pith. sign in

arxiv: 2604.14588 · v2 · submitted 2026-04-16 · 🌌 astro-ph.GA

Impact of Baseline, Cadence, and Host Contamination on AGN Variability Metrics: A Systematic Study with ZTF

Pith reviewed 2026-05-10 10:52 UTC · model grok-4.3

classification 🌌 astro-ph.GA
keywords AGN variabilityStetson indexsmoothness metricZwicky Transient Facilityhost galaxy contaminationlight curve analysisactive galactic nucleivariability metrics
0
0 comments X

The pith

The Stetson index J holds steady for AGN variability while the smoothness metric s shifts with cadence and host light.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper tests how two variability metrics respond to realistic changes in how AGN light curves are observed. Using ZTF data on 23 nearby active galactic nuclei, it finds both J and s stay consistent when the total observation span changes by roughly two years. Cadence changes, however, move s by more than 40 percent while J moves by less than 10 percent. Subtracting host galaxy light from the Mrk 493 light curve leaves J unchanged but raises s. The work therefore presents J as a stable choice for measuring variability tied to accretion onto supermassive black holes and s as one that needs extra care.

Core claim

Analysis of ZTF DR24 light curves for 23 nearby AGNs shows the Stetson index J varies by at most 10 percent under baseline shifts of about two years, different cadences, and host-galaxy subtraction in the representative case of Mrk 493, whereas the smoothness metric s varies by 40 percent or more with cadence and increases after host subtraction, supporting the conclusion that J is robust for characterizing AGN variability while s must be interpreted cautiously.

What carries the argument

The Stetson index J, a metric computed from flux distributions across temporally separated epochs in AGN light curves, which remains stable against changes in baseline length, sampling cadence, and host-galaxy contamination.

If this is right

  • J can be compared directly across surveys that differ in total baseline or sampling rate.
  • Host-galaxy light does not bias J, so the metric can be applied even when perfect host subtraction is unavailable.
  • Studies that rely on s must correct for cadence differences and host contamination before interpreting variability as a probe of accretion physics.
  • J offers a practical way to combine variability measurements from multiple facilities without large systematic offsets.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • J could become a default metric in upcoming wide-field surveys where cadence and host light vary across the sky.
  • The same stability test applied to other variability statistics would reveal which ones are safest for cross-survey work.
  • If the pattern holds, variability catalogs built from J could be used to study black-hole accretion rates with reduced observational bias.

Load-bearing premise

The assumption that results from 23 nearby AGNs plus the single Mrk 493 host-subtraction test apply to the full range of AGN populations and to surveys other than ZTF DR24.

What would settle it

Repeating the analysis on a larger and more distant AGN sample from a survey with different cadence or without host subtraction and finding large changes in J or no change in s would falsify the robustness claim.

Figures

Figures reproduced from arXiv: 2604.14588 by Diego Mart\'inez Collipal, Swayamtrupta Panda.

Figure 1
Figure 1. Figure 1: Upper left: ZTF DR24 measurements of J against those from MA24. The red line shows our fitted linear model obtained via Orthogonal distance regression (ODR), while the black line shows the 1:1 relation. Spearman correlation coefficient ρ and fitted parameters are shown in the top left corner. Upper right: Same as left panel, but for s. Middle panels: Representative ZTF r band light curves. Left: ”Assembled… view at source ↗
read the original abstract

Variability in active galactic nuclei (AGN) probes the physics of accretion onto supermassive black holes. This variability is characterized using metrics derived from the flux distributions of temporally separated epochs. We studied the stability of two variability metrics, the Stetson index "J" and the smoothness "s", against baseline, cadence, and host galaxy contamination. We studied 23 nearby AGNs using Zwicky Transient Facility's Data Release 24. Both metrics are robust to baseline variations of $\sim 2$ years. However, s is sensitive to cadence, showing variations $\gtrsim 40\%$, while J shows minor variations $\lesssim10\%$. We studied the host galaxy impact using Mrk 493 as a representative case. We found that J remains unchanged after host subtraction, while s increases. We concluded that J is a robust tool for characterizing AGN variability, while s should be interpreted with caution.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript presents an empirical study using ZTF DR24 data on 23 nearby AGNs to assess the stability of the Stetson index J and smoothness metric s against variations in baseline length (~2 years), cadence, and host-galaxy contamination (tested via host subtraction on Mrk 493 only). It reports that both metrics are robust to baseline changes, s varies by ≳40% with cadence while J varies by ≲10%, J is unchanged by host subtraction while s increases, and concludes that J is a robust tool for AGN variability while s requires caution.

Significance. If the differential robustness holds, the work offers practical guidance for metric selection in time-domain AGN studies with large surveys. A strength is the use of public data and standard published metrics to derive concrete quantitative estimates of sensitivity; the purely empirical approach avoids circularity.

major comments (2)
  1. The central claim that J is robust while s is not rests on a sample of only 23 nearby AGNs with host effects tested on a single case (Mrk 493). No cross-checks against higher-redshift AGNs, different black-hole masses/luminosities, or cadences from other surveys are provided, so the observed ~10% vs ≳40% variations and the generalization in the conclusion are not load-bearing supported.
  2. The reported percentage changes lack error bars, statistical significance tests, or details on sample selection criteria and full methodology (e.g., how baselines/cadences were subsampled). This weakens the quantitative support for the differential robustness ranking.
minor comments (1)
  1. The abstract and methods would benefit from explicit references to the original definitions of J and s, plus a brief description of the host-subtraction procedure applied to Mrk 493.

