SciPost Submission Page
Field-level inference in cosmology
by Florent Leclercq
Submission summary
| Authors (as registered SciPost users): | Florent Leclercq |
| Submission information | |
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| Preprint Link: | scipost_202509_00020v1 (pdf) |
| Date submitted: | Sept. 8, 2025, 9:23 p.m. |
| Submitted by: | Leclercq, Florent |
| Submitted to: | SciPost Physics Lecture Notes |
| for consideration in Collection: |
| Ontological classification | |
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| Academic field: | Physics |
| Specialties: |
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| Approach: | Computational |
The author(s) disclose that the following generative AI tools have been used in the preparation of this submission:
As a language editor (only).
Abstract
These lecture notes delve into field-level inference, a framework offering a robust way to extract more information and avoid biases compared to traditional methods for cosmological data analysis. The core idea is to analyse uncompressed maps to infer underlying physical fields and cosmological parameters. We introduce Bayesian hierarchical field-level models and discuss sampling techniques for exploring complex, high-dimensional posterior distributions. We review the framework that underpins field-level inference. Finally, we highlight some state-of-the-art applications across various cosmological probes, and the growing role of machine learning in enhancing field-level inference capabilities.
Current status:
Reports on this Submission
Report #1 by Nicolas Cerardi (Referee 1) on 2025-10-3 (Invited Report)
The referee discloses that the following generative AI tools have been used in the preparation of this report:
Generative AI was used on a few sentences for language edition.
Report
Minor comments
Section 1.1. From my understanding, forward modelling can also be a source of bias (e.g. selection effects in building the mock catalogues, or loss of power at small scales due to CDM simulation methods). It is therefore not only backward modelling that may introduce bias. Is it considered subdominant with respect to the biases from backward modelling, or do you assume an ideal bias-free forward model (e.g. one that includes all relevant physics from structure formation to observation)?
Section 1.2. You state that “any method that involves compression of the map-level data is not included”. However, in Section 1.1 you defined field-level inference as the method that uses the “full mock and observed catalogues”. This is a bit unclear to me: a catalogue isn’t already a compressed representation of the observed field? Can you clarify whether catalogues are included in your definition?
Section 2.1, line 127. Could you explain why the equation to retrieve C is not recursive?
Figure 2 (and related text). Is there a way to compute burn-in length from the samples, or is it always a visual estimate? How is this handled when dealing with hundreds or more parameters? Also, it would be useful to indicate in the legend that different colors correspond to different chains.
Section 5.2. Maybe you could expand on why we usually know the conditionals for cosmological applications of Gibbs sampling?
Recommendation
Ask for minor revision
