Motivation
Recovering a single relaxation law (e.g. Omori) from a memory kernel is consistency, not validation. By Bernstein’s theorem, a completely monotone kernel can represent essentially any relaxation curve, so matching one exponent constrains nothing.
A genuine test must be selective: it must relate two independently measured quantities in a way the theory forces.
Here, the candidate selective structure is the constitutive law
$$
K = \psi(G^{-1}F),
$$
linking:
-
information geometry (via $G^{-1}F$), and
-
coherence loss (via the generator $K$),
with $\psi$ a constitutive function (e.g. $\psi(\lambda)=\kappa/\lambda$, $\psi(\lambda)=\kappa/\lambda^p$, etc.).
Open question
Part 1 — Theory
-
Goal: Derive a fluctuation–dissipation cross‑exponent relation for the linear‑stochastic model that links:
- the memory‑kernel decay (from the dissipative part $K(\tau)$), and
- the fluctuation spectrum of the residual force $\langle F(t)F(s)^\top\rangle$ (from the null covariance),
under a constitutive law $K = \psi(G^{-1}F)$.
-
Task: Reduce this to a checkable relation between:
- a relaxation exponent (coherence‑loss / kernel decay), and
- an independently measurable fluctuation exponent (information content / residual‑force spectrum),
with explicit dependence on $\psi$ (e.g. $\psi(\lambda)=\kappa/\lambda$, $\psi(\lambda)=\kappa/\lambda^p$).
Part 2 — Data
Deliverables
-
Theory:
-
Sharp statement of the cross‑exponent relation for the linear model, explicitly showing how $\psi$ constrains the relation between relaxation and fluctuation exponents.
-
Constitutive‑law analysis: which choices of $\psi$ (e.g. $\kappa/\lambda$, $\kappa/\lambda^p$) are compatible with the derived relation.
-
Protocol:
-
Preregistered test protocol:
- what is measured (coherence‑loss exponent, fluctuation exponent),
- tolerance bands,
- null hypothesis (e.g. “no fixed relation between exponents”),
- thresholds fixed before looking at outcomes.
-
Data:
- Application to ≥ 1 real dataset, with:
- relaxation exponent estimated independently,
- fluctuation exponent estimated independently,
- constitutive prediction computed from $\psi$.
-
Verdict:
- Clear statement:
-
support: relation holds within preregistered tolerance → experimental support for the chosen constitutive law $K = \psi(G^{-1}F)$;
-
refutation: relation fails → the linear‑stochastic modelling or the specific $\psi$ is ruled out for that system.
Definition of done
A report containing:
- the derived cross‑exponent relation (theoretical part),
- the preregistered protocol (measurement and thresholds),
- at least one honest data confrontation (real system),
- a clear verdict on whether the constitutive law $K = \psi(G^{-1}F)$ is experimentally supported or refuted for that system.
Honesty requirements
- Calibration assumptions: State all calibration and baseline assumptions explicitly (e.g. null‑baseline condition from Pillar 1, stationarity assumptions, noise model).
- Negative results: Report negative results in full; a clean refutation of a constitutive law or of the linear‑stochastic model is a first‑class outcome.
- No fake confirmation: Do not present mere consistency (a fitted power law or a post‑hoc exponent match) as confirmation. Only preregistered, cross‑exponent agreement counts as support.
Contributor profile
- Theory: Statistical physics, information geometry, operator theory, control theory.
- Data: Time‑series analysis, experimental data analysis, seismology / condensed matter / electrical circuits / relaxation phenomena.
Motivation
Recovering a single relaxation law (e.g. Omori) from a memory kernel is consistency, not validation. By Bernstein’s theorem, a completely monotone kernel can represent essentially any relaxation curve, so matching one exponent constrains nothing.
A genuine test must be selective: it must relate two independently measured quantities in a way the theory forces.
Here, the candidate selective structure is the constitutive law
linking:
with$\psi$ a constitutive function (e.g. $\psi(\lambda)=\kappa/\lambda$ , $\psi(\lambda)=\kappa/\lambda^p$ , etc.).
Open question
Part 1 — Theory
Goal: Derive a fluctuation–dissipation cross‑exponent relation for the linear‑stochastic model that links:
under a constitutive law$K = \psi(G^{-1}F)$ .
Task: Reduce this to a checkable relation between:
with explicit dependence on$\psi$ (e.g. $\psi(\lambda)=\kappa/\lambda$ , $\psi(\lambda)=\kappa/\lambda^p$ ).
Part 2 — Data
Goal: Test the derived cross‑exponent relation on a real relaxation system where both exponents are separately measurable.
Candidate systems:
Task: Measure:
and compare:
Deliverables
Theory:
Protocol:
Data:
Verdict:
Definition of done
A report containing:
Honesty requirements
Contributor profile