ABSTRACT

From Baryon Acoustic Oscillation measurements with Sloan Digital Sky Survey SDSS DR14 galaxies, and the acoustic horizon angle ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$ measured by the Planck Collaboration, we obtain ${\Omega }_m=0.2724\pm 0.0047$, and $h+0.020\cdot {\displaystyle \sum }{m}_{\nu }=0.7038\pm 0.0060$, assuming flat space and a cosmological constant. We combine this result with the 2018 Planck “TT, TE, EE + lowE + lensing” analysis, and update a study of ${\displaystyle \sum }{m}_{\nu }$ with new direct measurements of ${\sigma }_8$, and obtain ${\displaystyle \sum }{m}_{\nu }=0.27\pm 0.08$ eV assuming three nearly degenerate neutrino eigenstates. Measurements are consistent with ${\Omega }_k=0$, and ${\Omega }_{\text{de}}\left(a\right)={\Omega }_{\Lambda }$ constant.

Keywords:

Cosmological Parameters, Baryon Acoustic Oscillations, Galaxy Distributions, Cosmic Microwave Background

1. Introduction and Summary

From a study of Baryon Acoustic Oscillations (BAO) with Sloan Digital Sky Survey (SDSS) data release DR13 galaxies and the “sound horizon” angle ${\theta }_{\text{MC}}$ measured by the Planck Collaboration we obtained ${\Omega }_m=0.281\pm 0.003$ assuming flat space and a cosmological constant [1]. At the time, the 2016 Review of Particle Physics quoted ${\Omega }_m=0.308\pm 0.012$ [2]. The new 2018 Planck “TT, TE, EE + lowE + lensing” measurement [3] obtains ${\Omega }_m=0.3153\pm 0.0073$, while the “TT, TE, EE + lowE + lensing+BAO” measurement obtains ${\Omega }_m=0.3111\pm 0.0056$ [3]. Due to the growing tension between these measurements, we decided to repeat the BAO analysis in Reference [1], this time with SDSS DR14 galaxies.

The main difficulty with the BAO measurements is to distinguish the BAO signal from the cosmological and statistical fluctuations. The aim of the present analysis is to be very conservative by choosing large bins in redshift z to obtain a larger significance of the BAO signal than in [1]. As a result, the present analysis is based on 6 independent BAO measurements, compared to 18 in [1].

We assume flat space, i.e. ${\Omega }_k=0$, and constant dark energy density, i.e. ${\Omega }_{\text{de}}\left(a\right)={\Omega }_{\Lambda }$, except in Tables 6-8 that include more general cases. We assume three neutrino flavors with eigenstates with nearly the same mass, so ${\displaystyle \sum }{m}_{\nu }\approx 3m_{\nu }$. We adopt the notation of the Particle Data Group 2018 [4]. All uncertainties have 68% confidence.

The analysis presented in this article obtains ${\Omega }_m=0.2724\pm 0.0047$ so the tension has increased further. We present full details of all fits to the galaxy-galaxy distance histograms of the present measurement so that the reader may cross-check each step of the analysis. Calibrating the BAO standard ruler we obtain $h+0.020\cdot {\displaystyle \sum }{m}_{\nu }=0.7038\pm 0.0060$, where $H_0\equiv 100h\text{km}\cdot {\text{s}}^{-1}\cdot {\text{Mpc}}^{-1}$.

Combining the direct measurement ${\Omega }_m=0.2724\pm 0.0047$ with the 2018 Planck “TT, TE, EE + lowE + lensing” analysis obtains ${\Omega }_m=0.2853\pm 0.0040$ and $h=0.6990\pm 0.0030$, at the cost of an increase of the Planck ${\chi }_{\text{P}}^2$ from 12956.78 to 12968.64.

Finally, we update the measurement of ${\displaystyle \sum }{m}_{\nu }$ of Reference [5] with the data of this Planck + Ω_m combination, and two new direct measurements of ${\sigma }_8$, and obtain ${\displaystyle \sum }{m}_{\nu }=0.27\pm 0.08$ eV. This result is sensitive to the accuracy of the direct measurements of ${\sigma }_8$.

