Cosmological constraints from neighbor-density-weighted marked correlation functions
Pith reviewed 2026-06-30 15:05 UTC · model grok-4.3
The pith
Neighbor-density-weighted marked correlation functions extract additional cosmological information beyond the standard two-point correlation function.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that relative to the two-point correlation function alone, combinations of three mark parameters improve the figure of merit in the Omega_m-sigma_8 plane by factors of 1.7 to 2.5, and five-mark combinations achieve gains of 1.9 to 2.4. Density-based and gradient-based marks are nearly redundant for scale statistics but add up to 43 percent more information when combined in angular statistics. The angular marked statistic keeps extra information even when the tracer selection changes.
What carries the argument
The neighbor-density-weighted marked correlation functions, implemented through the normalized scale statistic and the angular statistic, with varying mark parameter alpha, emulated via Gaussian processes from the simulation suite.
Load-bearing premise
The Gaussian process emulators accurately reproduce the marked statistics' dependence on cosmological parameters across the relevant range.
What would settle it
Measurements from an independent simulation suite or from actual galaxy survey data that fail to show the reported improvement in the figure of merit when using the marked statistics.
Figures
read the original abstract
We investigate whether neighbor-density-weighted marked correlation functions (MCFs) can extract cosmological information beyond the standard redshift-space two-point correlation function (2PCF). Using the Kun suite of 129 $w_0w_a$CDM$+\sum m_\nu$ simulations in $1~h^{-1}{\rm Gpc}$ boxes, we construct Gaussian-process emulators for the normalized scale statistic $\widehat{W}^{\alpha}(s)$ and the angular statistic $\widehat{W}^{\alpha}_{\Delta s}(\mu)$. We perform joint analyses combining multiple mark parameters $\alpha$ and quantify the information gain using the FoM in the $\Omega_m$--$\sigma_8$ plane. Relative to the 2PCF case, three-mark combinations improve the FoM by factors of $1.7$--$2.5$, while five-mark combinations increase the gain to $1.9$--$2.4$, depending on the statistic and mark definition. We further compare density and normalized-gradient marks, finding that they are nearly redundant for isotropic statistics but complementary for angular statistics, where their combination improves the FoM by up to $43\%$. Tests of scale range and halo selection show that the marked statistics remain robust under changes in analysis choices, with the angular statistic retaining additional cosmological information that is less sensitive to tracer selection. Our results demonstrate that MCFs substantially enhance cosmological constraints beyond the standard 2PCF and provide a robust probe for next-generation galaxy surveys.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that neighbor-density-weighted marked correlation functions (MCFs) extract additional cosmological information beyond the standard redshift-space 2PCF. Using 129 Kun-suite w0waCDM+∑mν simulations, Gaussian-process emulators are built for the normalized scale statistic Ŵ^α(s) and angular statistic Ŵ^α_Δs(μ). Joint analyses with multiple mark parameters α yield FoM gains in the Ωm–σ8 plane of 1.7–2.5 (three-mark) and 1.9–2.4 (five-mark) relative to the 2PCF, with density and normalized-gradient marks shown to be complementary for angular statistics (up to 43% FoM improvement) and the marked statistics robust to scale-range and halo-selection choices.
Significance. If the emulators are shown to be accurate, the work demonstrates that MCFs can meaningfully tighten constraints from next-generation surveys while remaining robust to analysis variations, offering a practical extension to standard 2PCF analyses.
major comments (2)
- [§3 and §4] §3 (Emulator construction) and §4 (Results): The headline FoM ratios (1.7–2.5 and 1.9–2.4) are obtained from GP predictions; however, the manuscript supplies no quantitative validation metrics such as leave-one-out cross-validation errors, maximum interpolation residuals, or tests against an independent cosmology. Without these, it is impossible to confirm that emulator modeling error is smaller than the differences driving the reported gains.
- [§4.2] §4.2 (Mark comparison): The claim that density and normalized-gradient marks are 'nearly redundant' for isotropic statistics but 'complementary' for angular statistics (43% FoM gain) rests on the emulator outputs; any systematic bias in the GP interpolation of the angular statistic would directly affect this complementarity result.
minor comments (2)
- [Abstract and §2] The abstract and §2 would benefit from a brief statement of the exact number of training simulations used per emulator and the range of α values explored.
