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Cosmicflows-4 Compilation

Updated 4 February 2026
  • Cosmicflows-4 is the largest catalog of galaxy distances and peculiar velocities, unifying eight measurement methods through robust Bayesian calibration.
  • It synthesizes photometric, spectroscopic, and geometric indicators to construct a high-fidelity 3D map of the local universe’s velocity and density fields.
  • The compilation enables precise cosmological tests, yielding accurate measurements of the Hubble constant, bulk flows, and structure formation.

The Cosmicflows-4 (CF4) compilation is the largest and most comprehensive catalog of galaxy distances and inferred peculiar velocities assembled to date, comprising approximately 56,000 galaxies grouped into 38,000 systems. It synthesizes photometric, spectroscopic, and geometric distance indicators to construct a high-fidelity three-dimensional map of the local universe's velocity and density fields, enabling precise cosmological tests and measurements of the Hubble constant and bulk flows. CF4 is the result of systematic data acquisition from multiple international radio and optical surveys, advanced calibration methods, and robust Bayesian statistical merging.

1. Dataset Structure and Composition

CF4 compiles individual distances for 55,877–56,000 galaxies (depending on the precise cut and grouping protocol) merged into 38,000–38,065 groups, using eight primary methodologies. The catalog brings together three principal subsamples:

  • “Others” (CF2-like):  ~23,000 groups at cz/100120cz/100\lesssim120, distributed nearly isotropically outside the Zone of Avoidance; includes classical Tully–Fisher (TF), Fundamental Plane (FP), and smaller surveys.
  • 6dFGS:  ~7,500 groups at 60cz/10016060\lesssim cz/100\lesssim160; dominant in the Southern Galactic hemisphere.
  • SDSS:  ~7,000 groups at 60cz/10030060\lesssim cz/100\lesssim300; confined to the Northern Galactic hemisphere.

The catalog relies on the following primary tracers and distance methodologies:

Method Number of Galaxies Typical Distance Uncertainty
TF/BTFR 12,412 / 9,967 0.3–0.4 mag (15–20%)
Fundamental Plane (FP) 42,223 0.3 mag (15%)
SN Ia 1,008 0.1–0.15 mag (5–7%)
SBF 480 0.05 mag (SBF method)
SN II 94 0.3 mag (15%)
TRGB 489
Cepheid 76
Maser 6

The sample extends out to cz24,000cz\sim24,000 km s1^{-1} (z0.08z\lesssim0.08), with the SN Ia subsample reaching z0.05z\sim0.05. Typical individual distance errors for galaxies are 20%\sim20\%, corresponding to 2000\sim2000 km s1^{-1} for cz/100=100cz/100=100.

2. Distance Indicators and Calibration Protocols

The absolute zero-point for all distance measurements is anchored by local geometric methods—chiefly Cepheid period–luminosity relations, Tip of the Red Giant Branch (TRGB) in the color-corrected II-band, and water maser distances to NGC 4258. Cross-calibration across methodologies leverages group overlaps using Bayesian Markov Chain Monte Carlo (MCMC) techniques, marginalizing over intrinsic zero-point offsets.

Tully–Fisher and Baryonic Tully–Fisher

For spirals, the TF relation in a given band λ\lambda is parameterized as

Mλ=aλlog10Wmxi+bλ,M_\lambda = a_\lambda \log_{10} W_{mx}^i + b_\lambda,

where WmxiW_{mx}^i is the inclination-corrected HI profile width, and aλa_\lambda, bλb_\lambda are empirically fit. Extensions to the Baryonic TF Relation (BTFR) incorporate the sum of stellar and gas mass:

log10(Mb/M)=a+b[log10(Wmxi/kms1)2.5].\log_{10}\left(M_b/M_\odot\right) = a + b [\log_{10}(W_{mx}^{i} / \mathrm{km\,s}^{-1}) - 2.5].