2. Measurement of Ω_m with BAO as an Uncalibrated Standard Ruler

We measure the comoving galaxy-galaxy correlation distance $d_{\text{drag}}$, in units of $c/H_0$, with galaxies in the Sloan Digital Sky Survey SDSS DR14 publicly released catalog [6] [7], with the method described in Reference [1]. Briefly, from the angle $\alpha$ between two galaxies as seen by the observer, and their red-shifts $z_1$ and $z_2$, we calculate their distance d, in units of $c/H_0$, assuming a reference cosmology [1]. At this “uncalibrated” stage in the analysis, the unit of distance $c/H_0$ is neither known nor needed. The adimensional distance d has a component $d_{\alpha }$ transverse to the line of sight, and a component $d_z$ along the line of sight, given by Equation (3) of [1]. We fill three histograms of d according to the orientation of the galaxy pairs with respect to the line of sight, i.e. $d_z/d_{\alpha }<1/3$, $d_{\alpha }/d_z<1/3$, and remaining pairs. Fitting these histograms we obtain excesses centered at ${\hat{d}}_{\alpha }$, ${\hat{d}}_z$, and ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$ respectively. Examples are shown in Figure 1 and Figure 2. From each BAO observable ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, or ${\hat{d}}_z$ we recover $d_{\text{drag}}$ for any given cosmology with Equations (5), (6), or (7) of Reference [1]. Requiring that $d_{\text{drag}}$ be independent of red shift z and orientation we obtain the space curvature ${\Omega }_k$, the dark energy density ${\Omega }_{\text{de}}\left(a\right)$ as a function of the expansion parameter $a=1/\left(1+z\right)$, and the matter density ${\Omega }_m=1-{\Omega }_{\text{de}}\left(1\right)-{\Omega }_k-{\Omega }_r$. Full details can be found in [1].

The challenge with these BAO measurements is to distinguish the BAO signal from the cosmological and statistical fluctuations of the background. Our strategy is three-fold: 1) redundancy of measurements with different cosmological fluctuations, 2) pattern recognition of the BAO signal, and 3) requiring all three fits for ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, and ${\hat{d}}_z$ to converge, and that the consistency relation

$Q={\hat{d}}_{/}/\left({\hat{d}}_{\alpha }^{0.57}{\hat{d}}_z^{0.43}\right)=1$ [1] be satisfied within $\pm \mathrm{3\; <mi>\; \%\; </mi>}$.

Regarding redundancy, we repeat the fits for the northern (N) and southern (S) galactic caps; we repeat the measurements for galaxy-galaxy (G-G) distances, galaxy-large galaxy (G-LG) distances, LG-LG distances, and galaxy-cluster (G-C) distances; and we fill histograms of d with weights ${0.033}^2/d^2$ or ${0.033}^2{F}_i{F}_j/d^2$, where $F_i$ and $F_j$ are absolute luminosities; see [1] for details. In the present analysis we have off-set the bins of redshift z with respect to Reference [1] to obtain different background fluctuations.

Now consider pattern recognition. Figure 1 and Figure 2 show that the BAO signal is approximately constant from d ≈ 0.032 to ≈0.037, corresponding to ≈137 Mpc to ≈158 Mpc. This characteristic shape of the BAO signal can be understood qualitatively with reference to Figure 1 of [8] : the radial mass profile of an initial point like adiabatic excess results, well after recombination, in peaks at radii 17 Mpc and $r_{\text{drag}}\approx 148$ Mpc, so we can expect the BAO signal to extend from approximately 148-17 Mpc to 148+17 Mpc, with $r_{\text{drag}}$ at the mid-point. From galaxy simulations described in [5], the smearing of $r_{\text{drag}}$ due to galaxy peculiar motions has a standard deviation approximately 7.6 Mpc at $z=0.5$, and 8.5 Mpc at $z=0.3$. So the observed BAO signal has an unexpected “step-up-step-down” shape, and is narrower than implied by the simulation in reference [8].

