Compression & memory · Research & Algorithms

Recalibrate a physical model after the raw data is gone

A sensor’s first calibration need not be its last. A compact scientific record can retain enough evidence to revise a physical interpretation—without pretending it preserves every possible interpretation.

EXPLORE THE IDEA

Calibration can happen later

Retain the quantities needed by a declared physical model.

AI-generated editorial physical contextEditorial illustration
LATER MODEL QUERYA changed calibration parameterCandidate frequency 2.00Computed illustration; no new measurements
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AI-generated editorial oscillator bench with a computed candidate sinusoid. The slider changes frequency, not experimental calibration evidence. The retained-products mechanism and archived physical-memory results appear below.

Follow the information

From input to outcome

Capture retains products without deciding the final oscillator parameters. Query-time frequency, damping, gain and offset hypotheses supply the likelihood calculation under the stated observation model.

Scroll the diagram horizontally to follow the route. Keyboard: focus the diagram, then use the arrow keys.

Oscillator measurements → Accumulate lag products → Compact retained record → Model-dependent likelihood → Posterior on fixed grid. Capture retains products without deciding the final oscillator parameters. Query-time frequency, damping, gain and offset hypotheses supply the likelihood calculation under the stated observation model.
Information-flow map. Restricted synthetic reanalysis; assurance cost is accounted for separately. Original vector schematic based on the method and evidence discussed in this article; signal shapes and icons are illustrative, not additional measurements. Open full-size diagram ↗

Read the main route from left to right; labelled side branches show additional inputs, checks or feedback. The sections below explain the operations and their experimental limits.

The measurements stay the same. The interpretation changes.

Imagine discovering that a sensor’s gain was slightly wrong after its raw recording has been discarded. A stored parameter estimate cannot generally repair itself. A record of the right quadratic information can support more: rerun a specified likelihood under revised gain, offset, or physical parameters. The scientific freedom comes from retaining evidence rather than only a conclusion.

The capture device does not choose the final model

During capture, a ring buffer and balanced accumulators retain lag products, endpoints, energy, and a sum. They do not need to select the final oscillator frequency or damping. At query time, a proposed model supplies a finite-conditioning predictor; the summary evaluates its likelihood using those retained products. Gain and offset hypotheses can also be revisited under the stated observation model.

A second computation asks how much omitted long conditioning could change this record’s answer. It combines model contraction with retained record energy, then transfers the likelihood-error range to a posterior bound over the declared finite grid. This assurance path is much more expensive than ordinary evaluation.

Capture once, revisit the physical hypothesis
Capture once, revisit the physical hypothesis. Original scientific diagram; the stated component and information flow, not an additional experiment. Open full-size figure ↗

Correlations become a computational memory

Our example is a stationary noisy oscillator. The record retains lag products, its beginning and end, a sum, and observation metadata. A later model supplies the covariance and finite-history predictor. Expanding its residual squares reduces the likelihood calculation to those retained statistics. There is no attempt to reconstruct every interior sample.

Ck=∑t=kN−1yt yt−k\begin{gathered}C_k=\sum_{t=k}^{N-1}y_t\,y_{t-k}\end{gathered}
Lag products preserve quadratic relationships at specified delays. Boundary samples and metadata complete the finite-conditioning calculation.

The model is part of what gets stored

Regular sampling, stationary dynamics, and known independent noise after detector gain are essential assumptions. Changing when noise enters the measurement equation changes the likelihood. Allowing both unknown forcing amplitude and unknown gain also creates an identifiability problem. A small file does not make those scientific ambiguities disappear.

The storage benefit survives a credible comparison

On the longer synthetic records, the roughly 12.6 kB summary is at least 40 times smaller than tested lossless raw storage and closely matches exact Kalman inference on a fixed 1271-hypothesis grid. A larger ordinary parameter bank also passes and has faster warm queries. For short records, raw inference is faster overall. The result is a tradeoff, not universal dominance.

An answer and an assurance calculation are different products

The ordinary query is much cheaper than independently enclosing its numerical error. A separate audit bounds posterior discrepancies using only retained data and model calculations, passing all 96 short-panel cases. That audit takes approximately 66 minutes. Saving transmission or retention could justify such work, but the assurance cost belongs beside the attractive byte count.

Measured storage/accuracy tradeoff and the separate long-duration bound failure. The comparison is to the same discrete model’s inference, not to ground-truth scientific uncertainty.
Measured storage/accuracy tradeoff and the separate long-duration bound failure. The comparison is to the same discrete model’s inference, not to ground-truth scientific uncertainty.

An instrument that permits later reinterpretation

The potential application is a scientific instrument that keeps enough evidence for a defined later reinterpretation. It is not lossless recording, and the study does not yet establish real-instrument utility. Its contribution is a compact answerable question together with a computable limit on how much discarded history can matter.

What a future instrument would need

The experiment demonstrates restricted reanalysis on synthetic data, not a calibrated optical instrument or maintenance alarm. A real application must decide which future revisions matter and compare against simpler exact statistics for that actual model. The compelling possibility remains: retain enough evidence to change an interpretation later, while being explicit about the interpretations that are no longer available.

Evidence & further reading

The links below distinguish the project record from foundational literature. This revised story does not add a new application-validation experiment.

  1. Revisable physical memory with bounded inference error. Spline research archive (2026). Local archive snapshot.
  2. Long-stream physical-memory qualification: study 06. Spline research archive (2026). Local archive snapshot.
  3. Finite dependence is not finite conditional memory. Spline research archive (2026). Local archive snapshot.