Simulated Author's Rebuttal

2 responses · 1 unresolved

We thank the referee for their constructive comments on our manuscript. We address each major comment below and indicate revisions made to strengthen the presentation of our empirical results.

read point-by-point responses
  1. Referee: The central claim that J is robust while s is not rests on a sample of only 23 nearby AGNs with host effects tested on a single case (Mrk 493). No cross-checks against higher-redshift AGNs, different black-hole masses/luminosities, or cadences from other surveys are provided, so the observed ~10% vs ≳40% variations and the generalization in the conclusion are not load-bearing supported.

    Authors: We acknowledge that the sample is limited to 23 nearby AGNs and that host subtraction was demonstrated on Mrk 493. This selection was intentional to target objects where host contamination is measurable and relevant, as it becomes negligible at higher redshifts. The observed differential behavior (J variations ≲10% vs s ≳40%) is consistent across all 23 objects for the baseline and cadence tests. We agree that the conclusions should not overgeneralize and have revised the final section to explicitly limit the claims to nearby AGNs with ZTF-like sampling, while noting that host effects are expected to be smaller at higher z. Cross-checks with other surveys or redshift ranges are outside the scope of the current ZTF DR24 analysis. revision: partial

  2. Referee: The reported percentage changes lack error bars, statistical significance tests, or details on sample selection criteria and full methodology (e.g., how baselines/cadences were subsampled). This weakens the quantitative support for the differential robustness ranking.

    Authors: We thank the referee for this observation. The revised manuscript now includes error bars on all percentage variations (computed via bootstrap resampling across the sample), reports the results of paired statistical tests confirming that cadence-induced changes in s are significant (p < 0.01) while those in J are not, and expands the Methods section with the full sample selection criteria (redshift < 0.1, ≥100 epochs in ZTF DR24, known AGN classification) and the exact subsampling procedures (random contiguous baseline subsets of 1–2 yr; uniform downsampling to target cadences of 1, 3, and 5 days). These additions provide the requested quantitative rigor. revision: yes

standing simulated objections not resolved
  • We lack the necessary multi-survey or higher-redshift datasets to perform the suggested cross-checks within the present study.

Circularity Check

0 steps flagged

No circularity: purely empirical application of standard metrics to public data

full rationale

The paper computes the published Stetson J and smoothness s metrics on ZTF DR24 light curves for 23 nearby AGNs, then directly measures how those metric values change when baseline length, cadence, or host subtraction is varied. No new quantities are derived from fitted parameters, no target result is used to define the inputs, and no self-citation chain is invoked to justify uniqueness or an ansatz. All reported behaviors (J stable to ~10%, s varying >40%, J unchanged after host subtraction on Mrk 493) are observational outcomes, not tautological re-statements of the data selection or metric definitions. The analysis is therefore self-contained and externally falsifiable against the same public survey data.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The work is data-driven and introduces no new free parameters, invented entities, or ad-hoc assumptions beyond standard domain expectations that variability metrics applied to light curves can inform accretion physics.

axioms (1)
  • domain assumption Variability metrics J and s applied to AGN light curves reflect intrinsic accretion processes rather than purely observational artifacts
    Implicit in the abstract's framing that these metrics probe the physics of accretion onto supermassive black holes.

pith-pipeline@v0.9.0 · 5467 in / 1379 out tokens · 96502 ms · 2026-05-10T10:52:32.997492+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

8 extracted references · 8 canonical work pages

  1. [1]

    2016, SNCosmo: Python library for supernova cosmology, Astrophysics Source Code Library, record ascl:1611.017

    Barbary, K., Barclay, T., Biswas, R., et al. 2016, SNCosmo: Python library for supernova cosmology, Astrophysics Source Code Library, record ascl:1611.017. http://ascl.net/1611.017

  2. [2]

    C., Kulkarni, S

    Bellm, E. C., Kulkarni, S. R., Graham, M. J., et al. 2019, PASP, 131, 018002, doi: 10.1088/1538-3873/aaecbe

  3. [3]

    R., & Bloom, J

    Butler, N. R., & Bloom, J. S. 2011, AJ, 141, 93, doi: 10.1088/0004-6256/141/3/93 DESI Collaboration, Karim, M. A., Adame, A. G., et al. 2025, arXiv e-prints, arXiv:2503.14745, doi: 10.48550/arXiv.2503.14745

  4. [4]

    J., Djorgovski, S

    Drake, A. J., Djorgovski, S. G., Mahabal, A., et al. 2009, ApJ, 696, 870, doi: 10.1088/0004-637X/696/1/870

  5. [5]

    LSST: From Science Drivers to Reference Design and Anticipated Data Products , journal =

    Guo, H., Shen, Y., & Wang, S. 2018, PyQSOFit: Python code to fit the spectrum of quasars, Astrophysics Source Code Library, record ascl:1809.008. http://ascl.net/1809.008 Ivezi´ c,ˇZ., Kahn, S. M., Tyson, J. A., et al. 2019, ApJ, 873, 111, doi: 10.3847/1538-4357/ab042c

  6. [6]

    2024, ApJ, 966, 5, doi: 10.3847/1538-4357/ad34d6

    Ma, Q., Wen, Y., Wu, X.-B., Gu, H., & Fu, Y. 2024, ApJ, 966, 5, doi: 10.3847/1538-4357/ad34d6

  7. [7]

    L., Ivezi´ c,ˇZ., Sesar, B., et al

    MacLeod, C. L., Ivezi´ c,ˇZ., Sesar, B., et al. 2012, ApJ, 753, 106, doi: 10.1088/0004-637X/753/2/106

  8. [8]

    , keywords =

    Welch, D. L., & Stetson, P. B. 1993, AJ, 105, 1813, doi: 10.1086/116556 ZTF Team. 2025, ZTF Lightcurves, IPAC, doi: 10.26131/IRSA598