- [§2] Notation for the normalized statistics Ŵ^α(s) and Ŵ^α_Δs(μ) is introduced without an explicit equation linking them to the underlying marked pair counts; adding this would improve readability.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments. We address the two major points below regarding emulator validation and will revise the manuscript to incorporate the requested metrics.
read point-by-point responses
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Referee: [§3 and §4] §3 (Emulator construction) and §4 (Results): The headline FoM ratios (1.7–2.5 and 1.9–2.4) are obtained from GP predictions; however, the manuscript supplies no quantitative validation metrics such as leave-one-out cross-validation errors, maximum interpolation residuals, or tests against an independent cosmology. Without these, it is impossible to confirm that emulator modeling error is smaller than the differences driving the reported gains.
Authors: We agree that quantitative validation metrics for the GP emulators are essential to support the reported FoM gains. In the revised manuscript we will add a dedicated subsection to §3 reporting leave-one-out cross-validation errors and maximum interpolation residuals for both Ŵ^α(s) and Ŵ^α_Δs(μ) across all mark parameters. We will also present results from holding out one cosmology from the 129-simulation suite as an independent test. These metrics confirm that emulator errors remain sub-dominant to the cosmological variations driving the 1.7–2.5× FoM improvements. revision: yes
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Referee: [§4.2] §4.2 (Mark comparison): The claim that density and normalized-gradient marks are 'nearly redundant' for isotropic statistics but 'complementary' for angular statistics (43% FoM gain) rests on the emulator outputs; any systematic bias in the GP interpolation of the angular statistic would directly affect this complementarity result.
Authors: We acknowledge that the reported complementarity (and 43% FoM gain) for the angular statistic depends on emulator fidelity. The new validation subsection in revised §3 will include LOO-CV errors and residuals specifically for Ŵ^α_Δs(μ) under density and normalized-gradient marks. We will additionally show that the interpolation uncertainties do not change the relative FoM when the two marks are combined, thereby confirming that the complementarity result is robust. revision: yes
Circularity Check
No circularity; results from independent simulations and emulators
full rationale
The derivation chain relies on N-body simulations from the Kun suite and Gaussian-process emulators to compute FoM gains for marked correlation functions relative to 2PCF. No equations reduce by construction to fitted inputs, no self-definitional steps appear, and no load-bearing self-citations or imported uniqueness theorems are invoked. The reported improvement factors are obtained by direct evaluation on emulated statistics, with the central claim remaining independent of the paper's own outputs.
Axiom & Free-Parameter Ledger
free parameters (1)
- mark parameter α
axioms (1)
- domain assumption The Kun suite of 129 w0waCDM+∑m_ν simulations in 1 h⁻¹ Gpc boxes accurately represent the target cosmology for emulator training.
Reference graph
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The first is the adaptive local density itself, 𝑤=𝜌 𝑛NB .(4) This mark directly upweights halos in dense environments
Choice of marks Weusetwoenvironmentalmarksinthelikelihoodanalysis. The first is the adaptive local density itself, 𝑤=𝜌 𝑛NB .(4) This mark directly upweights halos in dense environments. It is therefore sensitive to the clustering of halos in compact overdense structures. The second mark is the normalized density gradient, 𝑤= |∇𝜌 𝑛NB | 𝜌𝑛NB .(5) This quant...
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Marked two-point statistic We now incorporate the environmental marks into a two- point statistic. For a given mark𝑤and mark power𝛼, we define the marked correlation function as 𝑊 𝛼 (r)= ⟨𝛿(x)𝑤 𝛼 (x)𝛿(x+r)𝑤 𝛼 (x+r) ⟩ .(6) Here𝛿is the tracer overdensity field, and the exponent𝛼 controls how strongly the mark affects the pair weighting. Forcomparison,theord...
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Normalized marked correlation functions Forlikelihoodinference,wefocusontheshapeinformation rather than the overall integral of each marked statistic. We therefore define the normalized scale-dependent statistic as b𝑊 𝛼 (𝑠)= 𝑊 𝛼 (𝑠)∫ 𝑠max 𝑠min 𝑊 𝛼 (𝑠 ′)𝑑𝑠 ′ .(11) 5 FIG.2: Environmentalquantitiesina500×500(ℎ −1Mpc)2 sliceofaKunhalocatalog. Left: thelocal-d...
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Emulator covariance The emulator covariance quantifies the uncertainty intro- duced by interpolation across cosmological parameter space. We estimate this term using the leave-one-out validation de- scribed in the previous section. For the𝑗-th training cosmol- ogy, the emulator is trained on all other cosmologies and then evaluated at the omitted point. T...
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discussion (0)
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