Calibration employs a two-step process: (1) cluster regression for the TF/BTFR slope and (2) zero-point alignment using 64 galaxies with independent Cepheid and/or TRGB distances, referenced to LMC and NGC 4258 (Kourkchi et al., 2022, Kourkchi et al., 2020, Kourkchi et al., 2020).

Fundamental Plane (FP)

For early-type galaxies, the FP in SDSS bands is formulated as

logRe=alogσ+bμe+c,\log R_e = a \log \sigma + b \langle \mu_e \rangle + c,

with ReR_e the effective radius, σ\sigma the velocity dispersion, and μe\langle \mu_e \rangle the mean surface brightness. Uncertainties are controlled via strict photometric and kinematic cuts (Tully et al., 2022).

Other Methods

  • SN Ia: Standardized using light-curve shape and color corrections, yielding 5%\sim5\% uncertainties.
  • Supernova II: Standardized through expansion velocity and color.
  • SBF: I-band and IR HST calibrations yield 0.05\sim0.05 mag precision.

All methodologies are merged onto a common scale by maximizing the joint likelihood over group/distance correlations, with zero-point priors sampled in the MCMC merging (Tully et al., 2022).

3. HI Data Acquisition, Linewidths, and Sample Selection

The backbone of TF distances is the All-Digital HI Catalog, aggregating 21 cm width measurements from Parkes, Green Bank Telescope (GBT), and Arecibo (ALFALFA), uniformized through a common reduction pipeline.

Key HI width parameter:

  • Wm50W_{m50}: Width at 50% of mean flux within the 90% flux window.
  • Standardization through instrumental, redshift, and turbulence corrections yields WmxW_{mx}, corrected for inclination as Wmxi=Wmx/siniW_{mx}^i = W_{mx} / \sin i.

Inclinations are determined via the Galaxy Inclination Zoo (GIZ), a crowdsourced visual classification system, minimizing systematic bias and reducing error floors to 1°–5°, depending on ii (Kourkchi et al., 2020, Dupuy et al., 2021, Courtois et al., 2014).

Selection criteria for TF inclusion: S/N >> 10, eW<20e_W<20 km s1^{-1} in WmxW_{mx}, i>45i>45^\circ, morphologically classified as Sa or later, and well-determined photometric parameters. ALFALFA widths are harmonized as Wmx=Walf6W_{mx}=W_{alf}-6 km s1^{-1}. Internal extinction corrections exploit both parametric and machine learning (random forest) models, incorporating colors and surface-brightness.

4. Grouping Algorithms and Bayesian Merging

Galaxies are assigned to groups or clusters via friends-of-friends and virial scaling (using R2tM1/3R_{2t}\propto M^{1/3}), providing a robust statistical basis for cross-method calibration and error suppression.

Bayesian inference treats each methodology's zero-point Δμs\Delta\mu_s as a free parameter; the likelihood for group nn having distances DMn(s)DM_n^{(s)} from method ss is

Ln({Δμs})=s12πσn,s2exp[12(DMn(s)+ΔμsDMnσn,s)2],L_n(\{\Delta\mu_s\}) = \prod_s \frac{1}{\sqrt{2\pi\sigma_{n,s}^2}} \exp\left[-\frac{1}{2}\left(\frac{DM_n^{(s)}+\Delta\mu_s-\langle DM \rangle_n}{\sigma_{n,s}}\right)^2\right],

with the posterior sampled by the \texttt{emcee} implementation of affine-invariant MCMC (Tully et al., 2022).

Group merges are essential for suppressing non-linear virial motions, reducing peculiar-velocity noise, and leveraging overlaps in hybrid clusters (e.g., Coma: 209\sim209 FP, 50\sim50 TF, 7 SN Ia).

5. Velocity Field Reconstruction and Statistics

Peculiar velocities are extracted for groups via

Vpecds=fVcmbH0d1+H0d/c,V_{pec}^{ds} = \frac{fV_{cmb} - H_0 d}{1 + H_0 d / c},

with f=1+0.5(1q0)zf=1 + 0.5(1-q_0)z-\ldots the relativistic correction, or with alternative logarithmic formulations at large zz.