The selections of galaxies are as in [1] with the added requirements for SDSS DR14 galaxies that they be “sciencePrimary” and “bossPrimary”, and have a smaller redshift uncertainty zErr < 0.00025.

The fitting function has 6 free parameters, corresponding to a second degree polynomial for the background, and a “smooth step-up-step-down” function (described in [1] ) with a center $\hat{d}$, a half-width $\Delta$, and an amplitude A relative to the background. Each fit used for the final measurements is required to have a significance $A/{\sigma }_A>2$ (in the analysis of [1] this requirement was $A/{\sigma }_A>1$, which allows more bins of z).

Successful triplets of fits are presented in Table 1. Note the redundancy of measurements with $0.250<z<0.425$ and $0.425<z<800$. The independent triplets of fits selected for further analysis, are indicated with a “*”, and are shown in Figure 1 and Figure 2, with further details presented in Table 2. We note that each measurement of ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, or ${\hat{d}}_z$ in Table 1, together with the sound horizon angle ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$ obtained by the Planck experiment [3], is a sensitive measurement of ${\Omega }_m$ as shown in Table 3.

The peculiar motion corrections were studied with the galaxy generator described in [5] [9]. Results of these simulations are shown in Table 4, for G-G distances, for two cases: “correct $P\left(k\right)$ ” and “correct $P_{\text{gal}}\left(k\right)$ ”. The “correct $P\left(k\right)$ ” simulations have the predicted linear power spectrum of density fluctuations $P\left(k\right)$ of the ΛCDM model (Equation (8.1.42) of [10] ), while the “correct $P_{\text{gal}}\left(k\right)$ ” simulations have a steeper $P\left(k\right)$ input so that the generated galaxy power spectrum $P_{\text{gal}}\left(k\right)$ matches observations, see Figure 15 of [5]. (The need for the steeper $P\left(k\right)$ is currently not understood.) All of these G-G corrections, and also the corrections for LG-LG and G-C, are in agreement, to within a factor 2, with the corrections applied in [1] that where taken from a study in [11]. In summary, in the present analysis we apply the same peculiar motion corrections as in [1], i.e. we multiply the measured BAO distances ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, and ${\hat{d}}_z$, by correction factors $f_{\alpha }$, $f_{\mathrm{<mo>\; /\; </mo>}}$, and $f_z$, respectively, where

$\begin{array}{l}{f}_{\alpha }-1=0.00320\cdot a^{1.35},\\ f_{/}-1=0.00350\cdot a^{1.35},\\ f_z-1=0.00381\cdot a^{1.35}.\end{array}$ (1)

We take half of these corrections as a systematic uncertainty. The effect of these corrections is relatively small as shown in Table 6.

Uncertainties of ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, and ${\hat{d}}_z$ are presented in Table 5. These uncertainties are dominated by cosmological and statistical fluctuations, and are estimated from the root-mean-square fluctuations of many measurements, from the width of the distribution of Q, and from the issues discussed in the Appendix.

Fits to the two independent selected triplets ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, and ${\hat{d}}_z$ indicated by a “*” in Table 1, with the uncertainties in Table 5, are presented in Table 6.

Four Scenarios are considered. In Scenario 1 the dark energy density is constant, i.e. ${\Omega }_{\text{de}}\left(a\right)={\Omega }_{\Lambda }$. In Scenario 2 the observed acceleration of the expansion of the universe is due to a gas of negative pressure with an equation of state $w\equiv p/\rho <0$. We allow the index w to be a function of a [12] [13] : $w\left(a\right)=w_0+w_a\left(1-a\right)$. Scenario 3 is the same as Scenario 2, except that w is constant, i.e. $w_a=0$. In Scenario 4 we assume ${\Omega }_{\text{de}}\left(a\right)={\Omega }_{\text{de}}\left[1+w_1\left(1-a\right)\right]$.

