GHU Lab

Hypotheses: local response and experimental context

Compare nine recalibrated GHU benchmarks and inspect a separate CMS spectrum with its covariance. Each selection includes a reading of the calculated values and their scope.

Control names are kept as they appear in the application. Start with a reference, change one input at a time, and retain the assumptions with your result.

What this tool is for

Distinguish changes in model parameters, local couplings, full-field potential differences and experimental error structure. Theory and CMS are separate contexts until a compatible prediction exists.

First steps

  1. Open Same potential? and use the jump button for Hypotheses. Press Demo for the real-control walkthrough.
  2. Choose cases 1 and 6. Read the recalibrated coupling changes, then expand the potential interval.
  3. Choose CMS intervals i and j. Inspect the measured value, marginal error and signed correlation.
  4. Export the selected SVG, full JSON or observed CSV. Import the JSON to restore a validated selection.
  5. Open Certificates. Read each claim and its scope, then download its JSON or the existing catalogue ZIP.

Controls and inputs

ControlMeaningTry this
GHU caseOne of nine fixed recalibrated cases; changing the case may change multiple inputs and field multiplicities.Compare cases 1 and 6.
Potential intervalField θ in 0.06–0.14 or 0–π. The vacuum θH remains fixed at 0.1.Switch regions and read the vertical exponent.
CMS intervals i and jSelect one measured bin and a second bin for their experimental correlation.Set i=j, then select different intervals.

Reading the results

ResultMeaning
Four linked figuresParameter scatter and potential difference share the theory selection. Measured error bars and covariance-derived correlations share the CMS selection.
Downloads and importsJSON preserves provenance, full covariance and theory samples. SVG is standalone; CSV contains observed bins. Import restores inputs, not an external dataset or imported verdict.
Scoped certificatesTen rational Lean identities, exact covariance witnesses and three pointwise derivative enclosures. Full-integral error and observed-fit certification remain pending.

Read axes, units and source before comparing panels. Small coupling changes after recalibration do not establish experimental indistinguishability. The potential scale is fixed across cases within a region, and changes when the region changes.

Worked example

Follow the interactive demo

  1. Open Same potential? and use the jump button for Hypotheses. Press Demo for the real-control walkthrough.
  2. Choose cases 1 and 6. Read the recalibrated coupling changes, then expand the potential interval.
  3. Choose CMS intervals i and j. Inspect the measured value, marginal error and signed correlation.
  4. Export the selected SVG, full JSON or observed CSV. Import the JSON to restore a validated selection.
  5. Open Certificates. Read each claim and its scope, then download its JSON or the existing catalogue ZIP.

What to expect: The demo ends with separate theoretical and experimental readings. It never assigns an exclusion to the nine benchmarks.

Scope and limitations

  • Dominant-tower reconstruction, bottom omitted, physical uncertainty unquantified. The browser reads archived calculations; it does not rerun the Bessel integrals.
  • This study is independent of the exact SU(7) equivalence theorem in its host section. Its video chapter and interactive Demo share the same practical walkthrough.
  • No observed GHU fit or full physical certification is provided. A covariance alone does not supply a compatible theory prediction.
  • The about 7.4% quartic fit/table discrepancy is unresolved. Quadrature convergence is not a rigorous total error bound.

If something is unclear

The selected curve is zero.

Case 1 is compared with itself. Select another case.

Import is rejected.

Use this card’s JSON export with valid integer selections. Unrelated datasets require a separate audited adapter.

Sources and attribution

Current instrument guide. Archived editions retain their own scope.

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