Reconstruction of the 3D density (δL\delta_L) and velocity (vv) fields utilizes Bias Gaussianization correction (BGc) to address the lognormal error distribution of distances. After Gaussianizing, the Wiener Filter (WF) and Constrained Realizations (CRs) deliver minimum-variance estimates:

sWF(r)=s(r)dTddT1d,s_{WF}(r) = \langle s(r) d^T \rangle \langle dd^T \rangle^{-1} d,

with the prior drawn from the linear Λ\LambdaCDM power spectrum.

Key statistics:

  • Mean overdensity: ΔL(R)=(3/4πR3)r<RδL(r)d3r\Delta_L(R) = (3/4\pi R^3)\int_{|r|<R}\delta_L(r)\,d^3r
  • Bulk velocity: Vbulk(R)=(3/4πR3)r<Rv(r)d3rV_{bulk}(R) = (3/4\pi R^3)\int_{|r|<R}v(r)\,d^3r

CF4 finds Vbulk(R)V_{bulk}(R) and ΔL(R)\Delta_L(R) are within 1σ1\sigma of cosmic variance using “Others” alone. Inclusion of the 6dFGS introduces a 3.4σ3.4\sigma bulk flow excess at R250h1R\sim250\,h^{-1} Mpc, aligning mostly with the Supergalactic X axis (Shapley Concentration), and a 1.9σ–1.9\sigma underdensity at R190h1R\simeq190\,h^{-1} Mpc (Hoffman et al., 2023).

6. Cosmological Results and Implications

The joint dataset yields the following key cosmological measures:

  • Hubble constant (H0H_0): 74.6±0.874.6\pm0.8 (stat) ±3\pm\sim3 (sys) km s1^{-1} Mpc1^{-1} (global CF4), with internal consistency among TF, BTFR, and SN Ia—e.g., TF: 75.1±0.275.1\pm0.2 (stat) km s1^{-1} Mpc1^{-1}; BTFR: 75.5±2.575.5\pm2.5 (Kourkchi et al., 2022, Kourkchi et al., 2020, Tully et al., 2022).
  • Large-scale bulk flow: At R=300h1001R=300\,h_{100}^{-1} Mpc, Vb=230±136|V_{b}|=230\pm136 km s1^{-1}, directed toward the Sloan Great Wall; tidal analysis finds Vbulktidal129V_{bulk}^{tidal}\simeq129 km s1^{-1}, indicating 20%\sim20\% of CMB-frame motion arises from external structures (Hoffman et al., 2023, Courtois et al., 2022).
  • Structure growth (fσ8f\sigma_8): 0.36±0.050.36\pm0.05 (grouped), 0.38±0.040.38\pm0.04 (ungrouped); SN Ia: 0.30±0.060.30\pm0.06 (Courtois et al., 2022).
  • The inferred velocity field exhibits moderate (2(23)σ3)\sigma excess for bulk flows on $150$–300h1300\,h^{-1} Mpc scales, but within plausible cosmic-variance fluctuations of Λ\LambdaCDM.

7. Significance and Applications

CF4 provides the densest grid of peculiar velocities and distances to date, enabling rigorous mapping and analysis of large-scale flows, bulk motions, density monopoles, and comparisons against cosmological simulations. The systematic merging of eight distance indicators, anchored by geometric calibrations and robust group assembly, establishes a low-bias, high-precision foundation for cosmic velocity field studies and presents vital empirical constraints on H0H_0 and structure formation.

CF4 data products underpin analyses of gravitational basins (e.g., Laniakea), statistical isotropy, and tests for tension with Λ\LambdaCDM, facilitating critical investigations into both local and global cosmological parameters (Hoffman et al., 2023, Courtois et al., 2022, Tully et al., 2022).

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