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Euclid: Calibrating distances from surface brightness fluctuations with Early Release Observations of the Fornax cluster

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Mapping the Cosmic Distance Ladder with Pixel Noise

Astronomers use various tools to measure how far away a galaxy is. Many methods struggle with the scale of modern sky surveys. One such tool is Surface Brightness Fluctuations (SBF). This technique measures tiny, pixel-to-pixel variations in light. These variations are caused by the statistical distribution of individual stars. Because the "graininess" of a galaxy's image changes predictably with distance, SBF can calculate distances using only standard imaging data.

While SBF has succeeded with the Hubble Space Telescope, the Euclid mission promises to observe billions of galaxies. However, applying SBF to Euclid's specific data format is not a plug-and-play task. A new study from the Euclid Consortium presents the first successful application of SBF to Euclid's Early Release Observations (ERO). The authors report that even with a data pipeline not originally optimized for this purpose, they can extract robust distance measurements.

The challenge of measuring graininess

Standard distance methods often rely on "standard candles." These are objects with a known intrinsic brightness, like Type Ia supernovae. However, these are relatively rare. They can be difficult to find in the massive populations of galaxies that Euclid will encounter. SBF offers a versatile alternative. It relies on the inherent "mottled" appearance of a galaxy's light profile. This appearance arises because stars are discrete points rather than a continuous fluid.

The difficulty lies in the fact that this "graininess" is not a pure signal. The signal is easily contaminated by "spurious sources." These include globular clusters (dense groups of stars orbiting a galaxy) or background galaxies. These contaminants can look like part of the target's natural texture. Furthermore, the brightness of these fluctuations depends on the age and metal content of the stars. Without a precise calibration, the distance calculation fails.

Automating the extraction of stellar variance

To tackle this, the authors use the FAST-SBF (Flexible Automated Self-contained Tool for SBF) package. This Python-based pipeline automates the complex workflow of SBF measurement. The process follows a rigorous sequence to isolate the true stellar signal:

  1. Background and Model Subtraction: The code estimates the local sky background. It also creates a mathematical model of the galaxy's overall light profile. Subtracting these leaves a "residual image" containing only the fluctuations and noise.
  2. Source Masking: The pipeline identifies and masks compact objects like globular clusters. To prevent the algorithm from accidentally masking actual stellar fluctuations, the authors use a scaling parameter, $\kappa$. This parameter adjusts the signal-to-noise threshold for detection.
  3. Fourier Space Analysis: The code converts the residual image into Fourier space (a mathematical domain used to analyze frequencies). It then fits the resulting power spectrum using the model $P(k) = P_0 E(k) + P_1$. In this equation, $P_0$ represents the total amplitude of the fluctuations. Meanwhile, $P_1$ captures the "white noise" (random electronic or photon noise that lacks spatial structure). Separating $P_1$ is critical to ensure random noise does not inflate the stellar signal.
  4. Color Calibration: Since the fluctuation amplitude depends on the galaxy's color, the authors measure the $(I_{\text{E}}-H_{\text{E}})$ color to anchor the absolute magnitude.

The workflow is visualized in .

Figure 2
Fig. 2. Key steps in the SBF process are shown for FCC 190, a massive cluster member in the Fornax ERO image. Left panel, clockwise from upper left : (a) the original I E image of the galaxy; (b) the residual image after the background, galaxy model, and large-scale structure have been subtracted; (c) the annulus used for the measurements, with remaining spurious (non-SBF) sources masked; and (d) the fit to the combined luminosity function of GC and background galaxies. Note that the cutout size, which is fixed for the three images, was chosen for this display; FAST-SBF is run on a much larger cutout in order to accurately measure the background and model the outermost isophotes of the galaxy. The red bar in the upper right corner of figure (a) represents 30 ′′ . North is up and east is to the left. Right panel, from top to bottom : (i) the azimuthally averaged radial power spectrum profile, where the data is plotted in grey, the best-fit line is shown in blue and includes contributions from the power spectrum of the PSF (labelled PSFps; yellow dashed line) and a white noise (w.n.) component ( P 1; green), while the bounds of the fitting region are marked with red dashed lines; (ii) the difference between the model and the best-fit line as a function of the wavenumber k ; and (iii) the amplitude P 0 that would be extracted from the fit, if we iterate over the fitting region, increasing k ini by one data point each time. The best P 0 value is determined from the most stable value within a specified fraction of the total window fitting region, marked with black dashed lines. Similar plots for other massive galaxies in the cluster are shown in Appendix A.

This figure shows the transition from the original galaxy image to the final power spectrum fit.

Validating the Euclid calibration

The authors first applied the pipeline to 15 galaxies in the Fornax cluster. They established a baseline for the method. By anchoring the results to the Tip of the Red Giant Branch (TRGB)—a highly reliable distance indicator—they derived a third-order polynomial. This polynomial relates the absolute SBF magnitude ($M_{I\text{E}}$) to the galaxy's color .