Note in Table 6 that ${\Omega }_k$ is consistent with zero, and ${\Omega }_{\text{de}}\left(a\right)$ is consistent with being independent of the expansion parameter a. For ${\Omega }_k=0$ and ${\Omega }_{\text{de}}\left(a\right)\equiv {\Omega }_{\Lambda }$ constant we obtain from Table 6:

${\Omega }_m=0.288\pm 0.037,$ (2)

with ${\chi }^2=1.0$ for 4 degrees of freedom.

Final calculations are done with fits and numerical integrations. Never-theless, it is convenient to present approximate analytical expressions obtained from the numerical integrations for the case of flat space and a cosmological constant. At decoupling, $z_{*}=1089.92\pm 0.25$ from the Planck “TT, TE, EE + lowE + lensing” measurement [3]. The “angular distance” at decoupling is $D_A\left(z_{\mathrm{<mo>\; *\; </mo>}}\right)\equiv \chi \left(z_{\mathrm{<mo>\; *\; </mo>}}\right)a_{\mathrm{<mo>\; *\; </mo>}}c/H_0$, with

$\chi \left(z_{*}\right)=3.2675{\left(\frac{h+0.35{\displaystyle \sum }{m}_{\nu }}{0.7}\right)}^{0.01}{\left(\frac{0.28}{{\Omega }_m}\right)}^{0.4},$ (3)

which has negligible dependence on h or ${\displaystyle \sum }{m}_{\nu }$.

From the Planck “TT, TE, EE + lowE + lensing” measurement [3], ${\theta }_{*}=0.0104092\pm 0.0000031$. Then the comoving sound horizon at decoupling is $r_{\mathrm{<mo>\; *\; </mo>}}\equiv d_{\mathrm{<mo>\; *\; </mo>}}c/H_0$, with

$d_{*}={\theta }_{*}\chi \left(z_{*}\right)=0.03401{\left(\frac{0.28}{{\Omega }_m}\right)}^{0.4}.$ (4)

The BAO standard ruler for galaxies $r_{\text{drag}}$ is larger than $r_{\mathrm{<mo>\; *\; </mo>}}$ because last scattering of electrons occurs after last scattering of photons due to their different number densities. In the present analysis, we take $r_{\text{drag}}\equiv d_{\text{drag}}c/H_0$ with

$\frac{d_{\text{drag}}}{d_{\mathrm{<mo>\; *\; </mo>}}}=1.0184\pm 0.0004,$ (5)

from the Planck “TT, TE, EE + lowE + lensing” analysis, with the uncertainty from Equation (10) of Reference [3]. Note from (4) and Equation (10) of Reference [3] that (5) is insensitive to cosmological parameters, so the uncalibrated analysis decouples from h or ${\displaystyle \sum }{m}_{\nu }$.

We can test (5) experimentally. From Table 6 we obtain $d_{\text{drag}}=0.03487\pm 0.00052$. From (4) and (2) we obtain $d_{*}=0.03363\pm 0.00174$, so the measured $d_{\text{drag}}/d_{*}=1.037\pm 0.056$.

To the 6 independent galaxy BAO measurements, we add the sound horizon angle ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$, and obtain the results presented in Table 7. Note that measurements

are consistent with flat space and a cosmological constant. Note also that the constraint on ${\Omega }_k$ becomes tighter if ${\Omega }_{\text{de}}\left(a\right)$ is assumed constant, and that the constraint on ${\Omega }_{\text{de}}\left(a\right)$ becomes tighter if ${\Omega }_k$ is assumed zero. In the scenario of flat space and a cosmological constant we obtain

${\Omega }_m=0.2724\pm 0.0047,$ (6)

with ${\chi }^2=1.2$ for 5 degrees of freedom. This is the final result of the present analysis.

Adding two measurements in the quasar Lyman-alpha forest [1] [14] [15] we obtain the results presented in Table 8. In particular, for flat space and a cosmological constant we obtain

${\Omega }_m=0.2714\pm 0.0047,$ (7)

with ${\chi }^2=10.0$ for 7 degrees of freedom. Note that the Lyman-alpha measurements tighten the constraints on ${\Omega }_k$, $w_0$, $w_1$, and $w_a$.

