultaneously relax five cosmological discrepancies, namely, the H0, S8, and MB tensions along with the Ly−α and ωb anomalies, which prevail within the standard ΛCDM model as well as its canonical/simple extensions. In the present work, we extend the previous analysis by constraining the model using the Pantheon data (with and without the SH0ES MB prior) and/or the completed BAO data along with the full Planck CMB data. We find that ΛsCDM exhibits a better fit to the data compared to ΛCDM, and simultaneously relaxes the six discrepancies of ΛCDM, viz., the H0, MB, S8, Ly−α, t0, and ωb discrepancies, all of which are discussed in detail. When the MB prior is included in the analyses, ΛsCDM performs significantly better in relaxing the H0, MB, and S8 tensions with the constraint z†∼1.8 even when the Ly−α data (which imposed the z†∼2 constraint in the previous studies) are excluded. In contrast, the presence of the MB prior causes only negligible improvements for ΛCDM. Thus, the ΛsCDM model provides remedy to various cosmological tensions simultaneously, only that the galaxy BAO data hinder its success to some extent.


  • Open Access

    Inevitable manifestation of wiggles in the expansion of the late Universe

    by Ozgur Akarsu, Eoin O. Colgain, Emre Ozulker, Somyadip Thakur, Lu Yin

    Using the fact that the comoving angular diameter distance to the last scattering surface is strictly constrained almost model independently, we show that, for any model agreeing with the standard $\Lambda$CDM model on its background dynamics at $z\sim0$ and size of the comoving sound horizon at last scattering, the deviations of the Hubble radius from the one of the standard $\Lambda$CDM model must be a member of the set of admissible wavelets. The family of models characterized by this framework also offers nontrivial oscillatory behaviours in various functions that define the kinematics of the Universe, even when the wavelets themselves are very simple. We also discuss the consequences of attributing these kinematics to, first, dark energy, and second, varying gravitational coupling strength. Utilizing some simplest wavelets, we demonstrate the competence of this framework in describing the baryon acoustic oscillation (BAO) data without any modifications to the agreement with cosmic microwave background measurements. This framework also provides a natural explanation for the bumps found in nonparametric observational reconstructions of the Hubble parameter and dark energy density as compensations of the dips suggested by some BAO data, and questions the physical reality of their existence. We note that utilizing this framework on top of the models that agree with both the cosmic microwave background and local $H_0$ measurements but are held back by BAO data, one may resurrect these models through the wiggly nature of wavelets that can naturally accommodate the BAO data. Finally, we also suggest narrowing the plausible set of admissible wavelets to further improve our framework by imposing conditions from expected kinematics of a viable cosmological model or first principle fundamental physics such as energy conditions.