Figure 6
Fig. 6. Colour-magnitude diagram for the SBF targets in the Fornax galaxy cluster. The colour and SBF magnitude m IE , 0 are measured in the same annulus, and the galaxies used for the best-fit line are colour coded according to the total apparent magnitude that we measure for the galaxy. Around the best-fit line, we include two shaded regions, denoting uncertainties of m IE ± 0 . 1 and m IE ± 0 . 2 from the best-fit line; these are the typical uncertainties that we would expect from this process for massive and dwarf galaxies, respectively. For illustration purposes, the galaxies that were not included in the fit are shown in tan; see text for details.

A third-order fit was used to capture the complex relationship across different galaxy types.

The paper reports that this calibration holds up in different environments. When testing the Fornax-derived relation on the Perseus cluster, the authors found a distance of $69.5^{+4.6}{-4.4}$ Mpc. This aligns closely with existing literature. Similarly, for the dwarf satellites around NGC 6744, the study reports a distance of $9.6^{+0.5}$ Mpc. This is consistent with previous Hubble Space Telescope observations.

Crucially, the study demonstrates that Euclid data is high-quality enough to yield stable results. The power spectrum in Euclid's $I_{\text{E}}$ band lacks a prominent "plateau" of white noise. However, the authors show through stability tests and iterative fitting that the $P_0$ value remains consistent.

Figure 5
Fig. 5. Testing the sensitivity of our fitting routine on k end for a single galaxy: FCC 188. Top : the m IE we extract as a function of k end, when all other parameters are held constant. The ( χ 2 /ν )mod values are a modified reduced chi-squared statistic; see the text for a discussion. Lower three panels : the power spectrum of the galaxy for three values of k end. The colours are the same as in Fig. 3.
Figure 4
Fig. 4. Stability of the FAST-SBF results. For the nine galaxies with prior SBF measurements, we first obtained a good (or reasonable, in the case of FCC 170) galaxy model with a flat residual, then varied the input parameters to test the stability of our results. We changed: (a) κ , the deblending parameter that governs how point sources are detected above the surface brightness of the galaxy (orange); (b) the fitting interval used for the modelling the power spectrum ( k ini and k end; blue); and (c) the annulus in which the SBF signal is extracted (green). For each galaxy, we also included shaded bands around the reference value to highlight the expected errors: m ± 0 . 1 and colour ± 0 . 04. The output of the 'reference run' for each galaxy is shown in red.

This proves the method can work even with imperfect spectral shapes.

Limitations in the dwarf regime

Despite the success, the authors highlight several technical hurdles. First, the Euclid data reduction pipeline uses a bilinear interpolation kernel for near-infrared bands. This is not ideal for SBF. Ideally, a Lanczos3 kernel should be used. This minimizes correlations between pixels, which is vital since SBF assumes noise in each pixel is independent.

Second, the method struggles with the smallest and faintest dwarf galaxies. These objects have fewer pixels available for statistics. This makes the power spectrum fits prone to instability. The authors note that in these cases, SBF might only confirm group membership. It may not provide a precise distance. Finally, the current calibration is limited by a small sample size in Fornax. The relationship between color and magnitude for very blue, metal-poor galaxies is still being refined.

A new tool for cosmic mapping

The verdict is a qualified yes: Euclid is ready for SBF science. However, the community must adopt specialized data processing strategies. The study proves that SBF is a viable, redshift-independent distance indicator for Euclid. It can probe everything from massive elliptical galaxies to small dwarf satellites.

For practitioners, the takeaway is clear. The standard Euclid pipeline is not a complete solution for SBF. Custom stacks using Lanczos3 kernels will be necessary. This will preserve the integrity of the spatial power spectrum. If these refinements are implemented, SBF can move beyond niche studies. It could become a high-throughput engine for mapping the 3D structure of the nearby Universe.

Figures from the paper

Figure 1
Fig. 1. Transmission filters for Euclid compared to selected HST filters, which have been used for prior SBF measurements. Blakeslee et al. (2009) used HST / ACS g F475W and z F850LP observations to measure SBF distances for eight of the galaxies in our sample. Other studies have used the WFC3 F110W and F160W filters to measure SBF in the NIR (Jensen et al. 2021; Jensen et al. 2015). All transmission curves are from the Spanish Virtual observatory Filter Profile Service (Rodrigo & Solano 2020); this NISP filter curves can also be found in the paper by Euclid Collaboration: Schirmer et al. (2022).
Figure 3
Fig. 3. Top row : the power spectrum of three sky regions across the Fornax ERO image: an area with a typical noise level ( left ), in a stripe with higher noise ( middle ), and in the region with ICL ( right ). Bottom row, from left to right : the power spectrum of the background galaxy LEDA647424 ( d ∼ 250 Mpc; Morris et al. 2007), in the halo of the massive cluster member FCC147, and for the dwarf cluster member LEDA74791. The data (grey points) are fit with a function of the form P ( k ) = P 0 E ( k ) + P 1 (blue line; see text for details) in the k interval between the red dashed lines. The extracted white noise component, P 1, is plotted as a dashed green line when it can be distinguished from the best-fit line.
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#Euclid#Surface Brightness Fluctuations#Galaxy Distances#Fornax Cluster#Stellar Populations
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