As a cross-check of the z dependence, from the 4 independent fits to ${\hat{d}}_{\alpha }$ at different redshifts z presented in Figure 3, plus ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$, we obtain

${\Omega }_m=0.2745\pm 0.0040,$ (8)

with ${\chi }^2=3.0$ for 3 degrees of freedom, for flat space and a cosmological constant.

As a cross-check of isotropy, from the 3 independent fits to ${\hat{d}}_{\alpha }$ at $z=0.36$ shown in Figure 4 corresponding to different regions of the sky, we obtain

${\Omega }_m=0.2737\pm 0.0043,$ (9)

with ${\chi }^2=1.1$ for 2 degrees of freedom, for flat space and a cosmological constant.

To check the stability of ${\hat{d}}_{\alpha }$, ${\hat{d}}_{\mathrm{<mo>\; /\; </mo>}}$, and ${\hat{d}}_z$ with the data set and galaxy selections, we compare fits highlighted with “*” and “&” in Table 1, and also fits in Figure 5.

Additional studies are presented in the Appendix.

3. Measurement of H₀ with BAO as a Calibrated Standard Ruler

We consider the scenario of flat space and a cosmological constant. It is useful to present approximate analytic expressions, tho all final calculations are done directly with fits to the measurements marked with a “*” in Table 1 and numerical integrations to obtain correct uncertainties for correlated parameters. To calibrate the BAO measurements, we integrate the comoving photon-electron-baryon plasma sound speed from $t=0$ up to decoupling and obtain the “comoving acoustic horizon distance” $r_{\mathrm{<mo>\; *\; </mo>}}\equiv d_{\mathrm{<mo>\; *\; </mo>}}c/H_0$, with

$d_{*}=0.03407{\left(\frac{h+0.026{\displaystyle \sum }{m}_{\nu }}{0.7}\right)}^{0.513}{\left(\frac{0.28}{{\Omega }_m}\right)}^{0.244}{\left(\frac{0.0225}{{\Omega }_b{h}^2}\right)}^{0.097}.$ (10)

The acoustic angular scale is

${\theta }_{*}\equiv \frac{d_{*}}{\chi \left(z_{*}\right)}=0.010427{\left(\frac{h+0.020{\displaystyle \sum }{m}_{\nu }}{0.70}\right)}^{0.503}{\left(\frac{{\Omega }_m}{0.28}\right)}^{0.156}{\left(\frac{0.0225}{{\Omega }_b{h}^2}\right)}^{0.097},$ (11)

in agreement with Equation (11) of [3].

Let us now consider the measurement of h. From the galaxy BAO measurements in Table 6 we obtain ${\Omega }_m=0.288\pm 0.037$ and $d_{\text{drag}}=0.03487\pm 0.00052$. From Big Bang Nucleosynthesis, ${\Omega }_b{h}^2=0.0225\pm 0.0008$ at 68% confidence [4]. From this data and Equations (5) and (10), or the corresponding fit, we obtain

$h+0.026{\displaystyle \sum }{m}_{\nu }=0.716\pm 0.027,$ (12)

with ${\chi }^2=1.0$ for 4 degrees of freedom.

The Planck measurement of ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$ allows a more precise measurement of h. From Table 7, we obtain ${\Omega }_m=0.2724\pm 0.0047$. Then from Big Bang Nucleosynthesis and (11), or the corresponding fit, we obtain

$h+0.020{\displaystyle \sum }{m}_{\nu }=0.7038\pm 0.0060,$ (13)

with ${\chi }^2=1.2$ for 5 degrees of freedom. Note that the uncertainties of h and ${\Omega }_m$ are correlated through Equation (11).

