---
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---
## Inspect the claim, then choose a project
ASD connects spatial dynamics to recorded readouts by recalculating shared results, establishing experimental constraints and solving discriminating observables. These three entry points select work without changing any record's evidence status. Counts below come from the current experimental matrices and prediction registry, deduplicated separately by ID.
## Reproduced results
Chapter 1 calculations for Michelson–Morley and Sagnac, and Chapter 2 weak-field light deflection, Shapiro delay and perihelion advance, provide concrete routes from ASD constructions to classical observable relations. The [LVE matrix](/en/theory/lve/tests) and [gravity matrix](/en/tests/gravity) retain each configuration, equation and registered category.
REPRODUCED identifies a completed calculation of a shared result; REINTERPRETED identifies a reconstructed explanation. Neither category alone says that original observational data have been reanalysed. For the muon example, Eqs. (1.45)–(1.46) give $L=643\sqrt{999}\,\mathrm{m}\approx20323.3\,\mathrm{m}$. The inputs are approximate; this algebra is not a joint calculation of lifetime distributions, atmospheric production and detector acceptance. That task remains in the [muon workbench](/en/tests/muon-survival).
## Experimental constraints
A constraint connects model parameters, apparatus readouts, data and uncertainty. Inclusion here means a record is relevant to constraint research; a quantitative constraint requires that calculation to have been performed. The [directional-clock pilot](/en/research/clock-response-pilot) calculates a design matrix and identifiability for a specified geometry template. It neither predicts an ASD frequency-shift amplitude nor uses observational data.
Chapter 4 introduces common scale and three-dimensional directional deformation into the moving absorber's differential nuclear-transition response in a Mössbauer rotor. Approximately $0.69$ is a reported experimental coefficient cited by the manuscript; the associated material coefficient is inferred from it, not independently predicted as a universal constant. Independent material response, vibration and stress control, and a matched resonance comparison are required to turn the mechanism into a quantitative constraint. See [clocks and frequency standards](/en/theory/time/clocks-and-frequency) and [metrology](/en/theory/metrology).
## Priority discriminators
Priority identifies where to work. A closed discriminator specifies the apparatus observable $O$, $O_{\mathrm{ASD}}$, the comparison model's $O_{\mathrm{comparison}}$ and $\Delta O$, together with parameter sources, an error budget, systematic degeneracies and reproducible materials. A candidate without a calculated difference retains its registered status; speed, higher order and strong field do not themselves supply a nonzero prediction.
Ultrarelativistic transverse-wavefront coherence requires the phase or coherence residual after emission, propagation, reception and the frequency standard are treated together. The manuscript distinguishes common-scale phase cancellation, a fixed three-axis mapping and globally directed geometry. An ellipsoid diagram or transverse $\gamma$ factor alone does not calculate that residual. Strong-field higher-order deflection must first be checked within Chapter 2's chosen static exterior construction: where it has the Schwarzschild exterior form, higher-order expansion alone produces no difference. A difference requires an explicit, consistently applied additional physical input.
Chapter 5 also proposes directed-path and lattice-dispersion tests, composite-molecule interference with frozen internal states, causal establishment after ultrafast boundary switching, mixed gravitational-wave polarizations, and joint astrophysical dynamics and lensing. These connect to the existing [space-dynamics](/en/tests/space-dynamics), [quantum](/en/tests/quantum) and [gravity](/en/tests/gravity) matrices. Each apparatus calculation must use the appropriate effective level; the lattice fourth-order coefficient, for example, first requires the specific source-coefficient consistency check.
## Retain the module matrices
SI entries in [Metrology](/en/theory/metrology) are definition references, not experimental evidence for ASD. Module matrices retain their IDs, categories, evidence and readiness:
[LVE](/en/theory/lve/tests) · [Time](/en/theory/time/clocks-and-frequency) · [Dynamics](/en/theory/dynamics/tests) · [Gravity](/en/tests/gravity) · [Electromagnetism](/en/tests/electromagnetism) · [Space Dynamics](/en/tests/space-dynamics) · [Matter](/en/tests/matter) · [Quantum](/en/tests/quantum)
READY means a clearly scoped research task can begin. It means neither an independent prediction nor experimental confirmation.
## From candidate to experimental conclusion
Freeze the sources, equations, apparatus and inputs, then independently calculate the same readout and propagate theoretical, numerical and instrumental errors. Check whether calibration absorbs the proposed difference, then provide reviewable data processing, residuals and exclusion scope. [S301](/en/tests/case-studies/s301) remains DATA-GATED. [ASD Researcher](/en/researcher) can organize citations and research records; tool output does not replace the calculation or human review.