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Joint Curvature and Growth Rate Measurements with Supernova Peculiar Velocities and the CMB
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Type Ia supernova (SN) magnitudes present correlations due to the fact that their peculiar velocities are sourced by the large-scale structure of the Universe. This can be used to constrain properties related to the distribution and growth of matter perturbations. We analyze both Pantheon+ and Dark Energy Survey (DES-Y5) SN catalogues in combination with CMB data from Planck PR4 to constrain $\sigma_8$, optionally including both curvature and a modified growth index $\gamma$. We show that SN and CMB datasets are highly complementary and capable of measuring $\sigma_8$, $\gamma$ and $\Omega_k$ simultaneously. Using only SN, we find $\sigma_8 = 0.73 \pm 0.22$ ($0.87 \pm 0.31$) for Pantheon+ (DES-Y5) for the flat $\Lambda$CDM model. Interestingly, allowing for free $\gamma$ and $\Omega_k$, we find hints of positive curvature: $\Omega_k = -0.011 \pm 0.006$ $(-0.014 \pm 0.005)$, which exclude flatness at 2.2$\sigma$ (3.0$\sigma$), for the combination of CMB with Pantheon+ (DES-Y5). Such hints do not degrade if we also include a modified amplitude of CMB lensing $A_L$. We find that $\gamma = 0.519^{+0.061}_{-0.099}$ ($0.461^{+0.085}_{-0.069}$), consistent with the predictions of General Relativity. In terms of $f\sigma_8(z)$, we find $f\sigma_8(0.024)=0.461^{+0.066}_{-0.035}$ ($f\sigma_8(0.038) = 0.498^{+0.045}_{-0.050}$) for CMB + Pantheon+ (DES-Y5). Finally, the strong degeneracy between all three $\Omega_k$, $\gamma$ and $H_0$ results in a broader CMB $H_0$ posterior. However, if we include SH0ES $H_0$ data, which is in known strong tension with the CMB in flat $\Lambda$CDM, we find that the $H_0$ tension is recast in terms of a significantly negative curvature and suppressed growth of structures.
Title: Joint Curvature and Growth Rate Measurements with Supernova Peculiar Velocities and the CMB
Description:
Type Ia supernova (SN) magnitudes present correlations due to the fact that their peculiar velocities are sourced by the large-scale structure of the Universe.
This can be used to constrain properties related to the distribution and growth of matter perturbations.
We analyze both Pantheon+ and Dark Energy Survey (DES-Y5) SN catalogues in combination with CMB data from Planck PR4 to constrain $\sigma_8$, optionally including both curvature and a modified growth index $\gamma$.
We show that SN and CMB datasets are highly complementary and capable of measuring $\sigma_8$, $\gamma$ and $\Omega_k$ simultaneously.
Using only SN, we find $\sigma_8 = 0.
73 \pm 0.
22$ ($0.
87 \pm 0.
31$) for Pantheon+ (DES-Y5) for the flat $\Lambda$CDM model.
Interestingly, allowing for free $\gamma$ and $\Omega_k$, we find hints of positive curvature: $\Omega_k = -0.
011 \pm 0.
006$ $(-0.
014 \pm 0.
005)$, which exclude flatness at 2.
2$\sigma$ (3.
0$\sigma$), for the combination of CMB with Pantheon+ (DES-Y5).
Such hints do not degrade if we also include a modified amplitude of CMB lensing $A_L$.
We find that $\gamma = 0.
519^{+0.
061}_{-0.
099}$ ($0.
461^{+0.
085}_{-0.
069}$), consistent with the predictions of General Relativity.
In terms of $f\sigma_8(z)$, we find $f\sigma_8(0.
024)=0.
461^{+0.
066}_{-0.
035}$ ($f\sigma_8(0.
038) = 0.
498^{+0.
045}_{-0.
050}$) for CMB + Pantheon+ (DES-Y5).
Finally, the strong degeneracy between all three $\Omega_k$, $\gamma$ and $H_0$ results in a broader CMB $H_0$ posterior.
However, if we include SH0ES $H_0$ data, which is in known strong tension with the CMB in flat $\Lambda$CDM, we find that the $H_0$ tension is recast in terms of a significantly negative curvature and suppressed growth of structures.
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