4. Studies of CMB Fluctuations

In Table 9, we present a qualitative study of the sensitivity of the CMB power spectrum $l\left(l+1\right)C_{TT,l}^S/\left(2\pi \right)$ to constrain ${\Omega }_m$ and ${\displaystyle \sum }{m}_{\nu }$. We use the approximate analytic expression (7.2.41) of [10], modified to include ${\displaystyle \sum }{m}_{\nu }$, to compare the spectra with Planck 2018 “TT, TE, EE + lowE + lensing” parameters with the best fit spectra with fixed values ${\Omega }_m=0.2854$ and ${\displaystyle \sum }{m}_{\nu }=0.06,0.1,0.2,0.3,0.4,0.5$ eV. We find that the differences in spectra range from 0.11% to 0.3% of the first acoustic peak, see Figure 6. So the CMB power spectrum, while being very sensitive to constrain ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$, has low sensitivity to constrain ${\Omega }_m$ or ${\displaystyle \sum }{m}_{\nu }$.

In view of the low sensitivity of the CMB power spectra to constrain ${\Omega }_m$, the Planck analysis can benefit from a combination with the direct measurement of ${\Omega }_m$ given by Equation (6). The combination, obtained with the “base_mnu_plikHM_TTTEEE_lowTEB_lensing_*.txt MC chains” made public by the Planck Collaboration [3], is presented in Table 10. This combination is preliminary due to the sparseness of the MC chains at low values of ${\Omega }_m$.

5. Tensions

We consider four direct measurements: 1) $h=0.7348\pm 0.0166$ by the Sh₀es Team [16], 2) ${\sigma }_8\approx \left[0.746\pm 0.012\left(stat\right)\pm 0.022\left(syst\right)\right]{\left(0.3/{\Omega }_m\right)}^{0.47}$ from the abundance of rich galaxy clusters [4] [17], 3) ${\sigma }_8\approx \left[0.745\pm 0.039\right]{\left(0.3/{\Omega }_m\right)}^{0.5}$ from weak gravitational lensing [4] [18], and 4) ${\Omega }_m=0.2724\pm 0.0047$ from galaxy BAO and ${\theta }_{\mathrm{<mo>\; *\; </mo>}}$ from Planck, Equation (6) of this analysis. Comparing these measurements with Planck (left hand column of Table 10) we obtain differences of 3.5σ, 2.5σ, 1.8σ, and 4.9σ, respectively. Comparing these measurements with the Planck + Ω_m combination (right hand column of Table 10) we obtain differences of 2.1σ, 2.3σ, 1.5σ, and 2.1σ, respectively. In conclusion, the Planck + Ω_m combination reduces the tensions with the direct measurements. Note that the Planck + Ω_m combination has ${\sigma }_8$ greater than the direct measurements. This 2.7σ tension may be due to neutrino masses.

6. Update on Neutrino Masses

We consider the scenario of three neutrino flavors with eigenstates of nearly the same mass, so ${\displaystyle \sum }{m}_{\nu }\approx 3m_{\nu }$. Massive neutrinos suppress the power spectrum of linear density fluctuations $P\left(k\right)$ by a factor $1-8{\Omega }_{\nu }/{\Omega }_m$ for $k\gg 0.018\cdot {\Omega }_m^{1/2}{\left({\displaystyle \sum }{m}_{\nu }/1\text{eV}\right)}^{1/2}h$ Mpc⁻¹ [19]. This suppression affects ${\sigma }_8$ and the galaxy power spectrum $P_{\text{gal}}\left(k\right)$, but does not affect the Sachs-Wolfe effect at low k. So, by comparing fluctuations at large and small k it is possible to constrain or measure ${\displaystyle \sum }{m}_{\nu }$ [5].

To obtain ${\displaystyle \sum }{m}_{\nu }$ we minimize a ${\chi }^2$ with four terms corresponding to $N^2$, ${\sigma }_8$, and two parameters obtained from the Planck + Ω_m combination: $h=0.6990\pm 0.0030$, and $n_s=0.9726\pm 0.0017$. In the fit, ${\Omega }_m$ is obtained from Equation (11), and ${\Omega }_b{h}^2=0.02265\pm 0.00012$. ${\sigma }_8$ is obtained from the combination of the two direct measurements presented in Section 5.

