ASTR 410 · Lecture 12

Lecture 12: Inference with Galactic Surveys

Galactic Astronomy

Survey astronomy is an inverse problem: the catalogue is filtered by the instrument and by the scientist's cuts.

Objectives and route

Why this question is hard

Survey astronomy is an inverse problem: the catalogue is filtered by the instrument and by the scientist's cuts.

Galactic astronomy observes projected light, velocities, and abundances from one moving vantage point. The inverse problem is underdetermined until geometry, selection, and a physical model are made explicit.

datamodelposteriorp(theta|D)
Inference Triangle: a lecture-specific schematic or model plot. Axes and annotations identify the inference being made; it is not presented as a raw survey image.

Terms for This Lecture

Likelihood

Definition: A model for the probability of the observed data as a function of parameters, \(p(D|\theta)\).

Why it matters here: It encodes the measurement uncertainties used to compare Galactic models with survey data.

Relationship: For independent Gaussian rotation points it is related to a chi-square residual sum.

Limitation or common confusion: A convenient likelihood can be precise yet wrong if errors are correlated or non-Gaussian.

Physical tool

The central relation for this lecture is:

\(p(\theta|D)\propto p(D|\theta)p(\theta)\)

Define every symbol before substitution. State the coordinate system, units, and approximation. A formula is evidence only when its assumptions match the tracer and regime.

Evidence display

The evidence display for this lecture is the labeled model/data relationship introduced above. Read the axes and annotations before accepting the inferred trend.

Data context: the accompanying values are standard published or survey-like values; see the course reference log for provenance level and spot-check targets.

Worked calculation

A flat 232 km s^-1 model has chi^2 = 24.891 for the seven listed points when each uncertainty is 8 km s^-1.

A chi-square comparison needs a stated number of fitted parameters and a justified error model.

Write the units beside each intermediate quantity. The numerical result is generated from the shared course constants and recomputed independently during review.

Interpret the pattern

Boundary condition and misconception

Do not overread the model: A precise posterior can still be wrong when the selection function or likelihood is misspecified.

Ask whether changing the distance prior, selection function, or mass decomposition could move the conclusion. This is where a plausible diagram can become a misleading argument.

In-class reasoning

Prompt: Construct a simple likelihood for rotation-curve points with 8 km s^-1 errors and compare two models.

First estimate the direction of the answer. Then calculate. Finally name one assumption that could reverse the interpretation.

Connection across the course

Takeaways

References and data status

OpenStax Astronomy 2e, Chapter 25, sections 25.1–25.4, and Chapter 26 for comparative context. Exact section and embedded-figure offsets were checked against the local extracted text before release.

Additional sources: Gaia Collaboration (2018, 2021) releases; Bland-Hawthorn & Gerhard (2016), ARA&A 54, 529; McMillan (2017), MNRAS 465, 76; Eilers et al. (2019), ApJ 871, 120; Bland-Hawthorn et al. (2019), Science 365, 859.

References are standard published values not independently re-fetched in this production session unless explicitly marked level 1 in reference-log.md.