Cosmological tensions and systematic cross-checks
Quantify a dated one-parameter discrepancy and design cross-checks that distinguish correlated errors, model dependence, and new-physics proposals.
On this page
The question for today
What you’ll understand
- Calculate a Gaussian difference statistic with explicit covariance assumptions.
- Distinguish a measured observable from a model-conditioned derived parameter.
- Propose cross-checks with genuinely different calibration or astrophysical dependencies.
A tension is a statement about the consistency of specified datasets within a specified statistical and physical model. It is not a separate force in nature, and its significance is not invariant under every allowed model extension or nuisance treatment. Comparing two reported Hubble rates offers a concrete example, provided their dates and assumptions remain visible. We will calculate a restricted Gaussian discrepancy, examine covariance effects, and explain how cross-checks can distinguish missing calibration, astrophysical modeling, statistical choices, and proposed changes to cosmology.
Compare the same parameter under compatible definitions
The Hubble rate inferred from microwave-background spectra is a derived parameter linking early-universe physical scales and angular geometry through an assumed cosmology. A local distance ladder instead links geometric anchors, stellar indicators, and standardized supernovae to nearby expansion. Both can estimate the present rate, but their calibration and model dependencies differ. Neither description means one route has no assumptions. The comparison must specify background geometry, early-time physics, data selections, and uncertainty conventions.
For a historical exercise, the Planck 2018 base flat Lambda cold-dark-matter analysis of temperature, polarization, and lensing reports H zero = 67.4 plus or minus 0.5 km per second per megaparsec. The SH0ES 2022 baseline Cepheid–supernova analysis reports 73.04 plus or minus 1.04 in the same units. These are explicitly dated primary results, not a claim about the latest consensus or every analysis variant. Their one-number summaries permit an instructive calculation while omitting information contained in full likelihoods and alternative calibrations.
Covariance and the tested question change the result
Shared calibration can correlate estimates. A common error with the same sign may cancel in their difference, so positive covariance reduces the difference variance; adding all common errors independently can actually understate that particular discrepancy. Other shared ingredients can create more complicated dependence, including data reused in an inverse distance ladder. One must derive the covariance from the measurement model instead of assuming that every systematic broadens every comparison in the same way.
Multidimensional consistency cannot generally be summarized by selecting the most discrepant one-dimensional parameter after examining many projections. A covariance-weighted difference tests a specified vector under a Gaussian approximation, while posterior-predictive checks test replicated observables and Bayesian evidence asks another question. Priors, parameter boundaries, non-Gaussian likelihoods, and scanning many models can invalidate a naive sigma interpretation. The statistic and the question it answers should travel together whenever a tension is quoted.
Design cross-checks around the suspected failure mode
A useful cross-check changes a vulnerable dependency while preserving enough shared information to diagnose it. Distance ladders can compare geometric anchors, stellar populations, crowding corrections, passbands, and supernova host matching. Independent distance methods introduce different astrophysical calibrations but still require their own selection and likelihood models. Microwave analyses can vary frequency, sky region, foreground treatment, polarization, and experiment. Internal splits are valuable even when they are correlated; their interpretation must use the appropriate split covariance.
A proposed early-time change that reduces the sound horizon may alter an inferred Hubble rate while also shifting acoustic phases, damping, abundances, or growth. A late-time expansion change must confront distance and clustering observations together. Matching one scalar summary is therefore not sufficient evidence for a complete explanation. Blinded choices, injection tests, reproducible likelihoods, and genuinely different observations help identify whether a discrepancy survives. We do not assert a resolution or an up-to-date significance; this lesson demonstrates a dated comparison and a method for evaluating future evidence.
Work it through
A dated, explicitly restricted Gaussian comparison
Use the dated Planck 2018 value 67.4 ± 0.5 and SH0ES 2022 baseline value 73.04 ± 1.04, both in km/s/Mpc. For this exercise approximate the two reported summaries as independent Gaussians. Compute the difference, its standard deviation, and Z diff. Explain the limits of this calculation.
The estimate difference is . The quantity compared is the same present Hubble parameter, although each route infers it with different modeling assumptions.
Independence gives difference variance in squared rate units. Its square root is approximately 1.1540 km/s/Mpc.
Thus . Rounding, full likelihood shapes, analysis variants, and a different comparison procedure can alter a quoted significance. This restricted calculation does not identify a cause or update the dated datasets.
The illustrative independent-Gaussian difference is 5.64 ± 1.154 km/s/Mpc, or about 4.89 standard deviations under the declared assumptions.
The living notebook
Explore the model
Interactive lab · waves
Addition and cancellation are different comparisons
Reset, set Phase difference = 0° and Amplitude ratio = 1, and predict a summed wave with amplitude two. For a fresh comparison Reset, set Phase difference = 180° and Amplitude ratio = 1, and predict cancellation of the sum. Inspect the components and combined curve at the same fresh clock time.
- Sum at x = 0
- 0.866
- Resultant amplitude
- 1.732
- Phase difference
- 60°
Two waves share the same frequency and wave number. Playback advances t in sin(2x − t) + a sin(2x − t + phase). Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.
Look forEqual-frequency deterministic waves illustrate how a common contribution may add or cancel. They do not generate correlated measurement errors, a covariance estimate, a cosmological likelihood, or a significance calculation.
Pause & reason
Check your understanding
Your turn
Try it yourself
Two synthetic Gaussian estimates of a common rate are 70 ± 2 and 74 ± 2 in common units. Their covariance is 3 square units. Compute the difference variance and discrepancy statistic. Compare with treating them as independent and explain the direction of the change.
Take a moment to make a prediction or work it out on paper. Open a hint when you need one.
Give me a hint
Subtract twice the covariance when forming the variance of a difference. The supplied correlation is 3/4 and is physically allowed.
Compare with the solution
The difference is 4 units and its variance is square units, so . Ignoring covariance gives variance 8 and . Positive same-sign common uncertainty partially cancels in a difference, explaining the larger correlated-comparison statistic. This synthetic covariance is not assigned to the historical pair in the worked example.
Keep the idea
Take it with you
- A tension is conditional on datasets, models, and a specified statistical comparison.
- Shared uncertainty can cancel in a difference and must be modeled explicitly.
- A proposed resolution must survive complementary observables and calibration cross-checks.
Read further
Original sources and deeper explanations to follow at your own pace.
Optional progress, saved in this browser when available. Revisit any lesson at any time.
Lesson not marked complete.