For $N^2=\left(2.08\pm 0.33\right)\times {10}^{-10}$ [5] obtained from the Sachs-Wolfe effect measured by the COBE satellite (see list of references in [10] ) we obtain

${\displaystyle \sum }{m}_{\nu }=0.45\pm 0.20\text{eV},$ (14)

with zero degrees of freedom, in agreement with [5] where the method is explained in detail.

Since ${\displaystyle \sum }{m}_{\nu }<1.7$ eV, neutrinos are still ultra-relativistic at decoupling. Then there is no power suppression of the CMB fluctuations, and we can use the entire spectrum to fix the amplitude $N^2$. From the Planck + Ω_m combination of Table 10 we obtain $N^2\equiv A_s/\left(4\pi \right)=\left(1.7700\pm 0.0354\right)\times {10}^{-10}$, and

${\displaystyle \sum }{m}_{\nu }=0.26\pm 0.08\text{eV}\mathrm{,}$ (15)

with zero degrees of freedom.

To strengthen the constraints from the two direct measurements of ${\sigma }_8$, we add to the fit measurements of fluctuations of number counts of galaxies in spheres of radii 16/h, 32/h, 64/h, and 128/h Mpc, as explained in [5]. We obtain

${\displaystyle \sum }{m}_{\nu }=0.27\pm 0.08\text{eV},$ (16)

with ${\chi }^2=1.6$ for 2 degrees of freedom, and find no significant pulls on $N^2$, h, or n_s. These results are sensitive to the accuracy of the direct measurements of ${\sigma }_8$.

Acknowledgements

We have used data in the publicly released Sloan Digital Sky Survey SDSS DR14 catalog.

Funding for the Sloan Digital Sky Survey (SDSS) has been provided by the Alfred P. Sloan Foundation, the Participating Institutions, the National Aeronautics and Space Administration, the National Science Foundation, the US Department of Energy, the Japanese Monbukagakusho, and the Max Planck Society. The SDSS Web site is http://www.sdss.org/.

The SDSS is managed by the Astrophysical Research Consortium (ARC) for the Participating Institutions. The Participating Institutions are The University of Chicago, Fermilab, the Institute for Advanced Study, the Japan Participation Group, The Johns Hopkins University, Los Alamos National Laboratory, the Max-Planck-Institute for Astronomy (MPIA), the Max-Planck-Institute for Astrophysics (MPA), New Mexico State University, University of Pittsburgh, Princeton University, the United States Naval Observatory, and the University of Washington.

We have also used data publicly released by the Planck Collaboration [3] in the form of “MC chains”, and the corresponding analysis tool “GetDist GUI”.

Conflicts of Interest

The author declares no conflicts of interest regarding the publication of this paper.

Cite this paper

Hoeneisen, B. (2018) Measurements of the Cosmological Parameters Ω_m and H₀. International Journal of Astronomy and Astrophysics, 8, 386-405. https://doi.org/10.4236/ijaa.2018.84027

References

Appendix

1) Comparison with Reference [1]

Table 4 and Table 5 of Reference [1] can be compared with Table 6 and Table 7 of the present analysis. We find agreement between all measurements when d in Reference [1] is identified with $d_{\mathrm{<mo>\; *\; </mo>}}$ in the present analysis. We find that d in Table 4 of Reference [1] is biased low with respect to $d_{\text{drag}}$ in Table 6 of the present analysis. For the scenario of flat space and a cosmological constant, Table 4 of Reference [1] obtains ${\Omega }_m=0.284\pm 0.014$ and $d=0.0339\pm 0.0002$. From this ${\Omega }_m$ and Equation (4) we obtain $d_{*}=0.0338\pm 0.0007$, in good agreement with d, so in Reference [1] no correction for $d_{\text{drag}}/d_{\mathrm{<mo>\; *\; </mo>}}$ was needed or applied.

2) Bias of BAO measurements of small galaxy samples

We have investigated the difference of $d_{\text{drag}}$ between Reference [1] and the present analysis. This difference is not due to the change of data set from SDSS DR13 to SDSS DR14: we have compared the coordinates of selected galaxies and have found no changes in calibrations. The fluctuation is not caused by the tighter galaxy selection requirements of the present analysis: compare the entries with “&” and “*” in Table 1, and see Figure 5.

As an extreme test, we divide the bin $0.425<z<0.725$ into 6 sub-samples: $0.425<z<0.525$ N, $0.525<z<0.625$ N, $0.625<z<0.725$ N, $0.425<z<0.525$ S, $0.525<z<0.625$ S, and $0.625<z<0.725$ S. We try to fit each one, and average the successful fits (only about half are successful), and obtain ${\hat{d}}_{\alpha }=0.03358\pm 0.00015$, ${\hat{d}}_{/}=0.03415\pm 0.00027$, and ${\hat{d}}_z=0.03335\pm 0.00033$. We also fit the sum of these six bins, and obtain ${\hat{d}}_{\alpha }=0.03496\pm 0.00015$, ${\hat{d}}_{/}=0.03459\pm 0.00010$, and ${\hat{d}}_z=0.03464\pm 0.00034$. So there is evidence that fits become biased low as the number of galaxies is reduced and the significance of the fitted relative amplitude A of the BAO signal becomes marginal. The reason is that the observed BAO signal has a sharper and larger lower edge at $d\approx 0.032$ compared to the upper edge at ≈0.037, so the upper edge tends to get lost in the background fluctuations as the number of galaxies is reduced.

To reduce this bias, in the present analysis we require the significance of the fitted relative amplitudes $A/{\sigma }_A>2$, instead of >1 for Reference [1]. The price to pay is that we obtain only 2 independent bins of z, instead of 6.

3) A study of the BAO signal

The BAO signal has a “step-up-step-down” shape with center at $\hat{d}$ and half-width $\Delta$. The widths of fits vary typically from $\Delta =0.0017$ to 0.0025, see Table 2. We have used the center $\hat{d}$ as the BAO standard ruler, but could have used the lower edge of the signal at $\hat{d}-\Delta$, or the upper edge at $\hat{d}+\Delta$, or somewhere in between, i.e. $\hat{d}+ϵ\Delta$. We have investigated the value of $ϵ$ that minimizes the root-mean-square fluctuations of a representative selection of measurements. The result is $ϵ=-0.17$, and the difference in the r.m.s. values is negligible (0.00037 vs. 0.00039) so we keep the center of the signal as our standard ruler, i.e. $ϵ=0$. The r.m.s. fluctuation of the lower edge with $ϵ=-1$ is 0.00068, and the fluctuation of the upper edge with $ϵ=1$ is 0.00091, which again illustrates the bias described in Appendix 7.2, i.e. the lower edge fluctuates less than the upper edge.

A separate open question is whether this center $\hat{d}$ coincides with the $d_{\text{drag}}$ of Equation (5)?

Yet another question is this: what value of $ϵ$ would reproduce the Planck ${\Omega }_m$ ? We obtain $ϵ$ ranging from −0.81 for ${\hat{d}}_{\alpha }$ at $z=0.34$, to $ϵ=-0.43$ for ${\hat{d}}_z$ at $z=0.56$. These large values of $\left|ϵ\right|$, and their strong dependence on z and galaxy-galaxy orientation, do not seem plausible.

Finally, how well do we understand $d_{\text{drag}}/d_{\mathrm{<mo>\; *\; </mo>}}$ ? The present study takes $z_{\text{drag}}=1059.94\pm 0.30$ and $d_{\text{drag}}/d_{\mathrm{<mo>\; *\; </mo>}}=1.0184\pm 0.0004$ from the Planck analysis [3]. Note the extremely small uncertainty obtained by the Planck Collaboration. In comparison, from Equation (4) of Reference [20] we obtain $z_{\text{drag}}=1020.82$ and $d_{\text{drag}}/d_{\mathrm{<mo>\; *\; </mo>}}=1.044$.

An estimate of the uncertainties due to the issues discussed in this Appendix is included in Table 5.